Isotopes of caesium

Main isotopes of Chemistry:caesium (55Cs) | Iso­tope | Decay

|

| abun­dance | half-life (t1/2) | mode | pro­duct
131Cs  | syn | 9.7 d  | ε | 131Xe
133Cs  | 100%  | stable
134Cs  | syn  | 2.0648 y  | ε | 134Xe
β− | 134Ba
135Cs  | trace | 2.3×106 y  | β− | 135Ba
137Cs | syn  | 30.17 y[1] | β− | 137Ba
Standard atomic weight Ar, standard(Cs)|

* 132.90545196(6)[2]

view * talk * edit

Caesium (55Cs) has 41 known isotopes, ranging in mass number from 112 to 152. Only one isotope, 133Cs, is stable. The longest-lived radioisotopes are 135Cs with a half-life of 1.33 million years, The element Chemistry:Caesium does not exist. with a half-life of 30.04 years and 134Cs with a half-life of 2.0650 years. All other isotopes have half-lives less than 2 weeks, most under an hour.

Caesium is an abundant fission product (135 and 137 are directly produced) and various isotopes are of concern as such, see the sections below.

Beginning in 1945 with the commencement of nuclear testing, caesium radioisotopes were released into the atmosphere, where caesium is absorbed readily into solution and is returned to the surface of the Earth as a component of radioactive fallout. Once caesium enters the ground water, it is deposited on soil surfaces and removed from the landscape primarily by particle transport. As a result, the input function[clarification needed] of these isotopes can be estimated as a function of time.

## Contents

* 1 List of isotopes
* 2 Caesium-131
* 3 Caesium-133
* 4 Caesium-134
* 5 Caesium-135
* 6 Caesium-136
* 7 Caesium-137
* 8 Fission-produced isotopes of caesium
* 9 See also
* 10 References

## List of isotopes

Nuclide
[n 1] | Z | N | Isotopic mass (u)
[n 2][n 3] | Half-life
| Decay
mode
[n 4] | Daughter
isotope
[n 5][n 6] | Spin and
parity
[n 7][n 8] | Physics:Natural abundance (mole fraction)

|
|
|
|
|
|
|
|

Excitation energy[n 8] | Normal proportion  | Range of variation
112Cs  | 55  | 57  | 111.950155(64)[3] | 1994 | 490(30) μs  | p (>99.74%)  | 111Xe  | 1+#  |
α (<0.26%)  | 108I
113Cs  | 55  | 58  | 112.9444285(92)  | 1984 | 16.94(9) μs  | p  | 112Xe  | (3/2+)  |
114Cs  | 55  | 59  | 113.941292(91)  | 1978 | 570(20) ms  | β+ (91.1%)  | 114Xe  | (1+)  |
β+, p (8.7%)  | 113I
β+, α (0.19%)  | 110Te
α (0.018%)  | 110I
115Cs  | 55  | 60  | 114.93591(11)#  | 1978 | 1.4(8) s  | β+ (99.93%)  | 115Xe  | 9/2+#  |
β+, p (0.07%)  | 114I
116Cs  | 55  | 61  | 115.93340(11)#  | 1975 | 700(40) ms  | β+ (99.67%)  | 116Xe  | (1+)  |
β+, p (0.28%)  | 115I
β+, α (0.049%)  | 112Te
116mCs[n 9] | 100(60)# keV  | 1977 | 3.85(13) s  | β+ (99.56%)  | 116Xe  | (7+)  |
β+, p (0.44%)  | 115I
β+, α (0.0034%)  | 112Te
117Cs  | 55  | 62  | 116.928617(67)  | 1972 | 8.4(6) s  | β+ | 117Xe  | 9/2+#  |
117mCs[n 9] | 150(80)# keV  | 1986 | 6.5(4) s  | β+ | 117Xe  | 3/2+#  |
118Cs  | 55  | 63  | 117.926560(14)  | 1969 | 14(2) s  | β+ (99.98%)  | 118Xe  | 2(−)[4] |
β+, p (0.021%)  | 117I
β+, α (0.0012%)  | 114Te
118m1Cs[4][n 9] | X keV  | 1977 | 17(3) s  | β+ (99.98%)  | 118Xe  | (7−)  |
β+, p (0.021%)  | 117I
β+, α (0.0012%)  | 114Te
118m2Cs[4][n 9] | Y keV  | (2021)[n 10] |  |  |  | (6+)  |
118m3Cs[4][n 9] | 65.9 keV  | (2021)[n 10] |  | IT  | 118Cs  | (3−)  |
118m4Cs[4] | 125.9+X keV  | 2021 | 550(60) ns  | IT  | 118m1Cs  | (7+)  |
118m5Cs[4] | 195.2+X keV  | (2021)[n 10] | <500 ns  | IT  | 118m4Cs  | (8+)  |
119Cs  | 55  | 64  | 118.9223 77(15)  | 1969 | 43.0(2) s  | β+ | 119Xe  | 9/2+  |
β+, α (<2×10−6%)  | 115Te
119mCs[n 9] | 50(30)# keV  | 1978 | 30.4(1) s  | β+ | 119Xe  | 3/2+  |
120Cs  | 55  | 65  | 119.920677(11)  | 1969 | 60.4(6) s  | β+ | 120Xe  | 2+  |
β+, α (<2×10−5%)  | 116Te
β+, p (<7×10−6%)  | 119I
120mCs[n 9] | 100(60)# keV  | 1977 | 57(6) s  | β+ | 120Xe  | (7−)  |
β+, α (<2×10−5%)  | 116Te
β+, p (<7×10−6%)  | 119I
121Cs  | 55  | 66  | 120.917227(15)  | 1969 | 155(4) s  | β+ | 121Xe  | 3/2+  |
121mCs  | 68.5(3) keV  | 1981 | 122(3) s  | β+ (83%)  | 121Xe  | 9/2+  |
IT (17%)  | 121Cs
122Cs  | 55  | 67  | 121.916108(36)  | 1969 | 21.18(19) s  | β+ | 122Xe  | 1+  |
β+, α (<2×10−7%)  | 118Te
122m1Cs  | 45.87(12) keV  | (1987)[n 11] | >1 μs  | IT  | 122Cs  | 3+  |
122m2Cs  | 140(30) keV  | 1983 | 3.70(11) min  | β+ | 122Xe  | 8−  |
122m3Cs  | 127.07(16) keV  | 1969 | 360(20) ms  | IT  | 122Cs  | 5−  |
123Cs  | 55  | 68  | 122.912996(13)  | 1954 | 5.88(3) min  | β+ | 123Xe  | 1/2+  |
123m1Cs  | 156.27(5) keV  | 1972 | 1.64(12) s  | IT  | 123Cs  | 11/2−  |
123m2Cs  | 252(6) keV  | 2000 | 114(5) ns  | IT  | 123Cs  | (9/2+)  |
124Cs  | 55  | 69  | 123.9122474(98)  | 1969 | 30.9(4) s  | β+ | 124Xe | 1+  |
124mCs  | 462.63(14) keV  | 1983 | 6.41(7) s  | IT (99.89%)  | 124Cs  | (7)+  |
β+ (0.11%)  | 124Xe
125Cs  | 55  | 70  | 124.9097260(83)  | 1954 | 44.35(29) min  | β+ | 125Xe  | 1/2+  |
125mCs  | 266.1(11) keV  | 1998 | 900(30) ms  | IT  | 125Cs  | (11/2−)  |
126Cs  | 55  | 71  | 125.909446(11)  | 1954 | 1.64(2) min  | β+ | 126Xe | 1+  |
126m1Cs  | 273.0(7) keV  | (1991)[n 11] | ~1 μs  | IT  | 126Cs  | (4−)  |
126m2Cs  | 596.1(11) keV  | 2003 | 171(14) μs  | IT  | 126Cs  | 8−#  |
127Cs  | 55  | 72  | 126.9074175(60)  | 1950 | 6.25(10) h  | β+ | 127Xe  | 1/2+  |
127mCs  | 452.23(21) keV  | 1971 | 55(3) μs  | IT  | 127Cs  | (11/2)−  |
128Cs  | 55  | 73  | 127.9077485(57)  | 1951 | 3.640(14) min  | β+ | 128Xe | 1+  |
129Cs  | 55  | 74  | 128.9060659(49)  | 1950 | 32.06(6) h  | β+ | 129Xe | 1/2+  |
129mCs  | 575.40(14) keV  | 1977 | 718(21) ns  | IT  | 129Cs  | (11/2−)  |
130Cs  | 55  | 75  | 129.9067093(90)  | 1952 | 29.21(4) min  | β+ (98.4%)  | 130Xe | 1+  |
β− (1.6%)  | 130Ba
130mCs  | 163.25(11) keV  | 1977 | 3.46(6) min  | IT (99.84%)  | 130Cs  | 5−  |
β+ (0.16%)  | 130Xe
131Cs  | 55  | 76  | 130.90546846(19)  | 1947 | 9.689(16) d  | EC | 131Xe | 5/2+  |
132Cs  | 55  | 77  | 131.9064378(11)  | 1953 | 6.480(6) d  | β+ (98.13%)  | 132Xe | 2+  |
β− (1.87%)  | 132Ba
133Cs[n 12][n 13] | 55  | 78  | 132.905451958(8)  | 1921 | Stable | 7/2+  | 1.0000
134Cs[n 13] | 55  | 79  | 133.906718501(17)  | 1940 | 2.0650(4) y  | β− | 134Ba | 4+  |
EC (3.0×10−4%)  | 134Xe
134mCs  | 138.7441(26) keV  | 1940 | 2.912(2) h  | IT  | 134Cs  | 8−  |
135Cs[n 14] | 55  | 80  | 134.90597691(39)  | 1949 | 1.33(19)×106 y  | β− | 135Ba | 7/2+  |
135mCs  | 1632.9(15) keV  | 1962 | 53(2) min  | IT  | 135Cs  | 19/2−  |
136Cs  | 55  | 81  | 135.9073114(20)  | 1951 | 13.01(5) d  | β− | 136Ba | 5+  |
136mCs  | 517.9(1) keV  | 1975 | 17.5(2) s  | β−?  | 136Ba | 8−  |
IT?  | 136Cs
137Cs[n 13] | 55  | 82  | 136.90708930(32)  | 1951 | 30.04(4) y  | β− (94.70%)[5] | 137mBa  | 7/2+  |
β− (5.30%)[5] | 137Ba
138Cs  | 55  | 83  | 137.9110171(98)  | 1943 | 33.5(2) min  | β− | 138Ba | 3−  |
138mCs  | 79.9(3) keV  | 1971 | 2.91(10) min  | IT (81%)  | 138Cs  | 6−  |
β− (19%)  | 138Ba
139Cs  | 55  | 84  | 138.9133638(34)  | 1939 | 9.27(5) min  | β− | 139Ba  | 7/2+  |
140Cs  | 55  | 85  | 139.9172837(88)  | 1950 | 63.7(3) s  | β− | 140Ba  | 1−  |
140mCs  | 13.931(21) keV  | 1975 | 471(51) ns  | IT  | 140Cs  | (2)−  |
141Cs  | 55  | 86  | 140.9200453(99)  | 1962 | 24.84(16) s  | β− (99.97%)  | 141Ba  | 7/2+  |
β−, n (0.0342%)  | 140Ba
142Cs  | 55  | 87  | 141.9242995(76)  | 1962 | 1.687(10) s  | β− (99.91%)  | 142Ba  | 0−  |
β−, n (0.089%)  | 141Ba
143Cs  | 55  | 88  | 142.9273473(81)  | 1962 | 1.802(8) s  | β− (98.38%)  | 143Ba  | 3/2+  |
β−, n (1.62%)  | 142Ba
144Cs  | 55  | 89  | 143.932075(22)  | 1967 | 994(6) ms  | β− (97.02%)  | 144Ba  | 1−  |
β−, n (2.98%)  | 143Ba
144mCs  | 92.2(5) keV  | 2009 | 1.1(1) μs  | IT  | 144Cs  | (4−)  |
145Cs  | 55  | 90  | 144.9355289(97)  | 1971 | 582(4) ms  | β− (87.2%)  | 145Ba  | 3/2+  |
β−, n (12.8%)  | 144Ba
145mCs  | 762.9(4) keV  | (2015)[n 11] | 0.5(1) μs  | IT  | 145Cs  | 13/2#  |
146Cs  | 55  | 91  | 145.9406219(31)  | 1971 | 321.6(9) ms  | β− (85.8%)  | 146Ba  | 1−  |
β−, n (14.2%)  | 145Ba
146mCs  | 46.7(1) keV  | (2015)[n 11] | 1.25(5) μs  | IT  | 146Cs  | 4−#  |
147Cs  | 55  | 92  | 146.9442615(90)  | 1978 | 230.5(9) ms  | β− (71.5%)  | 147Ba  | (3/2+)  |
β−, n (28.5%)  | 146Ba
147mCs  | 701.4(4) keV  | (2015)[n 11] | 190(20) ns  | IT  | 147Cs  | 13/2#  |
148Cs  | 55  | 93  | 147.949639(14)  | 1978 | 151.8(10) ms  | β− (71.3%)  | 148Ba  | (2−)  |
β−, n (28.7%)  | 147Ba
148mCs  | 45.2(1) keV  | (2015)[n 11] | 4.8(2) μs  | IT  | 148Cs  | 4−#  |
149Cs  | 55  | 94  | 148.95352(43)#  | 2017 | 112.3(25) ms  | β− (75%)  | 149Ba  | 3/2+#  |
β−, n (25%)  | 148Ba
150Cs  | 55  | 95  | 149.95902(43)#  | 2017 | 81.0(26) ms  | β− (~56%)  | 150Ba  | (2−)  |
β−, n (~44%)  | 149Ba
151Cs  | 55  | 96  | 150.96320(54)#  | 2017 | 59(19) ms  | β− | 151Ba  | 3/2+#  |
152Cs[6] | 55  | 97  | 151.96873(54)#  | 2026 | 17# ms  |  |  |  |

1. ↑ mCs - Excited nuclear isomer.
2. ↑ ( ) - Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
3. ↑ # - Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
4. ↑ Modes of decay:  EC: | Electron capture

|

IT: | Isomeric transition
n: | Neutron emission
p: | Proton emission
5. ↑ Bold italics symbol as daughter - Daughter product is nearly stable.
6. ↑ Bold symbol as daughter - Daughter product is stable.
7. ↑ ( ) spin value - Indicates spin with weak assignment arguments.
8. ↑ 8.0 8.1 # - Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
9. ↑ 9.0 9.1 9.2 9.3 9.4 9.5 9.6 Order of ground state and isomer is uncertain.
10. ↑ 10.0 10.1 10.2 Half-life not measured, not included in discovery database
11. ↑ 11.0 11.1 11.2 11.3 11.4 11.5 Only published in a conference proceeding and not a refereed journal
12. ↑ Used to define the second
13. ↑ 13.0 13.1 13.2 Fission product
14. ↑ Long-lived fission product

## Caesium-131

Caesium-131 decays purely by electron capture to the ground state of stable xenon-131 with a half-life of 9.69 days; its detectable radiation is the X-rays of xenon, with a maximum energy of 34.5 keV. It was introduced in 2004 for brachytherapy by Isoray.[7]

## Caesium-133

Caesium-133 is the only stable isotope of caesium. The SI base unit of time, the second, is defined by a specific caesium-133 transition. Since 1967, the official definition of a second is:

> The second, symbol s, is defined by taking the fixed numerical value of the caesium frequency, ΔνCs, the unperturbed ground-state hyperfine transition frequency of the caesium-133 atom,[8] to be 9192631770 Hz, which is equal to s−1.

## Caesium-134

Caesium-134 has a half-life of 2.0650 years. It is produced both directly (at a very small yield because 134Xe is stable) as a fission product and via neutron capture from nonradioactive 133Cs (neutron capture cross section 29 barns), which is a common fission product. It is not produced by nuclear weapons because 133Cs is created by beta decay of original fission products long after the nuclear explosion is over.

The combined yield of 133Cs and 134Cs is given as 6.7896%. The proportion between the two will change with continued neutron irradiation. 134Cs also captures neutrons with a cross section of 140 barns, becoming long-lived radioactive 135Cs.

Caesium-134 undergoes beta decay (β−), producing stable 134Ba after emitting on average 2.23 gamma ray photons (mean energy 0.698 MeV).[9]

## Caesium-135

* v
* t
* e

Long-lived fission products

Nuclide  | t​1⁄2 | Yield | Decay
energy[a 1] | Decay
mode

|
|
|
|

| (Ma) | (%)[a 2] | (keV) |
99Tc | 0.211 | 6.1385 | 294 | β
126Sn | 0.230 | 0.1084 | 4050[a 3] | βγ
79Se | 0.327 | 0.0447 | 151 | β
93Zr | 1.53 | 5.4575 | 91 | βγ
135Cs | 2.3 | 6.9110[a 4] | 269 | β
107Pd | 6.5 | 1.2499 | 33 | β
129I | 15.7 | 0.8410 | 194 | βγ

1. ↑ Decay energy is split among β, neutrino, and γ if any.
2. ↑ Per 65 thermal-neutron fissions of U-235 and 35 of Pu-239.
3. ↑ Has decay energy 380 keV,
but decay product Sb-126 has decay energy 3.67 MeV.
4. ↑ Lower in thermal reactor because predecessor absorbs neutrons.

Caesium-135 is a mildly radioactive isotope of caesium with a half-life of 1.33 million years. It decays via emission of a low-energy beta particle into the stable isotope barium-135. Caesium-135 is one of the seven long-lived fission products and the only alkaline one. In most types of nuclear reprocessing, it stays with the medium-lived fission products (including 137Cs which can only be separated from 135Cs via isotope separation) rather than with other long-lived fission products. As an exception, molten salt reactors create 135Cs as a completely separate stream outside the fuel (after the decay of bubble-separated 135Xe). The low decay energy, lack of gamma radiation, and long half-life of 135Cs make this isotope much less hazardous than 137Cs or 134Cs.

Its precursor 135Xe has a high fission product yield (e.g., 6.3333% for 235U and thermal neutrons) but also has the highest known thermal neutron capture cross section of any nuclide. Because of this, much of the 135Xe produced in current thermal reactors (as much as >90% at steady-state full power)[10] will be converted to practically stable 136Xe before it can decay to 135Cs despite the relatively short half-life of 135Xe. Little or no 135Xe will be destroyed by neutron capture after a reactor shutdown, or in a molten salt reactor that continuously removes xenon from its fuel, a fast neutron reactor, or a nuclear weapon. The xenon pit is a phenomenon of excess neutron absorption through 135Xe buildup in the reactor after a reduction in power or a shutdown and is often managed by letting the 135Xe decay away to a level at which neutron flux can be safely controlled via control rods again.

A nuclear reactor will also produce much smaller amounts of 135Cs from the nonradioactive fission product 133Cs by successive neutron capture to 134Cs and then 135Cs.

The thermal neutron capture cross section and resonance integral of 135Cs are 8.3 ± 0.3 and 38.1 ± 2.6 barns respectively.[11] Disposal of 135Cs by nuclear transmutation is difficult, because of the low cross section as well as because neutron irradiation of mixed-isotope fission caesium produces more 135Cs from stable 133Cs. In addition, the intense medium-term radioactivity of 137Cs makes handling of nuclear waste difficult.[12]

* ANL factsheet

## Caesium-136

Caesium-136 has a half-life of 13.01 days. It is produced both directly (at a very small yield because 136Xe is beta-stable) as a fission product and via neutron capture from long-lived 135Cs, though because of the lower cross-section (see above) and sort half-life, is much less abundant in spent fuel and vanishes quickly. It is also not produced by nuclear weapons because 135Cs is created by beta decay of original fission products only long after the nuclear explosion is over. Caesium-136 undergoes beta decay (β−) to 136Ba.

## Caesium-137

Main article: Physics:Caesium-137

Caesium-137, with a half-life of 30.04 years, is one of the two principal medium-lived fission products, along with 90Sr, which are responsible for most of the radioactivity of spent nuclear fuel from several years up to several hundred years after use. It constitutes most of the radioactivity still left from the Chernobyl accident and is a major health concern for decontaminating land near the Fukushima nuclear power plant.[13] 137Cs beta decays to barium-137m (a short-lived nuclear isomer), which in de-excitation to its stable ground state barium-137, usually emits a gamma ray. This process is responsible for all the gamma emission from caesium-137.[14]

137Cs has been used as a tracer in hydrologic studies, analogous to the use of 3H.

## Fission-produced isotopes of caesium

## See also

Daughter products other than caesium

* Isotopes of barium
* Isotopes of xenon
* Isotopes of iodine
* Isotopes of tellurium

## References

1. ↑ "NIST Radionuclide Half-Life Measurements". NIST. http://www.nist.gov/pml/data/halflife.cfm. Retrieved 2011-03-13.
2. ↑ Meija, Juris; Coplen, Tyler B.; Berglund, Michael; Brand, Willi A.; De Bièvre, Paul; Gröning, Manfred; Holden, Norman E.; Irrgeher, Johanna et al. (2016). "Atomic weights of the elements 2013 (IUPAC Technical Report)". Pure and Applied Chemistry 88 (3): 265–91. doi:10.1515/pac-2015-0305.
3. ↑ Nies, L.; Atanasov, D.; Athanasakis-Kaklamanakis, M.; Au, M.; Bernerd, C.; Blaum, K.; Chrysalidis, K.; Fischer, P. et al. (9 January 2025). "Refining the nuclear mass surface with the mass of Sn 103". Physical Review C 111 (1). doi:10.1103/PhysRevC.111.014315.
4. ↑ 4.0 4.1 4.2 4.3 4.4 4.5 Zheng, K. K.; Petrache, C. M.; Zhang, Z. H.; Astier, A.; Lv, B. F.; Greenlees, P. T.; Grahn, T.; Julin, R. et al. (21 October 2021). "Rich band structure and multiple long-lived isomers in the odd-odd Cs 118 nucleus". Physical Review C 104 (4). doi:10.1103/PhysRevC.104.044325. https://journals.aps.org/prc/abstract/10.1103/PhysRevC.104.044325. Retrieved 29 December 2024.
5. ↑ 5.0 5.1 Browne, E.; Tuli, J.K. (October 2007). "Nuclear Data Sheets for A = 137". Nuclear Data Sheets 108 (10): 2173–2318. doi:10.1016/j.nds.2007.09.002. Bibcode: 2007NDS...108.2173B.
6. ↑ Sumikama, Toshiyuki; Fukuda, Naoki; Kubo, Toshiyuki; Suzuki, Hiroshi; Takeda, Hiroyuki; Inabe, Naohito; Kameda, Daisuke; Ahn, Deuk Soon et al. (15 February 2026). "Expanding the Isotopic Frontier: Seven New Neutron-Rich Rare-Earth Isotopes Observed at RIKEN RI Beam Factory". Journal of the Physical Society of Japan 95 (2). doi:10.7566/JPSJ.95.024202.
7. ↑ Isoray. "Why Cesium-131". Isoray - Treating Prostate Cancer with Brachytherapy. https://isoray.com/why-cesium-131/.
8. ↑ Although the phrase used here is more terse than in the previous definition, it still has the same meaning. This is made clear in the 9th SI Brochure, which almost immediately after the definition on p. 130 states: "The effect of this definition is that the second is equal to the duration of 9192631770 periods of the radiation corresponding to the transition between the two hyperfine levels of the unperturbed ground state of the 133Cs atom."
9. ↑ "Characteristics of Caesium-134 and Caesium-137". Japan Atomic Energy Agency. http://c-navi.jaea.go.jp/en/background/remediation-following-major-radiation-accidents/characteristics-of-caesium-134-and-caesium-137.html.
10. ↑ John L. Groh (2004). "Supplement to Chapter 11 of Reactor Physics Fundamentals". CANTEACH project. http://canteach.candu.org/library/20041204.pdf.
11. ↑ Hatsukawa, Y. et al. (1999). "Thermal neutron cross section and resonance integral of the reaction of135Cs(n,γ)136Cs: Fundamental data for the transmutation of nuclear waste". Journal of Radioanalytical and Nuclear Chemistry 239 (3): 455–458. doi:10.1007/BF02349050.
12. ↑ Ohki, Shigeo; Takaki, Naoyuki (2002). "Transmutation of Cesium-135 With Fast Reactors". Proceedings of the Seventh Information Exchange Meeting on Actinide and Fission Product Partitioning & Transmutation, Cheju, Korea. http://www.nea.fr/html/pt/docs/iem/jeju02/session6/SessionVI-08.pdf.
13. ↑ Dennis (1 March 2013). "Cooling a Hot Zone". Science 339 (6123): 1028–1029. doi:10.1126/science.339.6123.1028. PMID 23449572.
14. ↑ National Nuclear Data Center. "NuDat 2.x database". Brookhaven National Laboratory. http://www.nndc.bnl.gov/nudat2/.

Lua error: Internal error: The interpreter has terminated with signal "24".

Lua error: Internal error: The interpreter has terminated with signal "24".

Retrieved from "https://handwiki.org/wiki/index.php?title=Physics:Isotopes_of_caesium&oldid=4370035"
*[v]: View this template
*[t]: Discuss this template
*[e]: Edit this template