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Crystallography: Current Research Articles


 
Current research articles in the field of crystallography and crystall chemistry published in online journals.

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On this page considered biochemistry journals:


Crystal Research and Technology - published by Wiley-Interscience -
... is an international journal examining all aspects of research within experimental, industrial, and theoretical crystallography.

CrystEngComm - published by The Royal Society of Chemistry -
... has established itself as THE journal in which to publish cutting-edge crystal engineering research.

Journal of Chemical Crystallography - published by Springer -
... is an international and interdisciplinary publication dedicated to the rapid dissemination of research results in the general areas of crystallography and spectroscopy.

Crystallography Reports - published by Springer -
... publishes original papers, short communications, and reviews on different aspects of crystallography.



Current research articles of the mentioned journals:


Crystallization of unidirectionally oriented fibrous calcium carbonate on thermo-responsive polymer brush matrices

Surjith Kumar, Takahiro Ito, Yuki Yanagihara, Yuya Oaki, Tatsuya Nishimura, Takashi Kato
(Communication from CrystEngComm)
Surjith Kumar, CrystEngComm, 2010, DOI: 10.1039/b923049a
To cite this article before page numbers are assigned, use the DOI form of citation above.
The content of this RSS Feed (c) The Royal Society of Chemistry

Source: RSC - CrystEngComm latest articles | 20 Mar 2010 | 12:00 am CET

A new Cu(i) coordination polymer with the CdSO4 structure type prepared via biphasic solvothermal reaction

Tuoping Hu, Haiyan He, Fangna Dai, Xiaoliang Zhao, Daofeng Sun
(Communication from CrystEngComm)
Tuoping Hu, CrystEngComm, 2010, DOI: 10.1039/b919342c
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The content of this RSS Feed (c) The Royal Society of Chemistry

Source: RSC - CrystEngComm latest articles | 20 Mar 2010 | 12:00 am CET

High-quality LaCoO3 single crystal grown by optical floating zone method and its electromagnetic properties

A LaCoO3 single crystal with 4 mm in diameter and 30 mm in length has been grown by optical floating zone method. The as-grown crystal is highly crystalline with the rhombohedral perovskite structure (R3c) and grows parallel to the (121) direction. The room temperature resistivity of the as-grown crystal is 0.12 [Omega]·cm and the insulator-metal transition occurs around 500 K. The coercivity and the remanence of the as-grown crystal are 5 Oe and 6.61×10-5 [mu]B/f.u. at 5 K, respectively. In 1000 Oe under zero-field cooling, the magnetic susceptibility of the as-grown crystal shows an upturn in a Curie tail fashion below 35 K, and appears a wave crest over the interval 55 K[le]T[le]90 K. In addition, a slope change of 1/[chi](T) at about 12 K is observed in 50000 Oe under zero-field cooling. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 19 Mar 2010 | 2:22 pm CET

Effect of temperature programmes on protein crystallisation

Varying the temperature has been proven to be beneficial for improving the screening efficiency of protein crystallisation, and thus a crystallisation screening strategy based on this phenomenon can be developed. Such a temperature varying strategy can be applied in practical crystallisation screening, however, there are no guidelines for determining what temperature programme should be utilised. It is therefore necessary to investigate how the temperature programme affects the crystallisation process, so as to help people design a suitable temperature programme. For this purpose, we investigated the effect of temperature programmes on the protein crystallisation (lysozyme, proteinase K, and concanavalin A) that are characterised by different solubility behaviours with respect to temperature. Judging from the reproducibility studies of protein crystallisation with different temperature programmes, we recommend using linear temperature programmes for a moderate time period (24 to 48 h) and a large temperature range according to the properties of the proteins. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 19 Mar 2010 | 2:22 pm CET

Malic acid assisted precursor route to hierarchical structured nickel oxide

A novel malic acid assisted precursor route to prepare NiO materials with novel hierarchical structures has been investigated in this work. The Ni-based precursors can be synthesized by a malic acid-assisted hydrothermal route, which have been characterized by powder X-ray diffraction (XRD), field-emission scanning electron microscopy (FE-SEM), thermogravimetric analysis (TGA). NiO materials can be prepared via the thermal treatment of the precursor in ambient atmosphere. The XRD, SEM, Energy dispersive X-ray spectroscopy (EDS) and UV-Vis spectroscopy of the NiO materials were also examined. The effects of the reaction conditions, such as the reaction temperature, the quantity of the raw materials on the morphologies of the precursors were discussed, which indicates that it is an effective method to synthesize NiO materials with different hierarchical structures. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 19 Mar 2010 | 2:22 pm CET

C-HF-C hydrogen bonding in 1,2,3,5-tetrafluorobenzene and other fluoroaromatic compounds and the crystal structure of alloxan revisited

Tejender S. Thakur, Michael T. Kirchner, Dieter Blaser, Roland Boese, Gautam R. Desiraju
(Paper from CrystEngComm)
Tejender S. Thakur, CrystEngComm, 2010, DOI: 10.1039/b925082d
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The content of this RSS Feed (c) The Royal Society of Chemistry

Source: RSC - CrystEngComm latest articles | 17 Mar 2010 | 12:00 am CET

Combination of hydrogen and coordination bonding for the construction of one-dimensional networks based on a 7-azaindole appended dipyrrin

Dmitry Pogozhev, Stephane A. Baudron, Mir Wais Hosseini
(Paper from CrystEngComm)
Dmitry Pogozhev, CrystEngComm, 2010, DOI: 10.1039/b927348d
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The content of this RSS Feed (c) The Royal Society of Chemistry

Source: RSC - CrystEngComm latest articles | 17 Mar 2010 | 12:00 am CET

Nanoporous metal-organic framework comprising of 1D cobalt oxalate chains and flexible ligands exhibiting both dynamic gas adsorption and antiferromagnetic chain behaviours

Hong-Qing Hao, Zhuo-Jia Lin, Sheng Hu, Wen-Ting Liu, Yan-Zhen Zheng, Ming-Liang Tong
(Paper from CrystEngComm)
Hong-Qing Hao, CrystEngComm, 2010, DOI: 10.1039/b927200c
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The content of this RSS Feed (c) The Royal Society of Chemistry

Source: RSC - CrystEngComm latest articles | 15 Mar 2010 | 12:00 am CET

Synthesis of CuO nano- and micro-structures and their Raman spectroscopic studies

Wenzhong Wang, Qing Zhou, Xiangmin Fei, Yingbo He, Pengcheng Zhang, Guling Zhang, Lei Peng, Wenjuan Xie
(Paper from CrystEngComm)
Wenzhong Wang, CrystEngComm, 2010, DOI: 10.1039/b919043k
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The content of this RSS Feed (c) The Royal Society of Chemistry

Source: RSC - CrystEngComm latest articles | 15 Mar 2010 | 12:00 am CET

Synthesis and Crystal Structure of Bis (N,N,N′,N′-tetramethylethylendiammonium) Octaiodo Pentachloroantimonate (III)

Abstract  
The synthesis and Crystal structure are given for the bis (N,N,N′,N′-tetramethylethylendiammonium) octaiodo pentachloroantimonate (III) salt. An X-ray investigation has shown that the title compound crystallizes in a monoclinic system, space group P21/m with the following lattice parameters a = 9.786(2) Ǻ, b = 14.024(5) Ǻ, c = 14.336(3) Ǻ, β = 91.35(2)° and Z = 2. The structure was solved from 3085 independent reflections with R 1 = 0.0402 and wR 2 = 0.0952 and refined with 152 parameters. The structure shows a layer arrangement perpendicular to the
®
b
 
-axis: planes of [SbCl5]2−, I3 and I5 anions alternate with planes of [(CH2)2(NH(CH3)2)2]2+ cations. The [SbCl5]2− square pyramids present an active lone electron pair (LEP) on the Sb atoms and they are interconnected by means of N–H···Cl hydrogen bond originating from [(CH2)2(NH(CH3)2)2]2+ entities. The polyiodides (I3 and I5 ) anions form a planer zigzag polymeric chains via I···I linking interactions. These chains are linked to the [SbCl5]2− anions by a long range contact.
Index Abstract  
Built for [(CH2)2(NH(CH3)2)2]2+ entities, [SbCl5]2−, I3 and I5 anions.
MediaObjects/10870_2010_9725_Figa_HTML.gif

  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9725-7
  • Authors
    • H. Kharrat, Unité de Recherche de Chimie Industrielle et Matériaux, ENIS BP 1173 Sfax Tunisia
    • S. Kamoun, Unité de Recherche de Chimie Industrielle et Matériaux, ENIS BP 1173 Sfax Tunisia
    • H. F. Ayedi, Unité de Recherche de Chimie Industrielle et Matériaux, ENIS BP 1173 Sfax Tunisia
    • A. Driss, Université de Tunis-El Manar Laboratoire de Matériaux et Cristallochimie, Faculté des Sciences 2092 Tunis Tunisia

Source: Journal of Chemical Crystallography | 14 Mar 2010 | 12:27 pm CET

Spectroscopic Studies and Crystal Structure of 4-(2-Hydroxy-3-Methoxybenzylideneamino)-N-(5-Methylisoxazol-3-yl) Benzenesulfonamide

Abstract  
Schiff base 4-[(2-hydroxy-3-methoxybenzylideneamino)-N-(5-methylisoxazol-3-yl)benzene-sulfonamide has been synthesized from the reaction of 4-amino-N-(5-methylisoxazol-3-yl)benzenesulfonamide(sulfamethoxazole) with 2-hydroxy-3-methoxybenzaldehyde. It has been characterized by elemental analysis, MS, IR, 1H NMR, 13C NMR, HETCOR and UV–Visible techniques. The structure of it also has been examined crystallographically. For the compound exist as dominant form of enol-imines in both the solid state and the solutions. It crystallizes in the monoclinic space group P21/c with a = 8.2694(7), b = 8.3453(5), c = 26.260(2) Å, β = 97.142(7) °, V = 1798.1(2) Å3, D x  = 1.431 g cm−3, R 1 = 0.0529 and wR 2 = 0.1370 [I > 2σ(I)], respectively.
Index Abstract  
The tautomerism in the Schiff base ligands plays an important role for distinguishing their photochromic and thermochromic characteristics. Both phenomena is associated with a proton transfer (enol-imine, O–H···N, keto-amine, O···H–N).
MediaObjects/10870_2010_9723_Figa_HTML.gif

  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9723-9
  • Authors
    • Mustafa Yıldız, Çanakkale Onsekiz Mart University Department of Chemistry, Faculty of Science and Arts 17100 Çanakkale Turkey
    • Hüseyin Ünver, Ankara University Department of Physics, Faculty of Science 06100 Tandoğan, Ankara Turkey
    • Diğdem Erdener, Çanakkale Onsekiz Mart University Department of Chemistry, Faculty of Science and Arts 17100 Çanakkale Turkey
    • Nazan Ocak İskeleli, Ondokuz Mayıs University Department of Physics, Faculty of Science and Arts 55139 Kurupelit, Samsun Turkey

Source: Journal of Chemical Crystallography | 14 Mar 2010 | 12:27 pm CET

Synthesis and X-Ray Crystallographic Analysis of 2-(2, 4-Dimethyl Pyrrolyl) Benzothiazole

Abstract  
Synthesis of 2- (2, 4-dimethyl pyrrolyl) benzothiazole by chemical means and molecular structure by X-ray crystallographic techniques is reported. The compound crystallizes in the orthorhombic crystal system with space group Pbca and unit cell parameters: a = 12.161(9), b = 0.787(1), c = 16.792(2) Ǻ, V = 2202.8(4) Ǻ3 and Z = 8. The final reliability index is 0.073 for 7,959 observed reflections. The benzothiazole and pyrrole rings exist in planar conformations. The dihedral angle between the least-squares planes of both these moieties is 13.31°. There exists an isolated C4–H4···N1 intermolecular interaction, besides two C–H···S and C–H···N intermolecular interactions. The presence of C–H···S and C–H···N intramolecular interactions make the present molecule look like a virtual two-six-membered and three-five-membered ring structure.
Graphical Abstract  
Synthesis of 2- (2, 4-dimethyl pyrrolyl) benzothiazole by chemical means and molecular structure by X-ray crystallographic techniques is reported. The compound crystallizes in the orthorhombic crystal system with space group Pbca and unit cell parameters: a = 12.161(9), b = 0.787(1), c = 16.792(2) Ǻ, V = 2202.8(4) Ǻ3 and Z = 8. The final reliability index is 0.073 for 7,959 observed reflections. The benzothiazole and pyrrole rings exist in planar conformations. The dihedral angle between the least-squares planes of both these moieties is 13.31°. There exists an isolated C4–H4···N1 intermolecular interaction, besides two C–H···S and C–H···N intermolecular interactions. The presence of C–H···S and C–H···N intramolecular interactions make the present molecule look like a virtual two-six-membered and three-five-membered ring structure.
MediaObjects/10870_2010_9734_Figa_HTML.gif
Chemical structure of 2-(2, 4-dimethyl pyrrolyl) benzothiazole

  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9734-6
  • Authors
    • Rajnikant, University of Jammu X-ray Crystallography Laboratory, Department of Physics Jammu Tawi 180006 India
    • Sabeta Kohli, University of Jammu X-ray Crystallography Laboratory, Department of Physics Jammu Tawi 180006 India
    • M. B. Deshmukh, Shivaji University Department of Chemistry Kolhapur 416004 India
    • Kamni, Shri Mata Vaishno Devi University College of Sciences Udhampur Jammu and Kashmir 182301 India

Source: Journal of Chemical Crystallography | 11 Mar 2010 | 3:46 am CET

Structure of 2-[(Phenyl)-(3,5-Dimethyl-Pyrazol-1-yl)-Methyl]-Malonic Acid Diethyl Ester

Abstract  
The titled new functionalized ligand of type 2-[(phenyl)-(3,5-dimethyl-pyrazol-1-yl)-methyl]-malonic acid diethyl ester (4) is prepared in good yield through condensation of 3,5-dimethyl-pyrazole, with 2-arylidene-malonic acid diethyl esters 3. The structure of 4 was determined by spectral (IR, 1H and 13C NMR), elemental analyses and X-ray diffraction data. The title compound (4) crystallizes in the monoclinic space group P21/a, with a = 7.9253 (2), b = 17.1299 (5), c = 13.4522 (4) Å, β = 90.220 (2)°, V = 1,826.25 (9) Å3, Z = 4 and with R int = 0.021. The molecular conformation shows two possible pockets ready to coordinate two metal atoms. The crystal structure of (4) is stabilized by inter-molecular C–H⋯O and C–H⋯N hydrogen bonding.
Graphical Abstract  
[Structure of 2-[(phenyl)-(3,5-dimethyl-pyrazol-1-yl)-methyl]-malonic acid diethyl ester. I. Meskini, L. Toupet,* M. Daoudi, A. Kerbal, M. Akkurt,* Z. H. Chohan and T. Ben Hadda* The molecular conformation shows two possible pockets ready to coordinate two metal atoms. The crystal structure of (4) is stabilized by inter-molecular C–H⋯O and C–H⋯N hydrogen bonding interactions] -->
MediaObjects/10870_2010_9743_Figa_HTML.gif
.

  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9743-5
  • Authors
    • I. Meskini, Université Sidi Mohammed Ben Abdellah Laboratoire de Chimie Organique Fès Morocco
    • L. Toupet, Université de Rennes 1 Institut de Physique—IPR—UMR CNRS 6251 Rennes France
    • M. Daoudi, Université Sidi Mohammed Ben Abdellah Laboratoire de Chimie Organique Fès Morocco
    • A. Kerbal, Université Sidi Mohammed Ben Abdellah Laboratoire de Chimie Organique Fès Morocco
    • M. Akkurt, Erciyes University Department of Physics, F.A.S 38039 Kayseri Turkey
    • Z. H. Chohan, Bahauddin Zakariya University Department of Chemistry Multan Pakistan
    • T. Ben Hadda, Université Mohammed Premir Laboratoire de Chimie des Matériaux 60000 Oujda Morocco

Source: Journal of Chemical Crystallography | 10 Mar 2010 | 1:50 pm CET

Structural Studies of (Pyridine)3ZnFe(CO)4 and (Pyridine)(Neocuproin)CdFe(CO)4

Abstract  
The structure of the previously reported (py)3ZnFe(CO)4 (py = pyridine) has been determined, confirming the monomeric nature of this species. The complex has average Zn–N and Zn–Fe bond lengths of 2.0970(7) and 2.4017(3) Å, and features a coordination geometry about Fe which is intermediate between trigonal bipyramidal and face monocapped tetrahedral. The space group is P21/c, with a = 8.22080(10) Å, b = 16.1668(3) Å, c = 15.4669(3) Å, β = 102.5869(11)°, V = 2006.21(6) Å3, Dcalc. = 1.558 g/cm3 at 150(1) K. A monomeric cadmium analogue, (pyridine)(neocuproin)CdFe(CO)4, has also been synthesized, and found to possess a similar geometry, with average Cd–N and Cd–Fe bond lengths of 2.352(2) and 2.5380(5) Å. The space group is
P

1
 
with a = 10.8900(2) Å, b = 11.3042(3) Å, c = 15.5488(4) Å, α = 85.1251(10)°, β = 84.3468(14)°, γ = 72.0377(15)°, V = 1808.93(7) Å3, Dcalc. = 1.478 g/cm3 at 150(1) K.
Graphical Abstract  
The structures of the monomeric (py)3ZnFe(CO)4 and (py)(neocuproin)CdFe(CO)4 complexes have been determined, and suggest the use of significantly greater s character in the main group elements’ bonds with iron as opposed to nitrogen.
MediaObjects/10870_2010_9736_Figa_HTML.gif

  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9736-4
  • Authors
    • Brian E. Zaugg, University of Utah Department of Chemistry 315 South 1400 East, Room 2020 Salt Lake City UT 84112-0850 USA
    • Torsten Kolb, University of Utah Department of Chemistry 315 South 1400 East, Room 2020 Salt Lake City UT 84112-0850 USA
    • Atta M. Arif, University of Utah Department of Chemistry 315 South 1400 East, Room 2020 Salt Lake City UT 84112-0850 USA
    • Richard D. Ernst, University of Utah Department of Chemistry 315 South 1400 East, Room 2020 Salt Lake City UT 84112-0850 USA

Source: Journal of Chemical Crystallography | 10 Mar 2010 | 1:50 pm CET

Structural Studies of the Coupling Products Between (C6H5)CH=NR (R = C6H5, i-C3H7) and the Ti(C5H5)(2,4-C7H11) Fragment (C7H11 = dimethylpentadienyl)

Abstract  
The reactions of imines of the formula (C6H5)CH=NR (R = C6H5, i-C3H7) with Ti(C5H5)(2,4-C7H11)(PMe3) (C7H11 = dimethylpentadienyl) lead to expulsion of the PMe3 and coupling between the imine’s carbon atom and a single terminus of the 2,4-C7H11 ligand, resulting in C5H5, “diene,” and π-amide coordination in the 16 electron products. Examination of the Ti–C and C–C bonding parameters for the “diene” ligands reveals that they may be more appropriately regarded as enediyl ligands, leading to a formal +4 oxidation state for titanium. Both complexes crystallize in the triclinic space group
P

1
 
. For the R = C6H5 coupling product, a = 10.4590(2) Å, b = 11.6407(2) Å, c = 17.3729(3) Å, α = 74.7610(7)°, β = 79.8600(6)°, γ = 82.2895(11)°, V = 2000.28(6) Å3, D calc = 1.293 g/cm3 at 150(1) K. For the R = i-C3H7 coupling product, a = 8.1039(2) Å, b = 9.4115(2) Å, c = 13.0116(4) Å, α = 88.9906(18)°, β = 73.2780(15)°, γ = 83.3088(16)°, V = 943.82(4) Å3, D calc = 1.250 g/cm3 at 150(1) K.
Graphical Abstract  
Structural studies of the coupling products between imines and the Ti(C5H5)(2,4-C7H11) (C7H11 = dimethylpentadienyl) fragment reveal significant shortening of the Ti–N bond when a more electron donating substituent is present on the nitrogen center.
MediaObjects/10870_2010_9737_Figa_HTML.gif

  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9737-3
  • Authors
    • Benjamin G. Harvey, University of Utah Department of Chemistry 315 South 1400 East, Room 2020 Salt Lake City UT 84112-0850 USA
    • Atta M. Arif, University of Utah Department of Chemistry 315 South 1400 East, Room 2020 Salt Lake City UT 84112-0850 USA
    • Richard D. Ernst, University of Utah Department of Chemistry 315 South 1400 East, Room 2020 Salt Lake City UT 84112-0850 USA

Source: Journal of Chemical Crystallography | 10 Mar 2010 | 1:50 pm CET

3,6-Di(p-chlorophenyl)-2,7-dihydro-1,4,5-thiadiazepine: Crystal Structure and Decoding Intermolecular Interactions with Hirshfeld Surface Analysis

Abstract  
In 3,6-di(p-chlorophenyl)-2,7-dihydro-1,4,5-thiadiazepine, C16H12Cl2N2S, which crystallizes in the triclinic space group, P-1, with a = 8.4012(13) Å, b = 9.2087(15) Å, c = 10.4974(17) Å, α = 69.835(3)°, β = 77.091(4)°, γ = 81.820(4)°, V = 741.2(2) Å3 and Z = 2, the seven-membered ring adopts a distorted boat conformation. The structure was solved by direct methods and refined by full-matrix least squares based on F2 with weight w = 1/[σ2(
\textF\texto2
) + (0.0018P)2 + 1.5600P] where P = (
\textF\texto2
 + 
2 \textF\textc2
)/3. The new dnorm Hirshfeld surface and the breakdown of fingerprint plots were used for visualizing and exploring of title compound for quantifying intermolecular interactions in crystal lattice.
Graphical Abstract  
Crystal structure and Hirshfeld surface analysis of 3,6-di(p-chlorophenyl)-2,7-dihydro-1,4,5-thiadiazepine have been reported.
MediaObjects/10870_2010_9730_Figa_HTML.gif

  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9730-x
  • Authors
    • Mehdi Bakavoli, Ferdowsi University Department of Chemistry P.O. Box 91779 Mashhad Iran
    • Mohammad Rahimizadeh, Ferdowsi University Department of Chemistry P.O. Box 91779 Mashhad Iran
    • Babak Feizyzadeh, Ferdowsi University Department of Chemistry P.O. Box 91779 Mashhad Iran
    • Amir Aghaei Kaju, Khorasan Science & Technology Park Department of Chemistry P.O. Box 91735-139 Mashhad Iran
    • Reza Takjoo, Ferdowsi University Department of Chemistry P.O. Box 91779 Mashhad Iran

Source: Journal of Chemical Crystallography | 10 Mar 2010 | 1:50 pm CET

An X-ray Crystallographic Study of 1,4-Di[(E)-2-(p-tolyl)-1-diazenyl]piperazine

Abstract  
The crystal structure of methyl 1,4-di[(E)-2-(p-tolyl)-1-diazenyl]piperazine (4) has been determined by single crystal X-ray diffraction analysis. The bis-triazene (4) adopts a normal chair conformation in the piperazine ring, with puckering parameters : φ2 = −29(5)°, QT = 0.534(2) Å and θ2 = 177.0(2)°. The crystal structure of 4 is compared with the structure of the triazene (2a) and the closely related bis-triazenes (3 and 5a). The piperazine ring of 2a and 4 adopt a typical chair conformation, whereas the piperazine ring of 3 adopts an unusual pseudo-boat conformation. Crystal data: 4 C18H22N6, triclinic, space group
P

1
 
, a = 6.8925(2) Å, b = 7.8574(3) Å, c = 16.8856(8) Å, α = 103.103(2)°, β = 90.528(2)°, γ = 101.776(2)° and V = 870.44 (6) Å3, for Z = 2.
Graphical Abstract  
MediaObjects/10870_2010_9740_Figa_HTML.gif
The crystal structure of 1,4-di[(E)-2-(p-tolyl)-1-diazenyl]piperazine has been determined by single crystal X-ray diffraction analysis

  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9740-8
  • Authors
    • Vanessa Renee Little, Saint Mary’s University Department of Chemistry Halifax NS B3H 3C3 Canada
    • Valerio Bertolasi, Universita’ di Ferrara Dipartimento di Chimica and Centro di Strutturistica Diffrattometrica Via L. Borsari, 46 44100 Ferrara Italy
    • Keith Vaughan, Saint Mary’s University Department of Chemistry Halifax NS B3H 3C3 Canada

Source: Journal of Chemical Crystallography | 10 Mar 2010 | 1:50 pm CET

Synthesis, Characterization and X-Ray Crystal Structure of the Tri Aqua (3-Hydroxy-5-Hydroxymethyl-2-Methylpyridine-4-Carboxaldehyde-3-Methylisotiosemicarbazone: k3, O3, N7, N10) Ni(II) Nitrate

Abstract  
The title complex triaqua (3-hydroxy-5-hydroxymethyl-2-methylpyridine-4-carboxaldehyde-3-methylisothiosemicarbazone-k3,O3,N7,N10)Ni(II) nitrate ([Ni(PLITSC)(H2O)3](NO3)2, 1) represents the second transition metal complex incorporating an isothiosemicarbazide-pyridoxal based Schiff base that has been crystallographically characterized. Complex 1 crystallizes in a P21/n space group, with lattice constants: a = 11.2254(1) Å, b = 12.9941(2) Å, c = 12.8663(2), β = 96,7713(5)°, V = 1863.64(4) Å3, Z = 4, F(000) = 1016, R 1 = 0.0681, wR 2 = 0.1201. The central Ni(II) cation is found in a six-coordinate octahedral geometry formed by the tridentate Schiff base ligand PLITSC and three water molecules. The identity of 1 was further confirmed by elemental analysis, IR spectra, and conductometric and magnetochemical measurements.
Index Abstract  
The coordination sphere of the Ni(II) cation in the green, paramagnetic complex [Ni(C10H14N4O2S1)(H2O)3](NO3)2 (1, Fig. 1), which crystallizes in P21/n space group, consists of three water molecules and a single tridentate ligand (Schiff base) obtained from isothiosemicarbazide and pyridoxal (pyridoxal is 3-hydroxy-5-hydroxymethyl-2-methylpyridine-4-carboxaldehyde) moieties.
MediaObjects/10870_2010_9746_Figa_HTML.gif

  • Content Type Journal Article
  • Category REVIEW PAPER
  • DOI 10.1007/s10870-010-9746-2
  • Authors
    • Violeta Jevtovic, Prirodno-matematicki fakultet Departman za hemiju Trg Dositeja Obradovica 3 21000 Novi Sad Serbia
    • Dragoslav Vidovic, University of Oxford Department of Chemistry Mansfield Road Oxford OX1 3TA UK

Source: Journal of Chemical Crystallography | 10 Mar 2010 | 1:50 pm CET

Synthesis and Crystal Structure of Copper(II)-Hexafluoro-Acetylacetonate Complexes with Pyridyl-Substituted Nitronyl and Imino-Nitroxide Radicals

Abstract  
A one-dimensional chain compound was formed by copper (II) hexafluoroacetylacetonate (hfac) and nitroxide radical 2-(4-pyridyl)-4,4,5,5-tetramethyl-imidazoline-1-oxyl-oxide (NITpPy). The product was structurally characterized by single crystal X-ray diffraction. [Cu2(hfac)4NITpPy] n crystallizes in the monoclinic C2/c space group with a = 19.70(2), b = 16.834(19), c = 15.274(18) Å, β = 119.073, V = 4427(9) Å3, Z = 4, R = 0.0699 wR 2 (all data) = 0.1752. In the compound, two different Cu(hfac)2 units are bridged by NITpPy. The nitrogen atom of pyridine ring is coordinated with Cu(II) ion to afford a three-spin complex. Cu(II) ions of Cu(hfac)2 and the oxygen atoms of nitronyl nitroxide formed weak coordination bonds with the bond length 2.495(8) Å.
Graphical Abstract  
A one-dimensional chain compound [Cu2(hfac)4NITpPy]n was formed by copper (II) hexafluoroacetylacetonate (hfac) and nitroxide radical 2-(4-pyridyl)-4,4,5,5-tetramethyl-imidazoline-1-oxyl-oxide (NITpPy). In the compound, two different Cu(hfac)2 units are bridged by NITpPy forming a 1D zigzag chain with the weak coordination bond Cu–O bond length 2.495(8) Å.
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  • Content Type Journal Article
  • Category COMMUNICATION
  • DOI 10.1007/s10870-010-9731-9
  • Authors
    • Kun-Miao Wang, Yunnan University Key Laboratory of Medicinal Chemistry for Natural Resource, Department of Chemistry Education Ministry Kunming 650091 Yunnan China
    • Lin Du, Yunnan University Key Laboratory of Medicinal Chemistry for Natural Resource, Department of Chemistry Education Ministry Kunming 650091 Yunnan China
    • Rui-Bing Fang, Yunnan University Key Laboratory of Medicinal Chemistry for Natural Resource, Department of Chemistry Education Ministry Kunming 650091 Yunnan China
    • Qi-Hua Zhao, Yunnan University Key Laboratory of Medicinal Chemistry for Natural Resource, Department of Chemistry Education Ministry Kunming 650091 Yunnan China

Source: Journal of Chemical Crystallography | 10 Mar 2010 | 1:50 pm CET

A review of polytypism in lead iodide

Lead Iodide (PbI2) is an important inorganic solid for both basic scientific research and possible technological applications and in this brief review we discuss the structure of PbI2. Although the basic structure is a simple I-Pb-I layered structure with a [PbI6]4- near-octahedron being the basic building block, there are many ways of stacking the layers which results in many polytypes. We present 20 of the 23 entries for the structure of PbI2 from the Inorganic Structural Database and order them by polytype. This represents more than 80 years of crystallographic research in the structure of this compound. We present a simple way to view the 2H, 4H, 6H, and 6R polytypes and extend the procedure to higher-order polytypes. We note a relationship, not generally appreciated, between the distortion of the near [PbI6]4- octahedrons and the polytype. We suggest that the significance of vacancies has only recently been appreciated. We suggest that small discrepancies in structure determination are probably due to different distributions of vacancies and that there are, in practice, very many structures for macroscopic or even mesoscopic samples of a given polytype when vacancies are considered. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 10 Mar 2010 | 9:40 am CET

Controllable assembly of copper(i)-iodide coordination polymers by tecton design of benzotriazol-1-yl-based pyridyl ligands: from 2D layer to 3D self-penetrating or homochiral networks

Shao-Ming Fang, Qiang Zhang, Min Hu, Bo Xiao, Li-Ming Zhou, Guang-Hui Sun, Li-Jun Gao, Miao Du, Chun-Sen Liu
(Paper from CrystEngComm)
Shao-Ming Fang, CrystEngComm, 2010, DOI: 10.1039/c002030n
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Source: RSC - CrystEngComm latest articles | 10 Mar 2010 | 12:00 am CET

Hierarchical ZnO micro/nanoarchitectures: hydrothermal preparation, characterization and application in the detection of hydrazine

Yonghong Ni, Jingsong Zhu, Li Zhang, Jianming Hong
(Paper from CrystEngComm)
Yonghong Ni, CrystEngComm, 2010, DOI: 10.1039/b923857n
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Source: RSC - CrystEngComm latest articles | 10 Mar 2010 | 12:00 am CET

Solvothermally controllable synthesis of anatase TiO2 nanocrystals with dominant {001} facets and enhanced photocatalytic activity

Jian Zhu, Shaohua Wang, Zhenfeng Bian, Songhai Xie, Chenling Cai, Jinguo Wang, Huagui Yang, Hexing Li
(Paper from CrystEngComm)
Jian Zhu, CrystEngComm, 2010, DOI: 10.1039/c000128g
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Source: RSC - CrystEngComm latest articles | 10 Mar 2010 | 12:00 am CET

Effect of strontium chloride on the optical and mechanical properties of [gamma]-glycine crystals

Single crystals of [gamma]-glycine have been grown from aqueous solution in the presence of small amount of strontium chloride. Single crystal X-Ray diffraction analysis was used to measure the unit cell parameters and to confirm the crystal structure. The grown crystals have also been subjected to powder X-Ray diffraction study to identify the crystalline nature. The presence of all the functional groups of the [gamma]-glycine has been confirmed by Fourier Transform Infrared (FTIR) spectral analysis. The presence of hydrogen and carbon in the glycine molecules was confirmed by using proton and carbon nuclear magnetic resonance (NMR) spectral analyses. Optical behavior of the crystal was studied using UV - Visible absorbance spectroscopy and second harmonic generation (SHG) studies. The SHG efficiency of [gamma]-glycine is greater than that of standard potassium dihydrogen phosphate (KDP). Mechanical strength of the [gamma]-glycine crystal has been determined by microhardness studies. Thermal stability of the grown crystal is probed using thermo gravimetric analysis and differential thermal analysis. Laser damage threshold value has been determined using Q-switched Nd:YAG laser operating at 1064 nm and with 13 ns pulse width in single shot mode. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 8 Mar 2010 | 5:41 am CET

Smectic phases of liquid crystals based on dinuclear palladium(II) complexes with carboxylato bridge

In this paper we present the preparation and the investigation of the liquid crystal properties of a series of dinuclear carboxylato bridge Pd(II) complexes bearing six alkoxy peripheral chains in the molecule. Their structures were assigned based on elemental analysis, IR and 1H NMR spectroscopy whereas the thermal behaviour was investigated by polarizing optical microscopy and differential scanning calorimetry. The monotropic smectic A phase displayed by these materials was identified by miscibility studies with a previously reported mesogen. It was found that the transition temperatures and the SmA mesophase stability depend on the alkyl chain length of the carboxylato bridge. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 8 Mar 2010 | 5:41 am CET

Modelling diffraction patterns from one-dimensionally disordered structures of AIIBVI crystals by Monte Carlo Technique IV. The 6H structure with different kinds of stacking faults

To investigate the one-dimensionally disordered structures (ODDS) in the close packed (cp) crystals, the Monte Carlo computer simulation technique has been applied. Calculations of the diffraction intensity distributions along the 10.L reciprocal lattice row from the 6H(33) structure with the four different kinds of the stacking faults (SFs): growth, deformation, layer displacement and extrinsic fault are presented. In particular, using the simple frequency functions of the fault to fault distances, both random and non-random distributions of the SFs are considered. Distinctive features of the diffraction patterns corresponding to the chosen examples of the transformations from the parent 6H(33) structure into another small-period polytypes are discussed in detail. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 8 Mar 2010 | 5:41 am CET

Controlled vapor-phase synthesis of cobalt oxide nanomaterials with tuned composition and spatial organization

Davide Barreca, Alberto Gasparotto, Oleg I. Lebedev, Chiara Maccato, Andrea Pozza, Eugenio Tondello, Stuart Turner, Gustaaf Van Tendeloo
(Paper from CrystEngComm)
Davide Barreca, CrystEngComm, 2010, DOI: 10.1039/b926368n
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Source: RSC - CrystEngComm latest articles | 8 Mar 2010 | 12:00 am CET

Synthesis, crystal structure and characterization of a new layered gallium phosphite Ga(HPO3)F3[middle dot](trans-C6N2H16) with left- and right-handed helical chains

Liangliang Huang, Tianyou Song, Lirong Zhang, Yanli Chen, Jinhua Jiang, Jianing Xu, Li Wang
(Paper from CrystEngComm)
Liangliang Huang, CrystEngComm, 2010, DOI: 10.1039/b926096j
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Source: RSC - CrystEngComm latest articles | 8 Mar 2010 | 12:00 am CET

Reversible crystal to crystal transformation of a hydrogen-bonded polymer to another in a solid-gas reaction along with morphology change: nano-particles to nano-rods conversion

Somaye Khanjani, Ali Morsali, Pascal Retailleau
(Paper from CrystEngComm)
Somaye Khanjani, CrystEngComm, 2010, DOI: 10.1039/b918746d
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Source: RSC - CrystEngComm latest articles | 8 Mar 2010 | 12:00 am CET

A microporous metal-organic framework constructed from a 1D column made of linear trinuclear manganese secondary building units

Sehyun Jeong, Jungwook Choi, Mira Park, Minhak Oh, Dohyun Moon, Myoung Soo Lah
(Paper from CrystEngComm)
Sehyun Jeong, CrystEngComm, 2010, DOI: 10.1039/b927590h
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Source: RSC - CrystEngComm latest articles | 8 Mar 2010 | 12:00 am CET

pH-dependent self-assembly of divalent metals with a new ligand containing polycarboxylate: syntheses, crystal structures, luminescent and magnetic properties

Lei Chen, Guang-Juan Xu, Kui-Zhan Shao, Ya-Hui Zhao, Guang-Sheng Yang, Ya-Qian Lan, Xin-Long Wang, Hong-Bin Xu, Zhong-Min Su
(Paper from CrystEngComm)
Lei Chen, CrystEngComm, 2010, DOI: 10.1039/b918647f
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Source: RSC - CrystEngComm latest articles | 8 Mar 2010 | 12:00 am CET

Precursor template synthesis of three-dimensional mesoporous ZnO hierarchical structures and their photocatalytic properties

Lingling Xu, Zeming Li, Qinghai Cai, Hongxia Wang, Hong Gao, Wei Lv, Jia Liu
(Paper from CrystEngComm)
Lingling Xu, CrystEngComm, 2010, DOI: 10.1039/b924097g
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Source: RSC - CrystEngComm latest articles | 8 Mar 2010 | 12:00 am CET

Luminescence from the deep level N-N interstitials in GaAsN grown by metal organic chemical vapour deposition

Deny Sentosa, Tang Xiaohong, Chua Soo Jin
(Paper from CrystEngComm)
Deny Sentosa, CrystEngComm, 2010, DOI: 10.1039/b911491b
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Source: RSC - CrystEngComm latest articles | 5 Mar 2010 | 12:00 am CET

Organic small molecule-assisted synthesis of high active TiO2 rod-like mesocrystals

Li Li, Chun-yan Liu
(Paper from CrystEngComm)
Li Li, CrystEngComm, 2010, DOI: 10.1039/b924170a
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Source: RSC - CrystEngComm latest articles | 5 Mar 2010 | 12:00 am CET

Supramolecular assembly of [H(4-n)BPTC]n- with pipzH22+: 1D negatively charged rectangular tubes and a 2D neutral fes 4[middle dot]82 network

Weiming Xiao, Chao Chen, Shengjun Deng, Xuejin Mao, Bin Sun, Ning Zhang
(Communication from CrystEngComm)
Weiming Xiao, CrystEngComm, 2010, DOI: 10.1039/b922188c
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Source: RSC - CrystEngComm latest articles | 5 Mar 2010 | 12:00 am CET

Hydrogen bonded dimers vs. one-dimensional chains in 2-thiooxoimidazolidin-4-one (thiohydantoin) drug derivatives

Sushil Jha, Jon D. Silversides, Ross W. Boyle, Stephen J. Archibald
(Paper from CrystEngComm)
Sushil Jha, CrystEngComm, 2010, DOI: 10.1039/b924683e
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Source: RSC - CrystEngComm latest articles | 5 Mar 2010 | 12:00 am CET

Dipyrrin based homo- and hetero-metallic infinite architectures

Stephane A. Baudron
(Highlight from CrystEngComm)
Stephane A. Baudron, CrystEngComm, 2010, DOI: 10.1039/c001020k
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Source: RSC - CrystEngComm latest articles | 5 Mar 2010 | 12:00 am CET

Novel three-dimensional Ln-Ag 4d-4f heteropentametallic helix-based microporous metal-organic framework with unprecedented (3,4,5,6)-connected topology constructed from isonicotinate ligand

Zhao-Yang Li, Jing-Wei Dai, Shan-Tang Yue, Ying-Liang Liu
(Communication from CrystEngComm)
Zhao-Yang Li, CrystEngComm, 2010, DOI: 10.1039/c000058b
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Source: RSC - CrystEngComm latest articles | 5 Mar 2010 | 12:00 am CET

Growth morphology of [small alpha]-glycine crystals in solution environments: an extended interface structure analysis

Sivashangari Gnanasambandam, Raj Rajagopalan
(Paper from CrystEngComm)
Sivashangari Gnanasambandam, CrystEngComm, 2010, DOI: 10.1039/b922780f
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Source: RSC - CrystEngComm latest articles | 5 Mar 2010 | 12:00 am CET

On the Two Closely Related Phases of [Ru(C5Me5)(η6-1,3-(Me2NCH2)2C6H4)](BF4) and the Reversible Solid–Solid Order–Disorder Phase Transition

Abstract  
Crystals of the complex [Ru(C5Me5)(η6-1,3-(Me2NCH2)2C6H4)](BF4) have been examined over the temperature range 150–300 K via X-ray diffraction measurements. This study shows that the Ru complex is a two-phase system in this T-range and the solid–solid transition is reversible. At 150 K, phase II (P21/c, Z′ = 4) is ordered and non-merohedrally twinned, a = 16.4396 (9) Å, b = 17.3226 (4) Å, c = 32.1874 (11) Å, β = 91.375 (2)°. At 295 K, phase I (Pbca, Z′ = 1) is disordered, a = 8.5071 (3) Å, b = 17.1567 (3) Å, c = 32.8250 (8) Å. The relationship between the two phases is obvious because the packing remains similar in the two phases. The greatest structural changes between the two phases are found in the rows of adjacent cations [Ru(C5Me5)(η6-1,3-(Me2NCH2)2C6H4)]+ packed along the a direction. These rows are ordered in phase II but are disordered in phase I. The phase transition is first order. Significant changes in thermal motion for the cations are considered as being the driving force for the occurrence of this phase transition.
Graphical Abstract  
The X-ray diffraction study showed that the complex [Ru(C5Me5)(η6-1,3-(Me2NCH2)2C6H4)](BF4) is a two-phase system between 150 and 300 K.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9732-8
  • Authors
    • Maxime A. Siegler, Utrecht University Crystal and Structural Chemistry, Bijvoet Center for Biomolecular Research, Faculty of Science Padualaan 8 3584 CH Utrecht The Netherlands
    • Sylvestre Bonnet, Utrecht University Organic Synthesis and Catalysis, Debye Institute for Nanomaterials Science, Faculty of Science Padualaan 8 3584 CH Utrecht The Netherlands
    • Antoine M. M. Schreurs, Utrecht University Crystal and Structural Chemistry, Bijvoet Center for Biomolecular Research, Faculty of Science Padualaan 8 3584 CH Utrecht The Netherlands
    • Robertus J. M. Klein Gebbink, Utrecht University Organic Synthesis and Catalysis, Debye Institute for Nanomaterials Science, Faculty of Science Padualaan 8 3584 CH Utrecht The Netherlands
    • Gerard van Koten, Utrecht University Organic Synthesis and Catalysis, Debye Institute for Nanomaterials Science, Faculty of Science Padualaan 8 3584 CH Utrecht The Netherlands
    • Anthony L. Spek, Utrecht University Crystal and Structural Chemistry, Bijvoet Center for Biomolecular Research, Faculty of Science Padualaan 8 3584 CH Utrecht The Netherlands

Source: Journal of Chemical Crystallography | 3 Mar 2010 | 9:05 am CET

Large-scale, uniform, single-crystalline Cd(OH)2 hexagonal platelets for Cd-based functional applications

Hao Jiang, Junqing Hu, Chunzhong Li, Feng Gu, Jan Ma
(Communication from CrystEngComm)
Hao Jiang, CrystEngComm, 2010, DOI: 10.1039/b927097c
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Source: RSC - CrystEngComm latest articles | 2 Mar 2010 | 12:00 am CET

Effect of temperature and isomorphic atom substitution on optical absorption edge of TlInS2xSe2(1-x) mixed crystals (0.25 [le] x [le] 1)

The optical properties of the TlInS2xSe2(1-x)mixed crystals (0.25 [le] x [le] 1) have been investigated through the transmission and reflection measurements in the wavelength range of 400-1100 nm. The optical indirect band gap energies were determined by means of the analysis of the absorption data. It was found that the energy band gaps decrease with the increase of selenium atoms content in the TlInS2xSe2(1-x)mixed crystals. The transmission measurements carried out in the temperature range of 10-300 K revealed that the rates of change of the indirect band gaps with temperature are [gamma] = -9.2×10-4 eV/K, -6.1×10-4 eV/K, -4.7×10-4 eV/K and -5.6×10-4 eV/K for TlInS2, TlInS1.5Se0.5, TlInSSe and TlInS0.5Se1.5 crystals, respectively. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 1 Mar 2010 | 6:27 am CET

Important physical parameters of Bi2O3 thin films found by applying several models for optical data

Different optical parameters for thin solid films can be computed as functions of wavelength from the optical transmission and reflection spectra. Subsequently, several models can be tested on the obtained data, in order to check their validity with respect to the materials under study. Moreover, these models offer the possibility to estimate essential physical parameters. Such models are tested within this article for the refraction index and for the real part of the complex dielectric constant, for bismuth trioxide thin films deposited on glass substrates maintained at three different temperatures. Also, the model proposed by Tauc is applied for the absorption spectrum of the same films, in order to determine the type of electronic transition and to estimate the optical energy bandgap. It will be noticed that the optical parameters vary rather significantly with changing substrate temperature, while the structure of the films, as studied by means of X-ray diffractometry is almost insensitive to this change of deposition parameter. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 1 Mar 2010 | 6:27 am CET

Structure and humidity sensing properties of SnO2 zigzag belts

A novel method was developed for synthesizing ultralong SnO2 zigzag belts with the assistance of CuO powder. The crystalline structure and morphology of SnO2 zigzag belts were characterized using x-ray diffraction, scanning electron microscopy and transmission electron microscopy. The growth mechanism of the ultralong SnO2 zigzag belts and the catalytic behavior of the copper were discussed. The humidity sensor based on as-synthesized product shows high sensitivity and fast response time due to unique structure of the SnO2 zigzag belts with large surface-to-volume ratio. It can be found that the resistance of the SnO2 materials decreases obviously with increasing relative humidity (RH) at room temperature (26 °C). The results demonstrate that these SnO2 nanostructures are potential to be used as effective and high performance humidity sensors. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 1 Mar 2010 | 6:27 am CET

Structure and electrical properties of Mg-doped ZnO nanoparticles

MgxZn1-xO (x=0.01-0.3) nanoparticles were synthesized by the sol-gel technique using solutions of Mg and Zn based organometalic compounds. The electrical properties of Mg doped zinc oxide (ZnO) were studied within wide temperature range from 300 to 500 K under the N2 gas flow (flow rate: 20 sccm) and in the frequency range from 40 Hz to 1 MHz for ac electrical measurements. The dc conductivities and the activation energies were found to be in the range of 10-9-10-6 S/cm at the room temperature and 0.26-0.86 eV respectively depending on doping rate of these samples. The ac conductivity was well represented by the power law A[omega]s. The conduction mechanism for all doped ZnO could be related to correlated barrier hopping (CBH) model. The complex impedance plots (Nyquist plot) showed the data points lying on a single semicircle, implying the response originated from a single capacitive element corresponding to the nanoparticle grains. The crystal structures of the MgxZn1-xO nanoparticles were characterized using X-ray diffraction. The calculated average particle sizes values of Zn1-xMgxO samples are found between 29.72 and 22.43 nm using the Sherrer equation. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 1 Mar 2010 | 6:27 am CET

Interdiffusion phenomena in InGaAs/GaAs superlattice structures

We have studied structural properties of InGaAs/GaAs superlattice sample prepared by Molecular Beam Epitaxy (MBE) using high resolution X-ray diffractometer (HRXRD). Increasing strain relaxation and defect generations are observed with the increasing Rapid Thermal Annealing (RTA) temperature up to 775 °C. The higher temperatures bring out relaxation mechanisms; interdiffusion and favored migration. The defect structure and the defects which are observed with the increasing annealing temperature were analyzed. Firstly, the in-plane and out-of-plane strains after the annealing of sample were found. Secondly, the structural defect properties such as the parallel X-ray strain, perpendicular X-ray strain, misfit, degree of relaxation, x composition, tilt angles and dislocation that are obtained from X-ray diffraction (XRD) analysis were carried out at every temperature. As a result, we observed that the asymmetric peaks especially in asymmetric (224) plane was affected more than symmetric and asymmetric planes with lower polar or inclination angles due to c-direction at low temperature. These structural properties exhibit different unfavorable behaviors for every reflection direction at the increasing temperatures. The reason is the relaxation which is caused by spatially inhomogeneous strain distribution with the increasing annealing temperature. In the InGaAs superlattice samples, this process enhances preferential migration of In atoms along the growth direction. Further increase in the annealing temperature leads to the deterioration of the abrupt interfaces in the superlattice and degradation in its structural properties. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 1 Mar 2010 | 6:27 am CET

Growth and EBSD determination of Celestite SrSO4 dendrites

In this paper, the SrSO4 dendrites were prepared by diffusion method. Electron backscattered diffraction (EBSD) technique is used to determine the crystallographic orientations of SrSO4 dendrites. It is shown that the SrSO4 dendrites grow in (001) plane, and all short main branches grow along <100>, but the long main branches grow along <110>, <130> or <140> directions. The growth morphology of SrSO4 dendrites is controlled by not only their internal structure but also external growth conditions. The internal structure of SrSO4 dendrites influences the character of the growth direction vertically <001>. The change of the ions concentration in the diffusion system leads to the evolution from <110> to <140> of the long main branches. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Source: Crystal Research and Technology | 1 Mar 2010 | 6:27 am CET

Not just size and shape: spherically symmetrical d5 and d10 metal ions give different coordination nets with 4,2[prime or minute]:6[prime or minute],4[double prime]-terpyridines

Edwin C. Constable, Guoqi Zhang, Eugenio Coronado, Catherine E. Housecroft, Markus Neuburger
(Paper from CrystEngComm)
Edwin C. Constable, CrystEngComm, 2010, DOI: 10.1039/b926597j
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Source: RSC - CrystEngComm latest articles | 26 Feb 2010 | 12:00 am CET

Assembling and dissembling zinc-containing coordination polymers of 4[prime or minute]-phenyl-4,2[prime or minute]:6[prime or minute],4[double prime]-terpyridine

Edwin C. Constable, Guoqi Zhang, Catherine E. Housecroft, Markus Neuburger, Jennifer A. Zampese
(Paper from CrystEngComm)
Edwin C. Constable, CrystEngComm, 2010, DOI: 10.1039/b926598h
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Source: RSC - CrystEngComm latest articles | 26 Feb 2010 | 12:00 am CET

Synthesis and Crystal Structure of a Dinuclear Palladium (II) Complex with a Bulky Acridine-based Ligand

Abstract  
The reaction of PdCl2 with a bulky acridine-based ligand afforded a novel PdII complex [Pd2(L)Cl4(CH3CN)](CH3CN)0.5 (1) (L = 9-[3-(2-pyridyl)pyrazol-1-yl]-acridine) exhibiting intra- and intermolecular C–H···Pd H-bonding interactions, which was characterized by elemental analysis, IR, and single-crystal X-ray diffraction analysis (triclinic system, space group P-1, with a = 8.774(6), b = 12.742(9), c = 14.149(10) Å, α = 67.573(11), β = 72.601(11), γ = 83.674(12)°, V = 1395.4(17) Å3, and Z = 2). Complex 1 has an asymmetrical dinuclear structure, which are further assembled into a one-dimensional (1D), and then two-dimensional (2D) network via intra- and/or inter-molecular C–H···Pd and C–H···Cl H-bonding interactions from different crystallographic directions. This work offers a new example in which the N donor of the acridine ring coordinates to a metal ion in a supramolecular coordination system.
Graphical Abstract  
A dinuclear PdII complex exhibiting intra- and inter-molecular C–H···Pd H-bonding interactions has been successfully constructed by using a well-designed bulky acridine-based ligand, 9-[3-(2-pyridyl)pyrazol-1-yl]-acridine. This work offers a new example in which the N donor of the acridine ring coordinates to a metal ion in a supramolecular coordination system.
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  • Content Type Journal Article
  • Category Original paper
  • DOI 10.1007/s10870-010-9745-3
  • Authors
    • Chun-Sen Liu, Zhengzhou University of Light Industry Henan Provincial Key Laboratory of Surface and Interface Science 450002 Zhengzhou Henan People’s Republic of China
    • Qiang Zhang, Zhengzhou University of Light Industry Henan Provincial Key Laboratory of Surface and Interface Science 450002 Zhengzhou Henan People’s Republic of China

Source: Journal of Chemical Crystallography | 25 Feb 2010 | 6:57 pm CET

Synthesis and Crystal Structure of Two Diflunisal Carboxamides

Graphical abstract  
The title compounds, 2′,4′-difluoro-4-[(4-methylbenzoyl)oxy]-N-[4-nitro-3-(trifluoromethyl)phenyl]-[1,1′-biphenyl]-3-carboxamide 2a and 2′,4′-difluoro-4-[(4-chlorobenzoyl)oxy]-N-[4-nitro-3-(trifluoromethyl) phenyl]-[1,1′-biphenyl]-3-carboxamide 2b, synthesized from diflunisal, a registered anti-inflammatory drug, via amidation of carboxlic acid and esterification of phenolic hydroxy group, were confirmed by single- crystal X-ray diffraction showing their packing are stabilized by intermolecular hydrogen bonds
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9728-4
  • Authors
    • Guang-xiang Zhong, Zhejiang University of Technology College of Pharmaceutical Science Hangzhou 310032 People’s Republic of China
    • Hong-dan Hu, Zhejiang University of Technology College of Pharmaceutical Science Hangzhou 310032 People’s Republic of China
    • Chun-nian Xia, Zhejiang University of Technology College of Pharmaceutical Science Hangzhou 310032 People’s Republic of China
    • Jian-song Jiang, Zhejiang University of Technology College of Pharmaceutical Science Hangzhou 310032 People’s Republic of China
    • Ting-ting Chen, Zhejiang University of Technology College of Pharmaceutical Science Hangzhou 310032 People’s Republic of China

Source: Journal of Chemical Crystallography | 25 Feb 2010 | 6:57 pm CET

Crystal Structure of Diethyl[(4chlorophenyl)(dibenzylamino)methyl]propanedioate

Abstract  
The titled new functionalized N,O,O-ligand of type diethyl[(4-chlorophenyl)(dibenzylamino)methyl]propanedioate (4) is prepared in good yield through condensation of dibenzylamine, with 2-arylidene-malonic acid diethyl esters 3. The structure of 4 was determined by spectral (IR, 1H NMR), elemental analyses and X-ray diffraction data. The molecular conformation shows two possible pockets ready to coordinate two metal atoms.
Graphical Abstract  
The structure of compound was determined by spectral (IR, 1H NMR), elemental analyses and X-ray diffraction data. The molecular conformation shows two possible pockets ready to coordinate two metal atoms.
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  • Content Type Journal Article
  • Category Communication
  • DOI 10.1007/s10870-010-9742-6
  • Authors
    • I. Meskini, Université Sidi Mohammed Ben Abdellah Laboratoire de Chimie Organique Fès Morocco
    • L. Toupet, Institut de Physique - IPR - UMR CNRS 6251, Université de Rennes 1 Rennes France
    • M. Akkurt, Erciyes University Department of Physics, Faculty of Arts and Sciences 38039 Kayseri Turkey
    • M. Daoudi, Université Sidi Mohammed Ben Abdellah Laboratoire de Chimie Organique Fès Morocco
    • A. Kerbal, Université Sidi Mohammed Ben Abdellah Laboratoire de Chimie Organique Fès Morocco
    • Z. H. Chohan, Bahauddin Zakariya University Department of Chemistry Multan 60800 Pakistan
    • T. Ben Hadda, Université Med. 1ier Laboratoire de Chimie des Matériaux Oujda Morocco

Source: Journal of Chemical Crystallography | 25 Feb 2010 | 8:57 am CET

Synthesis and Crystal Structure of a New Cobalt(II) Complex: Bis(pyridine)bis(4,4,4-trifluoro-1-(6-methoxynaphthalen-2-yl)butane-1,3-dione) Cobalt(II)

Abstract  
A new Co(II) complex 2 with ligand 4,4,4-trifluoro-1-(6-methoxynaphthalen-2-yl) butane-1,3-dione 1 and pyridine are prepared and crystallized from an acetone solution. The obtained red and transparent crystal conforms to the empirical formula of Co(C15H10O3F3)2·(C5H5N)2. It crystallizes in monoclinic, space group C2/c with a = 23.3152(14), b = 12.0225(7), c = 15.3950(10) Å, β = 124.1360(10)°, V = 3571.8(4) Å3, Z = 4, C40H30CoF6N2O6, Mr = 807.59, F(000) = 1652, Dc = 1.502 g/cm3, μ = 0.564 mm−1, the final R = 0.0466 and wR = 0.1043 for 3901 observed reflections with I > 2σ(I). X-ray structural analysis revealed that the Co(II) atom is coordinated by two oxygen atoms of 1,3-dione ligands 1 and two nitrogen atoms of pyridines, forming a distorted octahedron coordination geometry.
Graphical Abstract  
A new cobalt complex 2 bis(pyridine)bis(4,4,4-trifluoro-1-(6-methoxynaphthalen-2-yl)butane-1,3-dione) Cobalt(II), Co(C15H10O3F3)2·(C5H5N)2, has been synthesized and characterized by X-ray structure determination. In the complex, the Co(II) atom is coordinated by four oxygen atoms of the β-diketonate ligands and two nitrogen atoms of pyridines, forming a distorted octahedron coordination geometry.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9739-1
  • Authors
    • Dun-Jia Wang, Hubei Normal University Department of Chemistry and Environmental Engineering Huangshi 435002 China
    • Ling Fan, Hubei Normal University Department of Chemistry and Environmental Engineering Huangshi 435002 China
    • Chun-Yang Zheng, Hubei Normal University Department of Chemistry and Environmental Engineering Huangshi 435002 China

Source: Journal of Chemical Crystallography | 25 Feb 2010 | 8:57 am CET

Synthesis, Crystal Structure and Spectroscopic Characterization of 6-[2-(2-chlorophenyl)-1,3-thiazol-4-yl]-2-oxo-1,3-benzothiazol-3(2H)-ylacetic acid

Abstract  
The title compound {6-[2-(2-chlorophenyl)-1,3-thiazol-4-yl]-2-oxo-1,3-benzothiazol-3(2H)-yl}acetic acid was prepared and characterized by elemental analyses, FT-IR, 1H NMR spectroscopy, X-ray diffraction. A quantum-chemical calculation was performed using the CNDO method. In the title compound, C18H11ClN2O3S2, the crystal structure is stabilized by intermolecular hydrogen bonds (C–H···O=C) to form centrosymmetric
R22
(16) dimers and the C–H···O, O–H···N, and C–H···N interactions generating the graph set motifs
R22
(9) and
R22
(22).
Index Abstract  
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Synthetic route of title compound

  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9744-4
  • Authors
    • Abdullah Aydın, Kastamonu University Department of Science Education, Faculty of Education 37200 Kastamonu Turkey
    • Mehmet Akkurt, Erciyes University Department of Physics, Faculty of Arts and Sciences 38039 Kayseri Turkey
    • Leyla Uzun, Gazi University Department of Pharmaceutical Chemistry, Faculty of Pharmacy 06330 Ankara Turkey
    • Leyla Yıldırım, Hacettepe University Department of Physics Engineering, Faculty of Engineering 06532 Ankara Turkey
    • Tijen Önkol, Gazi University Department of Pharmaceutical Chemistry, Faculty of Pharmacy 06330 Ankara Turkey

Source: Journal of Chemical Crystallography | 25 Feb 2010 | 8:57 am CET

Synthesis and Crystal Structure of MnII(OAc)2[15-MC MnIII(N)shi-5](Im)3(EtOH)3 (shi3− = salicylhydroximate, −OAc = acetate, Im = imidazole, and EtOH = ethanol)

Abstract  
The metallacrown complex MnII(OAc)2[15-MCMnIII (N)shi-5](Im)3(EtOH)3 has been synthesized and characterized by single-crystal X-ray diffraction and infrared spectroscopy. The compound crystallizes in the monoclinic space group P21/c with a = 24.3326(15) Å, b = 24.0354(15) Å, c = 27.0531(17) Å, α = 90.00°, β = 100.3883(11)°, γ = 90.00°, V = 15562.5(17) Å3, Z = 4, and Z′ = 2. Four of the five manganese(III) ions of the metallacrown ring adopt a distorted octahedral coordination geometry, and the fifth manganese(III) ion is five coordinate and exhibits a distorted square pyramidal environment. The configuration of the manganese(III) ions about the ring follows a pattern of ΔΛΔPP, with P representing planar. In addition, the imidazole units are bound to three separate ring manganese(III) ions, and the imidazole units are directed to the outside of the molecule. A manganese(II) ion is encapsulated in the central core of the molecule, and the central ion is seven coordinate with a face-capped trigonal prismatic geometry.
Index Abstract  
The metallacrown complex MnII(OAc)2[15-MCMnIII (N)shi-5](Im)3(EtOH)3 was synthesized and characterized by FT-IR and single-crystal X-ray diffraction.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9735-5
  • Authors
    • Brian Emerich, Shippensburg University Department of Chemistry 1871 Old Main Dr. Shippensburg PA 17257 USA
    • Matthew Smith, Shippensburg University Department of Chemistry 1871 Old Main Dr. Shippensburg PA 17257 USA
    • Matthias Zeller, Youngstown State University Department of Chemistry One University Plaza Youngstown OH 44555 USA
    • Curtis M. Zaleski, Shippensburg University Department of Chemistry 1871 Old Main Dr. Shippensburg PA 17257 USA

Source: Journal of Chemical Crystallography | 25 Feb 2010 | 8:57 am CET

Crystal Structure and Thermal Decomposition of Square Planar Ni (II) Complexes with ONS Type Ligands

Abstract  
Similar square planar complexes in the literature were prepared with ONS type N-(2-mercaptophenyl) salicylaldimine and Ni (II). The fourth coordination alongside the tridentate organic ligand was provided by the amine group. The complexes prepared were characterized with Elemental Analyses, IR Spectroscopy and Thermal Analyses. The molecular structures both of the complexes were also determined with X-ray diffraction. The Ni (II) complex was observed to have a highly distorted square planar structure. The temperature range where the nitrogen containing tridentates ligand left the structure and the corresponding heat changes were compared with those in the literature. The residue after thermal decomposition above 650 °C was found to be NiO.
Graphical Abstract  
Similar square planar complexes in the literature were prepared with ONS type N-(2-mercaptophenyl) salicylaldimine and Ni (II). The fourth coordination alongside the tridentate organic ligand was provided by the amine group. The complexes prepared were characterized with Elemental Analyses, IR Spectroscopy and Thermal Analyses. The molecular structures both of the complexes were also determined with X-ray diffraction. The Ni (II) complex was observed to have a highly distorted square planar structure. The temperature range where the nitrogen containing tridentates ligand left the structure and the corresponding heat changes were compared with those in the literature. The residue after thermal decomposition above 650 °C was found to be NiO.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9738-2
  • Authors
    • Sefa Durmuş, University of Abant İzzet Baysal Faculty of Education 14280 Gölköy Bolu Turkey
    • Cengiz Arıcı, University of Hacettepe Department of Engineering Physics 06800 Ankara Turkey
    • Ertan Şahin, University of Atatürk Department of Chemistry 25240 Erzurum Turkey
    • Ümit Ergun, University of Ankara Department of Chemistry 06100 Ankara Turkey
    • Orhan Atakol, University of Ankara Department of Chemistry 06100 Ankara Turkey

Source: Journal of Chemical Crystallography | 25 Feb 2010 | 8:57 am CET

Crystal Structure of 3-Hydroxy-3′,4′-Methylenedioxy Flavone-6-Carboxylic Acid Dimethylformamide Solvate

Abstract  
The optically pure 3-hydroxy-3′,4′-methylenedioxy flavone-6-carboxylic acid was obtained through the chalcone route. The structure of 3-hydroxy-3′,4′-methylenedioxy flavone-6-carboxylic acid was first elucidated by single crystal X-ray analysis: triclinic, space group, triclinic (P-1) with a = 8.1379(13) Å, b = 8.9831(14) Å, c = 13.198(2) Å, α = 88.413(2)°, β = 74.908(2)°, γ = 72.987(2)°. V = 889.5(2) Å3, Z = 2. The structure was solved by direct methods and refined to a final R = 0.0413 for 1630 reflections with I > 2σ(I). The crystal structure is stabilized by O–H···O and C–H···O hydrogen bondings and π–π stacking interactions.
Index Abstract  
The titled compound, 3-hydroxy-3′,4′-methylenedioxy flavone-6-carboxylic acid dimethylformamide solvate, was linked to one-dimensional molecular ribbons via intermolecular O–H···O and C–H···O hydrogen bondings.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9727-5
  • Authors
    • Hui-Liang Wen, Nanchang University State Key Laboratory of Food Science and Technology Nanchang 330047 People’s Republic of China
    • Yun-Hua Chen, Nanchang University Department of Chemistry Nanchang 330047 People’s Republic of China
    • Chong-Bo Liu, Nanchang Hangkong University College of Environmental and Chemical Engineering Nanchang 330063 People’s Republic of China
    • Dan-Dan Chen, Nanchang University Department of Chemistry Nanchang 330047 People’s Republic of China
    • Xiao-Bo Hu, Nanchang University State Key Laboratory of Food Science and Technology Nanchang 330047 People’s Republic of China

Source: Journal of Chemical Crystallography | 25 Feb 2010 | 8:57 am CET

Hydrogen Bonded, π···π Stacked and X···π Framework Structures in Bis(2,6-Lutidinium) Tetrahalocuprate(II) Complexes

Abstract  
In the crystal structures of (2,6-lutidinium)2[CuCl4], 1 and (2,6-lutidinium)2[CuBr4], 2, the anion CuX4 2− is connected to eight and four surrounding cations in 1 and 2, respectively, through (N–H···X) (H2C–H···X) and (C–H···X) hydrogen bonds to form two-dimensional layers approximately normal to the crystallographic b-axis. These layers are further connected by means of offset face-to-face interactions (parallel to b-axis) to give three-dimensional structures. The hydrogen bonding (type and number) around each anion could be influenced by the anion size, as same cation is used, allowing different cation…anion interpenetrations.
Graphical abstract  
Three dimensional framework structures of tetrahalocuprate(II) complexes assembled via (N–H···X), (H2C–H···X) and (C–H···X) hydrogen bonds along with π···π stacking and X···π interactions.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9724-8
  • Authors
    • Basem Fares Ali, Al al-Bayt University Department of Chemistry Mafraq 25113 Jordan
    • Rawhi Al-Far, Al-Balqa Applied University Faculty of Information Technology and Science Salt Jordan
    • Salim F. Haddad, The University of Jordan Department of Chemistry Amman Jordan

Source: Journal of Chemical Crystallography | 25 Feb 2010 | 8:57 am CET

Rational synthesis of a microporous metal-organic framework with PtS topology using a semi-rigid tetrahedral linker

Li-Li Liang, Jun Zhang, Shi-Bin Ren, Gen-Wu Ge, Yi-Zhi Li, Hong-Bin Du, Xiao-Zeng You
(Communication from CrystEngComm)
Li-Li Liang, CrystEngComm, 2010, DOI: 10.1039/b925903a
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Source: RSC - CrystEngComm latest articles | 25 Feb 2010 | 12:00 am CET

Isomer dependent self-penetrated topologies and cluster subunits in copper phenylenediacetate coordination polymers with flexible dipyridyl ligands

Laura K. Sposato, Joseph A. Nettleman, Robert L. LaDuca
(Paper from CrystEngComm)
Laura K. Sposato, CrystEngComm, 2010, DOI: 10.1039/b926914b
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Source: RSC - CrystEngComm latest articles | 25 Feb 2010 | 12:00 am CET

Shape-controlled electrodeposition of tin crystals from Sn(ii)-fluoroborate solutions

Andre Muller, Sara E. C. Dale, Miles A. Engbarth, Simon J. Bending, Laurence M. Peter
(Paper from CrystEngComm)
Andre Muller, CrystEngComm, 2010, DOI: 10.1039/b921713d
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Source: RSC - CrystEngComm latest articles | 25 Feb 2010 | 12:00 am CET

Synthesis and Crystal Structure of [Ni(L)(Phen)(H2O)]·3.75H2O

Abstract  
The title compound, [Ni(L)(Phen)(H2O)]·3.75H2O, where L = (E)-2-(5-formyl-2-oxidobenzylideneamino)ethanesulfonate, was synthesized in aqueous methanol in the presence of Ni(II), Phen and the potassium salt of 2-{[(E)-(2-hydroxy-5{[(2-sulfoethyl)imino]methyl}phenyl)methylidene]amino}-1-ethanesulfonic acid. The complex crystallized in the space group of P-1 with a = 13.751 (2) Å, b = 14.797 (2) Å, c = 15.543 (2) Å, α = 105.86 (1)°, β = 103.51 (1)°, γ = 114.38 (1)°, and Z = 2. In [Ni(L)(Phen)(H2O)], the Ni(II) was six coordinated with two O and one N from L, two N from Phen and one O from coordinated water, forming an octahedral geometry. There are two molecules in the asymmetric unit and concomitant differences in the Ni-ligand bond lengths.
Graphical Abstract  
The complex of [Ni(L)(Phen)(H2O)]·3.75H2O was synthesized in aqueous methanol and crystallized in the space group of P-1. There are two molecules in the asymmetric unit and concomitant differences in the Ni-ligand bond lengths.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9733-7
  • Authors
    • Ju-Lan Zeng, Changsha University of Science and Technology School of Chemistry and Biological Engineering 410076 Changsha People’s Republic of China
    • Sai-Bo Yu, China Tobacco Hunan Industrial Corporation 410007 Changsha People’s Republic of China
    • Yi-Min Jiang, Guangxi Normal University School of Chemistry and Chemical Engineering 541004 Guilin People’s Republic of China
    • Li-Xian Sun, Changsha University of Science and Technology School of Chemistry and Biological Engineering 410076 Changsha People’s Republic of China
    • Zhong Cao, Changsha University of Science and Technology School of Chemistry and Biological Engineering 410076 Changsha People’s Republic of China
    • Dao-Wu Yang, Changsha University of Science and Technology School of Chemistry and Biological Engineering 410076 Changsha People’s Republic of China

Source: Journal of Chemical Crystallography | 24 Feb 2010 | 7:53 am CET

Non-Parallel Stacking of a One-Dimensional Rod and Loop Chain Cd(II) Complex With the Semi-Rigid 3,3′-Bipyridyl Ligand

Abstract  
A new Cd(II) complex [Cd(L)1.5(NO3)2]n·2nCHCl3 (1) with a semi-rigid 3,3′-bipyridyl ligand [L = N,N′-bis(3-pyridylmethyl)pyromellitic diimide], has been synthesized and structurally characterized by X-ray diffraction analysis. It consists of one-dimensional rod and loop chains featuring the combination of Z c -(anti, cis) and Z t -(anti, trans) mode conformations for the coordinated ligands. The one-dimensional chains are assembled in parallel and non-parallel directions into three-dimensional networks by complicated supramolecular interactions. The solid photoluminescence of 1 was also investigated at room temperature.
Graphical Abstract  
The 1D rod and loop chains coordination polymer [Cd(L)1.5(NO3)2]n·2nCHCl3 (1) is obtained from the semi-rigid 3,3′-bipyridyl L ligand featuring the combination of Z c -(anti, cis) and Z t -(anti, trans) mode conformations. The one-dimensional chains are assembled in parallel and non-parallel directions into three-dimensional networks by complicated supramolecular interactions.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9729-3
  • Authors
    • Wenli Chai, Northwest University School of Chemical Engineering, Shaanxi Key Laboratory of Physico-Inorganic Chemistry Xi’an 710069 Shaanxi China
    • Xingqiang Lü, Northwest University School of Chemical Engineering, Shaanxi Key Laboratory of Physico-Inorganic Chemistry Xi’an 710069 Shaanxi China
    • Weiyu Bi, Northwest University School of Chemical Engineering, Shaanxi Key Laboratory of Physico-Inorganic Chemistry Xi’an 710069 Shaanxi China
    • Jirong Song, Northwest University School of Chemical Engineering, Shaanxi Key Laboratory of Physico-Inorganic Chemistry Xi’an 710069 Shaanxi China
    • Beisheng Kang, Sun Yat-Sen University School of Chemistry and Chemical Engineering Guangzhou 510275 Guangdong China

Source: Journal of Chemical Crystallography | 24 Feb 2010 | 7:53 am CET

Synthesis and Crystal Structure of (S)-2-((S)-2-(N-Ts-Amino)-3-methylbutanoyl)-3-(1H-indol-3-yl)-6-phenyl-3,4-dihydro-1,2,4-triazin-5(2H)-one

Abstract  
The diastereoselective synthesis, NMR and X-ray structure of (S)-2-((S)-2-(N-Ts-amino)-3-methylbutanoyl)-3-(1H-indol-3-yl)-6-phenyl-3,4-dihydro-1,2,4-triazin-5(2H)-one—a potential antivirus agent are reported. The compound crystallizes in the triclinic space group P1 with unit cell parameters: a = 5.9259(6) Å, b = 9.6370(12) Å, c = 12.9541(9) Å, α = 109.210(9)°, β = 90.804(7)°, γ = 105.074(10)° and Z = 1.
Graphical Abstract  
The diastereoselective synthesis, NMR and X-ray structure of (S)-2-((S)-2-(N-Ts-Amino)-3-methylbutanoyl)-3-(1H-indol-3-yl)-6-phenyl-3,4-dihydro-1,2,4-triazin-5(2H)-one—a potential antivirus agent are reported.
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  • Content Type Journal Article
  • Category Communication
  • DOI 10.1007/s10870-010-9741-7
  • Authors
    • Ilya N. Egorov, Urals State Technical University Department of Organic Chemistry 19, Ul. Mira Ekaterinburg 620002 Russian Federation
    • Vladimir L. Rusinov, Urals State Technical University Department of Organic Chemistry 19, Ul. Mira Ekaterinburg 620002 Russian Federation
    • Pavel A. Slepukhin, Ural Branch of the Russian Academy of Sciences Institute of Organic Synthesis 20, Ul. S. Kovalevskaya Ekaterinburg 620219 Russian Federation
    • Oleg N. Chupakhin, Urals State Technical University Department of Organic Chemistry 19, Ul. Mira Ekaterinburg 620002 Russian Federation

Source: Journal of Chemical Crystallography | 24 Feb 2010 | 7:53 am CET

Synthesis and Crystal Structure of a Fe(III) Complex with an Isonicotinyl Hydrazone Ligand, [Fe(N-Isonicotinamidosalicylaldimine)Cl2]

Abstract  
A new complex [Fe(N-isonicotinamidosalicylaldimine)Cl2] has been synthesized by template reaction at room temperature and structurally characterized by X-ray single-crystal analysis. The complex crystallizes in triclinic crystal system, Pī space group, a = 7.273(6) Å, b = 10.015(8) Å, c = 10.479(8) Å, α = 71.067(10)°, β = 89.964(11)°, γ = 75.528(10)°, V = 696.4(9) Å3 and Z = 2. The coordination geometry around the Fe(III) ion is a distorted trigonal bipyramid with a O2N1Cl2 donor set. In the crystal structure, N–H···Cl, C–H···O and C–H···Cl hydrogen bonds and π···π stacking interactions involving aromatic and unclosed π-systems link the molecules to form supramolecular double layers.
Index Abstract  
A new Fe(III) complex of N-isonicotinamidosalicylaldimine, an isonicotinyl hydrazone ligand, has been prepared and crystallographically characterized.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9726-6
  • Authors
    • Jin-Xiu Wang, Tianjin University Department of Chemistry Tianjin 300072 People’s Republic of China
    • Xiao-Zeng Li, Tianjin University Department of Chemistry Tianjin 300072 People’s Republic of China
    • Li-Na Zhu, Tianjin University Department of Chemistry Tianjin 300072 People’s Republic of China
    • Ji-Yao Wang, Tianjin University Department of Chemistry Tianjin 300072 People’s Republic of China
    • Hao Qu, Tianjin University Department of Chemistry Tianjin 300072 People’s Republic of China

Source: Journal of Chemical Crystallography | 24 Feb 2010 | 7:53 am CET

Hydrothermal Synthesis and Characterization of a New Strandberg-Type Polyoxotungstate Compound (H2dien)2[W5O15(HPO4)2]·H2O

Abstract  
A Strandberg-type polyoxotungstate compound, (H2dien)2[W5O15(HPO4)2]·H2O (dien = diethylenetriamine), has been hydrothermally synthesized and characterized by single crystal X-ray diffraction, elemental analyses and cyclic valtammetry measurements. The compound crystallizes in triclinic system, space group
P

1
 
with unit a = 9.1974(2) Å, b = 9.7731(2) Å, c = 18.4565(5) Å, α = 82.4540(10)°, β = 87.4230(10)°, γ = 63.3620(10) Å, V = 1469.89(6) Å3 and Z = 2. It was revealed that the Strandberg-type polyoxotungstate cluster can be considered as a ring formed by five distorted edge- and corner-sharing WO6 octahedra, capped on both poles by a phosphate tetrahedron sharing three vertices with the ring tungsten centers. The Strandberg clusters are connected with the organic amines through hydrogen-bonding interactions into a three-dimensional supramolecular network.
Graphical Abstract  
The Strandberg-type polyoxotungstate cluster can be considered as a ring formed by five distorted edge- and corner-sharing WO6 octahedra, capped on both poles by a phosphate tetrahedron sharing three vertices with the ring tungsten centers.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-009-9675-0
  • Authors
    • Xue-Gong Cao, Huaqiao University Department of Applied Chemistry 362021 Quanzhou People’s Republic of China
    • Li-Wen He, Huaqiao University Department of Applied Chemistry 362021 Quanzhou People’s Republic of China
    • Bi-Zhou Lin, Huaqiao University Department of Applied Chemistry 362021 Quanzhou People’s Republic of China
    • Zi-Jing Xiao, Huaqiao University Department of Applied Chemistry 362021 Quanzhou People’s Republic of China

Source: Journal of Chemical Crystallography | 24 Feb 2010 | 7:53 am CET

Sulfate encapsulation in three-fold interpenetrated metal-organic frameworks with bis(pyridylurea) ligands

Biao Wu, Jianjun Liang, Yuxin Zhao, Minrui Li, Shaoguang Li, Yanyan Liu, Yongping Zhang, Xiao-Juan Yang
(Paper from CrystEngComm)
Biao Wu, CrystEngComm, 2010, DOI: 10.1039/b920777e
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Source: RSC - CrystEngComm latest articles | 24 Feb 2010 | 12:00 am CET

Hydrate Stabilization in the Three-Dimensional Hydrogen-Bonded Structure of the Brucinium Compound, Bis(2,3-dimethoxy-10-oxostrychnidinium) Biphenyl-4,4′-disulfonate Hexahydrate

Abstract  
The crystal structure of the 2:1 proton-transfer compound of brucine with biphenyl-4,4 -disulfonate, bis(2,3-dimethoxy-10-oxostrychnidinium) biphenyl-4,4 -disulfonate hexahydrate (1) has been determined at 173 K. Crystals are monoclinic, space group P21 with Z = 2 in a cell with a = 8.0314(2), b = 29.3062(9), c = 12.2625(3) Å, β = 101.331(2)°. The crystallographic asymmetric unit comprises two brucinium cations, a biphenyl-4,4 -disulfonate dianion and six water molecules of solvation. The brucinium cations form a variant of the common undulating and overlapping head-to-tail sheet sub-structure. The sulfonate dianions are also linked head-to-tail by hydrogen bonds into parallel zig-zag chains through clusters of six water molecules of which five are inter-associated, featuring conjoint cyclic eight-membered hydrogen-bonded rings [graph sets R 33(8) and R 43(8)], comprising four of the water molecules and closed by sulfonate O acceptors. These chain structures occupy the cavities between the brucinium cation sheets and are linked to them peripherally through both brucine N+–H···Osulfonate and Ocarbonyl···H–Owater to sulfonate O bridging hydrogen bonds, forming an overall three-dimensional framework structure. This structure determination confirms the importance of water in the stabilization of certain brucine compounds which have inherent crystal instability.
Graphical Abstract  
The crystal structure determination of the 2:1 proton-transfer brucinium compound, bis(2,3-dimethoxy-10-oxostrychnidinium) biphenyl-4,4′-disulfonate hexahydrate shows the presence of two independent brucinium cations which form into semi-associated sheet substructures. The disulfonate dianions and the associated water molecules of solvation occupy the interstitial cavities between the brucinium substructures with which they are hydrogen-bonded, giving a three-dimensional framework structure.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9689-7
  • Authors
    • Graham Smith, Queensland University of Technology School of Physical and Chemical Sciences G.P.O. Box 2434 Brisbane QLD 4001 Australia
    • Urs D. Wermuth, Queensland University of Technology School of Physical and Chemical Sciences G.P.O. Box 2434 Brisbane QLD 4001 Australia
    • David J. Young, Griffith University School of Biomolecular and Physical Sciences Nathan QLD 4111 Australia

Source: Journal of Chemical Crystallography | 23 Feb 2010 | 9:10 am CET

A simple peptidomimetic that self-associates on the solid state to form a nanoporous architecture containing chiral [small pi]-channels

Jorge Becerril, Michael Bolte, M. Isabel Burguete, Jorge Escorihuela, Francisco Galindo, Santiago V. Luis
(Communication from CrystEngComm)
Jorge Becerril, CrystEngComm, 2010, DOI: 10.1039/b922172g
To cite this article before page numbers are assigned, use the DOI form of citation above.
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Source: RSC - CrystEngComm latest articles | 23 Feb 2010 | 12:00 am CET

1D [rightward arrow] 1D Two-fold parallel interpenetrated coordination polymers with a bis(pyridylurea) ligand

Shaoguang Li, Biao Wu, Yongjing Hao, Yanyan Liu, Xiao-Juan Yang
(Communication from CrystEngComm)
Shaoguang Li, CrystEngComm, 2010, DOI: 10.1039/b922566h
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The content of this RSS Feed (c) The Royal Society of Chemistry

Source: RSC - CrystEngComm latest articles | 22 Feb 2010 | 12:00 am CET

Mechanical and longitudinal electromechanical properties of Sb-doped ZnO nanobelts

Ya Yang, Junjie Qi, Wen Guo, Qingliang Liao, Yue Zhang
(Communication from CrystEngComm)
Ya Yang, CrystEngComm, 2010, DOI: 10.1039/b927165a
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Source: RSC - CrystEngComm latest articles | 22 Feb 2010 | 12:00 am CET

Structural Conformation of a Novel Piperidine-4-One Derivative: 1-Acryloyl-3-Methyl-2,6-Dip-Tolylpiperidine-4-One

Abstract  
The novel 3-methyl-2,6-dip-toylpiperidine-4-one was acylated by 3-chloropropanoychloride and subjected for dehydrohalogenation. The synthesized compound was characterized by spectroscopic techniques and finally confirmed by X-ray diffraction studies. The molecule crystallizes in the monoclinic crystal class in the space group C 2/c with cell parameters a = 18.538(2) Å, b = 9.9050(1) Å, c = 22.954(2) Å, β = 94.486(8)° and Z = 8. The piperidine ring adopts a twist boat conformation.
Graphical Abstract  
The title compound was synthesized by acylation of 3-methyl-2,6-dip-tolylpiperidin-4-one followed by dehydrohalogenation and recrystalisation in ethanol. The molecule crystallizes in the monoclinic crystal class in the space group C2/c with cell parameters a = 18.538(2)Å, b = 9.9050(1) Å, c = 22.954(2) Å, β =  94.486(8)° and Z = 8. The heterocyclic ring adopts a twisted boat conformation.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9722-x
  • Authors
    • B. N. Lakshminarayana, University of Mysore Department of Studies in Physics Manasagangotri Mysore 570 006 India
    • C. R. Gnanendra, University of Mysore Department of Studies in Chemistry Mysore 570 006 India
    • T. N. Mahadeva Prasad, University of Mysore Department of Studies in Physics Manasagangotri Mysore 570 006 India
    • M. A. Sridhar, University of Mysore Department of Studies in Physics Manasagangotri Mysore 570 006 India
    • Nagaraja Naik, University of Mysore Department of Studies in Chemistry Mysore 570 006 India
    • D. Chenne Gowda, University of Mysore Department of Studies in Chemistry Mysore 570 006 India
    • J. Shashidhara Prasad, University of Mysore Department of Studies in Physics Manasagangotri Mysore 570 006 India

Source: Journal of Chemical Crystallography | 20 Feb 2010 | 7:55 am CET

Crystal Structure and Spectroscopic Properties of trans-Dibromobis(1,2-ethanediamine)chromium(III) Perchlorate

Abstract  The crystal structure of trans-[Cr(en)2Br2]ClO4 (en = 1,2-ethanediamine) has been determined by a single-crystal X-ray diffraction study at 150 K. The complex crystallizes in the space group
P

1
 
of the triclinic system with two mononuclear formula units in a cell of dimensions a = 6.853(4), b = 8.109(5), c = 12.475(8) Å, α = 81.006(10)°, β = 77.005(10)° and γ = 74.981(10)°. The Cr atom is in a slightly distorted octahedral environment, coordinated by four nitrogen atoms of two en ligands and two bromine atoms in trans axial positions. The mean Cr–N(en) and Cr–Br bond lengths are 2.079(3) and 2.4743(10)Å, respectively. The five-membered rings are in stable gauche conformations with N1–Cr1–N2 and N3–Cr2–N4 angles of 82.81(11)° and 83.67(11)°, respectively. The crystal packing is stabilized by a network of N–H···O and N–H···Br hydrogen bonds. The infrared and electronic absorption spectra are consistent with the results of X-ray crystallography.
Graphical Abstract  The spectroscopic properties of the title complex are in good agreement with the result of X-ray crystallography, which shows that the chromium atom is in an octahedral environment, coordinated by two bidentate 1,2-ethanediamine ligands and two bromine atoms in trans positions.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9698-6
  • Authors
    • Jong-Ha Choi, Andong National University Department of Chemistry Andong 760-749 Korea
    • William Clegg, Newcastle University School of Chemistry Newcastle upon Tyne NE1 7RU UK
    • Ross W. Harrington, Newcastle University School of Chemistry Newcastle upon Tyne NE1 7RU UK
    • Sang Hak Lee, Kyungpook National University Department of Chemistry Daegu 702-701 Korea

Source: Journal of Chemical Crystallography | 15 Feb 2010 | 7:02 pm CET

Synthesis, Characterization and Crystal Structure of 4,5-Bis(Cyclohexanecarbonylthio)-1,3-dithiolane-2-thione Crystal

Abstract  A new crystal of 4,5-bis(cyclohexanecarbonylthio)-1,3-dithiolane-2-thione has been prepared at room temperature and characterized by elemental analysis, UV–Vis–NIR absorption spectrum and X-ray single crystal determination. The complex crystallized in triclinic space group P-1 with unit cell dimensions a = 5.37370(10) Å, b = 12.8618(2) Å, c = 15.2481(2) Å, α = 74.8530(10)°, β = 80.6000(10)°, γ = 85.9550(10)°, V = 1003.18(3) Å3, Z = 2, D x = 1.3861(1) g cm−3. The X-ray structure determination revealed that the crystal is centered-symmetrical and the molecules form dimers with a long intermolecular S···S interaction in the crystal.
Graphical Abstract  A new crystal of 4,5-bis(cyclohexanecarbonylthio)-1,3-dithiolane-2-thione with triclinic space group P − 1 [unit cell dimensions a = 5.37370(10) Å, b = 12.8618(2) Å, c = 15.2481(2) Å, α = 74.8530(10)º,β = 80.6000(10)º, γ = 85.9550(10)º, V = 1003.18(3) Å3, Z = 2, D x = 1.3861(1) g·cm−3] has been prepared and characterized by elemental analysis, UV–Vis–NIR absorption spectrum and X-ray single crystal determination.
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  • Content Type Journal Article
  • Category Original paper
  • DOI 10.1007/s10870-010-9685-y
  • Authors
    • Yan Ling Wang, China University of Petroleum (East China) School of Petroleum Engineering 266555 Qingdao People’s Republic of China
    • Mei Li, Material Science and Engineering of Shandong Institute of Light Industry 250353 Jinan People’s Republic of China
    • Jun Yao, China University of Petroleum (East China) School of Petroleum Engineering 266555 Qingdao People’s Republic of China
    • Ye Fei Wang, China University of Petroleum (East China) School of Petroleum Engineering 266555 Qingdao People’s Republic of China
    • Jing Jing Zheng, China University of Petroleum (East China) School of Petroleum Engineering 266555 Qingdao People’s Republic of China
    • Li Ma, China University of Petroleum (East China) School of Petroleum Engineering 266555 Qingdao People’s Republic of China

Source: Journal of Chemical Crystallography | 13 Feb 2010 | 7:49 am CET

Structural Studies of the 1:1 Complex of o-3,4-Dimethyltetrathiafulvalene (o-Me2TTF) and 1,2,4,5-Tetracyanobenzene (TCNB)

Abstract  The synthesis and crystal structure of the 1:1 complex o-Me2TTF-TCNB is reported. The complex crystallizes in the triclinic space group P-1 with a = 6.920(1) Å, b = 7.928(2) Å, c = 17.453(4) Å, α = 100.53(3)°, β = 99.66(3)°, and γ = 97.32(3)°. The bond length of the central C=C bond in o-Me2TTF is 1.342(2) Å, indicating a neutral state for the o-Me2TTF donor.
Graphical Abstract  The X-ray crystallographic structure of the complex o-Me2TTF-TCNB has been determined. Corresponding interatomic interactions, bond distances and its synthetic preparation are discussed.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9688-8
  • Authors
    • Eric W. Reinheimer, Texas A & M University Department of Chemistry College Station TX 77842-3012 USA
    • Hanhua Zhao, Texas A & M University Department of Chemistry College Station TX 77842-3012 USA
    • Kim R. Dunbar, Texas A & M University Department of Chemistry College Station TX 77842-3012 USA

Source: Journal of Chemical Crystallography | 12 Feb 2010 | 8:12 am CET

Two Different Compounds Formed from Copper(II) tetrafluoridoborate and [1,2,4]triazolo[1,5-a]pyrimidine. Synthesis, Spectroscopy and Single-Crystal Structures

Abstract  Two coordination compounds copper(II) with tetrafluoridoborate as the anion and [1,2,4]triazolo[1,5-a]pyrimidine (abbreviated as tp) as the ligand are presented, together with their crystal structure and spectroscopic properties. A light blue compound [Cu(tp)4(H2O)2](BF4)2(CH3OH) (1) with a tetragonal chromophore and a dark blue compound [Cu(tp)5](BF4)2(CH3OH) (2) are formed from the same batch. Compound (2) has a quite unusual geometry for Cu(II) with just 5 tp ligands, homoleptically coordinated to the metal ion. Both compounds show interesting hydrogen-bond interactions in the solid state, where coordinated water is intramolecularly bound to non-coordinated N atoms of tp (in 1), and methanol is attached to the anion (in 2).
Graphical Abstract  Cu(II) coordination compounds with the [1,2,4]triazolo[1,5-a]pyrimidine ligand are reported, including, the [Cu(tp)5] cation with for Cu(II) just 5 tp ligands, homoleptically coordinated to the metal ion.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9713-y
  • Authors
    • Eelke D. van den Bos, Leiden University Leiden Institute of Chemistry P.O. Box 9502 2300 RA Leiden The Netherlands
    • Ilpo Mutikainen, University of Helsinki Laboratory of Inorganic Chemistry, Department of Chemistry (A.I. Virtasen aukio 1) P.O. Box 55 00014 Helsinki Finland
    • Urho Turpeinen, University of Helsinki Laboratory of Inorganic Chemistry, Department of Chemistry (A.I. Virtasen aukio 1) P.O. Box 55 00014 Helsinki Finland
    • Gerard A. van Albada, Leiden University Leiden Institute of Chemistry P.O. Box 9502 2300 RA Leiden The Netherlands
    • Jaap G. Haasnoot, Leiden University Leiden Institute of Chemistry P.O. Box 9502 2300 RA Leiden The Netherlands
    • Jan Reedijk, Leiden University Leiden Institute of Chemistry P.O. Box 9502 2300 RA Leiden The Netherlands

Source: Journal of Chemical Crystallography | 12 Feb 2010 | 8:12 am CET

Preparation, Mechanism, and Supramolecular Structure Study of a Novel Benzimidazole-Hydrate

Abstract  A novel bis[2-(2-chloro-4-fluorophenyl)-1H-Benzimidazole]-hydrate was prepared from Schiff base, and its single crystalline was obtained. The single crystalline was characterized by X-ray crystallography, and the results shows that the title complex belongs to the triclinic system, space group (P1) with lattice parameters a = 7.592(2) Å, b = 7.595(2) Å, c = 11.886 (3) Å, V = 574(3) Å3, Mr = 352.33, Dc = 1.478 g/cm3, μ(MoKα) = 0.33 mm−1, F(000) = 262, Z = 1, the final R = 0.090 and wR = 0.209 for 2,315 observed reflections (I > (I)). The crystal structure is formed by two benzimidazole molecules which are linked by a water molecule. A UV–Vis spectrophotometer and a fluorophotometer were used to detect the benzimizadole-hydrate crystal transformation process, which shows that benzimidazole-hydrate can only be formed from Schiff base effectively when ortho-hydroxyl group does not exist in benzaldehyde. The synthesis mechanism was also discussed. Compared with its Schiff base, benzimidazole-hydrate displays stronger fluorescence.
Graphical Abstract  A novel bis[2-(2-chloro-4-fluorophenyl)-1H-Benzimidazole]-hydrate was prepared, and its single crystalline was obtained and characterized. Its synthesis mechanism was also discussed briefly.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9694-x
  • Authors
    • Yong Hong, Central South University College of Chemistry and Chemical Engineering 410083 Changsha Hunan China
    • Jing-Yi Xiao, Central South University College of Chemistry and Chemical Engineering 410083 Changsha Hunan China
    • Ke-Long Huang, Central South University College of Chemistry and Chemical Engineering 410083 Changsha Hunan China
    • Jin-Gang Yu, Central South University College of Chemistry and Chemical Engineering 410083 Changsha Hunan China
    • Du-Shu Huang, Central South University College of Chemistry and Chemical Engineering 410083 Changsha Hunan China

Source: Journal of Chemical Crystallography | 6 Feb 2010 | 7:07 pm CET

Synthesis, Characterziation and SOD Activity of Manganese(II) Complexes with Aza-Macrocyclic Ligand

Abstract  Two manganese(II) complexes, [Mn2(L)(H2O)4]Cl2·6H2O(1) and [Mn2L(NCS)2(H2O)2]·3H2O(2) (L is 1,2,4-triazolato)-4,12,17,25-tetramethyl-1,2,5,8,11,14,15,18,21,24-decaza-4,11,17,24-cyclohexaeicosatetraene) have been prepared by template synthesis method. They are characterized by elemental analysis and IR. Single-crystal X-ray analysis reveals that complex (1) crystallizes in space group P 21/c with a = 8.710(3), b = 14.720(5), c = 14.301(5) Å, α = 90, β = 105.801(14), γ = 90°. The complex [Mn2(L)(H2O)4]Cl2·6H2O consists of two manganese(II) macrocyclic complexes in which two Mn(II) centers are linked by two triazolate units of the macrocyclic framework. Each manganese(II) ion is coordinated by five nitrogen atoms from the macrocycle and two oxygen atoms of the coordinated water. The manganese(II) center is in an approximately pentagonal-bipyramidal environment. The SOD activities of both complexes have also been investigated.
Graphical Abstract  This paper reports the synthesis and characterziation two manganese(II) complexes with aza-macrocyclic ligand. Their SOD activities are also studied.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9721-y
  • Authors
    • Fuliang Zhang, Hangzhou Normal University College of Material Chemistry and Chemical Engineering 310036 Hangzhou People’s Republic of China
    • Liang Shen, Hangzhou Normal University College of Material Chemistry and Chemical Engineering 310036 Hangzhou People’s Republic of China

Source: Journal of Chemical Crystallography | 6 Feb 2010 | 7:07 pm CET

Low Temperature Crystal Structure of N-Acetyl-l-Glutamic Acid: Comparison with the DFT Calculated Structure

Abstract   N-acetyl-l-glutamic acid, crystallizes in the orthorhombic space group P212121 with unit cell parameters a = 4.747(3), b = 12.852(7), c = 13.906(7) Å, V = 848.5(8) Å3, Z = 4, density (calculated) = 1.481 mg/m3, linear absorption coefficient 0.127 mm−1. The crystal structure determination was carried out with MoKα X-ray data measured with liquid nitrogen cooling at 100(2) K temperature. In the final refinement cycle the data/restraints/parameter ratios were 1,691/0/131; goodness-of-fit on F 2 = 1.122. Final R indices for [I > 2sigma(I)] were R1 = 0.0430, wR2 = 0.0878 and R indices (all data) R1 = 0.0473, wR2 = 0.0894. The largest electron density difference peak and hole were 0.207 and −0.154 eÅ−3. Details of the molecular geometry are discussed and compared with a model DFT structure calculated using Gaussian 98.
Graphical Abstract  The low temperature X-ray structure of N-acetyl-l-glutamic acid, including absolute configuration, is described. Comparison with the DFT structure is also discussed. Molecular conformation of N-acetyl-l-glutamic acid: (a) drawn with MERCURY [22] and (b) surfaces drawn with VMD [26].
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9704-z
  • Authors
    • Nighat Kausar, University of Greenwich at Medway School of Science Chatham Maritime Kent ME4 4TB UK
    • Bruce D. Alexander, University of Greenwich at Medway School of Science Chatham Maritime Kent ME4 4TB UK
    • Rex A. Palmer, University of London School of Crystallography, Birkbeck College Malet Street London WC1E 7HX UK
    • Brian S. Potter, University of London School of Crystallography, Birkbeck College Malet Street London WC1E 7HX UK
    • Trevor J. Dines, University of Dundee Division of Electronic Engineering & Physics Dundee DD1 4HN UK
    • Madeleine Helliwell, University of Manchester School of Chemistry Brunswick Street Manchester M13 9PL UK
    • Babur Z. Chowdhry, University of Greenwich at Medway School of Science Chatham Maritime Kent ME4 4TB UK

Source: Journal of Chemical Crystallography | 5 Feb 2010 | 7:17 pm CET

Synthesis and Crystal Structure of (PzCH2CHOHCH2PzH)·(Ph2SnCl3) (Pz = 3,5-dimethylpyrazol-1-yl)

Abstract  Reaction of Ph2SnCl2 with 1,3-bis(3,5-dimethylpyrazol-1-yl)-2-propanol (L) in a 1:1 ratio yields L(SnPh2Cl2)2 adduct, which partly hydrolyzes to the title complex (C25H31Cl3N4OSn, Mr = 628.58) during crystal growing in the air. The title complex is of monoclinic, space group P21/n with a = 9.0338(9), b = 17.890(1), c = 17.340(1) Å, β = 95.533(1)o, V = 2798.9(5) Å3, Z = 4, Dc = 1.492 Mg/m3, λ(Mo) = 0.71073 Å, μ = 1.224 mm−1, F(000) = 1272, R = 0.023, wR = 0.054 for 4212 observed reflections with I ≥ (I). The crystal structure indicates that there is no direct interaction between the pyrazolyl ligand and the tin atom, but this complex forms a supramolecular structure through weak intermolecular C–H⋯Cl and O–H⋯Cl hydrogen bonds.
Graphical Abstract  Reaction of Ph2SnCl2 with 1,3-bis(3,5-dimethylpyrazol-1-yl)-2-propanol (L) in a 1:1 ratio yields L(SnPh2Cl2)2 adduct, which partly hydrolyzes to (PzCH2CHOHCH2PzH)·(Ph2SnCl3) (Pz = 3,5-dimethylpyrazol-1-yl) during crystal growing in the air.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9717-7
  • Authors
    • Ji-Ting Lu, Nankai University Department of Chemistry, State Key Laboratory of Elemento-Organic Chemistry Tianjin 300071 People’s Republic of China
    • Miao Du, Tianjin Normal University College of Chemistry and Life Science Tianjin 300074 People’s Republic of China
    • Liang-Fu Tang, Nankai University Department of Chemistry, State Key Laboratory of Elemento-Organic Chemistry Tianjin 300071 People’s Republic of China

Source: Journal of Chemical Crystallography | 5 Feb 2010 | 7:17 pm CET

Structural and Spectroscopic Characterization of Mer-[RhBr3(Me2pzH)3] (Me2pzH = 3, 5-Dimethylpyrazole); Interpreting the Results with Density Functional Theory Calculations

Abstract   Mer-RhBr3(Me2pzH)3 (Me2pzH = 3,5-dimethylpyrazole) (monoclinic, P21/n, a = 8.3300 (5) Å, b = 16.2889 (9) Å, c = 15.9299 (11) Å, α = 90°, β = 100.217 (5)°, γ = 90°; V = 2,127.2 (2) Å3; Z = 4) has been characterized by X-ray diffraction, 1H and 13C nuclear magnetic resonance spectroscopy, infrared spectroscopy, and electronic absorption spectroscopy, and modeled by density functional theory (DFT) and time-dependent density functional theory (TDDFT). Mer-RhBr3(Me2pzH)3 is an octahedral complex with a HOMO → LUMO transition at 486 nm. The DFT and TDDFT calculations predicted mer-RhBr3(Me2pzH)3 to be an octahedral complex with a HOMO → LUMO transition at 540 nm.
Graphical Abstract   Mer-RhBr3(Me2pzH)3 (Me2pzH = 3,5-dimethylpyrazole) has been structurally characterized by single crystal X-ray diffraction, spectroscopically characterized, and modeled by Density Functional Theory and Time-Dependent Density Functional Theory.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9701-2
  • Authors
    • Max M. Abrahams, Brown University Department of Physics Providence RI 02912 USA
    • Gregory W. Cushing, University of Virginia Department of Chemistry McCormick Road PO Box 400319 Charlottesville VA 22904-4319 USA
    • Zachary N. Pickett, University of Alaska Fairbanks Department of Chemistry & Biochemistry 900 Yukon Drive Fairbanks AK 99775-6160 USA
    • William A. Howard, University of Alaska Fairbanks Department of Chemistry & Biochemistry 900 Yukon Drive Fairbanks AK 99775-6160 USA
    • Kraig A. Wheeler, Eastern Illinois University Department of Chemistry 600 Lincoln Avenue Charleston IL 61920-3099 USA

Source: Journal of Chemical Crystallography | 5 Feb 2010 | 7:17 pm CET

Synthesis, Crystal Structure, and Rotational Energy Profile of 3-Cyclopropyl-1,2,4-benzotriazine 1,4-Di-N-oxide

Abstract  1,2,4-Benzotriazine 1,4-di-N-oxides are potent antitumor drug candidates that undergo in vivo bioreduction leading to selective DNA damage in the low oxygen (hypoxic) cells found in tumors. Tirapazamine (TPZ) is the lead compound in this family. Here we report on the synthesis, crystal structure, and conformational analysis of a new analog, 3-cyclopropyl-1,2,4-benzotriazine 1,4-di-N-oxide (3). Compound 3 (C10H10N3O2) crystallized in the monoclinic space group C2/c. Unit cell parameters for 3: a = 16.6306 (12), b = 7.799 (5), c = 16.0113 (11) Å, α = 90, β = 119.0440 (10), γ = 90, and z = 8.
Graphical Abstract  1,2,4-Benzotriazine 1,4-di-N-oxides are antitumor drug candidates that undergo in vivo bioreduction to yield DNA-damaging radical intermediates in hypoxic tumor cells. Here we report on the synthesis, crystal structure, and conformational analysis of a new analog, 3-cyclopropyl-1,2,4-benzotriazine 1,4-di-N-oxide (3).
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9707-9
  • Authors
    • Ujjal Sarkar, University of Missouri-Columbia Department of Chemistry, 125 Chemistry Building Columbia MO 65211 USA
    • Rainer Glaser, University of Missouri-Columbia Department of Chemistry, 125 Chemistry Building Columbia MO 65211 USA
    • Zack D. Parsons, University of Missouri-Columbia Department of Chemistry, 125 Chemistry Building Columbia MO 65211 USA
    • Charles L. Barnes, University of Missouri-Columbia Department of Chemistry, 125 Chemistry Building Columbia MO 65211 USA
    • Kent S. Gates, University of Missouri-Columbia Department of Chemistry, 125 Chemistry Building Columbia MO 65211 USA

Source: Journal of Chemical Crystallography | 4 Feb 2010 | 7:14 pm CET

Synthesis and Crystal Structure of Bis 2-[(cyclohexylimino)methyl]-4,6-dihydroselenophenolcopper(II)

Abstract  
A new Schiff base complex, Bis {2-[(cyclohexylimino)methyl]-4,6-dihydroselenophenol}copper(II), has been synthesized and structurally characterized by elemental analyses and X-ray diffraction. The title complex C26H32N2O2·Se4Cu crystallizes in the monoclinic space group P21/c with the cell parameters a = 15.308(3) Å, b = 12.857(2) Å, c = 14.161(3) Å, β = 93.23(3)°, V = 2782.8(10) Å3 and Z = 4. The central Copper(II) atom is four-coordinated by two O and two N atoms from the two Schiff base ligands, 2-[(cyclohexylimino)methyl]-4,6-dihydroselenophenol, forming a distorted square-planar coordination.
Graphical Abstract  
A new Schiff base complex, Bis {2-[(cyclohexylimino)methyl]-4,6-dihydroselenophenol}copper(II), has been synthesized and structurally characterized by elemental analyses and X-ray diffraction. The central Copper(II) atom is four-coordinated by two O and two N atoms from the two Schiff base ligands, 2-[(cyclohexylimino)methyl]-4,6-dihydroselenophenol, forming a distorted square-planar coordination.
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  • Content Type Journal Article
  • Category COMMUNICATION
  • DOI 10.1007/s10870-010-9715-9
  • Authors
    • Lei Shi, Anhui University of Technology Key Laboratory of Anhui Educational Department 243002 Maanshan People’s Republic of China
    • Hai-Liang Zhu, Anhui University of Technology Key Laboratory of Anhui Educational Department 243002 Maanshan People’s Republic of China

Source: Journal of Chemical Crystallography | 4 Feb 2010 | 7:14 pm CET

Refined Crystal Structure and Absolute Configuration of the Di-amino Acid Peptide Cyclo(l-Aspartyl-l-Aspartyl): Comparison with the DFT Calculated Structure

Abstract  The X-ray crystal structure of the di-amino acid peptide cyclo(l-Asp-l-Asp), C6H10N2O4, has been re-determined at 20 °C using CuKα radiation, λ = 1.54180 Å. The crystals are triclinic P1 with unit cell dimensions a = 5.0829(3), b = 5.0285(4), c = 18.8765(10) Å, α = 88.95(2)°, β = 83.72(2)°, γ = 74.79(2)°, unit cell volume 462.75(5) Å3, and Z = 2 independent molecules A and B per asymmetric unit. Final R indices [I > 2sigma(I)] are R1 = 0.0492, wR2 = 0.1039 for 2,540 independent reflections; R1 = 0.0686 and wR2 = 0.1112 for all 3,193 data; Goodness of Fit, S = 0.979, and the Flack x parameter = 0.1(3). In both molecules the overall shape of the diketopiperazine (DKP) ring displays an almost identical slightly distorted boat conformation with pseudo symmetry C2v (mm2). The two side chains of the cyclic peptide on opposite sides of both molecules differ in their conformations, one side being extended and the other coiled. The coiled chains are located away from the DKP ring plane while the extended chains lie approximately parallel to it. The crystal packing employs two strong hydrogen bonds, which traverse the entire crystal via translational repeats. The geometry of cyclo(l-Asp-l-Asp) derived from Ab initio calculations is compared with those of molecules A and B derived from the X-ray structure reported here. In this calculated model the DKP ring is in a pseudo twist boat conformation; both side chains are extended and lie approximately parallel to the DKP ring face as opposed to molecules A and B in the X-ray structure in each of which one side chain is approximately parallel and the other is folded away from the DKP ring face.
Graphical Abstract  Cyclic di-amino acid peptides are amongst the “simplest” peptide derivatives commonly found in nature and continue to be of long-standing interdisciplinary scientific interest with respect to potential pharmaceutical applications. Cyclo(l-Asp-l-Asp) is an example of a cyclic di-amino acid peptide, which has a six membered ring, and the amide linkage adopts a cis conformation. In contrast linear (l-Asp-l-Asp) is zwitterionic and has a single amide function which adopts the trans conformation. The synthesis and an X-ray structure of cyclo(l-Asp-l-Asp) have previously been reported, the latter being assigned the wrong absolute configuration. For the purposes of the present study, requiring precise molecular geometry, it was decided to carry out a re-determination of the crystal structure using a more complete measured set of independent intensities (94% against 36%) and correspondingly improved data/parameter ratio (3193/326 against 1215/369).
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9705-y
  • Authors
    • Rex A. Palmer, University of London School of Crystallography, Birkbeck College Malet Street London WC1E 7HX UK
    • Brian S. Potter, University of London School of Crystallography, Birkbeck College Malet Street London WC1E 7HX UK
    • Andrew P. Mendham, University of Greenwich at Medway School of Science Chatham Maritime Kent ME4 4TB UK
    • Trevor J. Dines, University of Dundee Division of Electronic Engineering & Physics Dundee DD1 4HN UK
    • Babur Z. Chowdhry, University of Greenwich at Medway School of Science Chatham Maritime Kent ME4 4TB UK

Source: Journal of Chemical Crystallography | 4 Feb 2010 | 7:14 pm CET

Synthesis and Crystal Structure of Hydrate Adduct of 6-Benzylaminopurine and 5-Sulfosalicylic Acid [(C12H12N5)(C7H5O6S)·H2O]

Abstract  The crystal structure of hydrate adduct of 6-benzylaminopurine and 5-sulfosalicylic acid [(C12H12N5)(C7H5O6S)·H2O] 1 is studied. It crystallizes in monoclinic system space group P21/n with a = 6.2128(9) Å, b = 20.762(3) Å, c = 15.675(2) Å, β = 92.040(2)°, V = 2,020.6(5) Å3, Z = 4, R gt(F) = 0.0494, wR ref(F 2) = 0.1112, and T = 173(2) K. Single-crystal X-ray diffraction analysis reveals that the asymmetric unit of 1 contains one 6-benzylaminopurine molecule and one 5-sulfosalicylic acid molecule, as well as one lattice water molecule. In 1, hydrogen bonds link the two monomers into one-dimensional double chain, two-dimensional layer network, and further a 3-D supramolecular network. Short ring-interactions with intra-chain ππ stacking are observed (distances between ring centroids are 3.964, 3.796 and 3.571 Å, and the dihedral angle between planes are 6.97°, 5.55°, and 5.66°, respectively).
Graphical Abstract  A novel hydrate adduct [(C12H12N5)(C7H5O6S)·H2O] 1, has been synthesized and consists of 6-benzylaminopurine and 5-sulfosalicylic acid molecules with one lattice water molecule. The monomers connect with each other via intermolecular hydrogen bonds C(N, O)–H···O(N) to form double chain, further two-dimensional layer, at last 3-D supramolecular structure network, along with ππ interactions within 4 Å.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9709-7
  • Authors
    • Min Xia, Huaiyin Normal University Jiangsu Key Laboratory for Chemistry of Low-Dimensional Materials, School of Chemistry and Chemical Engineering 223300 Huaian Jiangsu People’s Republic of China
    • Kui-Rong Ma, Huaiyin Normal University Jiangsu Key Laboratory for Chemistry of Low-Dimensional Materials, School of Chemistry and Chemical Engineering 223300 Huaian Jiangsu People’s Republic of China
    • Yulan Zhu, Huaiyin Normal University Jiangsu Key Laboratory for Chemistry of Low-Dimensional Materials, School of Chemistry and Chemical Engineering 223300 Huaian Jiangsu People’s Republic of China

Source: Journal of Chemical Crystallography | 3 Feb 2010 | 6:58 pm CET

The Synthesis and Crystal Structure Determination of Phenyl 2-(3,4-dihydro-1(2H)naphthalenylidine)hydrazinecarboxylate and Phenyl (2,4-dichlorophenyl-methylene)hydrazinecarboxylate

Abstract  (E)-Phenyl 2-(3,4-dihydro-1(2H)-naphthalenylidine)hydrazinecarboxylate and (E)-phenyl (2,4-dichlorophenylmethylene)hydrazinecarboxylate were prepared by the condensation of 1-tetralone or 2,4-dichlorobenzaldehyde with phenyl hydrazinecarboxylate. Crystals of C17H16N2O2 3 are monoclinic, C2/c, a = 17.763(4) Å, b = 8.353(2) Å, c = 40.233(8) Å, Z = 16, V = 5,839(2) Å3, R 1 = 0.0448 and wR 2 = 0.1104 for reflections with I > 2σ(I). Crystals of C14H10N2O2Cl2 5 are orthorhombic, P212121, a = 8.288(3) Å, b = 14.082(2) Å, c = 23.788(5) Å, Z = 8, V = 2,777(1) Å3, R 1 = 0.0815 and wR 2 = 0.2006 for reflections with I > 2σ(I). The molecular packing in the crystal for both compounds is the result of N–H···O hydrogen bonding.
Index Abstract  X-ray crystal analysis was important for the confirmation of the structure of phenyl 2-(3,4-dihydro-1(2H)-naphthalenylidine)hydrazinecarboxylate and phenyl (2,4-dichlorophenylmethylene)hydrazinecarboxylate that have been prepared by the 1:1 condensation of 1-tetralone or 2,4-dichlorobenzaldehyde with phenyl hydrazinecarboxylate.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9693-y
  • Authors
    • Chandra Potter, College of Charleston Department of Chemistry and Biochemistry Charleston SC 29424 USA
    • Amy M. Rhoden Smith, College of Charleston Department of Chemistry and Biochemistry Charleston SC 29424 USA
    • Clyde R. Metz, College of Charleston Department of Chemistry and Biochemistry Charleston SC 29424 USA
    • William T. Pennington, Clemson University Department of Chemistry Clemson SC 29634 USA
    • Donald G. VanDerveer, Clemson University Department of Chemistry Clemson SC 29634 USA
    • Charles F. Beam, College of Charleston Department of Chemistry and Biochemistry Charleston SC 29424 USA

Source: Journal of Chemical Crystallography | 3 Feb 2010 | 6:58 pm CET

Hydrothermal Synthesis, Structural Characterization and Luminescent Property of a New 1-D Chain-like [Er(NC6H4O2)3(H2O)2]n

Abstract  Erbium (III) coordination compound with the formula [Er(IN)3(H2O)2]n 1 (HIN = isonicotinic acid) was synthesized by mixing Er2O3 with isonicotinic acid under hydrothermal condition. The structure of the title compound was determined by single crystal X-ray diffraction analysis, which reveals that the 1-D chain-like structure is formed by the erbium polyhedra through the carboxyl groups of IN. It crystallizes in the monoclinic system, possesses space group C2/c, with lattice parameters: a = 20.229(10) Å, b = 11.594(6) Å, c = 9.871(5) Å, α = γ=90°, β = 115.509(6)°, V = 2089.3(18) Å3, and D calc = 1.811 mg/cm3 for Z = 4, F(000) = 1108, GOF = 1.109, R1 = 0.0675. Compound 1 has been characterized by IR absorption spectroscopy, ultraviolet excitation and emission spectrum.
Graphical Abstract  Erbium (III) coordination compound with the formula [Er(IN)3(H2O)2]n 1 (HIN = isonicotinic acid) was synthesized by mixing Er2O3 with isonicotinic acid under hydrothermal condition. The single crystal X-ray diffraction analysis reveals that the 1-D chain-like structure of 1 is formed by the erbium polyhedra through the carboxyl groups of IN.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9700-3
  • Authors
    • Lijie Han, Nanjing University of Technology College of Chemistry and Chemical Engineering, State Key Laboratory of Materials-Oriented Chemical Engineering 210009 Nanjing People’s Republic of China
    • Xiaochang Sun, Nanjing University of Technology College of Chemistry and Chemical Engineering, State Key Laboratory of Materials-Oriented Chemical Engineering 210009 Nanjing People’s Republic of China
    • Yalin Zhu, Nanjing University of Technology College of Chemistry and Chemical Engineering, State Key Laboratory of Materials-Oriented Chemical Engineering 210009 Nanjing People’s Republic of China
    • Wanli Zhou, Nanjing University of Technology College of Chemistry and Chemical Engineering, State Key Laboratory of Materials-Oriented Chemical Engineering 210009 Nanjing People’s Republic of China
    • Qi Chen, Nanjing University of Technology College of Chemistry and Chemical Engineering, State Key Laboratory of Materials-Oriented Chemical Engineering 210009 Nanjing People’s Republic of China
    • Yan Xu, Nanjing University of Technology College of Chemistry and Chemical Engineering, State Key Laboratory of Materials-Oriented Chemical Engineering 210009 Nanjing People’s Republic of China

Source: Journal of Chemical Crystallography | 3 Feb 2010 | 6:58 pm CET

Synthesis, Structure and Reactivity of Electron Deficient Triosmium Cluster Bearing 2,6-Dimethylbenzothiazolide Ligand

Abstract  Reaction of [Os3(CO)10(NCMe)2] with 2,6-dimethylbenzothiazole at room temperature affords [Os3(CO)10(μ-H){μ-η 2-C7H2NS(Me)2}] (1) in 45% yield. Decarbonylation of 1 in refluxing toluene furnishes the electron-deficient cluster [Os3(CO)9(μ-H){μ 3-η 2-C7H2NS(Me)2}] (2) in almost quantitative yield. Treatment of 2 with PPh3 at 40 °C gives the addition product [Os3(CO)9(PPh3)(μ-H){μ-η 2-C7H2NS(Me)2}] (3) in 85% in which the PPh3 ligand is coordinated to the rear osmium atom. A similar treatment of 2 with P(OMe)3 gives [Os3(CO)9{P(OMe)3}(μ-H){μ-η 2-C7H2NS(Me)2}] (4) in 60% yield with P(OMe)3 ligand also coordinated to the rear metal. Compounds 3 and 4 differ by the disposition of the hydride ligands. In compound 4 both the hydride and the heterocyclic ligands simultaneously bridge the same metal–metal edge whereas they bridge different metal–metal edges in 3. Compounds 14 have been characterized by a combination of elemental analysis, infrared, NMR and mass spectral data together with single crystal X-ray diffraction studies for 3. Compound 3 crystallizes in the monoclinic space group P21/n with a = 9.2659(10), b = 23.643(2), c = 16.382(3) Å, β = 91.324(12)°, Z = 4 and V = 3,587.8(8) Å3.
Graphical Abstract  Synthesis and reactivity of electron-deficient 2,6-dimethylbenzothiazole osmium cluster [Os3(CO)9(μ-H){μ 3-η 2-C7H2NS(Me)2}] (2) are described. Reaction of 2 with PR3 (R = Ph, OMe) furnishes [Os3(CO)9(PR3)(μ-H){μ-η 2-C7H2NS(Me)2}] (3, R = Ph; 4, R = OMe) in which the PR3 ligand is coordinated to the rear osmium atom.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9699-5
  • Authors
    • Shishir Ghosh, Jahangirnagar University Department of Chemistry Savar, Dhaka 1342 Bangladesh
    • Md. Nazim Uddin, Jahangirnagar University Department of Chemistry Savar, Dhaka 1342 Bangladesh
    • Noorjahan Begum, Sher-e-Bangla Agricultural University Department of Chemistry Savar, Dhaka 1342 Bangladesh
    • G. M. Golzar Hossain, Dhaka University Department of Chemistry Savar, Dhaka 1342 Bangladesh
    • Kazi A. Azam, Jahangirnagar University Department of Chemistry Savar, Dhaka 1342 Bangladesh
    • Shariff E. Kabir, Jahangirnagar University Department of Chemistry Savar, Dhaka 1342 Bangladesh

Source: Journal of Chemical Crystallography | 2 Feb 2010 | 6:52 pm CET

Synthesis and Crystal Structure of 2D Supramolecular Compound [Co(phth)(phen) (H2O)3]·H2O

Abstract  A 2D supramolecular compound [Co(phth)(phen) (H2O)3]·H2O has been synthysized by the reactions of Co(NO3)2·6H2O, 1, 10-phenanthroline(phen) and phthalate acid(H2phth) in NaOH solution with pH 7.0.The complex has been characterized by elemental analysis, IR, and single-crystal X-ray diffraction analysis which shows it belongs the monoclinic space group P2(1)/n, a = 7.571(2) Å, b = 13.737(3) Å, c = 20.015(4) Å, β = 95.56(1)°. V = 2071.9(8) Å3, Mr = 475.31, Dc = 1.524 g/cm−3, Z = 4, F(000) = 980, μ(MoKa) = 0.879 mm−1. The final R1 and wR2 are 0.0348 and 0.0711, respectively. The cobalt(II) ion is six-coordinated in a distorted octahedron to form a unit. Every unit is connected by hydrogen bonds forming 1D chain and 2D supramolecular network by π–π stacking interaction between adjoining chains.
Graphical Abstract  The molecular structure of the title complex.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9716-8
  • Authors
    • Li Tian, Hunan University of Science and Technology School of Chemistry and Chemical Engineering 411201 Xiangtan People’s Republic of China
    • Lin Chen, Hunan University of Science and Technology School of Chemistry and Chemical Engineering 411201 Xiangtan People’s Republic of China
    • Xin Zhang, Hunan University of Science and Technology School of Chemistry and Chemical Engineering 411201 Xiangtan People’s Republic of China

Source: Journal of Chemical Crystallography | 2 Feb 2010 | 6:52 pm CET

On crack nucleation in zinc upon interaction of basal and pyramidal dislocations

Abstract  The interaction of intersecting basal and pyramidal dislocation pileups in single-crystal zinc has been analyzed. Different versions of the formation of sessile (1/3[4
-
2
 
-
2
 
3]) and cleavage ([0001]) dislocations (microcrack nuclei) are considered. The merging of the head dislocations in pyramidal pileups is shown to be preferred. The conditions for thermally activated dislocation merging are derived. The conditions for crack opening according to the Gilman-Rozhanskiĭ mechanism are discussed. It is analytically established that the breaking stress, normal to the (0001) plane in the region of microcrack nucleation, exceeds the theoretical strength.

  • Content Type Journal Article
  • Category Real Structure of Crystals
  • DOI 10.1134/S1063774510010128
  • Authors
    • V. A. Fedorov, Derzhavin State University Internatsionalnaya 33 Tambov 392000 Russia
    • Yu. I. Tyalin, Derzhavin State University Internatsionalnaya 33 Tambov 392000 Russia
    • V. A. Tyalina, Derzhavin State University Internatsionalnaya 33 Tambov 392000 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

The crystal structure of calcium aquaethylenediaminetetraacetato(3-)nickelate(II) tetrahydrate, Ca[Ni(HEdta)(H2O)]2·4H2O

Abstract  The crystal structure of Ca[Ni(HEdta)(H2O)]2 · 4H2O (HEdta 3−is a protonated anion of ethylenediaminetetraacetic acid) is determined. The unit-cell parameters are as follows: a = 7.706(1), b = 14.923(9), and c = 26.570(5) Å; V = 3055.6(2.4) Å3; Z = 8; and space group Pbcn. Crystals are shaped as tetragonal prisms and colored green, which is not characteristic of this class of compounds. The structure is built of Ca2+ cations, octahedral [Ni(HEdta)(H2O)] complex anions, and crystallization water molecules. In the complex anion, one of the acetate branches is free of coordination, whereas the remaining three branches coordinate the central atom forming glycinate metallocycles. The structure is based on sandwich layers, which are formed by networks of flat tetragonal Ca[Ni(HEdta)(H2O)]4(H2O)2 fragments adjoining one another by vertices.

  • Content Type Journal Article
  • Category Structure of Organic Compounds
  • DOI 10.1134/S1063774510010086
  • Authors
    • A. S. Antsyshkina, Russian Academy of Sciences Kurnakov Institute of General and Inorganic Chemistry Leninskiĭ pr. 31 Moscow 119991 Russia
    • G. G. Sadikov, Russian Academy of Sciences Kurnakov Institute of General and Inorganic Chemistry Leninskiĭ pr. 31 Moscow 119991 Russia
    • A. L. Poznyak, National Academy of Sciences of Belarus Institute of Molecular and Atomic Physics pr. F. Skoriny 70 Minsk 220072 Belarus
    • V. S. Sergienko, Russian Academy of Sciences Kurnakov Institute of General and Inorganic Chemistry Leninskiĭ pr. 31 Moscow 119991 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Interaction of intrinsic point defects with dislocation stress fields in hcp zirconium crystal

Abstract  The crystallographic, energetic, and kinetic characteristics of intrinsic point defects (vacancy-self-interstitial atom) in stable, metastable, and saddle configurations in hcp zirconium crystal have been calculated by the molecular-statics method. The spatial dependences of the interaction energies of intrinsic point defects and stress fields of rectilinear dislocations with Burgers vectors of 1/3[11
-
2
 
0], 1/3 [11
-
2
 
3], and [0001] have been found within the anisotropic linear theory of elasticity. The most likely trajectories of intrinsic point defects in dislocation stress fields (trajectories with minimum energy barriers for motion) have been constructed. Such trajectories result in dislocation only for the interaction of self-interstitial atoms with an edge dislocation that has a Burgers vector of 1/3 [11
-
2
 
3].

  • Content Type Journal Article
  • Category Physical Properties of Crystals
  • DOI 10.1134/S1063774510010141
  • Authors
    • V. M. Chernov, JSC “A.A. Bochvar High-Technology Research Institute of Inorganic Materials,” Moscow 123098 Russia
    • D. A. Chulkin, JSC “A.A. Bochvar High-Technology Research Institute of Inorganic Materials,” Moscow 123098 Russia
    • A. B. Sivak, JSC “A.A. Bochvar High-Technology Research Institute of Inorganic Materials,” Moscow 123098 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Nanocrystalline zinc oxide: Pyrolytic synthesis and spectroscopic characteristics

Abstract  Nanocrystalline and microcrystalline ZnO powders are synthesized by the pyrolysis of organic zinc salts in the presence of a reducing catalyst represented by a porous cellulose carrier. The specimens obtained are characterized by X-ray powder diffraction, energy dispersive analysis, scanning electron microscopy, and pulse cathodoluminescence. Lasing characteristics of the specimens are studied. The synthesis conditions, under which specimens with the crystallite morphology optimal for a low-threshold lasing are obtained, are found.

  • Content Type Journal Article
  • Category Nanomaterials
  • DOI 10.1134/S1063774510010219
  • Authors
    • L. N. Demyanets, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • L. E. Li, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • A. S. Lavrikov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • S. V. Nikitin, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Diffusion of self-point defects in body-centered cubic iron crystal containing dislocations

Abstract  The energetic, crystallographic, and diffusion characteristics of self-point defects (SPDs) (vacancies and self-interstitial atoms (SIAs)) in body-centered cubic (bcc) iron crystal in the absence of stress fields have been obtained by the molecular statics and molecular dynamics methods. The effect of elastic stress fields of dislocations on the characteristics of SPDs (elastic dipoles) has been calculated by the methods of the anisotropic linear theory of elasticity. The SPD diffusion in the elastic fields of edge and screw dislocations (with Burgers vectors 1/2 〈111〉 and 〈100〉) at 293 K has been studied by the kinetic Monte Carlo method. The values of the SPD sink strength of dislocations of different types are obtained. Dislocations are more effective sinks for SIAs than for vacancies. The difference in the sink strengths for SIAs and vacancies in the case of edge dislocations is larger than the screw dislocations.

  • Content Type Journal Article
  • Category Physical Properties of Crystals
  • DOI 10.1134/S1063774510010153
  • Authors
    • A. B. Sivak, JSC “A.A. Bochvar High-Technology Research Institute of Inorganic Materials,” Moscow 123098 Russia
    • V. A. Romanov, Leipunsky Institute of Physics and Power Engineering Russian State Research Center Obninsk, Kaluga oblast 249033 Russia
    • V. M. Chernov, JSC “A.A. Bochvar High-Technology Research Institute of Inorganic Materials,” Moscow 123098 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Structural basis for the mechanism of inhibition of uridine phosphorylase from Salmonella typhimurium

Abstract  The three-dimensional structures of three complexes of Salmonella typhimurium uridine phosphorylase with the inhibitor 2,2′-anhydrouridine, the substrate PO4, and with both the inhibitor 2,2′-anhydrouridine and the substrate PO4 (a binary complex) were studied in detail by X-ray diffraction. The structures of the complexes were refined at 2.38, 1.5, and 1.75 Å resolution, respectively. Changes in the three-dimensional structure of the subunits in different crystal structures are considered depending on the presence or absence of the inhibitor molecule and (or) the phosphate ion in the active site of the enzyme. The presence of the phosphate ion in the phosphate-binding site was found to substantially change the orientations of the side chains of the amino-acid residues Arg30, Arg91, and Arg48 coordinated to this ion. A comparison showed that the highly flexible loop L9 is unstable. The atomic coordinates of the refined structures of the complexes and the corresponding structure factors were deposited in the Protein Data Bank (their PDB ID codes are 3DD0 and 3C74). The experimental data on the spatial reorganization of the active site caused by changes in its functional state from the unligated to the completely inhibited state suggest the structural basis for the mechanism of inhibition of Salmonella typhimurium uridine phosphorylase.

  • Content Type Journal Article
  • Category Structure of Macromolecular Compounds
  • DOI 10.1134/S1063774510010098
  • Authors
    • A. A. Lashkov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • N. E. Zhukhlistova, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • S. E. Sotnichenko, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • A. G. Gabdulkhakov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • A. M. Mikhailov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Intensities of circular dichroism and absorption bands and the states of d ions in absorbing media: II. Tetrahedrally coordinated positions of d ions

Abstract  The factors affecting the band intensity in the circular dichroism (CD) and absorption spectra of tetrahedrally coordinated d ions in an absorbing medium (symmetry selection rules, structural position, and bond covalence) are analyzed. It is shown by the examples of the Cr4+ ion in Ca3Ga2Ge4O14 crystal and the Fe2+ and Fe3+ ions in SiO4 crystal that the symmetry forbiddenness of the transitions from orbitally degenerate states and the covalence of the d-ion-ligand bond lead to changes in the intensity of the corresponding CD bands in a wide range, beginning from zero. It is shown by the example of Ca3Ga2Ge4O14, LiAlGeO4, LiGaGeO4, and LiGaSiO4 crystals activated with Cr4+ ions that the preferred ion localization position corresponds to a higher effective symmetry.

  • Content Type Journal Article
  • Category Physical Properties of Crystals
  • DOI 10.1134/S1063774510010177
  • Authors
    • T. F. Veremeĭchik, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Temporal characteristics and the sign of photoacoustic effect in high-resistivity CdS crystals

Abstract  The influence of light illumination on the nonelastic properties of high-resistivity light-sensitive CdS crystals under ultrasound (the so-called photoacoustic effect (PAE)) is studied. It is shown that the crystal steady state is attained with two different characteristic times τ1 and τ21 ≪ τ2), which correspond to switching on (>1) and switching off (τ2) light, respectively. The PAE sign (i.e., the increase or decrease in the ultrasonic attenuation) under illumination is not a permanent characteristic of CdS crystals.

  • Content Type Journal Article
  • Category Physical Properties of Crystals
  • DOI 10.1134/S106377451001013X
  • Authors
    • N. A. Tyapunina, Moscow State University Moscow 119992 Russia
    • G. V. Bushueva, Moscow State University Moscow 119992 Russia
    • G. M. Zinenkova, Moscow State University Moscow 119992 Russia
    • E. K. Naimi, Moscow Institute of Steel and Alloys (State Technological University) Leninskiĭ pr. 4 Moscow 119049 Russia
    • S. S. Novikov, Moscow State University Moscow 119992 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Synthesis and crystal structure of (NH4)3[UO2(CH3COO)3]2[UO2(CH3COO)(NCS)2(H2O)]

Abstract  Single crystals of the compound (NH4)3[UO2(CH3COO)3]2[UO2(CH3COO)(NCS)2(H2O)] (I) are synthesized, and their structure is investigated using X-ray diffraction. Compound I crystallizes in the monoclinic system with the unit cell parameters a = 18.3414(6) Å, b = 16.3858(7) Å, c = 12.4183(5) Å, β = 92.992(1)°, space group C2/c, Z = 4, V = 3727.1(3) Å3, and R = 0.0253. The uranium-containing structural units of crystals I are mononuclear complexes of two types with an island structure, i.e., the [UO2(CH3COO)3] anionic complexes belonging to the crystal-chemical group (AB 301 = UO22+, B 01 = CH3COO) of the uranyl complexes and the [UO2(CH3COO)(NCS)2(H2O)] anionic complexes belonging to the crystal-chemical group AB 01M31 (A = UO22+, B 01 = CH3COO, M 1 = NCS or H2O).

  • Content Type Journal Article
  • Category Structure of Inorganic Compounds
  • DOI 10.1134/S1063774510010050
  • Authors
    • L. B. Serezhkina, Samara State University ul. Akademika Pavlova 1 Samara 443011 Russia
    • E. V. Peresypkina, Russian Academy of Sciences Nikolaev Institute of Inorganic Chemistry, Siberian Branch pr. Akademika Lavrent’eva 3 Novosibirsk 630090 Russia
    • A. V. Virovets, Russian Academy of Sciences Nikolaev Institute of Inorganic Chemistry, Siberian Branch pr. Akademika Lavrent’eva 3 Novosibirsk 630090 Russia
    • M. O. Karasev, Samara State University ul. Akademika Pavlova 1 Samara 443011 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

The electrical and structural properties of InyGa1 − yAs/InxAl1 − xAs/InP quantum wells with different InAs content

Abstract  In x Al1 − x As/In y Ga1 − y As/In x Al1 − x As/InP HEMT structures has been investigated with a change in the InAs molar fraction both in the quantum well and the buffer layer. The electrical parameters of the samples are measured at different temperatures. The structural parameters of the layers and the characteristics of the interfaces between them are determined by double-crystal X-ray diffraction. An increase in the Hall mobility and electron concentration, as well as in the structural quality of the samples, is observed alongside an increase in the InAs molar fraction in the quantum well. It is established that high electron mobility is retained at small (to 5%) mismatches between the buffer layer and substrate.

  • Content Type Journal Article
  • Category Diffraction and Scattering of Ionizing Radiations
  • DOI 10.1134/S1063774510010025
  • Authors
    • I. S. Vasil’evskiĭ, Russian Academy of Sciences Institute of Ultrahigh-Frequency Semiconductor Electronics Moscow 117105 Russia
    • G. B. Galiev, Russian Academy of Sciences Institute of Ultrahigh-Frequency Semiconductor Electronics Moscow 117105 Russia
    • V. G. Mokerov, Russian Academy of Sciences Institute of Ultrahigh-Frequency Semiconductor Electronics Moscow 117105 Russia
    • E. A. Klimov, Russian Academy of Sciences Institute of Ultrahigh-Frequency Semiconductor Electronics Moscow 117105 Russia
    • R. M. Imamov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • I. A. Subbotin, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Melt nonstoichiometry and defect structure of ZnGeP2 crystals

Abstract  The defect structure of ZnGeP2 crystals grown from a melt by the vertical Bridgman method has been investigated. A deviation of the melt composition from stoichiometric leads to the formation of striations and the inclusions of other phases which are observed as structures (chains) oriented parallel to the growth axis. According to the microanalysis data, the inclusion composition corresponds to a mixture of ZnGeP2, Zn3P2, and Ge. Nanoinclusions of germanium phosphide are detected by transmission electron microscopy. X-ray topography reveals defects of four types. The main defects in the central part of an ingot are related to the composition fluctuations, and the newly formed dislocations are basically single ones. Most dislocations are formed at the crystal periphery.

  • Content Type Journal Article
  • Category Real Structure of Crystals
  • DOI 10.1134/S1063774510010116
  • Authors
    • G. A. Verozubova, Russian Academy of Sciences Institute of Monitoring of Climatic and Ecological Systems, Siberian Branch 10/3 ave Akademicheskii Tomsk 634021 Russia
    • A. Yu. Trofimov, Russian Academy of Sciences Institute of Monitoring of Climatic and Ecological Systems, Siberian Branch 10/3 ave Akademicheskii Tomsk 634021 Russia
    • E. M. Trukhanov, Russian Academy of Sciences Institute of Semiconductor Physics, Siberian Branch pr. Akademika Lavrentéva 13 Novosibirsk 630090 Russia
    • A. V. Kolesnikov, Russian Academy of Sciences Institute of Semiconductor Physics, Siberian Branch pr. Akademika Lavrentéva 13 Novosibirsk 630090 Russia
    • A. O. Okunev, Novgorod State University ul. Sankt-Peterburgskaya 41 Veliky Novgorod 173003 Russia
    • Yu. F. Ivanov, Russian Academy of Sciences Institute of High-Current Electronics, Siberian Branch Tomsk 634021 Russia
    • P. R. J. Galtier, Groupe d’Etude de la Matière Condensée (GEMaC) UMR 8635 CNRS-Université de Versailles-Saint Quentin 45, avenue des Etats-Unis 78035 Versailles Cedex France
    • S. A. Said Hassani, Groupe d’Etude de la Matière Condensée (GEMaC) UMR 8635 CNRS-Université de Versailles-Saint Quentin 45, avenue des Etats-Unis 78035 Versailles Cedex France

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Observation of strong virtual scattering under three-beam (220, 371) X-ray diffraction in TeO2 single crystal

Abstract  A strong effect of virtual scattering has been experimentally observed when studying the nearly coplanar three-beam (220, 371) X-ray diffraction in a paratellurite single crystal under high-resolution double-crystal X-ray diffraction using MoK α1 radiation. One characteristic feature of this effect is that the angular dependence of the first (strong) reflection intensity and its shape barely change in the three-beam range of parameters, whereas very strong changes are observed for the second (weak) reflection not only in the three-beam range but also far beyond it, which is related to the variation in the two-beam diffraction parameter due to virtual scattering. The changes observed are asymmetric and make it possible to determine the triplet combination of structure-factor phases.

  • Content Type Journal Article
  • Category Diffraction and Scattering of Ionizing Radiations
  • DOI 10.1134/S1063774510010037
  • Authors
    • A. E. Blagov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • M. V. Kovalchuk, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • V. G. Kohn, Kurchatov Institute Russian Research Centre pl. Akademika Kurchatova 1 Moscow 123182 Russia
    • Yu. V. Pisarevskiĭ, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • P. A. Prosekov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Structure of octaheme cytochrome c nitrite reductase from Thioalkalivibrio nitratireducens in a complex with phosphate

Abstract  Octaheme cytochrome c nitrite reductase from Thioalkalivibrio nitratireducens (TvNiR) catalyzes the reduction of nitrite and hydroxylamine to ammonia. The structures of the free enzyme and of the enzyme in complexes with the substrate (nitrite ion) and the inhibitor (azide ion) have been solved previously. In this study we report the structures of the oxidized complex of TvNiR with phosphate and of this complex reduced by europium(II) chloride (1.8- and 2.0-Å resolution, the R factors are 15.9 and 16.7%, respectively) and the structure of the enzyme in the complex with cyanide (1.76-Å resolution, the R factor is 16.5%), which was prepared by soaking a crystal of the oxidized phosphate complex of TvNiR. In the active site of the enzyme, the phosphate ion binds to the iron ion of the catalytic heme and to the side chains of the catalytic residues Arg131, Tyr303, and His361. The cyanide ion is coordinated to the heme-iron ion and is hydrogen bonded to the residue His361. In the structure of reduced TvNiR, the phosphate ion is bound in the same manner as in the structure of oxidized TvNiR, and the nine_coordinated europium ion is located on the surface of one of the crystallographically independent monomers of the enzyme.

  • Content Type Journal Article
  • Category Structure of Macromolecular Compounds
  • DOI 10.1134/S1063774510010104
  • Authors
    • A. A. Trofimov, Russian Academy of Sciences Engelhardt Institute of Molecular Biology ul. Vavilova 32 Moscow 119991 Russia
    • K. M. Polyakov, Russian Academy of Sciences Engelhardt Institute of Molecular Biology ul. Vavilova 32 Moscow 119991 Russia
    • K. M. Boĭko, Russian Academy of Sciences Bach Institute of Biochemistry Leninskiĭ pr. 33 Moscow 119071 Russia
    • A. A. Filimonenkov, Russian Academy of Sciences Bach Institute of Biochemistry Leninskiĭ pr. 33 Moscow 119071 Russia
    • P. V. Dorovatovskiĭ, Kurchatov Center for Synchrotron Radiation and Nanotechnology pl. Akademika Kurchatova 1 Moscow 123182 Russia
    • T. V. Tikhonova, Russian Academy of Sciences Bach Institute of Biochemistry Leninskiĭ pr. 33 Moscow 119071 Russia
    • V. O. Popov, Russian Academy of Sciences Bach Institute of Biochemistry Leninskiĭ pr. 33 Moscow 119071 Russia
    • M. V. Koval’chuk, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Nanostructured crystals of fluorite phases Sr1 − xRxF2 + x (R are rare-earth elements) and their ordering: IV. Study of the optical transmission spectra in the 2–17-μm wavelength range

Abstract  Transmission spectra of two-component crystals of Sr1−x R x F2+x (R = Y, La-Lu; 0 ≤ x ≤ 0.5) in the 1–17-μm wavelength range were studied. The spectral characteristics of these crystals and of single-component crystals of MF2 (M = Ca, Sr, or Ba) and RF3 (R = La-Nd) were compared. The transmission cutoff of Sr1−x R x F2+x crystals is shifted to shorter wavelengths with increasing x. The same tendency is observed with the increasing atomic number R of rare-earth elements for two isoconcentration series of Sr1−x R x F2+x (x ∼ 0.10 and 0.28). This tendency is pronounced at large x. The transmission cutoff of Sr1−x R x F2+x crystals can be varied in the range of from 10.7 to 12.2 μm by changing their qualitative (R) and quantitative (x) composition. Hence, these crystals can be assigned to multicomponent fluoride optical materials with controlled optical characteristics. The Sr1−x R x F2+x crystals, where R = Ce-Sm, were shown to be promising materials for the design of selective optical filters in the 2–10-μm spectral range.

  • Content Type Journal Article
  • Category Physical Properties of Crystals
  • DOI 10.1134/S1063774510010189
  • Authors
    • V. A. Fedorov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • D. N. Karimov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • O. N. Komar’kova, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • E. A. Krivandina, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • Z. I. Zhmurova, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • B. P. Sobolev, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Chemical transformations in the W-Al2O3 system under pressure P = 1 bar near the melting point of aluminum oxide

Abstract  The W-Al2O3 system has been considered at a temperature of 2400 K and a pressure of 1 bar. The main chemical processes providing the interaction between the components of the system have been determined. It is shown that evaporation of Al2O3 into the gas phase gives rise to numerous reactions, which involve not only tungsten but also Al2O3 melt. It is concluded that such interactions can be reduced by decreasing the Al2O3 evaporation, which can be done by increasing the inert gas pressure. This approach makes it possible both to optimize the parameters of sapphire crystal growth and increase the lifetime of a tungsten heater and other units of crystallization systems.

  • Content Type Journal Article
  • Category Crystal Growth
  • DOI 10.1134/S1063774510010232
  • Authors
    • D. V. Kostomarov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • Kh. S. Bagdasarov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • S. A. Kobzareva, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • E. V. Antonov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

X-ray diffraction study of p-(alkoxybenzylidene)-p′-toluidines: Crystal and molecular structure of C10H21O-C6H4-CH=N-C6H4-CH3

Abstract  The crystal and molecular structure of p-(decaoxybenzylidene)-p′-toluidine C10H21O-C6H4-CH=N-C6H4-CH3 is studied. The molecule is nearly planar. In the crystal packing, loose regions formed by aliphatic fragments of molecules alternate with pseudostacks of aromatic fragments of molecules that are related by the centers of symmetry. The stacks are built of dimers, in which molecules are linked by π-stacking interactions between benzene rings. There are no weak directional interactions between dimers in a stack. The presence of a single structure-forming element in the crystal, namely, the π-stacking interactions in the dimers, along with the similarity of the crystal packing to that of the C8H17O-homologue, which forms a nematic mesophase on melting, indicate that the crystals under study should exhibit nematic properties.

  • Content Type Journal Article
  • Category Structure of Organic Compounds
  • DOI 10.1134/S1063774510010074
  • Authors
    • L. G. Kuz’mina, Russian Academy of Sciences Kurnakov Institute of General and Inorganic Chemistry Leninskiĭ pr. 31 Moscow 119991 Russia
    • N. S. Kucherepa, Russian Academy of Sciences Kurnakov Institute of General and Inorganic Chemistry Leninskiĭ pr. 31 Moscow 119991 Russia
    • S. A. Syrbu, Ivanovo State University Faculty of Chemistry and Biology ul. Yermaka 39 Ivanovo 153025 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Crystallography of real nuclei during crystallization

Abstract  Refined expressions are suggested to calculate the critical sizes of crystal nuclei and the processes of their formation during liquid-phase crystallization with due regard for the crystallographic indices of faces and the directions of solid phase formation in the initial stage, as well as the unit-cell parameters, lattice types, and geometry of linear defects.

  • Content Type Journal Article
  • Category Crystal Growth
  • DOI 10.1134/S1063774510010220
  • Authors
    • V. D. Aleksandrov, Donbass National Academy of Civil Engineering and Architecture Makeyevka, Donetsk oblast 86123 Ukraine
    • N. V. Schebetovskaya, Donbass National Academy of Civil Engineering and Architecture Makeyevka, Donetsk oblast 86123 Ukraine

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Laboratory X-ray microtomographs with the use of monochromatic radiation

Abstract  The possibility and expediency of designing X-ray microtomographs based on X-ray diffractometers have been analyzed. Some biomedical objects have been investigated. It has been demonstrated that it is possible to achieve a resolution of the order 10 μm with a field of view of the order of 20 mm without recourse to magnifying X-ray optical elements.

  • Content Type Journal Article
  • Category Instruments and Equipment
  • DOI 10.1134/S1063774510010244
  • Authors
    • V. E. Asadchikov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • A. V. Buzmakov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • D. A. Zolotov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • R. A. Senin, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • A. S. Geranin, Moscow State Institute of Electronics and Mathematics Bol’shoĭ Trekhsvyatitel’skiĭ per. 3 Moscow 109028 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Estimation of the characteristic parameters of the multilayered film model using the patterson differential function

Abstract  The possibility of estimating the layered film structural parameters by constructing the autocorrelation function P F (z) (referred to as the Patterson differential function) for the derivative /dz of electron density along the normal to the sample surface has been considered. An analytical expression P F (z) is presented for a multilayered film within the box model of the electron density profile. The possibilities of selecting structural information about layered films by analyzing the features of this function are demonstrated by model and real examples, in particular, by applying the method of shifted systems of peaks for the function P F (z).

  • Content Type Journal Article
  • Category Surface and Thin Films
  • DOI 10.1134/S1063774510010190
  • Authors
    • S. B. Astaf’ev, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • B. M. Shchedrin, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • L. G. Yanusova, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Influence of surface topography on the multilayer film formation

Abstract  The relationship between the topography of substrates and multilayer films deposited on these substrates (which are used in ring laser gyroscopes) has been investigated. The surfaces were studied by atomic-force microscopy. The statistical properties of the surface topography are analyzed within the approach based on a comparative analysis of the power spectral density functions of roughness calculated for the substrate and film. The degree of correlation between the substrate nanotopography and multilayer film is determined, and the influence of the substrate roughness on the optical characteristics of the deposited mirrors is established.

  • Content Type Journal Article
  • Category Surface and Thin Films
  • DOI 10.1134/S1063774510010207
  • Authors
    • Yu. V. Grishchenko, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • M. L. Zanaveskin, Russian Research Centre Kurchatov Institute pl. Akademika Kurchatova 1 Moscow 123182 Russia
    • A. L. Tolstikhina, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Growth conditions and electrical properties of KDP crystals: II. Dielectric permittivity measurements

Abstract  The dielectric properties of potassium dihydrophosphate single crystals, which were grown from crystallization solutions at different pH, have been studied. The dielectric response of the single crystals is shown to vary substantially depending on the growth conditions and can be significantly different for samples from different growth sectors of the same single crystals and even within one sector. The results of this study are useful for optimizing the growth conditions of these single crystals.

  • Content Type Journal Article
  • Category Physical Properties of Crystals
  • DOI 10.1134/S1063774510010165
  • Authors
    • E. D. Yakushkin, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskĭĭ pr. 59 Moscow 119333 Russia
    • E. P. Efremova, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskĭĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

The crystal structure of aluminium, iron (III), and gallium acid phosphites

Abstract  The structures of three acid phosphites of trivalent metals [Al(HPO3H)3(H2O)] · H2O (I), K[Fe(HPO3H4)] (II), and Rb3[Ga(HPO3H)6] (III) have been determined. Structure I is layered, complex anions [Fe(HPO3H)4] form polymer chains in structure II, and structure III is insular.

  • Content Type Journal Article
  • Category Structure of Inorganic Compounds
  • DOI 10.1134/S1063774510010049
  • Authors
    • B. S. Zakharova, Russian Academy of Sciences Kurnakov Institute of General and Inorganic Chemistry Leninskiĭ pr. 31 Moscow 119991 Russia
    • A. B. Ilyukhin, Russian Academy of Sciences Kurnakov Institute of General and Inorganic Chemistry Leninskiĭ pr. 31 Moscow 119991 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Synthesis and crystal structure of Pb3[IO3]2Cl4, a representative of a new iodate-chloride class of compounds

Abstract  Compound Pb3[IO3]2Cl4 (space group C12/c1), representing a new iodate-chloride class of compounds, is synthesized under hydrothermal conditions. Only two minerals, schwartzembergite Pb3[IO3]Cl2O(OH) and seeligerite Pb3[IO3]Cl3O, the structures of which are unknown, are close in composition to this compound. In the iodate-chloride studied, the pentavalent iodine atom has an umbrella-like coordination, which is typical of iodates and consists of three O atoms at short distances and the fourth O atom at a longer distance. [IO4]3− tetrahedra share edges to form pairs. Lead ions form layers parallel to the ab plane. Along the c axis, these layers alternate with layers of iodate groups. Pb atoms are coordinated by O atoms of iodate groups and Cl atoms. The coordination sphere of the Pb(1) atom contains a free sector which is directed to more distant halogen atoms and possibly accommodates the lone electron pair.

  • Content Type Journal Article
  • Category Structure of Inorganic Compounds
  • DOI 10.1134/S1063774510010062
  • Authors
    • E. L. Belokoneva, Moscow State University Faculty of Geology Moscow 119992 Russia
    • O. V. Dimitrova, Moscow State University Faculty of Geology Moscow 119992 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

Partition of the probability space formally related to isomorphism of minerals

Abstract  A formally axiomatic approach to the phenomenon of isomorphism is considered. Empirical facts of isomorphism are investigated as subsets. The wide spread of isomorphism has the property ∀xP(x). The construction of subsets in the “main element-impurity element” coordinates revealed a structure that made it possible to statistically estimate the symmetry and dissymmetry of elements of this structure, construct the probability space (ω, ℱ, P), and divide this space into sectors reflecting the dimension of atomic/ionic radii.

  • Content Type Journal Article
  • Category Theory of Crystal Structures
  • DOI 10.1134/S1063774510010013
  • Authors
    • E. V. Kolonichenko, Vernadsky State Geological Museum of the Russian Academy of Sciences Moscow 125009 Russia

Source: Crystallography Reports | 2 Feb 2010 | 7:44 am CET

A Six-Connected 3D Europium Coordination Polymer Assembled by 5-Bromoisophthalic Acid (H2BIPA) and 1,10-Phenanthroline (phen): Synthesis, Characterization and Luminescent Property

Abstract  A novel three-dimensional coordination polymer, [Eu2(phen)2(BIPA)3]·2H2O (1) (BIPA = 5-bromoisophthalate), has been synthsized by the reaction 5-bromoisophthalic acid with Eu(NO3)3·6H2O under the hydrothermal conditions and characterized by IR, elemental analysis and single crystal X-ray diffraction. Complex 1 crystallizes in the triclinic space group Pī and affords a three-dimensional (3D) six-connected α-Po network. Complex 1 showed the characteristic emission spectra of the EuIII and appeared to have good fluorescence properties.
Graphical Abstract  Synthesis, crystal structure and photophysical property of europium coordination polymer assembled by 5-bromoisophthalic acid (H2BIPA) and 1,10-phenanthroline (phen) A novel three-dimensional coordination polymer, [Eu2(phen)2(BIPA)3]·2H2O (1) (BIPA = 5-bromoisophthalate), has been synthsized by the reaction 5-bromoisophthalic acid with Eu(NO3)3·6H2O under the hydrothermal conditions and characterized by IR, elemental analysis and single crystal X-ray diffraction. Complex 1 crystallizes in the triclinic space group Pī and affords a three-dimensional (3D) six-connected α-Po network. The photophysical property of 1 was investigated.
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  • Content Type Journal Article
  • Category Communication
  • DOI 10.1007/s10870-010-9720-z
  • Authors
    • Guang-Xiang Liu, Anqing Normal University Anhui Key Laboratory of Functional Coordination Compounds, College of Chemistry and Chemical Engineering 246003 Anqing People’s Republic of China
    • Rong-Yi Huang, Anqing Normal University Anhui Key Laboratory of Functional Coordination Compounds, College of Chemistry and Chemical Engineering 246003 Anqing People’s Republic of China
    • Liang-Fang Huang, Anqing Normal University Anhui Key Laboratory of Functional Coordination Compounds, College of Chemistry and Chemical Engineering 246003 Anqing People’s Republic of China
    • Heng Xu, Anqing Normal University Anhui Key Laboratory of Functional Coordination Compounds, College of Chemistry and Chemical Engineering 246003 Anqing People’s Republic of China
    • Xiao-Ming Ren, Anqing Normal University Anhui Key Laboratory of Functional Coordination Compounds, College of Chemistry and Chemical Engineering 246003 Anqing People’s Republic of China

Source: Journal of Chemical Crystallography | 1 Feb 2010 | 7:07 pm CET

The Structure of the Antioxidant 2,3,4-Trihydroxybenzoic Acid Dihydrate

Abstract  The structure of 2,3,4-trihydroxybenzoic acid dihydrate has been determined at 120 K from a twinned crystal. The compound crystallizes in the centrosymmetric space group
\textP
-
1
 
with Z = 2 and unit cell parameters a = 6.6165(14), b = 7.2341(14), c = 9.716(2) Å, α = 75.632(16), β = 76.818(17), γ = 77.520(16)°. There is extensive hydrogen bonding within the structure and evidence for intermolecular π–π interactions between parallel aromatic rings. The compound does not display the familiar carboxylic acid hydrogen-bonded dimer found in many similar compounds. The 2,3,4-trihydroxybenzoic acid molecules are however arranged in a head-to-tail chain and linked through two water molecules in an unusual intermolecular hydrogen bonding motif.
Graphical Abstract  The crystal structure of naturally occurring phenolic antioxidant 2,3,4-trihydroxybenzoic acid dihydrate was determined at 120 K from a twinned crystal.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9708-8
  • Authors
    • Timothy J. Prior, University of Hull Department of Chemistry Kingston upon Hull HU6 7RX UK
    • Andrew J. Sharp, University of Hull Department of Chemistry Kingston upon Hull HU6 7RX UK

Source: Journal of Chemical Crystallography | 1 Feb 2010 | 7:07 pm CET

Crystal Structures of Trinuclear Chlorido(N,N′-diethylthiourea)copper(I) and a Second Polymorph of Iodidotris(N,N′-diethylthiourea)copper(I)

Abstract  Reactions of N,N′-diethylthiourea (Detu) with copper(I) cyanide and copper(I) iodide in a 2:1 M ratio in acetonitrile resulted in the formation of [Cu(Detu)Cl]3·(CH3CN)0.5 (1) and [Cu(Detu)3I] (2), respectively. In compound 1 each copper atom is coordinated with one sulfur atom of Detu and with one chloride ion forming a centrosymmetric trinuclear core (Cu3S3Cl3) that exhibits a Cu–Cu separation of 2.7383(5) Ǻ indicating the existence of cuprophilic interactions. Complex 2 crystallizes with two independent molecules per asymmetric unit. Each copper atom is coordinated with three sulfur atoms of Detu and with one iodide ion in a tetrahedral arrangement.
Graphical Abstract  Reactions of N,N′-diethylthiourea (Detu) with copper(I) cyanide and copper(I) iodide in a 2:1 M ratio in acetonitrile resulted in the formation of [Cu(Detu)Cl]3·(CH3CN)0.5 (1) and [Cu(Detu)3I] (2), respectively. In compound 1 each copper atom is coordinated with one sulfur atom of Detu and with one chloride ion forming a centrosymmetric trinuclear core (Cu3S3Cl3) that exhibits a Cu–Cu separation of 2.7383(5) Ǻ indicating the existence of cuprophilic interactions. Complex 2 crystallizes with two independent molecules per asymmetric unit. Each copper atom is coordinated with three sulfur atoms of Detu and with one iodide ion in a tetrahedral arrangement.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9710-1
  • Authors
    • Saeed Ahmad, University of Engineering and Technology Department of Chemistry Lahore 54890 Pakistan
    • Muhammad Altaf, University of Neuchâtel Institute of Physics rue Emile-Argand 11 2009 Neuchâtel Switzerland
    • Helen Stoeckli-Evans, University of Neuchâtel Institute of Physics rue Emile-Argand 11 2009 Neuchâtel Switzerland
    • Tobias Rüffer, Technische Universität Chemnitz Lehrstuhl für Anorganische Chemie, Institut für Chemie Straβe der Nationen 62 09111 Chemnitz Germany
    • Heinrich Lang, Technische Universität Chemnitz Lehrstuhl für Anorganische Chemie, Institut für Chemie Straβe der Nationen 62 09111 Chemnitz Germany
    • Muhammad Mufakkar, Government College University Department of Chemistry Lahore Pakistan
    • Abdul Waheed, Government College University Department of Chemistry Lahore Pakistan

Source: Journal of Chemical Crystallography | 1 Feb 2010 | 7:07 pm CET

Crystal Structure of [Zn(2-Bromobenzoato)2]n and [Zn(2-Bromobenzoato)2(N-Methylnicotinamide)]2

Abstract  The syntheses and structural characterizations of two novel 2-bromobenzoatozinc(II) complexes—[Zn(2-BrC6H4COO)2] n (I) and [Zn(2-BrC6H4COO)2(mnad)]2 (II), where mnad is N-methylnicotinamide are reported. Compound (I) crystallized with a monoclinic lattice (space group P21/c) and is polymeric in solid state. Its cell parameters are: a = 7.37220(10) Å, b = 19.9639(3) Å, c = 30.2756(5) Å, β = 94.7510(7)°, V = 4440.59(12) Å3, Z = 4. The coordination environments of all zinc atoms are distorted tetrahedra built from four carboxylate oxygen atoms coming from four 2-bromobenzoato ligands. Compound (II) crystallized with a monoclinic lattice (space group P21/c) with a = 11.7488(2) Å, b = 20.3683(3) Å, c = 9.30130(10) Å, β = 100.3941(11)°, V = 2189.30(5) Å3, Z = 2. This dimeric molecule features a paddle-wheel [Zn2O8] cage in solid state; the coordination environment of the central atom is square pyramidal consisting of four carboxylate oxygen atoms and the pyridine N atom of the mnad ligand.
Graphical Abstract  Two new compounds [Zn(2-bromobenzoato)2] n and [Zn(2-bromobenzoato)2(N-methylnicotinamide)]2 have been prepared and structurally characterized by X-ray single crystal diffraction.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9712-z
  • Authors
    • Annamária Krajníková, P. J. Šafárik University Institute of Chemistry Moyzesova 11 041 54 Košice Slovak Republic
    • Róbert Gyepes, Charles University Department of Inorganic Chemistry, Faculty of Science Albertov 8 128 43 Praha 2 Czech Republic
    • Katarína Győryová, P. J. Šafárik University Institute of Chemistry Moyzesova 11 041 54 Košice Slovak Republic

Source: Journal of Chemical Crystallography | 1 Feb 2010 | 7:07 pm CET

Synthesis and Spectral Studies on N,N,N′,N′-Tetramethylethylenediamine Adducts of Bis(4-methylpiperidinecarbodithioato-S,S′)M(II) (M = zinc, cadmium): Single Crystal X-Ray Structure of Bis(4-methylpiperidinecarbodithioato-S,S′) (N,N,N′,N′-Tetramethylethylenediamine)zinc(II)

Abstract  Bis(4-methylpiperidinecarbodithioato-S,S′)(N,N,N′,N′-tetramethylethylenediamine)zinc(II), [Zn(4-mpipdtc)2(TMED)] (1) and bis(4-methylpiperidinecarbodithioato-S,S′)(N,N,N′,N′-tetramethylethylenediamine)cadmium(II), [Cd(4-mpipdtc)2(TMED)] (2) adducts were synthesized and characterized by IR and NMR (1H and 13C) spectra. A single crystal X-ray structural analysis was carried out for complex 1. IR spectra of the complexes show the contribution of the thioureide form to the structures. Reduction in νC–N(thioureide) for the adducts is attributed to the change in coordination number from four to six. In the 13C NMR spectra, the downfield shift of NCS2 carbon signal for 2 (205.20 ppm) from the chemical shift value of 1 (202.05 ppm) in due to large size of cadmium ion in 2 experiences less steric effect involved in transformation from tetrahetral to octahedral. Single crystal X-ray structural analysis of 1 showed that zinc is in a distorted octahedral environment with a ZnS4N2 chromophore. The Zn–S distances in 1 are longer than those in parent [Zn(4-mpipdtc)2]. The acceptance of an additional neutral ligand by the [Zn(4-mpipdtc)2] to form an octahedral adduct causes an increase in the Zn–S bond lengths and a consequent lowering of the S–Zn–S bite angle. The piperidine ring in the dithiocarbamate fragment is in the normal chair conformation.
Graphical Abstract  Bis(4-methylpiperidinecarbodithioato-S,S′)(N,N,N′,N′-tetramethylethylene-diamine)zinc(II) (1), and bis(4-methylpiperidinecarbodithioato-S,S′)(N,N,N′,N′-tetramethylethylene- diamine)cadmium(II) (2) were synthesized and characterized by IR and NMR (1H and 13C) spectra and the structure of 1 was determined by single crystal X-ray crystallography.
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  • Content Type Journal Article
  • Category Original paper
  • DOI 10.1007/s10870-010-9686-x
  • Authors
    • N. Srinivasan, Annamalai University Department of Chemistry Annamalainagar 608 002 Tamil Nadu India
    • S. Thirumaran, Annamalai University Department of Chemistry Annamalainagar 608 002 Tamil Nadu India
    • Sabeta Kohli, University of Jammu X-Ray Crystallography Laboratory, Department of Physics Jammu Tawi 180 006 India
    • Rajnikant, University of Jammu X-Ray Crystallography Laboratory, Department of Physics Jammu Tawi 180 006 India

Source: Journal of Chemical Crystallography | 1 Feb 2010 | 7:07 pm CET

Poly (Isonicotinic Acid N-Oxide–Isonicotinate-N-Oxide-Chloro-Uranyl): The Interpenetrating Grids Created by Coordination and Hydrogen Bonds

Abstract  The building blocks of the title compound, [UO2 2+·Cl·(C6H4NO3) · (C6H5NO3)]n–uranyl fragment, chloride ion, one deprotonated isonicotinate N-oxide and one isonicotinic acid N-oxide, are arranged in the complicated three dimensional network by means of both coordination and hydrogen bonds. The uranium ion is seven-coordinated, in the fashion intermediate between the pentagonal bipyramid and capped octahedron. The coordination one-dimensional polymer chains are connected by strong carboxyl—carboxyl hydrogen bonds into two dimensional grids. These grids interpenetrate each other like the chain-links.
Graphical Abstract  The coordination one-dimensional polymer chains are connected by strong carboxyl—carboxyl hydrogen bonds into two dimensional grids, which interpenetrate each other like the chain-links.
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  • Content Type Journal Article
  • Category Original Paper
  • DOI 10.1007/s10870-010-9711-0
  • Authors
    • Stefan Lis, Adam Mickiewicz University Department of Chemistry Grunwaldzka 6 60-780 Poznań Poland
    • Zbigniew Glatty, Adam Mickiewicz University Department of Chemistry Grunwaldzka 6 60-780 Poznań Poland
    • Guenther Meinrath, RER Consultants Schiessstattweg 3a D-94032 Passau Germany
    • Maciej Kubicki, Adam Mickiewicz University Department of Chemistry Grunwaldzka 6 60-780 Poznań Poland

Source: Journal of Chemical Crystallography | 1 Feb 2010 | 7:07 pm CET

Vsevolod Vladimirovich Gladkiĭ (January 2, 1934–December 25, 2008)

Vsevolod Vladimirovich Gladkiĭ (January 2, 1934–December 25, 2008)

  • Content Type Journal Article
  • Category Obituaries
  • DOI 10.1134/S1063774509060285

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Nina Georgievna Furmanova (On the occasion of her 70th birthday)

Nina Georgievna Furmanova (On the occasion of her 70th birthday)

  • Content Type Journal Article
  • Category Jubilees
  • DOI 10.1134/S1063774509060261

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Mikhail Grigor’evich Mil’vidskiĭ (August 2, 1932–April 22, 2009)

Mikhail Grigor’evich Mil’vidskiĭ (August 2, 1932–April 22, 2009)

  • Content Type Journal Article
  • Category Obituaries
  • DOI 10.1134/S1063774509060273

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Dispersion equation for polaritons at the interface between an optically uniaxial crystal and isotropic medium

Abstract  A compact analytical representation for the dispersion equation, which determins the propagation velocity of surface polaritons in an arbitrarily oriented interface between an optically uniaxial crystal and isotropic medium, is proposed. The equation obtained is reduced to a rational fourth-order equation with respect to the square of velocity. The approximate form of this equation for the limiting case (the medium adjacent to a crystal is a metal with a high complex permittivity) coincides with the result following from the Leontovich impedance approximation.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060078
  • Authors
    • V. N. Lyubimov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • A. Radowicz, Kielce University of Technology 25-314 Kielce Poland

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Autowave model of crystal plasticity: Macro- and microdefects

Abstract  A new approach to the problem of the plastic flow of solid crystals is proposed. This approach is based on studying the macroscopic localization patterns of plastic deformation, which can be considered as different types of autowave processes of defect self-organization. An unambiguous correspondence between the localization patterns and stages of plastic flow in single crystals and polycrystals is established. The propagation velocity of localized plasticity autowaves is inversely proportional to the strain-hardening coefficient, and the dispersion relation is quadratic. A new model is proposed to describe the development of plastic flow localization.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060169
  • Authors
    • L. B. Zuev, Russian Academy of Sciences Institute of Strength Physics and Materials Science, Siberian Branch Tomsk 634021 Russia
    • S. A. Barannikova, Russian Academy of Sciences Institute of Strength Physics and Materials Science, Siberian Branch Tomsk 634021 Russia
    • V. I. Danilov, Russian Academy of Sciences Institute of Strength Physics and Materials Science, Siberian Branch Tomsk 634021 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

A statistical description of dislocation mobility at stresses close to the threshold of unlocking from the atmosphere of adsorbed impurities

Abstract  A model is developed to describe the effect of impurities adsorbed by dislocation cores on the dislocation mobility in materials with a high potential relief (Peierls barriers). It is shown that the statistical fluctuations in the impurity distribution, which are due to the adsorption randomness, significantly change the conditions of dislocation kink formation. This model explains and describes the qualitative phenomenon experimentally found in semiconductor crystals: the immobilization of dislocations at stresses σ below a certain threshold value σ unl (σ < σ unl ). An analytical solution is obtained based on an analogy with the well-studied and urgent problem of calculating the ruin probability for insurance or other financial companies in the mathematical theory of mass service. A slight generalization of the methods developed in the theory made it possible to calculate the degree of “spread” of the threshold stress due to the random character of impurity distribution as well.

  • Content Type Journal Article
  • DOI 10.1134/S106377450906011X
  • Authors
    • B. V. Petukhov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Multiwave diffraction, phase problem, and extinction in imperfect crystals

Abstract  The extinction effects of multiwave diffraction in imperfect crystals have been investigated. It is shown that the presence of extinction in the direct diffraction channel may lead to errors in determining the relative phases of structural amplitudes by the multiwave diffraction method (i.e., by interference with indirect excitation). The reason is that the dependence of the reflection intensity on the structural amplitude in imperfect crystals is generally nonquadratic (as in the kinematic theory), nonlinear (as in the dynamic theory), and is not even somewhat intermediate. These effects open up new possibilities for using multiwave diffraction for the direct study of the extinction and, therefore, quantitatively characterize the imperfection of crystal structures with known values and phases of structural amplitudes.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060054
  • Authors
    • V. E. Dmitrienko, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Self-blocking of dislocations: A new concept

Abstract  The effect of self-blocking (transformation of dislocations at zero external stress from sliding configurations into blocked ones) was theoretically predicted and then found in Ni3(Al, Nb) and TiAl alloys. The physical reasons for self-blocking are revealed. The thermally activated dislocation flip from a shallow potential relief valley into a deep one is shown to be the controlling process. It occurs through the formation of a double kink with its subsequent reorientation, leading to the formation of an asymmetric kink and the extension of dislocation along the preferred direction. The driving force of this process is calculated and its conditions are formulated. It is shown on the basis of a set of experimental data that the multivalley character of the potential relief plays a key role in the dislocation blocking and self-blocking. It is proven that both effects—the yield stress anomaly and self-blocking—have the same nature: a two-valley potential relief of dislocation.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060121
  • Authors
    • B. A. Greenberg, Russian Academy of Sciences Institute of Metal Physics, Ural Division Yekaterinburg 620041 Russia
    • M. A. Ivanov, National Academy of Sciences of Ukraine Kurdjumov Institute of Metal Physics Kiev Ukraine

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Physical aspects of the structure and function of helicases as rotary molecular motors

Abstract  Helicases were shown to have common physical properties with rotary molecular motors, such as F 0 F 1-ATP synthase and type I restriction-modification (RM) enzymes. The necessary conditions for action of molecular motors are chirality, the presence of the C 2 (or lower) symmetry axis within rather large atomic groups, and polarization properties. The estimates were made for the material parameters of helicases, which translocate DNA due to moving chiral kinks without DNA cleavage and are characterized by higher viscosity, low mobility, and smaller chiral kinetic coefficients than type II RM enzymes. This paper discusses the efficiency of helicases with opposite polarities that drive DNA translocation in opposite directions.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060042
  • Authors
    • S. A. Pikin, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Storage of dislocations during plastic deformation of polycrystalline copper-manganese solid solutions

Abstract  The regularities of dislocation storage during the deformation of homogeneous polycrystalline solid solutions with different degrees of solid-solution hardening have been studied and described. The effect of alloy concentration and test temperature is considered. The role of different dislocation density components (average scalar dislocation density, excess density, and dislocation density in walls and cells) is selected. Particular attention has been paid to the parameters of cellular substructure measured at different test temperatures and alloying concentrations. The important role of the solid-solution hardening in the regularities of dislocation storage is established.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060182
  • Authors
    • É. V. Kozlov, Tomsk State University of Architecture and Building Tomsk 634003 Russia
    • L. I. Trishkina, Tomsk State University of Architecture and Building Tomsk 634003 Russia
    • N. A. Koneva, Tomsk State University of Architecture and Building Tomsk 634003 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Internal friction and physicomechanical properties of solids

Abstract  Different aspects of applying the physical acoustics methods (in particular, internal friction method) in mechanics, optics, and radiation solid-state physics are considered. The results of acoustic experiments in situ upon plastic deformation and under the irradiation of crystals by high-energy (8 MeV) protons are discussed. The acoustic technique for studying the microplasticity of solids in a wide range of vibrational stress amplitudes is described. An example of studying the acoustooptic interactions in the defect structure of a wide-gap HgI2 semiconductor crystal is shown. The possibility of using acoustic measurements for investigating the mechanisms of brittle-ductile transition in bcc alloys is discussed.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060170
  • Authors
    • B. K. Kardashev, Russian Academy of Sciences Ioffe Physical Technical Institute Politekhnicheskaya ul. 26 St. Petersburg 194021 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Local reversible martensitic transformations as mechanisms of crystal deformation and reorientation in fcc metals

Abstract  The results of studying the new mechanisms of crystal lattice deformation and reorientation—forward + reverse (over alternative systems) martensitic transformations in fcc metals (pure metals, austenitic steels, Ni3Al alloys)—are generalized. The experimental results lying in the basis of the concepts developed are briefly reviewed. The atomic models of these transformations are presented. The mechanisms proposed make it possible to describe in a unified way a number of plastic deformation phenomena: dislocation nucleation, mechanical twinning, and the formation of strain localization bands with high-angle misorientation boundaries.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060145
  • Authors
    • A. N. Tyumentsev, Russian Academy of Sciences Institute of Strength Physics and Materials Science, Siberian Branch Tomsk 634021 Russia
    • A. D. Korotaev, Tomsk State University Tomsk 634050 Russia
    • V. M. Chernov, Bochvar High-Technology Research Institute of Inorganic Materials Moscow 123098 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Band intensities in the circular dichroism and absorption spectra and the states of d ions in absorbing media: I. Octahedrally coordinated positions of d ions

Abstract  The factors affecting the band intensity in circular dichroism (CD) and absorption spectra (selection rules, point group of structural position, and the electron density of the ground state of octahedrally coordinated d ion in absorbing medium) are considered. The intensities of CD and absorption bands are calculated and compared with the experimental data. It is shown that the differences in the spatial inversion of the electric- and magnetic-dipole moment transformations lead to a more rigorous validity of the symmetry selection rules and increase the resolution of peaks and transparency window of medium absorption in CD spectra (in contrast to absorption ones). Some criteria for estimating the valence and structural states of d ions are formulated.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060248
  • Authors
    • T. F. Veremeĭchik, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Grain boundary faceting-roughening in Zn

Abstract  The change in the grain-boundary (GB) shape with an increase in temperature near the GB faceting-roughening phase transition has been studied. The GB facet length decreases with an increase in temperature to complete facet disappearance. The facet orientation is determined by the constrained coincidence site lattice (CCSL). Facets are located along close-packed CCSL planes. Above the roughening temperature T R, the tangents to the faceted and rough GB portions at the point of emergence of the first-order ridge are located along the close-packed CCSL planes (as facets below T R). The faceting-roughening phase transition is reversible. The presence of temperature hysteresis is indicative of first-order phase transition.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060236
  • Authors
    • B. B. Straumal, Russian Academy of Sciences Institute of Solid State Physics Chernogolovka, Moscow oblast 142432 Russia
    • A. S. Gornakova, Russian Academy of Sciences Institute of Solid State Physics Chernogolovka, Moscow oblast 142432 Russia
    • V. G. Sursaeva, Russian Academy of Sciences Institute of Solid State Physics Chernogolovka, Moscow oblast 142432 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Crowdions in elasticity theory

Abstract  A crowdion, which is a defect in a crystal structure, is described within the mechanics of continuous linear elastic medium. In the continual approximation, the crowdion is defined, analogously with dislocations, as a singular “carrier” of the plastic deformation of the medium and as a source of elastic deformation. The geometric and force parameters of this singularity are associated with the characteristics of the lattice crowdion. The structure of the strain and stress fields of a crowdion in an anisotropic elastic continuum is described in the general form, and explicit expressions for these fields in an isotropic medium are derived.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060133
  • Authors
    • V. D. Natsik, National Academy of Sciences of Ukraine B. Verkin Institute for Low Temperature Physics and Engineering Kharkov 61103 Ukraine
    • S. N. Smirnov, National Academy of Sciences of Ukraine B. Verkin Institute for Low Temperature Physics and Engineering Kharkov 61103 Ukraine

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Bulk and surface components of electric influence on the magnetoplasticity

Abstract  The influence of weak electric fields on the magnetically induced mobility of individual dislocations in NaCl crystals has been investigated. It is shown that the strong influence of an electric field on the magnetoplasticity, which is caused by the transformation of impurity centers at dislocations from the diamagnetic state (Me ++) to the paramagnetic state (Me +), has both bulk and surface components. The surface effect dominates over the bulk one in weak electric fields (E < 0.5 kV/m), which are insufficient for the exciting bulk electromigration of charged defects near dislocations. However, the contribution of the surface effects becomes insignificant in comparison with the bulk processes in stronger fields E. Lacquering crystal faces to block the surface electromigration of defects excludes this stimulation component at any E. It is shown that dislocation motions occurring due to a rapid switching on an electromagnet also disappear in lacquered samples. These effects observed may be related to the same surface electromigration of defects under the vortex electric fields induced by switching on a magnetic field.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060091
  • Authors
    • V. I. Alshits, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • E. V. Darinskaya, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • E. A. Petrzhik, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

1D electro-elastic fields in piezoelectrics excited by intrinsic strains

Abstract  The electro-elastic fields induced by the transversely 1D distribution of intrinsic strains in an arbitrary infinite piezoelectric plate with metallized surfaces are determined. The results obtained generalize the well-known theory of internal stresses in anisotropic purely elastic plates developed by Indenbom, Sil’vestrova, and Sirotin [1]. The coupled fields found in the piezoelectric are expressed in terms of the 4D formalism and the corresponding generalized planar tensor of electro-elastic moduli. It is shown that the limiting transitions from a piezoelectric plate to an unbounded medium and half-space lead to identical formulas.

  • Content Type Journal Article
  • DOI 10.1134/S106377450906008X
  • Authors
    • V. I. Alshits, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • J. P. Nowacki, Polish-Japanese Institute of Information Technology 02-008 Warsaw Poland
    • A. Radowicz, Kielce University of Technology 25-314 Kielce Poland

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Evolution of atomic collision cascades in vanadium crystal with internal structure

Abstract  The formation of radiation-damage regions (radiation-damage cascades) in vanadium crystallites with internal structures (intergrain boundary) has been simulated by the molecular-dynamic method. The interatomic interaction is described within the embedded-atom method. A relatively small number of clusters of intrinsic point defects (vacancies and self-interstitial atoms) are formed both in ideal vanadium crystallites and in crystallites with boundaries after the relaxation of atomic-displacement cascades. The evolutionary character of atomic-displacement cascades is determined in many respects by the presence of extended boundaries in materials. The intergrain boundaries hinder the propagation of atomic-displacement cascades and store many radiation-induced defects.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060157
  • Authors
    • S. G. Psakhie, Russian Academy of Sciences Institute of Strength Physics and Materials Science, Siberian Branch Tomsk 634021 Russia
    • K. P. Zolnikov, Russian Academy of Sciences Institute of Strength Physics and Materials Science, Siberian Branch Tomsk 634021 Russia
    • D. S. Kryzhevich, Russian Academy of Sciences Institute of Strength Physics and Materials Science, Siberian Branch Tomsk 634021 Russia
    • A. V. Zheleznyakov, Russian Academy of Sciences Institute of Strength Physics and Materials Science, Siberian Branch Tomsk 634021 Russia
    • V. M. Chernov, Bochvar High-Technology Research Institute of Inorganic Materials Moscow 123098 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

The plastic deformation of ultrafine grained aluminum at 0.52 K

Abstract  The plastic deformation of ultra-fine-grained aluminum subjected to equal-channel angular pressing has been studied at a temperature below the superconducting transition point. The stress-strain curves σ(ɛ) for polycrystals and the effect of the superconducting transition on the jump of flow stress Δσ NS have been investigated. It is shown that the grain refinement, along with the increase in the flow stress, leads to a correlated change in the shapes of the dependences σ(ɛ) and Δσ NS (σ). The results obtained are explained by the features of dislocation accumulation in ultra-fine-grained polycrystals and by the manifestation of the inertial properties of dislocations under low-temperature plastic deformation.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060194
  • Authors
    • Yu. Z. Estrin, Monash University Clayton Victoria Australia
    • N. V. Isaev, National Academy of Sciences of Ukraine Verkin Institute for Low Temperature Physics and Engineering Kharkov 61103 Ukraine
    • T. V. Grigorova, National Academy of Sciences of Ukraine Verkin Institute for Low Temperature Physics and Engineering Kharkov 61103 Ukraine
    • V. V. Pustovalov, National Academy of Sciences of Ukraine Verkin Institute for Low Temperature Physics and Engineering Kharkov 61103 Ukraine
    • V. S. Fomenko, National Academy of Sciences of Ukraine Verkin Institute for Low Temperature Physics and Engineering Kharkov 61103 Ukraine
    • S. É. Shumilin, National Academy of Sciences of Ukraine Verkin Institute for Low Temperature Physics and Engineering Kharkov 61103 Ukraine

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

The influence of a magnetic field on the microhardness of K, Rb, Cs, NH4, and Tl acid phthalate crystals

Abstract  The influence of a magnetic field on the microhardness of potassium acid phthalate has been studied for different magnetic inductions, exposure times, sample orientations in a magnetic field, and impurity compositions of the crystals. It was shown that the magnetic field effect is multiply repeated on the (010) face after relaxation. The influence of magnetic treatment on ammonium, rubidium, thallium, and cesium acid phthalate crystals is analyzed. The reasons for the observed changes in the crystal microhardness in the magnetic field are discussed.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060108
  • Authors
    • M. V. Koldaeva, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • T. N. Turskaya, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • R. M. Zakalyukin, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • E. V. Darinskaya, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Mean-field theory about the critical size in ferroelectricity

Abstract  The problem of critical size in ferroelectric crystals and films is considered within the mean-field theory. It is shown that, when the boundary conditions are correctly chosen, the critical size can be either very small or even absent; i.e., ferroelectricity can exist in one unit cell.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060029
  • Authors
    • V. M. Fridkin, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

X-ray fluorescence studies for the elemental composition and molecular organization of protein films on the surface of the liquid subphase

Abstract  This paper reports on the results of the investigation of protein films that are based on alkaline phosphatase and glucose oxidase enzymes and formed on the surface of the liquid subphase. The experimental studies have been performed using total external reflection X-ray fluorescence spectrometry at the European Synchrotron Radiation Facility (Grenoble, France). The self-organization processes that occur in protein systems on the surface of the liquid subphase under the conditions where the protein molecules retain their mobility have been investigated using X-ray fluorescence measurements for the first time.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060030
  • Authors
    • S. I. Zheludeva, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • N. N. Novikova, Russian Research Centre “Kurchatov Institute,” Kurchatov Centre for Synchrotron Radiation and Nanotechnology pl. Akademika Kurchatova 1 Moscow 123182 Russia
    • M. V. Kovalchuk, Russian Research Centre “Kurchatov Institute,” Kurchatov Centre for Synchrotron Radiation and Nanotechnology pl. Akademika Kurchatova 1 Moscow 123182 Russia
    • N. D. Stepina, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • O. V. Konovalov, European Synchrotron Radiation Facility Grenoble BP-220 E-38043 France
    • É. A. Yurieva, Ministry of Health of the Russian Federation Moscow Research Institute of Pediatrics and Child Surgery ul. Taldomskaya 2 Moscow 124150 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

An observation of amorphous-crystalline phase transitions at severe plastic deformation of the Ti50Ni25Cu25 alloy

Abstract  The features of structural and phase transitions during severe plastic deformation (in Bridgman anvils) of the amorphous Ti50Ni25Cu25 alloy have been studied by X-ray diffraction and transmission electron microscopy. Application of successively increasing deformation has revealed three cycles of successive phase transitions from amorphous to crystalline state and vice versa. The results obtained are explained in terms of the superposition of the different channels of elastic energy dissipation, which are activated during severe plastic deformation.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060212
  • Authors
    • G. I. Nosova, Bardin Science State Center for Ferrous Metallurgy Kurdyumov Institute for Physical Metallurgy Moscow Russia
    • A. V. Shalimova, Bardin Science State Center for Ferrous Metallurgy Kurdyumov Institute for Physical Metallurgy Moscow Russia
    • R. V. Sundeev, Bardin Science State Center for Ferrous Metallurgy Kurdyumov Institute for Physical Metallurgy Moscow Russia
    • A. M. Glezer, Bardin Science State Center for Ferrous Metallurgy Kurdyumov Institute for Physical Metallurgy Moscow Russia
    • M. N. Pankova, Bardin Science State Center for Ferrous Metallurgy Kurdyumov Institute for Physical Metallurgy Moscow Russia
    • A. V. Shelyakov, Moscow Engineering Physics Institute (State University) Moscow 115409 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Yield stress and plasticity of nanostructured titanium of different purity at 300, 77, and 4.2 K

Abstract  Specimens of nanostructured titanium with different dopant concentrations were prepared by intense plastic deformation via equal-channel-angular pressing. The low-temperature mechanical characteristics of the specimens subjected to active deformation under uniaxial tension and compression were studied. The yield stress and the limit uniform deformation of nanostructured and coarse-grained polycrystalline titanium were compared.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060224
  • Authors
    • E. D. Tabachnikova, National Academy of Sciences of Ukraine B. Verkin Institute for Low Temperature Physics and Engineering pr. Lenina 47 Kharkov 61103 Ukraine
    • V. Z. Bengus, National Academy of Sciences of Ukraine B. Verkin Institute for Low Temperature Physics and Engineering pr. Lenina 47 Kharkov 61103 Ukraine
    • A. V. Podol’skiĭ, National Academy of Sciences of Ukraine B. Verkin Institute for Low Temperature Physics and Engineering pr. Lenina 47 Kharkov 61103 Ukraine
    • S. N. Smirnov, National Academy of Sciences of Ukraine B. Verkin Institute for Low Temperature Physics and Engineering pr. Lenina 47 Kharkov 61103 Ukraine
    • R. Z. Valiev, Ufa State Aviation Technical University Institute of Physics of Advanced Materials ul. K. Marksa 12 Ufa 450000 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

Bulk polaritons in a biaxial crystal at the interface with a perfect metal

Abstract  The orientation of the plane where the tangential electric field component becomes zero is indicated for any plane bulk electromagnetic wave propagating in an infinite transparent medium of arbitrary anisotropy. Thus, the existence of this wave (bulk polariton) in this plane (interface with an ideal conductor) is ensured. The characteristics of such polaritons of two independent branches with coinciding wave normals (isonormal polaritons) or Poynting vector directions (isoray polaritons) are compared.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060066
  • Authors
    • V. I. Alshits, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia
    • V. N. Lyubimov, Russian Academy of Sciences Shubnikov Institute of Crystallography Leninskiĭ pr. 59 Moscow 119333 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET

TEM and EBSD investigation of the structural state under high-strength superplastic flow in ECAP aluminum alloy

Abstract  The features of structure evolution during superplastic flow have been studied. It is established that stationary superplastic flow deformation is implemented for the structural state in the material bulk, which corresponds to the dynamic stationary behavior of the characteristics of structure elements. It is shown that the superplastic flow in the hardening and softening stages occurs via dislocation slip in grains and grainboundary slip, respectively.

  • Content Type Journal Article
  • DOI 10.1134/S1063774509060200
  • Authors
    • M. M. Myshlyaev, Russian Academy of Sciences Institute of Solid State Physics ul. Institutskaya 2 Chernogolovka, Moscow oblast 142432 Russia
    • S. Yu. Mironov, Russian Academy of Sciences Institute of Metal Superplasticity Problems ul. Khalturina 39 Ufa 450001 Russia
    • E. V. Konovalova, Surgut State University pr. Lenina 1 Surgut 618412 Russia

Source: Crystallography Reports | 17 Dec 2009 | 7:55 am CET




 


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