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Lanthan-Isotope

Liste, Daten und Eigenschaften aller bekannten natürlichen und künstlichen Isotope des Lanthans sowie radioaktive Zerfallsprodukte bzw. Zwischenprodukte.



Lanthan Isotope

Unter Lanthan-Isotope werden alle Atomkerne des chemischen Elements Lanthan zusammengefasst; diese bestehen allesamt aus einem Atomkern mit 57 Protonen und im ungeladenen Zustand aus 57 Elektronen. Der Unterschied zwischen den einzelnen Lanthan-Isotopen beruht auf der Anzahl der Neutronen im Kern.

 

Natürlich auftretende Lanthan-Isotope

In der Natur treten zwei Lanthannuklide auf: Lanthan-139 und das mit einer Halbwertszeit von 1011 Jahren radioaktiv zerfallende Lanthan-138. Die anderen Lanthanisotope zerfallen radioaktiv; La-137 besitzt eine Halbwertszeit von etwa 60000 Jahren. Die radioaktiven Lanthannuklide finden zur Zeit keine technische oder medizinische Verwendung.

Atommasse ArAnteilHalbwertszeitSpin
Lanthan
Isotopengemisch
138,90547 u100 %
Isotop 138La137,907118(3) u0,08881(71) %1,02(1) × 1011 Jahre5+
Isotop 139La138,90636(2) u99,91119(71) %stabil7/2+

 

Isotopentabelle: Lanthan

Isotop
Nuklid
ZANNameAtommasse
[Kernmasse]
{Massenüberschuss}
Spin I
(h/2π)
μA-Nuk
123456789
116La5711659Lanthan-116
117La5711760Lanthan-117116,95011(21) u
[116,9188431 u]
{-46,47224 MeV}
(3/2)+-
117mLa5711760Lanthan-117m116,95011(21) u
[116,9188431 u]
{-46,47224 MeV}
(9/2+)
118La5711861Lanthan-118117,94673(32) u
[117,9154631 u]
{-49,62069 MeV}
119La5711962Lanthan-119118,94099(43) u
[118,9097231 u]
{-54,96746 MeV}
11/2-~119Ce
120La5712063Lanthan-120119,93820(32) u
[119,9069331 u]
{-57,56633 MeV}
120Ce
121La5712164Lanthan-121120,93324(32) u
[120,9019731 u]
{-62,18654 MeV}
(11/2-)121Ce
122La5712265Lanthan-122121,93071(32) u
[121,8994431 u]
{-64,54322 MeV}
122Ce
123La5712366Lanthan-123122,92630(21) u
[122,8950331 u]
{-68,65111 MeV}
(11/2-)123Ce
124La5712467Lanthan-124123,92457(6) u
[123,8933031 u]
{-70,26259 MeV}
8-124Ce
124mLa5712467Lanthan-124m123,92457(6) u
[123,8933031 u]
{-70,26259 MeV}
(8-)
125La5712568Lanthan-125124,920816(28) u
[124,8895491 u]
{-73,75942 MeV}
(3/2+)125Ce
125mLa5712568Lanthan-125m124,920816(28) u
[124,8895491 u]
{-73,75942 MeV}
126La5712669Lanthan-126125,91951(10) u
[125,8882431 u]
{-74,97595 MeV}
(5+)126Ce
126mLa5712669Lanthan-126m125,91951(10) u
[125,8882431 u]
{-74,97595 MeV}
127La5712770Lanthan-127126,916375(28) u
[126,8851081 u]
{-77,89619 MeV}
(11/2-)127Ce
127mLa5712770Lanthan-127m126,916375(28) u
[126,8851081 u]
{-77,89619 MeV}
(3/2+)
128La5712871Lanthan-128127,91559(6) u
[127,8843231 u]
{-78,62741 MeV}
(5+)128Ce
128mLa5712871Lanthan-128m127,91559(6) u
[127,8843231 u]
{-78,62741 MeV}
(1+,2-)
129La5712972Lanthan-129128,912694(23) u
[128,8814271 u]
{-81,32502 MeV}
(3/2+)129Ce
129mLa5712972Lanthan-129m128,912694(23) u
[128,8814271 u]
{-81,32502 MeV}
(11/2-)
130La5713073Lanthan-130129,912369(28) u
[129,8811021 u]
{-81,62775 MeV}
3(+)130Ce
131La5713174Lanthan-131130,91007(3) u
[130,8788031 u]
{-83,76926 MeV}
3/2+131Ce
131mLa5713174Lanthan-131m130,91007(3) u
[130,8788031 u]
{-83,76926 MeV}
11/2-
132La5713275Lanthan-132131,91012(4) u
[131,8788531 u]
{-83,72268 MeV}
2-132Ce
132mLa5713275Lanthan-132m131,91012(4) u
[131,8788531 u]
{-83,72268 MeV}
6-
133La5713376Lanthan-133132,90822(3) u
[132,8769531 u]
{-85,49252 MeV}
5/2+133Ce
134La5713477Lanthan-134133,908514(21) u
[133,8772471 u]
{-85,21866 MeV}
1+134Ce
135La5713578Lanthan-135134,906985(10) u
[134,8757181 u]
{-86,64291 MeV}
5/2++3,70(9)135Ce
136La5713679Lanthan-136135,90763(6) u
[135,8763631 u]
{-86,0421 MeV}
1++ 3,7
136mLa5713679Lanthan-136m135,90763(6) u
[135,8763631 u]
{-86,0421 MeV}
(7-)
137La5713780Lanthan-137136,9064506(18) u
[136,8751837 u]
{-87,1407 MeV}
7/2++2,696(6)137Ce
138La5713881Lanthan-138137,907118(3) u
[137,8758511 u]
{-86,51903 MeV}
5++3,7084(2)
138mLa5713881Lanthan-138m137,907118(3) u
[137,8758511 u]
{-86,51903 MeV}
(3)++2,89(5)
139La5713982Lanthan-139138,90636(2) u
[138,8750931 u]
{-87,2251 MeV}
7/2++2,7791(2)139Ce
139Ba
140La5714083Lanthan-140139,9094832(22) u
[139,8782163 u]
{-84,31586 MeV}
3-+ 0,730(15)140Ba
141La5714184Lanthan-141140,910969(5) u
[140,8797021 u]
{-82,93184 MeV}
(7/2+)141Ba
142La5714285Lanthan-142141,914090(7) u
[141,8828231 u]
{-80,02465 MeV}
2-142Ba
143La5714386Lanthan-143142,916079(8) u
[142,8848121 u]
{-78,17191 MeV}
(7/2)+143Ba
144La5714487Lanthan-144143,919646(14) u
[143,8883791 u]
{-74,84927 MeV}
(3-)144Ba
145La5714588Lanthan-145144,921808(13) u
[144,8905411 u]
{-72,83538 MeV}
(5/2+)145Ba
146La5714689Lanthan-146145,92587(4) u
[145,8946031 u]
{-69,05165 MeV}
2-146Ba
146mLa5714689Lanthan-146m145,92587(4) u
[145,8946031 u]
{-69,05165 MeV}
(6-)
147La5714790Lanthan-147146,928418(11) u
[146,8971511 u]
{-66,6782 MeV}
(3/2+)147Ba
148La5714891Lanthan-148147,932679(21) u
[147,9014121 u]
{-62,70911 MeV}
(2-)148Ba
149La5714992Lanthan-149148,93535(21) u
[148,9040831 u]
{-60,22109 MeV}
(3/2-)149Ba
150La5715093Lanthan-150149,93974(47) u
[149,9084731 u]
{-56,13183 MeV}
(3+)150Ba
151La5715194Lanthan-151150,94277(47) u
[150,9115031 u]
{-53,3094 MeV}
(1/2+)151Ba
152La5715295Lanthan-152151,94708(32) u
[151,9158131 u]
{-49,29466 MeV}
(2-)152Ba
153La5715396Lanthan-153152,95055(32) u
[152,9192831 u]
{-46,06238 MeV}
(1/2+)153Ba
154La5715497Lanthan-154153,95542(32) u
[153,9241531 u]
{-41,526 MeV}
(2-)
155La5715598Lanthan-155154,95928(43) u
[154,9280131 u]
{-37,93044 MeV}
(1/2+)
156La5715699Lanthan-156155,96452(43) u
[155,9332531 u]
{-33,04941 MeV}
(4+)

 

 

IsotopZerfall (radioaktiver Zerfall)AEMehr
HalbwertszeitZerfallsartAnteilEnergieInfo
1101112131415
La-116AL
La-11723,5(25) msp zu 116Ba
β+ zu 117Ba
93,9(7) %
6,1(7) %

10,99(32) MeV
AL
La-117m10(5) msp zu 116Ba
β+ zu 117Ba
97,4(13) %
2,6(13) %

151(12) keVAL
La-118~200 msβ+ zu 118Ba
β+ zu


AL
La-119~1 sβ+ zu 119BaAL
La-1202,8(2) sEE/β+ zu 120Ba
EE, p zu 119Cs
< 100 %
> 0 %
11,32(42) MeV
AL
La-1215,3(2) sβ+ zu 121Ba100 %8,55(33) MeVAL
La-1228,6(5) sEE/β+ zu 122Ba
EE, p zu 121Cs
100 %
?
10,07(30) MeV
AL
La-12317(3) sEE/β+ zu 123Ba100 %7,00(20) MeVAL
La-12421(4) sEE/β+ zu 124Ba100 %8,83(6) MeVAL
La-124m29,21(17) sEE/β+ zu 124Ba100 %100 keVAL
La-12564,8(12) sEE/β+ zu 125Ba100 %5,909(28) MeVAL
La-125m0,39(4) s107,00(10) keVAL
La-12654(2) sEE/β+ zu 126Ba?7,79(9) MeVAL
La-126m50 sEE/β+ zu 126Ba
Iso zu 126La
?
?

+z keVAL
La-1275,1(1) MinutenEE/β+ zu 127Ba100 %4,922(28) MeVAL
La-127m3,7(4) MinutenEE/β+ zu 127Ba100 %14,2(4) keVAL
La-1285,18(14) MinutenEE/β+ zu 128Ba100 %6,75(5) MeVAL
La-128m1,4 MinutenEE zu 128Ba100 %~ 100 keVAL
La-12911,6(2) Minutenβ+ zu 129Ba100 %3,739(24) MeVAL
La-129m0,56(5) sIso zu 129La100 %172,33(20) keVAL
La-1308,7(1) MinutenEE/β+ zu 130Ba5,634(26) MeVAL
La-13159(2) MinutenEE/β+ zu 131Ba100 %2,914(28) MeVAL
La-131m170(7) μsIso zu 131La100 %304,52(24) keVAL
La-1324,8(2) StundenEE/β+ zu 132Ba100 %4,71(4) MeVAL
La-132m24,3(5) MinutenIso zu 132La
EE/β+ zu 132Ba
76 %
24 %

188,20(11) keVAL
La-1333,912(8) StundenEE/β+ zu 133Ba100 %2,059(28) MeVAL
La-1346,45(16) MinutenEE/β+ zu 134Ba100 %3,731(20) MeVAL
La-13519,5(2) StundenEE/β+ zu 135Ba100 %1,207(9) MeVAL
La-1369,87(3) MinutenEE/β+ zu 136Ba100 %2,85(5) MeVAL
La-136m114(5) msIso zu 136La100 %259,5(3) keVAL
La-13760000 JahreEE zu 137Ba100 %0,5805(17) MeVAL
La-1381,02(1) × 1011 Jahreβ+ zu 138Ba
β- zu 138Ce
65,6(5) %
34,4(5) %
1,742(3) MeV
1,052(4) MeV
AL
La-138m116(5) ns72,57(3) keVAL
La-139stabilAL
La-1401,67858(21) Tageβ- zu 140Ce100 %3,7602(17) MeVAL
La-1413,92(3) Stundenβ- zu 141Ce100 %2,501(4) MeVAL
La-14291,1(5) Minutenβ- zu 142Ce100 %4,509(6) MeVAL
La-14314,2(1) Minutenβ- zu 143Ce100 %3,435(8) MeVAL
La-14440,8(4) sβ- zu 144Ce100 %5,582(13) MeVAL
La-14524,8(20) sβ- zu 145Ce100 %4,23(4) MeVAL
La-1466,1(3) sβ- zu 146Ce
β-, n zu 145Ce
99,99 %
0,007 %
6,59(3) MeV
AL
La-146m9,8(4) sβ- zu 146Ce
Iso zu 146La
100 %
?
6,7 MeV
130(130) keVAL
La-1474,06(4) sβ- zu 147Ce
β-, n zu 146Ce
99,96 %
0,041(4) %
5,336(14) MeV
0,886(20) MeV
AL
La-1481,26(8) sβ- zu 148Ce
β-, n zu 147Ce
99,85 %
0,15(3) %
7,690(22) MeV
1,234(21) MeV
AL
La-1491,05(3) sβ- zu 149Ce
β-, n zu 148Ce
98,6 %
1,43(28) %
6,45(20) MeV
2,11(20) MeV
AL
La-1500,59(11) sβ- zu 150Ce
β-, n zu 149Ce
97,3 %
2,7(3) %
8,72(44) MeV
2,47(44) MeV
AL
La-151457 msβ- zu 151Ce
β-, n zu 150Ce
100 %
?
7,91(44) MeV
3,47(44) MeV
AL
La-152298 msβ- zu 152Ce
β-, n zu 151Ce
100 %
?
9,69(36) MeV
3,86(20) MeV
AL
La-153245(18) msβ- zu 153Ce
β-, n zu 152Ce
100 %
?
8,85(36) MeV
4,85(36) MeV
AL
La-154161(15) msβ- zu 154Ce
β-, n zu 153Ce
100 %
?
10,69(36) MeV
5,31(36) MeV
AL
La-155101(28) msβ- zu 155Ce
β-, n zu 154Ce
100 %
?
9,85(50) MeV
6,22(45) MeV
AL
La-15684(78) msβ- zu 156Ce
β-, n zu 155Ce
100 %
?
11,77(50) MeV
6,66(50) MeV

 

Erläuterungen zu den einzelnen Spalten:

1 - Symbol mit Nukleonenzahl.
2 - Z = Anzahl der Protonen (Ordnungszahl).
3 - Massenzahl A.
4 - N = Anzahl der Neutronen.
5 - Bezeichnung des Lanthan-Isotops; gegebenenfalls Trivialnamen.
6 - Relative Atommasse des Lanthan-Isotops (Isotopenmasse inklusive Elektronen) und in eckigen Klammern die Masse des Atomkerns (Kernmasse, Nuklidmasse ohne Elektronen), jeweils bezogen auf 12C = 12,00000 [2]. Zusätzlich ist der Massenüberschuss (Massenexzess) in MeV angegeben.
7 - Kernspin I, Einheit: h/2π.
8 - Kernmagnetisches Moment μmag.
9 - Ausgangsnuklide: Mögliche, angenommene oder tatsächliche Ausgangs-Nuklide (Mutternuklide, Elternnuklide). Die entsprechenden Zerfalls-Modi sind gegebenenfalls bei den Daten des jeweiligen Ausgangsnuklids zu finden.
10 - Zerfall: Halbwertszeiten des Lanthan-Isotops mit a = Jahre; ; d = Tage; h = Stunden; min = Minuten; s = Sekunden.
11 - Zerfall: Zerfallsart in die jeweiligen Tochternuklide mit n = Neutronenemission; p = Protonenemission; α = Alpha-Zerfall; ß- = Beta-Minus-Zerfall unter Elektronenemission; EE = Elektroneneinfang; ß+ = Positronenemission; ε = ß+ und/oder EE; Iso = Isomerieübergang; CZ = Cluster-Zerfall; SZ = Spontanzerfall.
12 - Zerfall: Zerfallsanteil in Prozent (%).
13 - Zerfall: Zerfallsenergie; Partikelenergie bezogen auf Zerfallsart.
14 - AE = Anregungsenergie für metastabile Kerne.
15 - Sonstige Informationen und Hinweise: AL = Weitere Niveaus, so genannte Adopted Levels (Verlinkung auf externe Daten [1]).

Sonstige:

()- Eingeklammerte Ziffern: Unsicherheit zur Darstellung der Streubreite des angegebenen Wertes.
~ - Theoretische Werte oder systematische Trends.
  - ungelistet-: Nuklide, die in der Literatur bereits erwänhnt wurden, aber aus irgendwelchen Gründen in den aktuellen Nuklidtabellen nicht mehr zu finden sind, weil sich deren Entdeckung z. B. nicht bestätigt hat.

 

NMR-aktive Lanthan-Nuklide

Nuklid
Anteil
Spin I
Kernmagnetisches
Moment
μ/μN
Gyromagnetisches
Verhältnis
107 rad T-1 s-1
Quadrupol-
Moment
Q fm-2
Resonanz-
Frequenz
v0 bei 1 T
Relative
Empfindlichkeit
H0 = const.
v0 = const. *
138La
0,08881(71) %
5+
+3,7084(2)3,5575+ 45,0(20)5,66150,09404
5,3189
139La
99,91119(71) %
7/2+
+2,7791(2)3,801+ 20,6(4)6,06120,06058
2,9895

*) bezogen auf 1H = 1,000

 

Strahlenschutz

Für den Umgang mit den Lanthan-Radionukliden gelten gemäß Strahlenschutzverordnung (StrlSchV 2018) unter anderem folgende Werte (Spalten 1 bis 7):

NuklidFreigrenzenHRQ-SchwelleOFKTochternuklideHalbwertszeit
La-131106 Bq10 Bq/g59,0 Minuten
La-132106 Bq10 Bq/g4,8 Stunden
La-135107 Bq1000 Bq/g19,5 Stunden
La-137107 Bq100 Bq/g6,0 × 104 Jahre
La-138107 Bq0,1 Bq/g1,0 × 1011 Jahre
La-140105 Bq1 Bq/g0,03 TBq1 Bq cm-240,3 Stunden
La-141105 Bq100 Bq/g3,9 Stunden
La-142105 Bq10 Bq/g91,1 Minuten
La-143105 Bq100 Bq/g14,1 Minuten

(HRQ = Hochradioaktive Quellen; OFK = Oberflächenkontamination)

 

Kernisobare Nuklide des Lanthans

Zu den Lanthan-Nukliden isobare Atomkerne befinden sich in der jeweiligen Tabellenzeile; Z = Ordnungszahl; A = Nukleonenzahl (Massenzahl).

Z:4243444546474849505152535455565758596061626364656667686970717273
AMoTcRuRhPdAgCdInSnSbTeIXeCsBaLaCePrNdPmSmEuGdTbDyHoErTmYbLuHfTa
116116Mo116Tc116Ru116Rh116Pd116Ag116Cd116In116Sn116Sb116Te116I116Xe116Cs116Ba116La
117117Mo117Tc117Ru117Rh117Pd117Ag117Cd117In117Sn117Sb117Te117I117Xe117Cs117Ba117La
118118Tc118Ru118Rh118Pd118Ag118Cd118In118Sn118Sb118Te118I118Xe118Cs118Ba118La
119119Tc119Ru119Rh119Pd119Ag119Cd119In119Sn119Sb119Te119I119Xe119Cs119Ba119La119Ce
120120Tc120Ru120Rh120Pd120Ag120Cd120In120Sn120Sb120Te120I120Xe120Cs120Ba120La120Ce
121121Ru121Rh121Pd121Ag121Cd121In121Sn121Sb121Te121I121Xe121Cs121Ba121La121Ce121Pr
122122Ru122Rh122Pd122Ag122Cd122In122Sn122Sb122Te122I122Xe122Cs122Ba122La122Ce122Pr
123123Ru123Rh123Pd123Ag123Cd123In123Sn123Sb123Te123I123Xe123Cs123Ba123La123Ce123Pr
124124Ru124Rh124Pd124Ag124Cd124In124Sn124Sb124Te124I124Xe124Cs124Ba124La124Ce124Pr124Nd
125125Rh125Pd125Ag125Cd125In125Sn125Sb125Te125I125Xe125Cs125Ba125La125Ce125Pr125Nd
126126Rh126Pd126Ag126Cd126In126Sn126Sb126Te126I126Xe126Cs126Ba126La126Ce126Pr126Nd126Pm
127127Pd127Ag127Cd127In127Sn127Sb127Te127I127Xe127Cs127Ba127La127Ce127Pr127Nd127Pm
128128Pd128Ag128Cd128In128Sn128Sb128Te128I128Xe128Cs128Ba128La128Ce128Pr128Nd128Pm128Sm
129129Ag129Cd129In129Sn129Sb129Te129I129Xe129Cs129Ba129La129Ce129Pr129Nd129Pm129Sm
130130Ag130Cd130In130Sn130Sb130Te130I130Xe130Cs130Ba130La130Ce130Pr130Nd130Pm130Sm130Eu
131131Cd131In131Sn131Sb131Te131I131Xe131Cs131Ba131La131Ce131Pr131Nd131Pm131Sm131Eu
132132Cd132In132Sn132Sb132Te132I132Xe132Cs132Ba132La132Ce132Pr132Nd132Pm132Sm132Eu
133133Cd133In133Sn133Sb133Te133I133Xe133Cs133Ba133La133Ce133Pr133Nd133Pm133Sm133Eu
134134In134Sn134Sb134Te134I134Xe134Cs134Ba134La134Ce134Pr134Nd134Pm134Sm134Eu134Gd
135135In135Sn135Sb135Te135I135Xe135Cs135Ba135La135Ce135Pr135Nd135Pm135Sm135Eu135Gd135Tb
136136Sn136Sb136Te136I136Xe136Cs136Ba136La136Ce136Pr136Nd136Pm136Sm136Eu136Gd136Tb
137137Sn137Sb137Te137I137Xe137Cs137Ba137La137Ce137Pr137Nd137Pm137Sm137Eu137Gd137Tb
138138Sn138Sb138Te138I138Xe138Cs138Ba138La138Ce138Pr138Nd138Pm138Sm138Eu138Gd138Tb138Dy
139139Sb139Te139I139Xe139Cs139Ba139La139Ce139Pr139Nd139Pm139Sm139Eu139Gd139Tb139Dy
140140Sb140Te140I140Xe140Cs140Ba140La140Ce140Pr140Nd140Pm140Sm140Eu140Gd140Tb140Dy140Ho
141141Te141I141Xe141Cs141Ba141La141Ce141Pr141Nd141Pm141Sm141Eu141Gd141Tb141Dy141Ho
142142Te142I142Xe142Cs142Ba142La142Ce142Pr142Nd142Pm142Sm142Eu142Gd142Tb142Dy142Ho
143143Te143I143Xe143Cs143Ba143La143Ce143Pr143Nd143Pm143Sm143Eu143Gd143Tb143Dy143Ho143Er
144144I144Xe144Cs144Ba144La144Ce144Pr144Nd144Pm144Sm144Eu144Gd144Tb144Dy144Ho144Er144Tm
145145I145Xe145Cs145Ba145La145Ce145Pr145Nd145Pm145Sm145Eu145Gd145Tb145Dy145Ho145Er145Tm
146146Xe146Cs146Ba146La146Ce146Pr146Nd146Pm146Sm146Eu146Gd146Tb146Dy146Ho146Er146Tm
147147Xe147Cs147Ba147La147Ce147Pr147Nd147Pm147Sm147Eu147Gd147Tb147Dy147Ho147Er147Tm
148148Xe148Cs148Ba148La148Ce148Pr148Nd148Pm148Sm148Eu148Gd148Tb148Dy148Ho148Er148Tm148Yb
149149Cs149Ba149La149Ce149Pr149Nd149Pm149Sm149Eu149Gd149Tb149Dy149Ho149Er149Tm149Yb
150150Cs150Ba150La150Ce150Pr150Nd150Pm150Sm150Eu150Gd150Tb150Dy150Ho150Er150Tm150Yb150Lu
151151Cs151Ba151La151Ce151Pr151Nd151Pm151Sm151Eu151Gd151Tb151Dy151Ho151Er151Tm151Yb151Lu
152152Ba152La152Ce152Pr152Nd152Pm152Sm152Eu152Gd152Tb152Dy152Ho152Er152Tm152Yb152Lu
153153Ba153La153Ce153Pr153Nd153Pm153Sm153Eu153Gd153Tb153Dy153Ho153Er153Tm153Yb153Lu153Hf
154154La154Ce154Pr154Nd154Pm154Sm154Eu154Gd154Tb154Dy154Ho154Er154Tm154Yb154Lu154Hf
155155La155Ce155Pr155Nd155Pm155Sm155Eu155Gd155Tb155Dy155Ho155Er155Tm155Yb155Lu155Hf155Ta

 

Kernisotone Nuklide des Lanthans

Die zu den Lanthan-Kernen isotonen Nuklide befinden sich in der jeweiligen Tabellenzeile; N = Anzahl der Neutronen.


59606162636465666768697071727374757677787980818283848586878889909192939495969798
92As
93Se94Se
94Br95Br96Br97Br98Br
95Kr96Kr97Kr98Kr99Kr100Kr101Kr
96Rb97Rb98Rb99Rb100Rb101Rb102Rb
97Sr98Sr99Sr100Sr101Sr102Sr103Sr104Sr105Sr106Sr107Sr
98Y99Y100Y101Y102Y103Y104Y105Y106Y107Y108Y109Y
99Zr100Zr101Zr102Zr103Zr104Zr105Zr106Zr107Zr108Zr109Zr110Zr111Zr112Zr
100Nb101Nb102Nb103Nb104Nb105Nb106Nb107Nb108Nb109Nb110Nb111Nb112Nb113Nb114Nb115Nb
101Mo102Mo103Mo104Mo105Mo106Mo107Mo108Mo109Mo110Mo111Mo112Mo113Mo114Mo115Mo116Mo117Mo
102Tc103Tc104Tc105Tc106Tc107Tc108Tc109Tc110Tc111Tc112Tc113Tc114Tc115Tc116Tc117Tc118Tc119Tc120Tc
103Ru104Ru105Ru106Ru107Ru108Ru109Ru110Ru111Ru112Ru113Ru114Ru115Ru116Ru117Ru118Ru119Ru120Ru121Ru122Ru123Ru124Ru
104Rh105Rh106Rh107Rh108Rh109Rh110Rh111Rh112Rh113Rh114Rh115Rh116Rh117Rh118Rh119Rh120Rh121Rh122Rh123Rh124Rh125Rh126Rh
105Pd106Pd107Pd108Pd109Pd110Pd111Pd112Pd113Pd114Pd115Pd116Pd117Pd118Pd119Pd120Pd121Pd122Pd123Pd124Pd125Pd126Pd127Pd128Pd
106Ag107Ag108Ag109Ag110Ag111Ag112Ag113Ag114Ag115Ag116Ag117Ag118Ag119Ag120Ag121Ag122Ag123Ag124Ag125Ag126Ag127Ag128Ag129Ag130Ag
107Cd108Cd109Cd110Cd111Cd112Cd113Cd114Cd115Cd116Cd117Cd118Cd119Cd120Cd121Cd122Cd123Cd124Cd125Cd126Cd127Cd128Cd129Cd130Cd131Cd132Cd133Cd
108In109In110In111In112In113In114In115In116In117In118In119In120In121In122In123In124In125In126In127In128In129In130In131In132In133In134In135In
109Sn110Sn111Sn112Sn113Sn114Sn115Sn116Sn117Sn118Sn119Sn120Sn121Sn122Sn123Sn124Sn125Sn126Sn127Sn128Sn129Sn130Sn131Sn132Sn133Sn134Sn135Sn136Sn137Sn138Sn
110Sb111Sb112Sb113Sb114Sb115Sb116Sb117Sb118Sb119Sb120Sb121Sb122Sb123Sb124Sb125Sb126Sb127Sb128Sb129Sb130Sb131Sb132Sb133Sb134Sb135Sb136Sb137Sb138Sb139Sb140Sb
111Te112Te113Te114Te115Te116Te117Te118Te119Te120Te121Te122Te123Te124Te125Te126Te127Te128Te129Te130Te131Te132Te133Te134Te135Te136Te137Te138Te139Te140Te141Te142Te143Te
112I113I114I115I116I117I118I119I120I121I122I123I124I125I126I127I128I129I130I131I132I133I134I135I136I137I138I139I140I141I142I143I144I145I
113Xe114Xe115Xe116Xe117Xe118Xe119Xe120Xe121Xe122Xe123Xe124Xe125Xe126Xe127Xe128Xe129Xe130Xe131Xe132Xe133Xe134Xe135Xe136Xe137Xe138Xe139Xe140Xe141Xe142Xe143Xe144Xe145Xe146Xe147Xe148Xe
114Cs115Cs116Cs117Cs118Cs119Cs120Cs121Cs122Cs123Cs124Cs125Cs126Cs127Cs128Cs129Cs130Cs131Cs132Cs133Cs134Cs135Cs136Cs137Cs138Cs139Cs140Cs141Cs142Cs143Cs144Cs145Cs146Cs147Cs148Cs149Cs150Cs151Cs
115Ba116Ba117Ba118Ba119Ba120Ba121Ba122Ba123Ba124Ba125Ba126Ba127Ba128Ba129Ba130Ba131Ba132Ba133Ba134Ba135Ba136Ba137Ba138Ba139Ba140Ba141Ba142Ba143Ba144Ba145Ba146Ba147Ba148Ba149Ba150Ba151Ba152Ba153Ba
116La117La118La119La120La121La122La123La124La125La126La127La128La129La130La131La132La133La134La135La136La137La138La139La140La141La142La143La144La145La146La147La148La149La150La151La152La153La154La155La
119Ce120Ce121Ce122Ce123Ce124Ce125Ce126Ce127Ce128Ce129Ce130Ce131Ce132Ce133Ce134Ce135Ce136Ce137Ce138Ce139Ce140Ce141Ce142Ce143Ce144Ce145Ce146Ce147Ce148Ce149Ce150Ce151Ce152Ce153Ce154Ce155Ce156Ce
121Pr122Pr123Pr124Pr125Pr126Pr127Pr128Pr129Pr130Pr131Pr132Pr133Pr134Pr135Pr136Pr137Pr138Pr139Pr140Pr141Pr142Pr143Pr144Pr145Pr146Pr147Pr148Pr149Pr150Pr151Pr152Pr153Pr154Pr155Pr156Pr157Pr
124Nd125Nd126Nd127Nd128Nd129Nd130Nd131Nd132Nd133Nd134Nd135Nd136Nd137Nd138Nd139Nd140Nd141Nd142Nd143Nd144Nd145Nd146Nd147Nd148Nd149Nd150Nd151Nd152Nd153Nd154Nd155Nd156Nd157Nd158Nd
126Pm127Pm128Pm129Pm130Pm131Pm132Pm133Pm134Pm135Pm136Pm137Pm138Pm139Pm140Pm141Pm142Pm143Pm144Pm145Pm146Pm147Pm148Pm149Pm150Pm151Pm152Pm153Pm154Pm155Pm156Pm157Pm158Pm159Pm
128Sm129Sm130Sm131Sm132Sm133Sm134Sm135Sm136Sm137Sm138Sm139Sm140Sm141Sm142Sm143Sm144Sm145Sm146Sm147Sm148Sm149Sm150Sm151Sm152Sm153Sm154Sm155Sm156Sm157Sm158Sm159Sm160Sm
130Eu131Eu132Eu133Eu134Eu135Eu136Eu137Eu138Eu139Eu140Eu141Eu142Eu143Eu144Eu145Eu146Eu147Eu148Eu149Eu150Eu151Eu152Eu153Eu154Eu155Eu156Eu157Eu158Eu159Eu160Eu161Eu
134Gd135Gd136Gd137Gd138Gd139Gd140Gd141Gd142Gd143Gd144Gd145Gd146Gd147Gd148Gd149Gd150Gd151Gd152Gd153Gd154Gd155Gd156Gd157Gd158Gd159Gd160Gd161Gd162Gd
135Tb136Tb137Tb138Tb139Tb140Tb141Tb142Tb143Tb144Tb145Tb146Tb147Tb148Tb149Tb150Tb151Tb152Tb153Tb154Tb155Tb156Tb157Tb158Tb159Tb160Tb161Tb162Tb163Tb
138Dy139Dy140Dy141Dy142Dy143Dy144Dy145Dy146Dy147Dy148Dy149Dy150Dy151Dy152Dy153Dy154Dy155Dy156Dy157Dy158Dy159Dy160Dy161Dy162Dy163Dy164Dy
140Ho141Ho142Ho143Ho144Ho145Ho146Ho147Ho148Ho149Ho150Ho151Ho152Ho153Ho154Ho155Ho156Ho157Ho158Ho159Ho160Ho161Ho162Ho163Ho164Ho165Ho
143Er144Er145Er146Er147Er148Er149Er150Er151Er152Er153Er154Er155Er156Er157Er158Er159Er160Er161Er162Er163Er164Er165Er166Er
144Tm145Tm146Tm147Tm148Tm149Tm150Tm151Tm152Tm153Tm154Tm155Tm156Tm157Tm158Tm159Tm160Tm161Tm162Tm163Tm164Tm165Tm166Tm167Tm
148Yb149Yb150Yb151Yb152Yb153Yb154Yb155Yb156Yb157Yb158Yb159Yb160Yb161Yb162Yb163Yb164Yb165Yb166Yb167Yb168Yb
150Lu151Lu152Lu153Lu154Lu155Lu156Lu157Lu158Lu159Lu160Lu161Lu162Lu163Lu164Lu165Lu166Lu167Lu168Lu169Lu
153Hf154Hf155Hf156Hf157Hf158Hf159Hf160Hf161Hf162Hf163Hf164Hf165Hf166Hf167Hf168Hf169Hf170Hf
155Ta156Ta157Ta158Ta159Ta160Ta161Ta162Ta163Ta164Ta165Ta166Ta167Ta168Ta169Ta170Ta171Ta
158W159W160W161W162W163W164W165W166W167W168W169W170W171W172W
159Re160Re161Re162Re163Re164Re165Re166Re167Re168Re169Re170Re171Re172Re173Re
161Os162Os163Os164Os165Os166Os167Os168Os169Os170Os171Os172Os173Os174Os
164Ir165Ir166Ir167Ir168Ir169Ir170Ir171Ir172Ir173Ir174Ir175Ir
166Pt167Pt168Pt169Pt170Pt171Pt172Pt173Pt174Pt175Pt176Pt
170Au171Au172Au173Au174Au175Au176Au177Au
171Hg172Hg173Hg174Hg175Hg176Hg177Hg178Hg
176Tl177Tl178Tl179Tl
178Pb179Pb180Pb

 

Literatur und Hinweise

Eigenschaften der Lanthan-Isotope

[1] - NuDat: National Nuclear Data Center, Brookhaven National Laboratory, based on ENSDF and the Nuclear Wallet Cards.

[2] - G. Audi et. al.: The NUBASE evaluation of nuclear and decay properties. Nuclear Physics, (2003), DOI 10.1016/j.nuclphysa.2003.11.001.

[3] - Live Chart of Nuclides. Nuclear structure and decay data.

Lanthan: Kernmagnetische Eigenschaften - 138La-NMR, 139La-NMR

[4] - N. J. Stone: Table of nuclear magnetic dipole and electric quadrupole moments. Atomic Data and Nuclear Data Tables, (2005), DOI 10.1016/j.adt.2005.04.001.

[5] - Pekka Pyykkö: Year-2008 nuclear quadrupole moments. Molecular Physics, (2008), DOI 10.1080/00268970802018367.

[6] - Pekka Pyykkö: Year-2017 nuclear quadrupole moments. Molecular Physics, (2018), DOI 10.1080/00268976.2018.1426131.

[7] - N. J. Stone: Table of recommended nuclear magnetic dipole moments. IAEA, (2019).

Weitere Quellen:

[8] - Isotopenhäufigkeiten, Atommassen und Isotopenmassen: Siehe unter dem jeweiligen Stichwort.

 


Kategorie: Chemische Elemente

Letzte Änderung am 05.07.2020.



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