Information about Isotopes Of Cadmium

Naturally occurring Cadmium (Cd) is composed of 8 isotopes. For two of them, natural radioactivity was observed, and three others are predicted to be radioactive but their decays were never observed, due to extremely long half-life times. The two natural radioactive isotopes are 113Cd (beta decay, half-life is 7.7 × 1015 years) and 116Cd (two-neutrino double beta decay, half-life is 2.9 × 1019 years). The other three are 106Cd, 108Cd (double electron capture), and 114Cd (double beta decay); only lower limits on their half-life times have been set. At least three isotopes - 110Cd, 111Cd, and 112Cd - are absolutely stable. Among the isotopes absent in the natural cadmium, the most long-lived are 109Cd with a half-life of 462.6 days, and 115Cd with a half-life of 53.46 hours. All of the remaining radioactive isotopes have half-lives that are less than 2.5 hours and the majority of these have half-lives that are less than 5 minutes. This element also has 8 known meta states with the most stable being 113mCd (t½ 14.1 years), 115mCd (t½ 44.6 days) and 117mCd (t½ 3.36 hours).

The known isotopes of cadmium range in atomic mass from 94.950 u (95Cd) to 131.946 u (132Cd). The primary decay mode before the second most abundant stable isotope, 112Cd, is electron capture and the primary modes after are beta emission and electron capture. The primary decay product before 112Cd is element 47 (silver) and the primary product after is element 49 (indium).
Standard atomic mass: 112.411(8) u

Table

nuclide
symbol
Z(p) N(n)  
isotopic mass (u)
 
half-life nuclear
spin
representative
isotopic
composition
(mole fraction)
range of natural
variation
(mole fraction)
excitation energy
95Cd484794.94987(64)#5# ms9/2+#
96Cd484895.93977(54)#1# s0+
97Cd484996.93494(43)#2.8(6) s9/2+#
98Cd485097.92740(8)9.2(3) s0+
98mCd2427.5(6) keV190(20) ns8+#
99Cd485198.92501(22)#16(3) s(5/2+)
100Cd485299.92029(10)49.1(5) s0+
101Cd4853100.91868(16)1.36(5) min(5/2+)
102Cd4854101.91446(3)5.5(5) min0+
103Cd4855102.913419(17)7.3(1) min5/2+
104Cd4856103.909849(10)57.7(10) min0+
105Cd4857104.909468(12)55.5(4) min5/2+
106Cd4858105.906459(6)STABLE [>410E+18 a]0+0.0125(6)
107Cd4859106.906618(6)6.50(2) h5/2+
108Cd4860107.904184(6)STABLE [>410E+15 a]0+0.0089(3)
109Cd4861108.904982(4)461.4(12) d5/2+
109m1Cd59.6(4) keV12(2) µs1/2+
109m2Cd463.0(5) keV10.9(5) µs11/2-
110Cd4862109.9030021(29)STABLE0+0.1249(18)
111Cd4863110.9041781(29)STABLE1/2+0.1280(12)
111mCd396.214(21) keV48.50(9) min11/2-
112Cd4864111.9027578(29)STABLE0+0.2413(21)
113Cd4865112.9044017(29)7.7(3)E+15 a1/2+0.1222(12)
113mCd263.54(3) keV14.1(5) a11/2-
114Cd4866113.9033585(29)STABLE [>6.4E+18 a]0+0.2873(42)
115Cd4867114.9054310(29)53.46(5) h1/2+
115mCd181.0(5) keV44.56(24) d(11/2)-
116Cd4868115.904756(3)3.1(4)E+19 a0+0.0749(18)
117Cd4869116.907219(4)2.49(4) h1/2+
117mCd136.4(2) keV3.36(5) h(11/2)-
118Cd4870117.906915(22)50.3(2) min0+
119Cd4871118.90992(9)2.69(2) min(3/2+)
119mCd146.54(11) keV2.20(2) min(11/2-)#
120Cd4872119.90985(2)50.80(21) s0+
121Cd4873120.91298(9)13.5(3) s(3/2+)
121mCd214.86(15) keV8.3(8) s(11/2-)
122Cd4874121.91333(5)5.24(3) s0+
123Cd4875122.91700(4)2.10(2) s(3/2)+
123mCd316.52(23) keV1.82(3) s(11/2-)
124Cd4876123.91765(7)1.25(2) s0+
125Cd4877124.92125(7)0.65(2) s(3/2+)#
125mCd50(70) keV570(90) ms11/2-#
126Cd4878125.92235(6)0.515(17) s0+
127Cd4879126.92644(8)0.37(7) s(3/2+)
128Cd4880127.92776(32)0.28(4) s0+
129Cd4881128.93215(32)#242(8) ms3/2+#
129mCd0(200)# keV104(6) ms11/2-#
130Cd4882129.9339(3)162(7) ms0+
131Cd4883130.94067(32)#68(3) ms7/2-#
132Cd4884131.94555(54)#97(10) ms0+

Notes

  • The precision of the isotope abundances and atomic mass is limited through variations. The given ranges should be applicable to any normal terrestrial material.
  • Geologically exceptional samples are known in which the isotopic composition lies outside the reported range. The uncertainty in the atomic mass may exceed the stated value for such specimens.
  • Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
  • Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC which use expanded uncertainties.

References

Isotopes of silverIsotopes of cadmiumIsotopes of indium
Index to isotope pages
Cadmium (IPA: /ˈkædmiəm/) is a chemical element in the periodic table that has the symbol Cd and atomic number 48.
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Isotopes are any of the several different forms of an element each having different atomic mass (mass number). Isotopes of an element have nuclei with the same number of protons (the same atomic number) but different numbers of neutrons.
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Radioactive decay is the process in which an unstable atomic nucleus loses energy by emitting radiation in the form of particles or electromagnetic waves. This decay, or loss of energy, results in an atom of one type, called the parent nuclide
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Radioactive decay is the process in which an unstable atomic nucleus loses energy by emitting radiation in the form of particles or electromagnetic waves. This decay, or loss of energy, results in an atom of one type, called the parent nuclide
..... Click the link for more information.
For , see .
The half-life of a quantity, subject to exponential decay, is the time required for the quantity to decay to half of its initial value.
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beta decay is a type of radioactive decay in which a beta particle (an electron or a positron) is emitted. In the case of electron emission, it is referred to as "beta minus" (β), while in the case of a positron emission as "beta plus" (β+).
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For , see .
The half-life of a quantity, subject to exponential decay, is the time required for the quantity to decay to half of its initial value.
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Emission processes: Neutron emission Positron emission Proton emission
Capturing: Electron capture Neutron capture
Stellar nucleosynthesis pp-Chain CNO cycle α process Triple-α Carbon burning Ne burning O burning Si burning R-process S-process P-process
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For , see .
The half-life of a quantity, subject to exponential decay, is the time required for the quantity to decay to half of its initial value.
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Double electron capture is a decay mode of atomic nucleus. For a nuclide (A, Z) with number of nucleons A and atomic number Z, double electron capture is only possible if the mass of the nuclide of (A, Z-2) is lower.
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Emission processes: Neutron emission Positron emission Proton emission
Capturing: Electron capture Neutron capture
Stellar nucleosynthesis pp-Chain CNO cycle α process Triple-α Carbon burning Ne burning O burning Si burning R-process S-process P-process
..... Click the link for more information.
For , see .
The half-life of a quantity, subject to exponential decay, is the time required for the quantity to decay to half of its initial value.
..... Click the link for more information.
Radioactive decay is the process in which an unstable atomic nucleus loses energy by emitting radiation in the form of particles or electromagnetic waves. This decay, or loss of energy, results in an atom of one type, called the parent nuclide
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A nuclear isomer is a metastable state of an atomic nucleus caused by the excitation of one or more of its nucleons. A nuclear isomer occupies a higher energy state than the corresponding non-excited nucleus, called the ground state.
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atomic mass (ma) is the mass of an atom at rest, most often expressed in unified atomic mass units.[1] The atomic mass may be considered to be the total mass of protons, neutrons and electrons in a single atom (when the atom is motionless).
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The unified atomic mass unit (u), or dalton (Da), is a small unit of mass used to express atomic and molecular masses. It is defined to be one twelfth of the mass of an unbound atom of the carbon-12 nuclide, at rest and in its ground state.
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Radioactive decay is the process in which an unstable atomic nucleus loses energy by emitting radiation in the form of particles or electromagnetic waves. This decay, or loss of energy, results in an atom of one type, called the parent nuclide
..... Click the link for more information.
Electron capture (sometimes called Inverse Beta Decay) is a decay mode for isotopes that will occur when there are too many protons in the nucleus of an atom and insufficient energy to emit a positron; however, it continues to be an inviable decay mode for radioactive
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beta decay is a type of radioactive decay in which a beta particle (an electron or a positron) is emitted. In the case of electron emission, it is referred to as "beta minus" (β), while in the case of a positron emission as "beta plus" (β+).
..... Click the link for more information.
Electron capture (sometimes called Inverse Beta Decay) is a decay mode for isotopes that will occur when there are too many protons in the nucleus of an atom and insufficient energy to emit a positron; however, it continues to be an inviable decay mode for radioactive
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In nuclear physics, a decay product, also known as a daughter product, daughter isotope or daughter nuclide, is a nuclide resulting from the radioactive decay of a parent isotope or precursor nuclide.
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Silver (IPA: /ˈsɪlvə(ɹ)/) is a chemical element with the symbol Ag (Latin: argentum) and atomic number 47.
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Indium (IPA: /ˈɪndiəm/) is a chemical element with chemical symbol In and atomic number 49. This rare, soft, malleable and easily fusible poor metal is chemically similar to aluminium or gallium but more
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The unified atomic mass unit (u), or dalton (Da), is a small unit of mass used to express atomic and molecular masses. It is defined to be one twelfth of the mass of an unbound atom of the carbon-12 nuclide, at rest and in its ground state.
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Proton

The quark structure of the proton.
Composition: 2 up, 1 down
Family: Fermion
Group: Quark
Interaction: Gravity, Electromagnetic, Weak, Strong
Antiparticle: Antiproton
Discovered: Ernest Rutherford (1919)
Symbol: p+
Mass: 1.
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Neutron

The quark structure of the neutron.
Composition: one up, two down
Family: Fermion
Group: Quark
Interaction: Gravity, Electromagnetic, Weak, Strong
Antiparticle: Antineutron
Discovered: James Chadwick[1]
Symbol: n
Mass: 1.
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FPs / 106 thermal 235U
Nuclide Halflife Yield
155Eu 4.76 < 330
85Kr 10.76 2717
113mCd 14.1 <    3
90Sr 28.9 57518
137Cs 30.23 60899
121mSn 43.
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Naturally occurring Silver (Ag) is composed of the two stable isotopes 107Ag and 109Ag with 107Ag being the more abundant (51.839% natural abundance). Standard atomic mass: 107.8682(2) u.
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Indium (In)
Standard atomic mass: 114.818(3) u

Table


nuclide
symbol Z(p) N(n)  
isotopic mass (u)
  half-life nuclear
spin representative
isotopic
composition
(mole fraction) range of natural
variation
(mole fraction)
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Index to the isotopes of <element> pages
1
H 2
He
3
Li 4
Be 5
B 6
C 7
N 8
O 9
F 10
Ne
11
Na 12
Mg 13
Al 14
Si 15
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