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Rhodium-Isotope

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



Rhodium Isotope

Unter Rhodium-Isotope werden alle Atomkerne des chemischen Elements Rhodium zusammengefasst; diese bestehen allesamt aus einem Atomkern mit 45 Protonen und im ungeladenen Zustand aus 45 Elektronen. Der Unterschied zwischen den einzelnen Rhodium-Isotopen beruht auf der Anzahl der Neutronen im Kern.

 

Natürlich auftretende Rhodium-Isotope

In der Natur tritt nur ein einziges Isotop des Rhodiums auf: 103Rh, Standard-Atommasse 102,90550(2) u; es zählt damit zu den mononukliden Elementen (Reinelemente).

 

Alle anderen bisher bekannten und charakterisierten Rhodium-Nuklide sind instabil und besitzen keinerlei Bedeutung für technische Anwendungen.

 

Isotopentabelle: Rhodium

Isotop
Nuklid
ZANNameAtommasse
[Kernmasse]
{Massenüberschuss}
Spin I
(h/2π)
μA-Nuk
123456789
89Rh458944Rhodium-8988,95077(39) u
[88,9260852 u]
{-45,85745 MeV}
7/2+
90Rh459045Rhodium-9089,94450(32) u
[89,9198152 u]
{-51,69792 MeV}
91Rh459146Rhodium-9190,93712(32) u
[90,9124352 u]
{-58,57234 MeV}
(9/2+)
91mRh459146Rhodium-91m90,93712(32) u
[90,9124352 u]
{-58,57234 MeV}
(1/2-)
92Rh459247Rhodium-9291,932368(5) u
[91,9076832 u]
{-62,9988 MeV}
(6+)92Ru
92mRh459247Rhodium-92m91,932368(5) u
[91,9076832 u]
{-62,9988 MeV}
(2+)
93Rh459348Rhodium-9392,9259128(28) u
[92,901228 u]
{-69,01178 MeV}
(9/2+)93Pd
94Rh459449Rhodium-9493,921730(4) u
[93,8970452 u]
{-72,90804 MeV}
(4+)94Pd
95Ag
94mRh459449Rhodium-94m93,921730(4) u
[93,8970452 u]
{-72,90804 MeV}
(8+)
95Rh459550Rhodium-9594,915898(4) u
[94,8912132 u]
{-78,34051 MeV}
9/2+95Pd
95mRh459550Rhodium-95m94,915898(4) u
[94,8912132 u]
{-78,34051 MeV}
(1/2)-
96Rh459651Rhodium-9695,914452(11) u
[95,8897672 u]
{-79,68745 MeV}
6+96Pd
96mRh459651Rhodium-96m95,914452(11) u
[95,8897672 u]
{-79,68745 MeV}
3+
97Rh459752Rhodium-9796,91133(4) u
[96,8866452 u]
{-82,59557 MeV}
9/2+97Pd
98Ag
97mRh459752Rhodium-97m96,91133(4) u
[96,8866452 u]
{-82,59557 MeV}
1/2-
98Rh459853Rhodium-9897,910708(13) u
[97,8860232 u]
{-83,17496 MeV}
(2)+98Pd
98mRh459853Rhodium-98m97,910708(13) u
[97,8860232 u]
{-83,17496 MeV}
(5+)
99Rh459954Rhodium-9998,908125(7) u
[98,8834402 u]
{-85,58101 MeV}
1/2-99Pd
99mRh459954Rhodium-99m98,908125(7) u
[98,8834402 u]
{-85,58101 MeV}
9/2+5,62(6)
100Rh4510055Rhodium-10099,908114(19) u
[99,8834292 u]
{-85,59126 MeV}
1-100Pd
100m1Rh4510055Rhodium-100m199,908114(19) u
[99,8834292 u]
{-85,59126 MeV}
(2)++4,324(8)
100m2Rh4510055Rhodium-100m299,908114(19) u
[99,8834292 u]
{-85,59126 MeV}
(5+)
100m3Rh4510055Rhodium-100m399,908114(19) u
[99,8834292 u]
{-85,59126 MeV}
(7+)+4,69(14)
101Rh4510156Rhodium-101100,906159(6) u
[100,8814742 u]
{-87,41233 MeV}
1/2-101Pd
101mRh4510156Rhodium-101m100,906159(6) u
[100,8814742 u]
{-87,41233 MeV}
9/2++ 5,43(6)
102Rh4510257Rhodium-102101,906834(7) u
[101,8821492 u]
{-86,78357 MeV}
(2-)0,5(4)
102mRh4510257Rhodium-102m101,906834(7) u
[101,8821492 u]
{-86,78357 MeV}
6(+)4,01(4)
103Rh4510358Rhodium-103102,90550(2) u
[102,8808152 u]
{-88,02618 MeV}
1/2-- 0,08829(3)103Pd
103Ru
103mRh4510358Rhodium-103m102,90550(2) u
[102,8808152 u]
{-88,02618 MeV}
7/2++ 4,50(5)
104Rh4510459Rhodium-104103,9066453(25) u
[103,8819605 u]
{-86,95934 MeV}
1+
104mRh4510459Rhodium-104m103,9066453(25) u
[103,8819605 u]
{-86,95934 MeV}
5+
105Rh4510560Rhodium-105104,9056878(27) u
[104,881003 u]
{-87,85125 MeV}
7/2+4,41(5)105Ru
105mRh4510560Rhodium-105m104,9056878(27) u
[104,881003 u]
{-87,85125 MeV}
1/2-
106Rh4510661Rhodium-106105,907286(6) u
[105,8826012 u]
{-86,36253 MeV}
1+2,55(3)106Ru
106mRh4510661Rhodium-106m105,907286(6) u
[105,8826012 u]
{-86,36253 MeV}
(6)+
107Rh4510762Rhodium-107106,906748(13) u
[106,8820632 u]
{-86,86368 MeV}
7/2+107Ru
107mRh4510762Rhodium-107m106,906748(13) u
[106,8820632 u]
{-86,86368 MeV}
1/2-
108Rh4510863Rhodium-108107,908715(15) u
[107,8840302 u]
{-85,03143 MeV}
1+108Ru
108mRh4510863Rhodium-108m107,908715(15) u
[107,8840302 u]
{-85,03143 MeV}
(5+)
109Rh4510964Rhodium-109108,908749(4) u
[108,8840642 u]
{-84,99976 MeV}
7/2+109Ru
109mRh4510964Rhodium-109m108,908749(4) u
[108,8840642 u]
{-84,99976 MeV}
3/2+
110Rh4511065Rhodium-110109,911080(19) u
[109,8863952 u]
{-82,82845 MeV}
(1+)
110mRh4511065Rhodium-110m109,911080(19) u
[109,8863952 u]
{-82,82845 MeV}
(6+)
111Rh4511166Rhodium-111110,911643(7) u
[110,8869582 u]
{-82,30402 MeV}
(7/2+)111Ru
112Rh4511267Rhodium-112111,91440(5) u
[111,8897152 u]
{-79,73589 MeV}
(1+)112Ru
112mRh4511267Rhodium-112m111,91440(5) u
[111,8897152 u]
{-79,73589 MeV}
(6+)
113Rh4511368Rhodium-113112,915440(8) u
[112,8907552 u]
{-78,76713 MeV}
(7/2+)113Ru
114Rh4511469Rhodium-114113,91872(8) u
[113,8940352 u]
{-75,71183 MeV}
1+114Ru
114mRh4511469Rhodium-114m113,91872(8) u
[113,8940352 u]
{-75,71183 MeV}
(7-)
115Rh4511570Rhodium-115114,920311(8) u
[114,8956262 u]
{-74,22983 MeV}
(7/2+)115Ru
116Rh4511671Rhodium-116115,92406(8) u
[115,8993752 u]
{-70,73765 MeV}
1+
116mRh4511671Rhodium-116m115,92406(8) u
[115,8993752 u]
{-70,73765 MeV}
(6-)
117Rh4511772Rhodium-117116,926036(10) u
[116,9013512 u]
{-68,89702 MeV}
(7/2+)
118Rh4511873Rhodium-118117,930340(26) u
[117,9056552 u]
{-64,88787 MeV}
119Rh4511974Rhodium-119118,932557(10) u
[118,9078722 u]
{-62,82275 MeV}
(7/2+)
120Rh4512075Rhodium-120119,93686(21) u
[119,9121752 u]
{-58,81453 MeV}
120mRh4512075Rhodium-120m119,93686(21) u
[119,9121752 u]
{-58,81453 MeV}
121Rh4512176Rhodium-121120,93961(66) u
[120,9149252 u]
{-56,25292 MeV}
122Rh4512277Rhodium-122121,94409(32) u
[121,9194052 u]
{-52,07983 MeV}
122mRh4512277Rhodium-122m121,94409(32) u
[121,9194052 u]
{-52,07983 MeV}
123Rh4512378Rhodium-123122,94701(43) u
[122,9223252 u]
{-49,35987 MeV}
124Rh4512479Rhodium-124123,95181(43) u
[123,9271252 u]
{-44,8887 MeV}
125Rh4512580Rhodium-125124,95491(54) u
[124,9302252 u]
{-42,00106 MeV}
126Rh4512681Rhodium-126125,95996(54) u
[125,9352752 u]
{-37,29702 MeV}
127Rh4512782Rhodium-127126,96347(64) u
[126,9387852 u]
{-34,02748 MeV}

 

 

IsotopZerfall (radioaktiver Zerfall)AEMehr
HalbwertszeitZerfallsartAnteilEnergieInfo
1101112131415
Rh-89120 nsEE/β+ zu 89Ru
EE, p zu 88Tc
p zu 88Ru
?
?
?
12,40(47) MeV

AL
Rh-90150 nsAL
Rh-911,47(22) sEE/β+ zu 91Ru
β+, p zu 90Tc
98,7 %
1,3(5) %
9,67(30) MeV
AL
Rh-91m1,46(11) sEE/β+ zu 91Ru
Iso zu 91Rh
?
?

172,9(4) keV
Rh-924,66(25) sEE/β+ zu 92Ru
β+, p zu 91Tc
98,1 %
1,9(1) %
11,302(5) MeV
AL
Rh-92m0,53(37) sEE/β+ zu 92Ru100 %+ X
Rh-9312,2(7) sEE/β+ zu 93Ru100 %8,205(3) MeVAL
Rh-9470,6(6) sEE/β+ zu 94Ru
ε, p zu 93Tc
98,2(5) %
1,8(5) %
9,676(5) MeV
AL
Rh-94m25,8(2) sEE/β+ zu 94Ru100 %+x keV
Rh-955,02(10) MinutenEE/β+ zu 95Ru100 %5,117(10) MeVAL
Rh-95m1,96(4) MinutenEE/β+ zu 95Ru
Iso zu 95Rh
12(5) %
88(5) %

543,3(3) keV
Rh-969,90(10) MinutenEE/β+ zu 96Ru100 %6,393(10) MeVAL
Rh-96m1,51(2) MinutenEE/β+ zu 96Ru
Iso zu 96Rh
40(5) %
60(5) %

51,98(9) keV
Rh-9730,7(6) MinutenEE/β+ zu 97Ru100 %3,52(4) MeVAL
Rh-97m46,2(16) MinutenEE/β+ zu 97Ru
Iso zu 97Rh
94,4(6) %
5,6(6) %

258,76(18) keV
Rh-988,72(12) MinutenEE/β+ zu 98Ru100 %5,050(14) MeVAL
Rh-98m3,6(2) MinutenEE/β+ zu 98Ru
Iso zu 98Rh
11(5) %
89(5) %

+x keV
Rh-9916,1(2) TageEE/β+ zu 99Ru100 %2,044(7) MeVAL
Rh-99m4,7(1) StundenEE/β+ zu 99Ru
Iso zu 99Rh
> 99,84 %
< 0,16 %

64,4(5) keV
Rh-10020,8(1) StundenEE/β+ zu 100Ru100 %3,636(18) MeVAL
Rh-100m1214,0(20) ns74,782(14) keV
Rh-100m24,6(2) MinutenEE/β+ zu 100Ru
Iso zu 100Rh
ca. 1,7 %
ca. 98,3 %

107,60(20) MeV
Rh-100m3130(10) ns219,61(22) keV
Rh-1013,3(3) JahreEE zu 101Ru100 %0,546(6) MeVAL
Rh-101m4,34(1) TageEE zu 101Ru
Iso zu 101Rh
92,80(25) %
7,20(25) %

157,32(3) keV
Rh-102207,3(17) TageEE/β+ zu 102Ru
β- zu 102Pd
78(5) %
22(5) %
2,323(6) MeV
1,120(6) MeV
AL
Rh-102m3,742(10) JahreEE/β+ zu 103Ru
Iso zu 102Rh
99,767(24) %
0,233(24) %

140,73(9) keV
Rh-103stabilAL
Rh-103m56,114(9) MinutenIso zu 103Rh100 %39,753(6) keV
Rh-10442,3(4) sEE/β+ zu 104Ru
β- zu 104Pd
0,45(10) %
99,55(10) %
1,136(3) MeV
2,4358(27) MeV
AL
Rh-104m4,34(3) MinutenIso zu 104Rh
β- zu 104Pd
99,87(1) %
0,13(1) %

128,9679(5) keV
Rh-10535,36(6) Stundenβ- zu 105Pd100 %0,566(23) MeVAL
Rh-105m42,9(3) sIso zu 105Rh100 %129,782(4) keV
Rh-10630,07(35) sβ- zu 106Pd100 %3,545(5) MeVAL
Rh-106m131(2) Minutenβ- zu 106Pd100 %137(13) keV
Rh-10721,7(4) Minutenβ- zu 107Pd100 %1,5109(12) MeVAL
Rh-107m10 μs268,36(4) keV
Rh-10816,8(5) sβ- zu 108Pd100 %4,492(14) MeVAL
Rh-108m6,0(3) Minutenβ- zu 108Pd
Iso zu 108Rh
< 100 %
?

+x keV
Rh-10980,8(7) sβ- zu 109Pd100 %2,607(4) MeVAL
Rh-109m1,66(4) μs225,873(19) keV
Rh-1103,35(12) sβ- zu 110Pd100 %5,502(18) MeVAL
Rh-110m28,0(13) sβ- zu 110Pd100 %+y keV
Rh-11111(1) sβ- zu 111Pd100 %3,681(7) MeVAL
Rh-1123,6(3) sβ- zu 112Pd100 %6,59(4) MeV+ XAL
Rh-112m6,76(12) sβ- zu 112Pd100 %+y keV
Rh-1132,80(12) sβ- zu 113Pd100 %4,824(10) MeVAL
Rh-1141,85(5) sβ- zu 114Pd100 %7,78(7) MeVAL
Rh-114m1,85(5) sβ- zu 114Pd100 %+x keV
Rh-1150,99(5) sβ- zu 115Pd100 %6,197(15) MeVAL
Rh-1160,68(6) sβ- zu 116Pd100 %9,10(7) MeVAL
Rh-116m0,57(5) sβ- zu 116Pd100 %150 keV
Rh-1170,44(4) sβ- zu 117Pd100 %7,527(11) MeVAL
Rh-118266 msβ- zu 118Pd
β-, n zu 117Pd
96,9(14) %
3,1(14) %
10,501(24) MeV
3,466(25) MeV
AL
Rh-119171(18) msβ- zu 119Pd
β-, n zu 118Pd
93,6(16) %
6,4(16) %
8,585(12) MeV
4,495(10) MeV
AL
Rh-120132 msβ- zu 120Pd
β-, n zu 119Pd
> 94,6 %
< 5,4 %
11,47(20) MeV
4,52(20) MeV
AL
Rh-120m0,294 μsIso zu 120Rh100 %157,2(7) keV
Rh-121151 msβ- zu 121Pd
β-, n zu 120Pd
< 100 %
?
9,93(62) MeV
5,96(62) MeV
AL
Rh-122300 nsβ- zu 122Pd
β-, n zu 121Pd
β-, 2n zu 120Pd
?
?
?
12,54(30) MeV
6,03(30) MeV
AL
Rh-122m0,82 μsIso zu 122Rh100 %271,0(7) keV
Rh-12342(4) msβ- zu 123Pd
β-, n zu 122Pd
β-, 2n zu 121Pd
100 %
?
?
11,07(88) MeV
7,18(40) MeV
AL
Rh-12430(2) msβ- zu 124Pd
β-, n zu 123Pd
β-, 2n zu 122Pd
100 %
?
?
13,50(50) MeV
7,47(88) MeV
AL
Rh-12526,5(20) msβ- zu 125Pd
β-, n zu 124Pd
β-, 2n zu 123Pd
100 %
?
?
12,12(64) MeV
8,32(58) MeV
AL
Rh-12619(3) msβ- zu 126Pd
β-, n zu 125Pd
β-, 2n zu 124Pd
100 %
?
?
14,56(64) MeV
8,75(64) MeV
AL
Rh-12720 msβ- zu 127Pd
β-, n zu 126Pd
β-, 2n zu 125Pd
100 %
?
?
13,15(78) MeV
9,76(72) 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 Rhodium-Isotops; gegebenenfalls Trivialnamen.
6 - Relative Atommasse des Rhodium-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 Rhodium-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 Rhodium-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. *
103Rh
100 %
1/2-
- 0,08829(3)- 0,84681,34770,00003
0,0317

*) bezogen auf 1H = 1,000

 

Strahlenschutz

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

NuklidFreigrenzenHRQ-SchwelleOFKTochternuklideHalbwertszeit
Rh-99106 Bq10 Bq/g16,1 Tage
Rh-99m106 Bq10 Bq/g4,7 Stunden
Rh-100106 Bq10 Bq/g20,8 Stunden
Rh-101107 Bq1 Bq/g0,3 TBq3,2 Jahre
Rh-101m107 Bq100 Bq/g4,3 Tage
Rh-102106 Bq0,1 Bq/g0,03 TBq2,9 Jahre
Rh-102m106 Bq1 Bq/g0,1 TBq219,0 Tage
Rh-103m108 Bq10000 Bq/g900 TBq100 Bq cm-256,1 Minuten
Rh-105107 Bq100 Bq/g0,9 TBq10 Bq cm-235,4 Stunden
Rh-106m105 Bq10 Bq/g2,2 Stunden
Rh-107106 Bq100 Bq/g21,7 Minuten

(HRQ = Hochradioaktive Quellen; OFK = Oberflächenkontamination)

 

Kernisobare Nuklide des Rhodiums

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

Z:323334353637383940414243444546474849505152535455565758596061
AGeAsSeBrKrRbSrYZrNbMoTcRuRhPdAgCdInSnSbTeIXeCsBaLaCePrNdPm
8989Ge89As89Se89Br89Kr89Rb89Sr89Y89Zr89Nb89Mo89Tc89Ru89Rh
9090As90Se90Br90Kr90Rb90Sr90Y90Zr90Nb90Mo90Tc90Ru90Rh
9191As91Se91Br91Kr91Rb91Sr91Y91Zr91Nb91Mo91Tc91Ru91Rh91Pd
9292As92Se92Br92Kr92Rb92Sr92Y92Zr92Nb92Mo92Tc92Ru92Rh92Pd
9393Se93Br93Kr93Rb93Sr93Y93Zr93Nb93Mo93Tc93Ru93Rh93Pd93Ag
9494Se94Br94Kr94Rb94Sr94Y94Zr94Nb94Mo94Tc94Ru94Rh94Pd94Ag
9595Br95Kr95Rb95Sr95Y95Zr95Nb95Mo95Tc95Ru95Rh95Pd95Ag95Cd
9696Br96Kr96Rb96Sr96Y96Zr96Nb96Mo96Tc96Ru96Rh96Pd96Ag96Cd
9797Br97Kr97Rb97Sr97Y97Zr97Nb97Mo97Tc97Ru97Rh97Pd97Ag97Cd97In
9898Br98Kr98Rb98Sr98Y98Zr98Nb98Mo98Tc98Ru98Rh98Pd98Ag98Cd98In
9999Kr99Rb99Sr99Y99Zr99Nb99Mo99Tc99Ru99Rh99Pd99Ag99Cd99In99Sn
100100Kr100Rb100Sr100Y100Zr100Nb100Mo100Tc100Ru100Rh100Pd100Ag100Cd100In100Sn
101101Kr101Rb101Sr101Y101Zr101Nb101Mo101Tc101Ru101Rh101Pd101Ag101Cd101In101Sn
102102Rb102Sr102Y102Zr102Nb102Mo102Tc102Ru102Rh102Pd102Ag102Cd102In102Sn
103103Sr103Y103Zr103Nb103Mo103Tc103Ru103Rh103Pd103Ag103Cd103In103Sn103Sb
104104Sr104Y104Zr104Nb104Mo104Tc104Ru104Rh104Pd104Ag104Cd104In104Sn104Sb
105105Sr105Y105Zr105Nb105Mo105Tc105Ru105Rh105Pd105Ag105Cd105In105Sn105Sb105Te
106106Sr106Y106Zr106Nb106Mo106Tc106Ru106Rh106Pd106Ag106Cd106In106Sn106Sb106Te
107107Sr107Y107Zr107Nb107Mo107Tc107Ru107Rh107Pd107Ag107Cd107In107Sn107Sb107Te
108108Y108Zr108Nb108Mo108Tc108Ru108Rh108Pd108Ag108Cd108In108Sn108Sb108Te108I
109109Y109Zr109Nb109Mo109Tc109Ru109Rh109Pd109Ag109Cd109In109Sn109Sb109Te109I109Xe
110110Zr110Nb110Mo110Tc110Ru110Rh110Pd110Ag110Cd110In110Sn110Sb110Te110I110Xe
111111Zr111Nb111Mo111Tc111Ru111Rh111Pd111Ag111Cd111In111Sn111Sb111Te111I111Xe
112112Zr112Nb112Mo112Tc112Ru112Rh112Pd112Ag112Cd112In112Sn112Sb112Te112I112Xe112Cs
113113Nb113Mo113Tc113Ru113Rh113Pd113Ag113Cd113In113Sn113Sb113Te113I113Xe113Cs
114114Nb114Mo114Tc114Ru114Rh114Pd114Ag114Cd114In114Sn114Sb114Te114I114Xe114Cs114Ba
115115Nb115Mo115Tc115Ru115Rh115Pd115Ag115Cd115In115Sn115Sb115Te115I115Xe115Cs115Ba
116116Mo116Tc116Ru116Rh116Pd116Ag116Cd116In116Sn116Sb116Te116I116Xe116Cs116Ba116La
117117Mo117Tc117Ru117Rh117Pd117Ag117Cd117In117Sn117Sb117Te117I117Xe117Cs117Ba117La
118118Tc118Ru118Rh118Pd118Ag118Cd118In118Sn118Sb118Te118I118Xe118Cs118Ba118La
119119Tc119Ru119Rh119Pd119Ag119Cd119In119Sn119Sb119Te119I119Xe119Cs119Ba119La119Ce
120120Tc120Ru120Rh120Pd120Ag120Cd120In120Sn120Sb120Te120I120Xe120Cs120Ba120La120Ce
121121Ru121Rh121Pd121Ag121Cd121In121Sn121Sb121Te121I121Xe121Cs121Ba121La121Ce121Pr
122122Ru122Rh122Pd122Ag122Cd122In122Sn122Sb122Te122I122Xe122Cs122Ba122La122Ce122Pr
123123Ru123Rh123Pd123Ag123Cd123In123Sn123Sb123Te123I123Xe123Cs123Ba123La123Ce123Pr
124124Ru124Rh124Pd124Ag124Cd124In124Sn124Sb124Te124I124Xe124Cs124Ba124La124Ce124Pr124Nd
125125Rh125Pd125Ag125Cd125In125Sn125Sb125Te125I125Xe125Cs125Ba125La125Ce125Pr125Nd
126126Rh126Pd126Ag126Cd126In126Sn126Sb126Te126I126Xe126Cs126Ba126La126Ce126Pr126Nd126Pm

 

Kernisotone Nuklide des Rhodiums

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


4445464748495051525354555657585960616263646566676869707172737475767778798081
67V
68Cr
69Mn
70Fe71Fe72Fe
71Co72Co73Co74Co75Co76Co
72Ni73Ni74Ni75Ni76Ni77Ni78Ni
73Cu74Cu75Cu76Cu77Cu78Cu79Cu80Cu81Cu82Cu
74Zn75Zn76Zn77Zn78Zn79Zn80Zn81Zn82Zn83Zn84Zn
75Ga76Ga77Ga78Ga79Ga80Ga81Ga82Ga83Ga84Ga85Ga86Ga87Ga
76Ge77Ge78Ge79Ge80Ge81Ge82Ge83Ge84Ge85Ge86Ge87Ge88Ge89Ge
77As78As79As80As81As82As83As84As85As86As87As88As89As90As91As92As
78Se79Se80Se81Se82Se83Se84Se85Se86Se87Se88Se89Se90Se91Se92Se93Se94Se
79Br80Br81Br82Br83Br84Br85Br86Br87Br88Br89Br90Br91Br92Br93Br94Br95Br96Br97Br98Br
80Kr81Kr82Kr83Kr84Kr85Kr86Kr87Kr88Kr89Kr90Kr91Kr92Kr93Kr94Kr95Kr96Kr97Kr98Kr99Kr100Kr101Kr
81Rb82Rb83Rb84Rb85Rb86Rb87Rb88Rb89Rb90Rb91Rb92Rb93Rb94Rb95Rb96Rb97Rb98Rb99Rb100Rb101Rb102Rb
82Sr83Sr84Sr85Sr86Sr87Sr88Sr89Sr90Sr91Sr92Sr93Sr94Sr95Sr96Sr97Sr98Sr99Sr100Sr101Sr102Sr103Sr104Sr105Sr106Sr107Sr
83Y84Y85Y86Y87Y88Y89Y90Y91Y92Y93Y94Y95Y96Y97Y98Y99Y100Y101Y102Y103Y104Y105Y106Y107Y108Y109Y
84Zr85Zr86Zr87Zr88Zr89Zr90Zr91Zr92Zr93Zr94Zr95Zr96Zr97Zr98Zr99Zr100Zr101Zr102Zr103Zr104Zr105Zr106Zr107Zr108Zr109Zr110Zr111Zr112Zr
85Nb86Nb87Nb88Nb89Nb90Nb91Nb92Nb93Nb94Nb95Nb96Nb97Nb98Nb99Nb100Nb101Nb102Nb103Nb104Nb105Nb106Nb107Nb108Nb109Nb110Nb111Nb112Nb113Nb114Nb115Nb
86Mo87Mo88Mo89Mo90Mo91Mo92Mo93Mo94Mo95Mo96Mo97Mo98Mo99Mo100Mo101Mo102Mo103Mo104Mo105Mo106Mo107Mo108Mo109Mo110Mo111Mo112Mo113Mo114Mo115Mo116Mo117Mo
87Tc88Tc89Tc90Tc91Tc92Tc93Tc94Tc95Tc96Tc97Tc98Tc99Tc100Tc101Tc102Tc103Tc104Tc105Tc106Tc107Tc108Tc109Tc110Tc111Tc112Tc113Tc114Tc115Tc116Tc117Tc118Tc119Tc120Tc
88Ru89Ru90Ru91Ru92Ru93Ru94Ru95Ru96Ru97Ru98Ru99Ru100Ru101Ru102Ru103Ru104Ru105Ru106Ru107Ru108Ru109Ru110Ru111Ru112Ru113Ru114Ru115Ru116Ru117Ru118Ru119Ru120Ru121Ru122Ru123Ru124Ru
89Rh90Rh91Rh92Rh93Rh94Rh95Rh96Rh97Rh98Rh99Rh100Rh101Rh102Rh103Rh104Rh105Rh106Rh107Rh108Rh109Rh110Rh111Rh112Rh113Rh114Rh115Rh116Rh117Rh118Rh119Rh120Rh121Rh122Rh123Rh124Rh125Rh126Rh
91Pd92Pd93Pd94Pd95Pd96Pd97Pd98Pd99Pd100Pd101Pd102Pd103Pd104Pd105Pd106Pd107Pd108Pd109Pd110Pd111Pd112Pd113Pd114Pd115Pd116Pd117Pd118Pd119Pd120Pd121Pd122Pd123Pd124Pd125Pd126Pd127Pd
93Ag94Ag95Ag96Ag97Ag98Ag99Ag100Ag101Ag102Ag103Ag104Ag105Ag106Ag107Ag108Ag109Ag110Ag111Ag112Ag113Ag114Ag115Ag116Ag117Ag118Ag119Ag120Ag121Ag122Ag123Ag124Ag125Ag126Ag127Ag128Ag
95Cd96Cd97Cd98Cd99Cd100Cd101Cd102Cd103Cd104Cd105Cd106Cd107Cd108Cd109Cd110Cd111Cd112Cd113Cd114Cd115Cd116Cd117Cd118Cd119Cd120Cd121Cd122Cd123Cd124Cd125Cd126Cd127Cd128Cd129Cd
97In98In99In100In101In102In103In104In105In106In107In108In109In110In111In112In113In114In115In116In117In118In119In120In121In122In123In124In125In126In127In128In129In130In
99Sn100Sn101Sn102Sn103Sn104Sn105Sn106Sn107Sn108Sn109Sn110Sn111Sn112Sn113Sn114Sn115Sn116Sn117Sn118Sn119Sn120Sn121Sn122Sn123Sn124Sn125Sn126Sn127Sn128Sn129Sn130Sn131Sn
103Sb104Sb105Sb106Sb107Sb108Sb109Sb110Sb111Sb112Sb113Sb114Sb115Sb116Sb117Sb118Sb119Sb120Sb121Sb122Sb123Sb124Sb125Sb126Sb127Sb128Sb129Sb130Sb131Sb132Sb
105Te106Te107Te108Te109Te110Te111Te112Te113Te114Te115Te116Te117Te118Te119Te120Te121Te122Te123Te124Te125Te126Te127Te128Te129Te130Te131Te132Te133Te
108I109I110I111I112I113I114I115I116I117I118I119I120I121I122I123I124I125I126I127I128I129I130I131I132I133I134I
109Xe110Xe111Xe112Xe113Xe114Xe115Xe116Xe117Xe118Xe119Xe120Xe121Xe122Xe123Xe124Xe125Xe126Xe127Xe128Xe129Xe130Xe131Xe132Xe133Xe134Xe135Xe
112Cs113Cs114Cs115Cs116Cs117Cs118Cs119Cs120Cs121Cs122Cs123Cs124Cs125Cs126Cs127Cs128Cs129Cs130Cs131Cs132Cs133Cs134Cs135Cs136Cs
114Ba115Ba116Ba117Ba118Ba119Ba120Ba121Ba122Ba123Ba124Ba125Ba126Ba127Ba128Ba129Ba130Ba131Ba132Ba133Ba134Ba135Ba136Ba137Ba
116La117La118La119La120La121La122La123La124La125La126La127La128La129La130La131La132La133La134La135La136La137La138La
119Ce120Ce121Ce122Ce123Ce124Ce125Ce126Ce127Ce128Ce129Ce130Ce131Ce132Ce133Ce134Ce135Ce136Ce137Ce138Ce139Ce
121Pr122Pr123Pr124Pr125Pr126Pr127Pr128Pr129Pr130Pr131Pr132Pr133Pr134Pr135Pr136Pr137Pr138Pr139Pr140Pr
124Nd125Nd126Nd127Nd128Nd129Nd130Nd131Nd132Nd133Nd134Nd135Nd136Nd137Nd138Nd139Nd140Nd141Nd
126Pm127Pm128Pm129Pm130Pm131Pm132Pm133Pm134Pm135Pm136Pm137Pm138Pm139Pm140Pm141Pm142Pm
128Sm129Sm130Sm131Sm132Sm133Sm134Sm135Sm136Sm137Sm138Sm139Sm140Sm141Sm142Sm143Sm
130Eu131Eu132Eu133Eu134Eu135Eu136Eu137Eu138Eu139Eu140Eu141Eu142Eu143Eu144Eu
134Gd135Gd136Gd137Gd138Gd139Gd140Gd141Gd142Gd143Gd144Gd145Gd
135Tb136Tb137Tb138Tb139Tb140Tb141Tb142Tb143Tb144Tb145Tb146Tb
138Dy139Dy140Dy141Dy142Dy143Dy144Dy145Dy146Dy147Dy
140Ho141Ho142Ho143Ho144Ho145Ho146Ho147Ho148Ho
143Er144Er145Er146Er147Er148Er149Er
144Tm145Tm146Tm147Tm148Tm149Tm150Tm
148Yb149Yb150Yb151Yb
150Lu151Lu152Lu
153Hf

 

Literatur und Hinweise

Eigenschaften der Rhodium-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.

Rhodium: Kernmagnetische Eigenschaften - 103Rh-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] - John W. Arblaster:
The Discoverers of the Rhodium Isotopes.
In: Platinum Metals Review, (2011), DOI 10.1595/147106711X555656.

[10] - A. M. Parker, M. Thoennessen:
Discovery of rubidium, strontium, molybdenum, and rhodium isotopes.
In: Atomic Data and Nuclear Data Tables, (2012), DOI 10.1016/j.adt.2012.06.001.

 


Kategorie: Chemische Elemente

Letzte Änderung am 05.07.2020.



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