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Antimon-Isotope

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



Antimon Isotope

Unter Antimon-Isotope werden alle Atomkerne des chemischen Elements Antimon zusammengefasst; diese bestehen allesamt aus einem Atomkern mit 51 Protonen und im ungeladenen Zustand aus 51 Elektronen. Der Unterschied zwischen den einzelnen Antimon-Isotopen beruht auf der Anzahl der Neutronen im Kern.

 

Natürlich auftretende Antimon-Isotope

Die irdischen Antimonvorkommen setzen sich aus den beiden stabilen Isotopen Antimon-121 und Antimon-123 im Verhältnis von etwa 3:2 zusammen.

Atommasse ArAnteilHalbwertszeitSpin
Antimon
Isotopengemisch
121,760 u100 %
Isotop 121Sb120,90381(2) u57,21(5) %stabil5/2+
Isotop 123Sb122,90421(2) u42,79(5) %stabil7/2+

 

Neben den natürlichen Nukliden des Antimons sind etwa 35 weitere Radionuklide und eine Vielzahl an Kernisomeren bekannt. Radioisotope des Antimons werden gelegentlich auch als Radioantimon bezeichnet.

Technische Anwendungen für einzelne, reine Antimonisotope gibt es nicht.

 

Isotopentabelle: Antimon

Isotop
Nuklid
ZANNameAtommasse
[Kernmasse]
{Massenüberschuss}
Spin I
(h/2π)
μA-Nuk
123456789
103Sb5110352Antimon-103102,93969(32) u
[102,9117141 u]
{-56,1784 MeV}
5/2+
104Sb5110453Antimon-104103,93647(13) u
[103,9084941 u]
{-59,17781 MeV}
105Sb5110554Antimon-105104,931277(23) u
[104,9033011 u]
{-64,01506 MeV}
(5/2+)
106Sb5110655Antimon-106105,928638(8) u
[105,9006621 u]
{-66,47327 MeV}
(2+)110I
107Sb5110756Antimon-107106,924151(4) u
[106,8961751 u]
{-70,65289 MeV}
(5/2+)111I
108Sb5110857Antimon-108107,922227(6) u
[107,8942511 u]
{-72,44508 MeV}
(4+)112I
109Sb5110958Antimon-109108,918141(6) u
[108,8901651 u]
{-76,25117 MeV}
(5/2+)113I
109Te
110Sb5111059Antimon-110109,916854(6) u
[109,8888781 u]
{-77,45 MeV}
(3+)110Te
111Sb5111160Antimon-111110,913218(9) u
[110,8852421 u]
{-80,83691 MeV}
(5/2+)
112Sb5111261Antimon-112111,912400(19) u
[111,8844241 u]
{-81,59887 MeV}
(3+)112Te
113Sb5111362Antimon-113112,909375(18) u
[112,8813991 u]
{-84,41664 MeV}
5/2+113Te
114Sb5111463Antimon-114113,909289(23) u
[113,8813131 u]
{-84,49675 MeV}
3++ 1,72(8)114Te
115Sb5111564Antimon-115114,906598(17) u
[114,8786221 u]
{-87,0034 MeV}
5/2++ 3,46(1)115Te
116Sb5111665Antimon-116115,906793(6) u
[115,8788171 u]
{-86,82176 MeV}
3+2,715(9)116Te
116m1Sb5111665Antimon-116m1115,906793(6) u
[115,8788171 u]
{-86,82176 MeV}
1++2,47(9)
116m2Sb5111665Antimon-116m2115,906793(6) u
[115,8788171 u]
{-86,82176 MeV}
8-2,59(22)
117Sb5111766Antimon-117116,904842(9) u
[116,8768661 u]
{-88,63911 MeV}
5/2++ 3,43(6)117Te
118Sb5111867Antimon-118117,905532(3) u
[117,8775561 u]
{-87,99638 MeV}
1+2,46(7)118Te
118m1Sb5111867Antimon-118m1117,905532(3) u
[117,8775561 u]
{-87,99638 MeV}
(3)++2,63(5)
118m2Sb5111867Antimon-118m2117,905532(3) u
[117,8775561 u]
{-87,99638 MeV}
8-2,32(4)
119Sb5111968Antimon-119118,903946(8) u
[118,8759701 u]
{-89,47372 MeV}
5/2++ 3,45(1)119Te
119m1Sb5111968Antimon-119m1118,903946(8) u
[118,8759701 u]
{-89,47372 MeV}
(19/2-)+3,14(6)
119m2Sb5111968Antimon-119m2118,903946(8) u
[118,8759701 u]
{-89,47372 MeV}
(27/2+)
120Sb5112069Antimon-120119,905080(8) u
[119,8771041 u]
{-88,41741 MeV}
1+2,3(2)
120m1Sb5112069Antimon-120m1119,905080(8) u
[119,8771041 u]
{-88,41741 MeV}
8-2,34(3)
120m2Sb5112069Antimon-120m2119,905080(8) u
[119,8771041 u]
{-88,41741 MeV}
3++2,584(6)
120m3Sb5112069Antimon-120m3119,905080(8) u
[119,8771041 u]
{-88,41741 MeV}
(6)
121Sb5112170Antimon-121120,90381(2) u
[120,8758341 u]
{-89,60041 MeV}
5/2++ 3,3580(16)121Te
121Sn
121mSb5112170Antimon-121m120,90381(2) u
[120,8758341 u]
{-89,60041 MeV}
(25/2)
122Sb5112271Antimon-122121,9051681(28) u
[121,8771922 u]
{-88,33535 MeV}
2-- 1,90(2)
122m1Sb5112271Antimon-122m1121,9051681(28) u
[121,8771922 u]
{-88,33535 MeV}
3++2,983(12)
122m2Sb5112271Antimon-122m2121,9051681(28) u
[121,8771922 u]
{-88,33535 MeV}
(5)++ 3,05(10)
122m3Sb5112271Antimon-122m3121,9051681(28) u
[121,8771922 u]
{-88,33535 MeV}
(8)-
123Sb5112372Antimon-123122,90421(2) u
[122,8762341 u]
{-89,22781 MeV}
7/2++ 2,5457(12)123Sn
123Te
124Sb5112473Antimon-124123,9059358(16) u
[123,8779599 u]
{-87,62024 MeV}
3-1,20(2)
124m1Sb5112473Antimon-124m1123,9059358(16) u
[123,8779599 u]
{-87,62024 MeV}
5+
124m2Sb5112473Antimon-124m2123,9059358(16) u
[123,8779599 u]
{-87,62024 MeV}
(8)-
124m3Sb5112473Antimon-124m3123,9059358(16) u
[123,8779599 u]
{-87,62024 MeV}
3+,4++2,970(33)
125Sb5112574Antimon-125124,9052530(28) u
[124,8772771 u]
{-88,25626 MeV}
7/2++ 2,63(4)125Sn
126Sb5112675Antimon-126125,90725(3) u
[125,8792741 u]
{-86,39607 MeV}
(8-)1,28(7)126Sn
126m1Sb5112675Antimon-126m1125,90725(3) u
[125,8792741 u]
{-86,39607 MeV}
(5+)
126m2Sb5112675Antimon-126m2125,90725(3) u
[125,8792741 u]
{-86,39607 MeV}
(3-)
126m3Sb5112675Antimon-126m3125,90725(3) u
[125,8792741 u]
{-86,39607 MeV}
(3+)
127Sb5112776Antimon-127126,906924(6) u
[126,8789481 u]
{-86,69974 MeV}
7/2+2,70(4)127Sn
127m1Sb5112776Antimon-127m1126,906924(6) u
[126,8789481 u]
{-86,69974 MeV}
(15/2-)
127m2Sb5112776Antimon-127m2126,906924(6) u
[126,8789481 u]
{-86,69974 MeV}
128Sb5112877Antimon-128127,909146(21) u
[127,8811701 u]
{-84,62996 MeV}
8-1,31(2)128Sn
128mSb5112877Antimon-128m127,909146(21) u
[127,8811701 u]
{-84,62996 MeV}
5+
129Sb5112978Antimon-129128,909147(23) u
[128,8811711 u]
{-84,62902 MeV}
7/2+2,79(4)129Sn
129m1Sb5112978Antimon-129m1128,909147(23) u
[128,8811711 u]
{-84,62902 MeV}
(19/2-)
129m2Sb5112978Antimon-129m2128,909147(23) u
[128,8811711 u]
{-84,62902 MeV}
(15/2-)
130Sb5113079Antimon-130129,911663(15) u
[129,8836871 u]
{-82,28539 MeV}
(8-)130Sn
130mSb5113079Antimon-130m129,911663(15) u
[129,8836871 u]
{-82,28539 MeV}
(4,5)+
131Sb5113180Antimon-131130,9119893(22) u
[130,8840134 u]
{-81,98144 MeV}
(7/2+)2,89(4)131Sn
131m1Sb5113180Antimon-131m1130,9119893(22) u
[130,8840134 u]
{-81,98144 MeV}
(15/2-)
131m2Sb5113180Antimon-131m2130,9119893(22) u
[130,8840134 u]
{-81,98144 MeV}
(19/2-)
131m3Sb5113180Antimon-131m3130,9119893(22) u
[130,8840134 u]
{-81,98144 MeV}
(23/2+)
132Sb5113281Antimon-132131,9145080(26) u
[131,8865321 u]
{-79,63529 MeV}
(4)+132Sn
133Sn
248Cm
132m1Sb5113281Antimon-132m1131,9145080(26) u
[131,8865321 u]
{-79,63529 MeV}
(8-)
133Sb5113382Antimon-133132,915272(3) u
[132,8872961 u]
{-78,92362 MeV}
(7/2+)3,00(4)133Sn
134Sb5113483Antimon-134133,9205357(18) u
[133,8925598 u]
{-74,02052 MeV}
(0-)134Sn
135Sn
248Cm
134mSb5113483Antimon-134m133,9205357(18) u
[133,8925598 u]
{-74,02052 MeV}
(7-)
135Sb5113584Antimon-135134,9251844(28) u
[134,8972085 u]
{-69,69028 MeV}
(7/2+)135Sn
136Sn
248Cm
136Sb5113685Antimon-136135,930749(6) u
[135,9027731 u]
{-64,50689 MeV}
(1-)
137Sb5113786Antimon-137136,93552(6) u
[136,9075441 u]
{-60,06273 MeV}
(7/2+)
138Sb5113887Antimon-138137,94179(114) u
[137,9138141 u]
{-54,22227 MeV}
(3-)
139Sb5113988Antimon-139138,94655(43) u
[138,9185741 u]
{-49,78835 MeV}
(7/2+)
140Sb5114089Antimon-140139,95283(64) u
[139,9248541 u]
{-43,93857 MeV}
(3-,4-)
141Sb5114190Antimon-141140,95801(54) u
[140,9300341 u]
{-39,11343 MeV}

 

 

IsotopZerfall (radioaktiver Zerfall)AEMehr
HalbwertszeitZerfallsartAnteilEnergieInfo
1101112131415
Sb-10349 nsp zu 102SnAL
Sb-1040,44 sEE/β+ zu 104Sn
ε, p zu 103In
p zu 103Sn
> 92 %
< 7 %
< 1 %


AL
Sb-1051,22(11) sEE β+ zu 105Sn
p zu 104Sn
99 %
1 %
9,323(22) MeV
2,34 MeV
AL
Sb-1060,6(2) sEE β+ ? zu 106Sn?10,880(9) MeVAL
Sb-1074,0(2) sEE/β+ zu 107Sn100 %7,859(7) MeVAL
Sb-1087,4(3) sEE/β+ zu 108Sn100 %9,625(8) MeVAL
Sb-10917,2(5) sEE/β+ zu 109Sn100 %6,379(10) MeVAL
Sb-11023,6(3) sEE/β+ zu 110Sn100 %8,392(15) MeVAL
Sb-11175(1) sEE/β+ zu 111Sn100 %5,102(10) MeVAL
Sb-11253,5(6) sEE/β+ zu 112Sn100 %7,056(18) MeVAL
Sb-1136,67(7) MinutenEE/β+ zu 113Sn100 %3,911(17) MeVAL
Sb-1143,49(3) MinutenEE/β+ zu 114Sn100 %6,063(22) MeVAL
Sb-11532,1(3) MinutenEE/β+ zu 115Sn100 %3,030(16) MeVAL
Sb-11615,8(8) MinutenEE/β+ zu 116Sn100 %4,704(5) MeVAL
Sb-116m1194(4) ns93,99(5) keV
Sb-116m260,3(6) MinutenEE/β+ zu 116Sn100 %383(40) keV
Sb-1172,80(1) StundenEE β+ zu 117Sn
β+
83 %
1,7(3) %
1,758(8) MeV
AL
Sb-1183,6(1) MinutenEE/β+ zu 118Sn100 %3,6557(3) MeVAL
Sb-118m120,6(6) μs50,814(21) s
Sb-118m25,00(2) StundenEE/β+ zu 118Sn100 %250(6) keV
Sb-11938,19(22) StundenEE zu 119Sn100 %0,591(8) MeVAL
Sb-119m1130(3) ns2553,6(3) keV
Sb-119m20,85(9) sIso zu 119Sb100 %2841,7+x keV
Sb-12015,89(4) MinutenEE/β+ zu 120Sn100 %2,681(7) MeVAL
Sb-120m15,76(2) TageEE/β+ zu 120Sn100 %+x keV
Sb-120m2246(2) ns78,16(5) keV
Sb-120m3400(8) ns2328,3+x keV
Sb-121stabilAL
Sb-121m179(6) μsIso zu 121Sb100 %2721,5+x keV
Sb-1222,7238(2) TageEE/β+ zu 122Sn
β- zu 122Te
2,41(12) %
97,59(12) %
1,606(4) MeV
1,9791(21) MeV
AL
Sb-122m11,86(8) μs61,4131(5) keV
Sb-122m20,53(3) msIso zu 122Sb100 %137,4726(8) keV
Sb-122m34,191(3) MinutenIso zu 122Sb100 %163,5591(17) keV
Sb-123stabilAL
Sb-12460,20(3) Tageβ- zu 124Te100 %2,90507(13) MeVAL
Sb-124m193(5) sβ- zu 124Te
Iso zu 124Sb
25(5) %
75(5) %

10,8627(8) keV
Sb-124m220,2(2) MinutenIso zu 124Sb100 %36,8440(14) keV
Sb-124m33,2(3) μs40,8038(7) keV
Sb-1252,75856(25) Jahreβ- zu 125Te100 %0,7666(21) MeVAL
Sb-12612,35(6) Tageβ- zu 126Te100 %3,67(3) MeVAL
Sb-126m119,15(8) Minutenβ- zu 126Te
Iso zu 126Sb
86(4) %
14(4) %

17,7(3) keV
Sb-126m211 sIso zu 126Sb100 %40,4(3) keV
Sb-126m3553(5) ns104,6(3) keV
Sb-1273,85(5) Tageβ- zu 127Te100 %1,582(5) MeVAL
Sb-127m111(7) μs1920,19(21) keV
Sb-127m20,165(20) μs2324,7(4) keV
Sb-1289,05(4) Stundenβ- zu 128Te100 %4,363(19) MeVAL
Sb-128m10,41(18) Minutenβ- zu 128Te
Iso zu 128Sb
96,4 %
3,6 %

+x keV
Sb-1294,366(26) Stundenβ- zu 129Te100 %2,375(21) MeVAL
Sb-129m117,7(1) Minutenβ- zu 129Te
Iso zu 129Sb
85 %
15 %

1851,31(6) keV
Sb-129m22,2(2) μsIso zu 129Sb1861,06(5) keV
Sb-13039,5(8) Minutenβ- zu 130Te100 %5,067(14) MeVAL
Sb-130m6,3(2) Minutenβ- zu 130Te100 %4,8(2) keV
Sb-13123,03(4) Minutenβ- zu 131Te100 %3,2296(21) MeVAL
Sb-131m191(4) μs1676,06(6) keV
Sb-131m24,3(8) μs1687,2(9) keV
Sb-131m31,1(2) μs2165,6(15) keV
Sb-1322,79(7) Minutenβ- zu 132Te100 %5,553(4) MeVAL
Sb-132m14,10(5) Minutenβ- zu 132Te100 %+x keV
Sb-1332,34(5) Minutenβ- zu 133Te100 %4,014(4) MeVAL
Sb-1340,78(6) sβ- zu 134Te100 %8,513(3) MeVAL
Sb-134m10,07(5) sβ- zu 134Te
β-, n zu 133Te
99,922 %
0,088(4) %

279(1) keV
Sb-1351,679(15) sβ- zu 135Te
β-, n zu 134Te
88(3) %
22(3) %
8,038(3) MeV
4,772(4) MeV
AL
Sb-136923(14) msβ- zu 136Te
β-, n zu 135Te
β-, 2n zu 134Te
81,5 %
18,5(18) %
< 1 %
9,95 MeV
5,31 MeV
AL
Sb-137450(50) msβ- zu 137Te
β-, n zu 136Te
51 %
49(10) %
9,24(5) MeV
6,29(5) MeV
AL
Sb-138348(15) msβ-, n 137Te
β-, 2n zu 138Te
β- zu 136Te
72(8) %
?
?
7,01 MeV

AL
Sb-13993(13) msβ- zu 139Te
β-, n zu 138Te
β-, 2n zu 137Te
β-, 3n zu 138Te
100 %
90(10) %
?
?
10,4 MeV


AL
Sb-140173(12) msβ- zu 140Te
β-, n zu 139Te
β-, 2n zu 138Te
69,4 %
23(4) %
7,6(25) %
12,64(60) MeV

AL
Sb-141β- zu 141Te
β-, n zu 140Te
β-, 2n zu 139Te
100 %
?
?
11,38(64) MeV
9,39(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 Antimon-Isotops; gegebenenfalls Trivialnamen.
6 - Relative Atommasse des Antimon-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 Antimon-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 Antimon-Nuklide

Nuklid
Anteil
Spin I
Kernmagnetisches
Moment
μ/μN
Gyromagnetisches
Verhältnis
107 rad T-1 s-1
Quadrupol-
Moment
Q [barn]
Resonanz-
Frequenz
v0 bei 1 T
Relative
Empfindlichkeit
H0 = const.
v0 = const. *
121Sb
57,21(5) %
5/2+
+ 3,3580(16)6,4442-0,543(11)10,25510,16302
2,8101
123Sb
42,79(5) %
7/2+
+ 2,5457(12)3,4904- 0,692(14)5,55320,04659
2,7390

*) bezogen auf 1H = 1,000

 

Strahlenschutz

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

NuklidFreigrenzenHRQ-SchwelleOFKTochternuklideHalbwertszeit
Sb-115106 Bq10 Bq/g32,1 Minuten
Sb-116106 Bq10 Bq/g15,8 Minuten
Sb-116m105 Bq10 Bq/g60,3 Minuten
Sb-117107 Bq100 Bq/g2,8 Stunden
Sb-118m106 Bq10 Bq/g5,0 Stunden
Sb-119107 Bq1000 Bq/g38,3 Stunden
Sb-120m106 Bq10 Bq/g5,8 Tage
Sb-122104 Bq10 Bq/g0,1 TBq10 Bq cm-22,7 Tage
Sb-124106 Bq1 Bq/g0,04 TBq1 Bq cm-260,2 Tage
Sb-125+106 Bq0,1 Bq/g0,2 TBq10 Bq cm-2Te-125m2,8 Jahre
Sb-126105 Bq10 Bq/g0,02 TBq12,4 Tage
Sb-126m105 Bq10 Bq/g19,1 Minuten
Sb-127+106 Bq10 Bq/g3,9 Tage
Sb-128m105 Bq10 Bq/g9,0 Stunden
Sb-129+106 Bq10 Bq/g4,4 Stunden
Sb-130105 Bq10 Bq/g39,5 Minuten
Sb-131106 Bq10 Bq/g23,0 Minuten

(HRQ = Hochradioaktive Quellen; OFK = Oberflächenkontamination)

 

Kernisobare Nuklide des Antimons

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

Z:383940414243444546474849505152535455565758596061626364656667
ASrYZrNbMoTcRuRhPdAgCdInSnSbTeIXeCsBaLaCePrNdPmSmEuGdTbDyHo
103103Sr103Y103Zr103Nb103Mo103Tc103Ru103Rh103Pd103Ag103Cd103In103Sn103Sb
104104Sr104Y104Zr104Nb104Mo104Tc104Ru104Rh104Pd104Ag104Cd104In104Sn104Sb
105105Sr105Y105Zr105Nb105Mo105Tc105Ru105Rh105Pd105Ag105Cd105In105Sn105Sb105Te
106106Sr106Y106Zr106Nb106Mo106Tc106Ru106Rh106Pd106Ag106Cd106In106Sn106Sb106Te
107107Sr107Y107Zr107Nb107Mo107Tc107Ru107Rh107Pd107Ag107Cd107In107Sn107Sb107Te
108108Y108Zr108Nb108Mo108Tc108Ru108Rh108Pd108Ag108Cd108In108Sn108Sb108Te108I
109109Y109Zr109Nb109Mo109Tc109Ru109Rh109Pd109Ag109Cd109In109Sn109Sb109Te109I109Xe
110110Zr110Nb110Mo110Tc110Ru110Rh110Pd110Ag110Cd110In110Sn110Sb110Te110I110Xe
111111Zr111Nb111Mo111Tc111Ru111Rh111Pd111Ag111Cd111In111Sn111Sb111Te111I111Xe
112112Zr112Nb112Mo112Tc112Ru112Rh112Pd112Ag112Cd112In112Sn112Sb112Te112I112Xe112Cs
113113Nb113Mo113Tc113Ru113Rh113Pd113Ag113Cd113In113Sn113Sb113Te113I113Xe113Cs
114114Nb114Mo114Tc114Ru114Rh114Pd114Ag114Cd114In114Sn114Sb114Te114I114Xe114Cs114Ba
115115Nb115Mo115Tc115Ru115Rh115Pd115Ag115Cd115In115Sn115Sb115Te115I115Xe115Cs115Ba
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

 

Kernisotone Nuklide des Antimons

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


5253545556575859606162636465666768697071727374757677787980818283848586878889
81Cu82Cu
82Zn83Zn84Zn
83Ga84Ga85Ga86Ga87Ga
84Ge85Ge86Ge87Ge88Ge89Ge
85As86As87As88As89As90As91As92As
86Se87Se88Se89Se90Se91Se92Se93Se94Se
87Br88Br89Br90Br91Br92Br93Br94Br95Br96Br97Br98Br
88Kr89Kr90Kr91Kr92Kr93Kr94Kr95Kr96Kr97Kr98Kr99Kr100Kr101Kr
89Rb90Rb91Rb92Rb93Rb94Rb95Rb96Rb97Rb98Rb99Rb100Rb101Rb102Rb
90Sr91Sr92Sr93Sr94Sr95Sr96Sr97Sr98Sr99Sr100Sr101Sr102Sr103Sr104Sr105Sr106Sr107Sr
91Y92Y93Y94Y95Y96Y97Y98Y99Y100Y101Y102Y103Y104Y105Y106Y107Y108Y109Y
92Zr93Zr94Zr95Zr96Zr97Zr98Zr99Zr100Zr101Zr102Zr103Zr104Zr105Zr106Zr107Zr108Zr109Zr110Zr111Zr112Zr
93Nb94Nb95Nb96Nb97Nb98Nb99Nb100Nb101Nb102Nb103Nb104Nb105Nb106Nb107Nb108Nb109Nb110Nb111Nb112Nb113Nb114Nb115Nb
94Mo95Mo96Mo97Mo98Mo99Mo100Mo101Mo102Mo103Mo104Mo105Mo106Mo107Mo108Mo109Mo110Mo111Mo112Mo113Mo114Mo115Mo116Mo117Mo
95Tc96Tc97Tc98Tc99Tc100Tc101Tc102Tc103Tc104Tc105Tc106Tc107Tc108Tc109Tc110Tc111Tc112Tc113Tc114Tc115Tc116Tc117Tc118Tc119Tc120Tc
96Ru97Ru98Ru99Ru100Ru101Ru102Ru103Ru104Ru105Ru106Ru107Ru108Ru109Ru110Ru111Ru112Ru113Ru114Ru115Ru116Ru117Ru118Ru119Ru120Ru121Ru122Ru123Ru124Ru
97Rh98Rh99Rh100Rh101Rh102Rh103Rh104Rh105Rh106Rh107Rh108Rh109Rh110Rh111Rh112Rh113Rh114Rh115Rh116Rh117Rh118Rh119Rh120Rh121Rh122Rh123Rh124Rh125Rh126Rh
98Pd99Pd100Pd101Pd102Pd103Pd104Pd105Pd106Pd107Pd108Pd109Pd110Pd111Pd112Pd113Pd114Pd115Pd116Pd117Pd118Pd119Pd120Pd121Pd122Pd123Pd124Pd125Pd126Pd127Pd128Pd
99Ag100Ag101Ag102Ag103Ag104Ag105Ag106Ag107Ag108Ag109Ag110Ag111Ag112Ag113Ag114Ag115Ag116Ag117Ag118Ag119Ag120Ag121Ag122Ag123Ag124Ag125Ag126Ag127Ag128Ag129Ag130Ag
100Cd101Cd102Cd103Cd104Cd105Cd106Cd107Cd108Cd109Cd110Cd111Cd112Cd113Cd114Cd115Cd116Cd117Cd118Cd119Cd120Cd121Cd122Cd123Cd124Cd125Cd126Cd127Cd128Cd129Cd130Cd131Cd132Cd133Cd
101In102In103In104In105In106In107In108In109In110In111In112In113In114In115In116In117In118In119In120In121In122In123In124In125In126In127In128In129In130In131In132In133In134In135In
102Sn103Sn104Sn105Sn106Sn107Sn108Sn109Sn110Sn111Sn112Sn113Sn114Sn115Sn116Sn117Sn118Sn119Sn120Sn121Sn122Sn123Sn124Sn125Sn126Sn127Sn128Sn129Sn130Sn131Sn132Sn133Sn134Sn135Sn136Sn137Sn138Sn
103Sb104Sb105Sb106Sb107Sb108Sb109Sb110Sb111Sb112Sb113Sb114Sb115Sb116Sb117Sb118Sb119Sb120Sb121Sb122Sb123Sb124Sb125Sb126Sb127Sb128Sb129Sb130Sb131Sb132Sb133Sb134Sb135Sb136Sb137Sb138Sb139Sb140Sb
105Te106Te107Te108Te109Te110Te111Te112Te113Te114Te115Te116Te117Te118Te119Te120Te121Te122Te123Te124Te125Te126Te127Te128Te129Te130Te131Te132Te133Te134Te135Te136Te137Te138Te139Te140Te141Te
108I109I110I111I112I113I114I115I116I117I118I119I120I121I122I123I124I125I126I127I128I129I130I131I132I133I134I135I136I137I138I139I140I141I142I
109Xe110Xe111Xe112Xe113Xe114Xe115Xe116Xe117Xe118Xe119Xe120Xe121Xe122Xe123Xe124Xe125Xe126Xe127Xe128Xe129Xe130Xe131Xe132Xe133Xe134Xe135Xe136Xe137Xe138Xe139Xe140Xe141Xe142Xe143Xe
112Cs113Cs114Cs115Cs116Cs117Cs118Cs119Cs120Cs121Cs122Cs123Cs124Cs125Cs126Cs127Cs128Cs129Cs130Cs131Cs132Cs133Cs134Cs135Cs136Cs137Cs138Cs139Cs140Cs141Cs142Cs143Cs144Cs
114Ba115Ba116Ba117Ba118Ba119Ba120Ba121Ba122Ba123Ba124Ba125Ba126Ba127Ba128Ba129Ba130Ba131Ba132Ba133Ba134Ba135Ba136Ba137Ba138Ba139Ba140Ba141Ba142Ba143Ba144Ba145Ba
116La117La118La119La120La121La122La123La124La125La126La127La128La129La130La131La132La133La134La135La136La137La138La139La140La141La142La143La144La145La146La
119Ce120Ce121Ce122Ce123Ce124Ce125Ce126Ce127Ce128Ce129Ce130Ce131Ce132Ce133Ce134Ce135Ce136Ce137Ce138Ce139Ce140Ce141Ce142Ce143Ce144Ce145Ce146Ce147Ce
121Pr122Pr123Pr124Pr125Pr126Pr127Pr128Pr129Pr130Pr131Pr132Pr133Pr134Pr135Pr136Pr137Pr138Pr139Pr140Pr141Pr142Pr143Pr144Pr145Pr146Pr147Pr148Pr
124Nd125Nd126Nd127Nd128Nd129Nd130Nd131Nd132Nd133Nd134Nd135Nd136Nd137Nd138Nd139Nd140Nd141Nd142Nd143Nd144Nd145Nd146Nd147Nd148Nd149Nd
126Pm127Pm128Pm129Pm130Pm131Pm132Pm133Pm134Pm135Pm136Pm137Pm138Pm139Pm140Pm141Pm142Pm143Pm144Pm145Pm146Pm147Pm148Pm149Pm150Pm
128Sm129Sm130Sm131Sm132Sm133Sm134Sm135Sm136Sm137Sm138Sm139Sm140Sm141Sm142Sm143Sm144Sm145Sm146Sm147Sm148Sm149Sm150Sm151Sm
130Eu131Eu132Eu133Eu134Eu135Eu136Eu137Eu138Eu139Eu140Eu141Eu142Eu143Eu144Eu145Eu146Eu147Eu148Eu149Eu150Eu151Eu152Eu
134Gd135Gd136Gd137Gd138Gd139Gd140Gd141Gd142Gd143Gd144Gd145Gd146Gd147Gd148Gd149Gd150Gd151Gd152Gd153Gd
135Tb136Tb137Tb138Tb139Tb140Tb141Tb142Tb143Tb144Tb145Tb146Tb147Tb148Tb149Tb150Tb151Tb152Tb153Tb154Tb
138Dy139Dy140Dy141Dy142Dy143Dy144Dy145Dy146Dy147Dy148Dy149Dy150Dy151Dy152Dy153Dy154Dy155Dy
140Ho141Ho142Ho143Ho144Ho145Ho146Ho147Ho148Ho149Ho150Ho151Ho152Ho153Ho154Ho155Ho156Ho
143Er144Er145Er146Er147Er148Er149Er150Er151Er152Er153Er154Er155Er156Er157Er
144Tm145Tm146Tm147Tm148Tm149Tm150Tm151Tm152Tm153Tm154Tm155Tm156Tm157Tm158Tm
148Yb149Yb150Yb151Yb152Yb153Yb154Yb155Yb156Yb157Yb158Yb159Yb
150Lu151Lu152Lu153Lu154Lu155Lu156Lu157Lu158Lu159Lu160Lu
153Hf154Hf155Hf156Hf157Hf158Hf159Hf160Hf161Hf
155Ta156Ta157Ta158Ta159Ta160Ta161Ta162Ta
158W159W160W161W162W163W
159Re160Re161Re162Re163Re164Re
161Os162Os163Os164Os165Os
164Ir165Ir166Ir
166Pt167Pt

 

Literatur und Hinweise

Eigenschaften der Antimon-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.

Antimon: Kernmagnetische Eigenschaften - 121Sb-NMR, 123Sb-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.

[9] - Olivier Rouxel, John Ludden, Yves Fouquet:
Antimony isotope variations in natural systems and implications for their use as geochemical tracers.
In: Chemical Geology, (2003), DOI 10.1016/S0009-2541(03)00121-9.

[10] - J. Kathawa, C. Fry, M. Thoennessen:
Discovery of palladium, antimony, tellurium, iodine, and xenon isotopes.
In: Atomic Data and Nuclear Data Tables, (2013), DOI 10.1016/j.adt.2012.01.004.

 


Kategorie: Chemische Elemente

Letzte Änderung am 12.12.2022.


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