Einsteinium isotopes include all of the atomic nuclei of the chemical element einsteinium; these consist of an atomic nucleus with 99 protons and in the uncharged state of 99 electrons. The difference between the individual einsteinium isotopes lies in the number of neutrons in the nucleus - and thus in the mass number.
Einsteinium
is an artificially created chemical element, of which 17 different isotopes have been created and characterized so far. Einsteinium-253 was the first nuclide to be discovered in the nuclear fallout of a hydrogen bomb test in 1952.
Einsteinium-252 has the longest half-life at 472 days.
Isotope Nuclide | E | N | Atomic Mass [Nuclear Mass] {Mass Excess} | Spin I (h/2π) | Parent |
---|---|---|---|---|---|
1 | 2 | 3 | 4 | 5 | 6 |
Einsteinium-240 | 24099Es | 141 | 240.06892(43) u [240.0146185 u] {64.19857 MeV} | (1+) | |
Einsteinium-241 | 24199Es | 142 | 241.06856(24) u [241.0142585 u] {63.86323 MeV} | (3/2-) | 245Md |
Einsteinium-242 | 24299Es | 143 | 242.06957(27) u [242.0152685 u] {64.80404 MeV} | 246Md | |
Einsteinium-243 | 24399Es | 144 | 243.06951(22) u [243.0152085 u] {64.74815 MeV} | (7/2+) | 247Md |
Einsteinium-244 | 24499Es | 145 | 244.07088(19) u [244.0165785 u] {66.02429 MeV} | 248Md | |
Einsteinium-245 | 24599Es | 146 | 245.07125(21) u [245.0169485 u] {66.36895 MeV} | (3/2-) | 249Md |
Einsteinium-246 | 24699Es | 147 | 246.07289(24) u [246.0185885 u] {67.8966 MeV} | 250Md | |
Einsteinium-247 | 24799Es | 148 | 247.073622(21) u [247.0193205 u] {68.57845 MeV} | (7/2+) | 251Md 247Fm |
Einsteinium-248 | 24899Es | 149 | 248.07547(6) u [248.0211685 u] {70.29985 MeV} | (2-,0+) | |
Einsteinium-249 | 24999Es | 150 | 249.07641(3) u [249.0221085 u] {71.17546 MeV} | 7/2+ | |
Einsteinium-250 | 25099Es | 151 | 250.07861(11) u [250.0243085 u] {73.22474 MeV} | (6+) | 250Fm |
Einsteinium-250m | 250m99Es | 151 | 250.07861(11) u [250.0243085 u] {73.22474 MeV} | 1(-) | |
Einsteinium-251 | 25199Es | 152 | 251.079992(6) u [251.0256905 u] {74.51207 MeV} | 3/2- | 255Md 251Fm |
Einsteinium-252 | 25299Es | 153 | 252.08298(5) u [252.0286785 u] {77.29537 MeV} | (5-) | 256Md |
Einsteinium-253 | 25399Es | 154 | 253.0848213(13) u [253.0305198 u] {79.01053 MeV} | 7/2+ | 257Md 253Fm 253Cf |
Einsteinium-254 | 25499Es | 155 | 254.088021(4) u [254.0337195 u] {81.99103 MeV} | (7+) | 258Md |
Einsteinium-254m | 254m99Es | 155 | 254.088021(4) u [254.0337195 u] {81.99103 MeV} | 2+ | |
Einsteinium-255 | 25599Es | 156 | 255.090274(12) u [255.0359725 u] {84.08969 MeV} | (7/2+) | 255Cf |
Einsteinium-256 | 25699Es | 157 | 256.09360(11) u [256.0392985 u] {87.18784 MeV} | (1+,0-) | |
Einsteinium-256m | 256m99Es | 157 | 256.09360(11) u [256.0392985 u] {87.18784 MeV} | (8+) | |
Einsteinium-257 | 25799Es | 158 | 257.09598(44) u [257.0416785 u] {89.40479 MeV} | (7/2+) |
Isotope | Radioactive Decay | Extern | |||
---|---|---|---|---|---|
Half-life | Decay Mode | Probability | Energy | ||
7 | 8 | 9 | 10 | 11 | 12 |
Es-240 | 6(2) s | α → 236Bk EC/β+ → 240Cf EC, SS div | 70(10) % 30(10) % | 8.23(57) MeV | |
Es-241 | ca. 8 s | α → 237Bk EC/β+ → 241Cf | ? ? | 8.25(2) MeV 4.54(28) MeV | AL |
Es-242 | 13.5(25) s | α → 238Bk EC/β+ → 242Cf | > 0 % > 0 % | 8.16(2) MeV 5.41(26) MeV | AL |
Es-243 | 21(2) s | α → 239Bk EC/β+ → 243Cf SF | 61(6) % 39(6) % < 1 % | 8.072(10) MeV 3.76(24) MeV | AL |
Es-244 | 37(4) s | α → 240Bk EC → 244Cf | ca. 4 % ca. 96 % | 7.94(10) MeV 4.55(18) MeV | AL |
Es-245 | 1.1(1) min | α → 241Bk EC → 245Cf | 40(10) % 60(10) % | 7.9090(3) MeV 2.98(20) MeV | AL |
Es-246 | 7.5(5) min | α → 242Bk EC/β+ → 246Cf | 9.9(18) % 90.1(18) % | 7.74(10) MeV 3.81(22) MeV | AL |
Es-247 | 4.55(26) min | α → 243Bk EC/β+ → 247Cf | 7 % 93 % | AL | |
Es-248 | 24(3) min | α → 244Bk EC → 248Cf | 0.25 % 99.7(3) % | 7.16(5) MeV 3.06(5) MeV | AL |
Es-249 | 102.2(6) min | α → 245Bk EC/β+ → 249Cf | 0.57(8) % 99.43(8) % | 6.94(3) MeV 1.45(3) | AL |
Es-250 | 8.6(1) h | α → 246Bk EC → 250Cf | < 3 % > 97 % | 6.834(117) MeV 2.055(100) MeV | AL |
Es-250m | 2.22(5) h | EC → 250Cf | ≤ 100 % | AL | |
Es-251 | 33(1) h | α → 247Bk EC → 251Cf | 0.5(2) % 99.5(2) % | 6.598(3) MeV 0.377(7) MeV | AL |
Es-252 | 471.7(19) d | α → 248Bk EC → 252Cf | 78(2) % 22(2) % | 6.79(5) MeV 1.26(5) MeV | AL |
Es-253 | 20.47(3) d | α → 249Bk SF div | < 100 % 0.0000087 % | 6.73924(5) MeV | AL |
Es-254 | 275.7(5) d | α → 250Bk EC → 254Cf SF div β- → 254Fm | ca. 100 % ? < 1 % < 1 % | 6.6157(15) MeV 0.649(12) MeV 1.088(3) MeV | AL |
Es-254m | 39.3(2) h | β- → 254Fm Iso → 254Es α → 250Bk EC → 254Cf SF div | < 3 % 0.32(1) % 0.076(7) % < 0.045 % | AL | |
Es-255 | 39.8(12) d | α → 251Bk SF div β- → 255Fm | 8.0(4) % 0.0041(2) % 92 % | 6.4363(13) MeV 0.290(10) MeV | AL |
Es-256 | 25.4(24) min | β- → 256Fm | 100 % | 1.70(10) MeV | AL |
Es-256m | 7.6 h | β- → 256Fm SF, β- → | 99.998 % 0.002 % | AL | |
Es-257 | 7.7(2) d | β- → 257Fm SF div | ? ? | 0.81(41) MeV | AL |
Notes (related to the columns):
1 - name of the nuclide, isotope.
2 - E: isotope symbol with mass number (superscript; number of nucleons) and Atomic number (subscript; number of protons).
3 - N: number of neutrons.
4 - relative atomic mass of the Einsteinium isotope (isotopic mass including electrons) and the mass of the atomic nucleus in square brackets (nuclear mass, nuclide mass without electrons), each related to 12C = 12.00000 [2]. In addition, the mass excess is given in MeV.
5 - nuclear spin I, unit: h/2π.
6 - source nuclides: Possible, assumed or actual source nuclides (mother nuclides, parent nuclides). If applicable, the corresponding decay modes can be found in the data for the respective starting nuclide.
7 - isotope notation in short form.
8 - decay: half-live of the Einsteinium isotope (a = years; ; d = days; h = hours; min = minutes; s = seconds).
9 - decay mode: type of decay into the respective daughter nuclides with n = neutron emission; p = proton emission; α = alpha decay; β- = beta minus decay with electron emission; EC = electron capture; β+ = positron emission; ε = β+ and/or EC; Iso = isomeric transition; CD = cluster decay; SF = spontaneous decay.
10 - decay probability in percent (%).
11 - decay energy; Particle energy related to decay type.
12 - other information and notes: AL = Adopted Levels (link to external data [1]).
Miscellaneous:
()- Numbers in brackets: uncertainty to represent the spread of the reported value.
~ - Theoretical values or systematic trends.
- unlisted-: Nuclides that have already been mentioned in the literature but for some reason can no longer be found in the current nuclide tables because their discovery e.g. has not confirmed.
According to the Radiation Protection Ordinance (StrlSchV 2018, Germany), the following values (columns 1 to 7) apply to the handling of Einsteinium radionuclides:
Nuclide | Limit Value | HASS limit | SC | Daughter Nuclides | Half-life | |
---|---|---|---|---|---|---|
Es-250 | 106 Bq | 100 Bq/g | 8.6 h | |||
Es-251 | 107 Bq | 100 Bq/g | 33.0 h | |||
Es-253 | 105 Bq | 100 Bq/g | 1 Bq cm-2 | 20.5 d | ||
Es-254+ | 104 Bq | 0,1 Bq/g | 1 Bq cm-2 | Bk-250 | 275.7 d | |
Es-254m+ | 106 Bq | 10 Bq/g | 1 Bq cm-2 | Bk-250, Fm-254 | 39.3 h |
(HASS = High-Activity Sealed Radioactive Sources; SC = surface contamination)
Properties of the Einsteinium nucleides
[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.
Einsteinium: NMR properties
[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).
More sources:
[8] - Isotopic abundances, atomic weights and isotopic masses: see respective keyword.
Last update: 2022-12-12
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