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Isotopes of berkelium

(Redirected fromBerkelium-250)

Berkelium (97Bk) is anartificial element, and thus astandard atomic weight cannot be given. Like all artificial elements, it has nostable isotopes. The firstisotope to be synthesized was243Bk in 1949. There are twenty knownradioisotopes, from233Bk and233Bk to253Bk (except235Bk and237Bk), and sixnuclear isomers. The longest-lived isotope is247Bk with ahalf-life of 1,380 years.

Isotopes ofberkelium (97Bk)
Main isotopes[1]Decay
abun­dancehalf-life(t1/2)modepro­duct
245Bksynth4.94 dε245Cm
α241Am
246Bksynth1.8 dα242Am
β+246Cm
247Bksynth1380 yα243Am
248Bksynth>9 y[2]α244Am
249Bksynth330 dβ249Cf
α245Am
SF

List of isotopes

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Nuclide
[n 1]
ZNIsotopic mass(Da)[3]
[n 2][n 3]
Half-life[1]
Decay
mode
[1]
[n 4]
Daughter
isotope

Spin and
parity[1]
[n 5][n 6]
Excitation energy[n 6]
233Bk97136233.05665(25)#40(30) sα229Am3/2-#
β+?233Cm
234Bk97137234.05732(16)#20(5) sα (>80%)230Am3-#
β+ (<20%)234Cm
β+,SF?[4](various)
236Bk97139236.05748(39)#26(10) sβ+ (99.96%)236Cm4+#
β+, SF (0.04%)(various)
α?232Am
238Bk97141238.05820(28)#2.40(8) minβ+ (99.95%)238Cm1#
β+, SF (0.048%)(various)
α?234Am
239Bk97142239.05824(22)#100# sβ+239Cm(7/2+)
α?235Am
SF?(various)
240Bk97143240.05976(16)#4.8(8) minβ+?240Cm7−#
β+, SF (0.0020%)(various)
α?236Am
241Bk97144241.06010(18)#4.6(4) minβ+?241Cm(7/2+)
α?237Am
242Bk97145242.06198(22)#7.0(13) minβ+242Cm3+#
β+, SF (<3×10−5%)(various)
α?238Am
242mBk2000(200)# keV600(100) nsSF(various)
IT?242Bk
243Bk97146243.0630059(49)4.6(2) hβ+ (99.85%)243Cm3/2−
α (.15%)239Am
244Bk97147244.065179(15)5.02(3) hβ+?244Cm4−
α (0.006%)240Am
244mBk1500(500)# keV820(60) nsSF(various)
IT?244Bk
245Bk97148245.0663598(19)4.95(3) dEC (99.88%)245Cm3/2−
α (.12%)241Am
246Bk97149246.068671(64)1.80(2) dβ+246Cm2(−)
α?242Am
247Bk97150247.0703059(56)1.38(25)×103 yα243Am3/2−
SF?(various)
248Bk97151248.073142(54)>9 yα?244Am6+#
EC?248Cm
248mBk[n 7]−20(50) keV23.7(2) hβ (70%)248Cf1(−)
EC (30%)248Cm
α?244Am
249Bk97152249.0749831(13)327.2(3) dβ249Cf7/2+
α (.00145%)245Am
SF (4.7×10−8%)(various)
249mBk8.777(14) keV300 μsIT249Bk3/2−
250Bk97153250.0783172(31)3.212(5) hβ250Cf2−
250m1Bk35.59(10) keV29(1) μsIT250Bk4+
250m2Bk85.6(16) keV213(8) μsIT250Bk7+
251Bk97154251.080761(12)55.6(11) minβ251Cf(3/2−)
251mBk35.5(13) keV58(4) μsIT251Bk(7/2+)
252Bk97155252.08431(22)#1.8(5) minβ?252Cf
α?248Am
253Bk97156253.08688(39)#60# minβ?253Cf3/2-#
This table header & footer:
  1. ^mBk – Excitednuclear 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


    SF:Spontaneous fission
  5. ^( ) spin value – Indicates spin with weak assignment arguments.
  6. ^ab# – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  7. ^Order of ground state and isomer is uncertain.

Actinides vs fission products

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Actinides and fission products by half-life
Actinides[5] bydecay chainHalf-life
range (a)
Fission products of235U byyield[6]
4n4n + 14n + 24n + 34.5–7%0.04–1.25%<0.001%
228Ra4–6 a155Euþ
248Bk[7]> 9 a
244Cmƒ241Puƒ250Cf227Ac10–29 a90Sr85Kr113mCdþ
232Uƒ238Puƒ243Cmƒ29–97 a137Cs151Smþ121mSn
249Cfƒ242mAmƒ141–351 a

No fission products have ahalf-life
in the range of 100 a–210 ka ...

241Amƒ251Cfƒ[8]430–900 a
226Ra247Bk1.3–1.6 ka
240Pu229Th246Cmƒ243Amƒ4.7–7.4 ka
245Cmƒ250Cm8.3–8.5 ka
239Puƒ24.1 ka
230Th231Pa32–76 ka
236Npƒ233Uƒ234U150–250 ka99Tc126Sn
248Cm242Pu327–375 ka79Se
1.33 Ma135Cs
237Npƒ1.61–6.5 Ma93Zr107Pd
236U247Cmƒ15–24 Ma129I
244Pu80 Ma

... nor beyond 15.7 Ma[9]

232Th238U235Uƒ№0.7–14.1 Ga

References

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  1. ^abcdKondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021)."The NUBASE2020 evaluation of nuclear properties"(PDF).Chinese Physics C.45 (3): 030001.doi:10.1088/1674-1137/abddae.
  2. ^Milsted, J.; Friedman, A. M.; Stevens, C. M. (1965). "The alpha half-life of berkelium-247; a new long-lived isomer of berkelium-248".Nuclear Physics.71 (2): 299.doi:10.1016/0029-5582(65)90719-4.
  3. ^Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*".Chinese Physics C.45 (3): 030003.doi:10.1088/1674-1137/abddaf.
  4. ^Kaji, D.; Morimoto, K.; Haba, H.; Ideguchi, E.; Koura, H.; Morita, K. (2016)."Decay Properties of New Isotopes234Bk and230Am, and Even–Even Nuclides234Cm and230Pu"(PDF).Journal of the Physical Society of Japan.84 (15002): 015002.Bibcode:2016JPSJ...85a5002K.doi:10.7566/JPSJ.85.015002.
  5. ^Plus radium (element 88). While actually a sub-actinide, it immediately precedes actinium (89) and follows a three-element gap of instability afterpolonium (84) where no nuclides have half-lives of at least four years (the longest-lived nuclide in the gap isradon-222 with a half life of less than fourdays). Radium's longest lived isotope, at 1,600 years, thus merits the element's inclusion here.
  6. ^Specifically fromthermal neutron fission of uranium-235, e.g. in a typicalnuclear reactor.
  7. ^Milsted, J.; Friedman, A. M.; Stevens, C. M. (1965). "The alpha half-life of berkelium-247; a new long-lived isomer of berkelium-248".Nuclear Physics.71 (2): 299.Bibcode:1965NucPh..71..299M.doi:10.1016/0029-5582(65)90719-4.
    "The isotopic analyses disclosed a species of mass 248 in constant abundance in three samples analysed over a period of about 10 months. This was ascribed to an isomer of Bk248 with a half-life greater than 9 [years]. No growth of Cf248 was detected, and a lower limit for the β half-life can be set at about 104 [years]. No alpha activity attributable to the new isomer has been detected; the alpha half-life is probably greater than 300 [years]."
  8. ^This is the heaviest nuclide with a half-life of at least four years before the "sea of instability".
  9. ^Excluding those "classically stable" nuclides with half-lives significantly in excess of232Th; e.g., while113mCd has a half-life of only fourteen years, that of113Cd is eightquadrillion years.

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