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Isotopes of arsenic

Arsenic (33As) has 32 known isotopes and at least 10 isomers. Only one of these isotopes, 75As, is stable; as such, it is considered a monoisotopic element. The longest-lived radioisotope is 73As with a half-life of 80 days.

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List of isotopes

Nuclide1ZNIsotopic mass (Da)234Half-life5Decaymode67Daughterisotope89Spin andparity101112Isotopicabundance
Excitation energy13
64As333163.95756(22)#69.0(14) msβ+64Ge0+#
β+, p?63Ga
65As333264.949611(91)130.3(6) msβ+65Ge3/2−#
β+, p?64Ga
66As333365.9441488(61)95.77(23) msβ+66Ge0+
66m1As1356.63(17) keV1.14(4) μsIT66As5+
66m2As3023.(3) keV7.98(26) μsIT66As9+
67As333466.93925111(48)42.5(12) sβ+67Ge(5/2−)
68As333567.9367741(20)151.6(8) sβ+68Ge3+
68mAs425.1(2) keV111(20) nsIT68As1+
69As333668.932246(34)15.2(2) minβ+69Ge5/2−
70As333769.9309346(15)52.6(3) minβ+70Ge4+
70mAs32.046(23) keV96(3) μsIT70As2+
71As333870.9271136(45)65.30(7) hβ+71Ge5/2−
72As333971.9267523(44)26.0(1) hβ+72Ge2−
73As334072.9238291(41)80.30(6) dEC73Ge3/2−
73mAs427.902(21) keV5.7(2) μsIT73As9/2+
74As334173.9239286(18)17.77(2) dβ+ (66%)74Ge2−
β− (34%)74Se
75As334274.92159456(95)Stable3/2−1.0000
75mAs303.9243(8) keV17.62(23) msIT75As9/2+
76As334375.92239201(95)1.0933(38) dβ−76Se2−
76mAs44.425(1) keV1.84(6) μsIT76As(1)+
77As334476.9206476(18)38.79(5) hβ−77Se3/2−
77mAs475.48(4) keV114.0(25) μsIT77As9/2+
78As334577.921828(10)90.7(2) minβ−78Se2−
79As334678.9209484(57)9.01(15) minβ−79Se3/2−
79mAs772.81(6) keV1.21(1) μsIT79As(9/2)+
80As334779.9224744(36)15.2(2) sβ−80Se1+
81As334880.9221323(28)33.3(8) sβ−81Se3/2−
82As334981.9247387(40)19.1(5) sβ−82Se(2−)
82mAs131.6(5) keV13.6(4) sβ−82Se(5-)
83As335082.9252069(30)13.4(4) sβ−83Se5/2−#
84As335183.9293033(34)3.16(58) sβ− (99.72%)84Se(2−)
β−, n (.28%)83Se
85As335284.9321637(33)2.022(7) sβ−, n (62.6%)84Se(5/2−)
β− (37.4%)85Se
86As335385.9367015(37)945(8) msβ− (64.5%)86Se(1−,2−)
β−, n (35.5%)85Se
β−, 2n?84Se
87As335486.9402917(32)492(25) msβ− (84.6%)87Se(5/2−,3/2−)
β−, n (15.4%)86Se
β−, 2n?85Se
88As335587.94584(22)#270(150) msβ−88Se
β−, n?87Se
89As335688.95005(32)#220# ms [>150 ns]β−?89Se5/2−#
β−, n?88Se
β−, 2n?87Se
90As335789.95600(43)#70# ms [>300 ns]β−?90Se
β−, n?89Se
β−, 2n?88Se
90mAs124.5(5) keV220(100) nsIT90As
91As335890.96082(43)#100# ms [>300 ns]β−?91Se5/2−#
β−, n?90Se
β−, 2n?89Se
92As335991.96739(54)#45# ms [>300 ns]β−?92Se
β−, n?91Se
β−, 2n?90Se
93As143360
94As153361
95As163362
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References

  1. mAs – Excited nuclear isomer. /wiki/Nuclear_isomer

  2. 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. /wiki/Doi_(identifier)

  3. ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.

  4. # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).

  5. Kondev, 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. https://www-nds.iaea.org/amdc/ame2020/NUBASE2020.pdf

  6. Kondev, 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. https://www-nds.iaea.org/amdc/ame2020/NUBASE2020.pdf

  7. Modes of decay: EC:Electron capturen:Neutron emissionp:Proton emission /wiki/Electron_capture

  8. Bold italics symbol as daughter – Daughter product is nearly stable.

  9. Bold symbol as daughter – Daughter product is stable.

  10. Kondev, 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. https://www-nds.iaea.org/amdc/ame2020/NUBASE2020.pdf

  11. ( ) spin value – Indicates spin with weak assignment arguments.

  12. # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).

  13. # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).

  14. Shimizu, Y.; Kubo, T.; Sumikama, T.; Fukuda, N.; Takeda, H.; Suzuki, H.; Ahn, D. S.; Inabe, N.; Kusaka, K.; Ohtake, M.; Yanagisawa, Y.; Yoshida, K.; Ichikawa, Y.; Isobe, T.; Otsu, H.; Sato, H.; Sonoda, T.; Murai, D.; Iwasa, N.; Imai, N.; Hirayama, Y.; Jeong, S. C.; Kimura, S.; Miyatake, H.; Mukai, M.; Kim, D. G.; Kim, E.; Yagi, A. (8 April 2024). "Production of new neutron-rich isotopes near the N = 60 isotones Ge 92 and As 93 by in-flight fission of a 345 MeV/nucleon U 238 beam". Physical Review C. 109 (4). doi:10.1103/PhysRevC.109.044313. /wiki/Doi_(identifier)

  15. Shimizu, Y.; Kubo, T.; Sumikama, T.; Fukuda, N.; Takeda, H.; Suzuki, H.; Ahn, D. S.; Inabe, N.; Kusaka, K.; Ohtake, M.; Yanagisawa, Y.; Yoshida, K.; Ichikawa, Y.; Isobe, T.; Otsu, H.; Sato, H.; Sonoda, T.; Murai, D.; Iwasa, N.; Imai, N.; Hirayama, Y.; Jeong, S. C.; Kimura, S.; Miyatake, H.; Mukai, M.; Kim, D. G.; Kim, E.; Yagi, A. (8 April 2024). "Production of new neutron-rich isotopes near the N = 60 isotones Ge 92 and As 93 by in-flight fission of a 345 MeV/nucleon U 238 beam". Physical Review C. 109 (4). doi:10.1103/PhysRevC.109.044313. /wiki/Doi_(identifier)

  16. Shimizu, Y.; Kubo, T.; Sumikama, T.; Fukuda, N.; Takeda, H.; Suzuki, H.; Ahn, D. S.; Inabe, N.; Kusaka, K.; Ohtake, M.; Yanagisawa, Y.; Yoshida, K.; Ichikawa, Y.; Isobe, T.; Otsu, H.; Sato, H.; Sonoda, T.; Murai, D.; Iwasa, N.; Imai, N.; Hirayama, Y.; Jeong, S. C.; Kimura, S.; Miyatake, H.; Mukai, M.; Kim, D. G.; Kim, E.; Yagi, A. (8 April 2024). "Production of new neutron-rich isotopes near the N = 60 isotones Ge 92 and As 93 by in-flight fission of a 345 MeV/nucleon U 238 beam". Physical Review C. 109 (4). doi:10.1103/PhysRevC.109.044313. /wiki/Doi_(identifier)