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Isotopes of copper

From Wikipedia, the free encyclopedia

Isotopes ofcopper (29Cu)
Main isotopes[1]Decay
Isotopeabun­dancehalf-life(t1/2)modepro­duct
63Cu69.2%stable
64Cusynth12.70 hβ+64Ni
β64Zn
65Cu30.9%stable
67Cusynth61.83 hβ67Zn
Standard atomic weightAr°(Cu)

Copper (29Cu) has two stable isotopes,63Cu and65Cu, along with 28 known radioisotopes from55Cu to84Cu. The most stable radioisotope,67Cu, has ahalf-life of only 61.83 hours, then follow64Cu at 12.70 hours and61Cu at 3.34 hours. The others have half-lives all under an hour and most under a minute. The isotopes with mass below 63 generally undergopositron emission andelectron capture tonickel isotopes, while isotopes with mass above 65 generally undergoβ decay tozinc isotopes. The single example in between,64Cu, decays both ways.

There are at least 10metastable isomers of copper, of which the most stable is68mCu with a half-life of 3.75 minutes.

List of isotopes

[edit]


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

[n 5]
Spin and
parity[1]
[n 6][n 7]
Natural abundance(mole fraction)
Excitation energy[n 7]Normal proportion[1]Range of variation
55Cu292654.965854(27)[5]55.9(15) msβ+55Ni3/2−#
β+,p (?%)54Co
56Cu292755.9585293(69)80.8(6) msβ+ (99.60%)56Ni(4+)
β+, p (0.40%)55Co
57Cu292856.94921169(54)196.4(7) msβ+57Ni3/2−
58Cu292957.94453228(60)3.204(7) sβ+58Ni1+
59Cu293058.93949671(57)81.5(5) sβ+59Ni3/2−
60Cu293159.9373638(17)23.7(4) minβ+60Ni2+
61Cu293260.9334574(10)3.343(16) hβ+61Ni3/2−
62Cu293361.9325948(07)9.672(8) minβ+62Ni1+
63Cu293462.92959712(46)Stable3/2−0.6915(15)
64Cu293563.92976400(46)12.7004(13) hβ+ (61.52%)64Ni1+
β (38.48%)64Zn
65Cu293664.92778948(69)Stable3/2−0.3085(15)
66Cu293765.92886880(70)5.120(14) minβ66Zn1+
66mCu1154.2(14) keV600(17) nsIT66Cu(6)−
67Cu293866.92772949(96)61.83(12) hβ67Zn3/2−
68Cu293967.9296109(17)30.9(6) sβ68Zn1+
68mCu721.26(8) keV3.75(5) minIT (86%)68Cu6−
β (14%)68Zn
69Cu294068.929429267(15)2.85(15) minβ69Zn3/2−
69mCu2742.0(7) keV357(2) nsIT69Cu(13/2+)
70Cu294169.9323921(12)44.5(2) sβ70Zn6−
70m1Cu101.1(3) keV33(2) sβ (52%)70Zn3−
IT (48%)70Cu
70m2Cu242.6(5) keV6.6(2) sβ (93.2%)70Zn1+
IT (6.8%)70Cu
71Cu294270.9326768(16)19.4(14) sβ71Zn3/2−
71mCu2755.7(6) keV271(13) nsIT71Cu(19/2−)
72Cu294371.9358203(15)6.63(3) sβ72Zn2−
72mCu270(3) keV1.76(3) μsIT72Cu(6−)
73Cu294472.9366744(21)4.20(12) sβ (99.71%)73Zn3/2−
β,n (0.29%)72Zn
74Cu294573.9398749(66)1.606(9) sβ (99.93%)74Zn2−
β, n (0.075%)73Zn
75Cu294674.94152382(77)1.224(3) sβ (97.3%)75Zn5/2−
β, n (2.7%)74Zn
75m1Cu61.7(4) keV0.310(8) μsIT75Cu1/2−
75m2Cu66.2(4) keV0.149(5) μsIT75Cu3/2−
76Cu294775.9452370(21)[6]656(2) ms[7]β (?%)76Zn(6−)[7]
β, n (?%)75Zn
76mCu[6][n 8]64.8(25) keV656(2) ms[7]β (?%)76Zn3−
β, n (?%)75Zn
77Cu294876.9475436(13)470.3(17) msβ (69.9%)77Zn5/2−
β, n (30.1%)76Zn
78Cu294977.9519206(81)[8]330.7(20) msβ, n (50.6%)77Zn(6−)
β (49.4%)78Zn
78mCu[9]1143+X keV3.8(4) msIT78Cu(0−)
79Cu295078.95447(11)241.3(21) msβ, n (66%)78Zn(5/2−)
β (34%)79Zn
80Cu295179.96062(32)#113.3(64) msβ, n (59%)79Zn
β (41%)80Zn
81Cu295280.96574(32)#73.2(68) msβ, n (81%)80Zn5/2−#
β (19%)81Zn
82Cu295381.97238(43)#34(7) msβ82Zn
83Cu295482.97811(54)#21# ms [>410 ns]5/2−#
84Cu[10]295583.98527(54)#
This table header & footer:
  1. ^mCu – 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:
    IT:Isomeric transition
    n:Neutron emission
    p:Proton emission
  5. ^Bold symbol as daughter – Daughter product is stable.
  6. ^( ) spin value – Indicates spin with weak assignment arguments.
  7. ^ab# – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  8. ^Order of ground state and isomer is uncertain.

Copper nuclear magnetic resonance

[edit]

Both stable isotopes of copper (63Cu and65Cu) havenuclear spin of 3/2−, and thus producenuclear magnetic resonance spectra, although the spectral lines are broad due toquadrupolar broadening.63Cu is the more sensitive nucleus while65Cu yields very slightly narrower signals. Usually though63Cu NMR is preferred.[11]

Copper-64 and other potential medical isotopes

[edit]

Copper offers a relatively large number ofradioisotopes that are potentially useful fornuclear medicine.

There is growing interest in the use of64Cu,62Cu,61Cu, and60Cu for diagnostic purposes and67Cu and64Cu for targetedradiotherapy. For example,64Cu has a longer half-life than most positron-emitters (12.7 hours) and is thus ideal for diagnostic PET imaging of biological molecules.[12]

Copper-76

[edit]

Copper-76 is a radioactive istope of copper with one long-lived isomercopper-76m, whose half-lives are disputed. A 1990 study by Wingeret al. atKEK reported two long-lived states with half-lives of 0.57(6) s and 1.27(3) s, with the longer-lived state being the isomer and having lower spin.[13] Subsequent experiments could not identify the claimed long-lived isomer, with the isomer that was observed later being assigned a spin of 3− based on the levels of76Zn populated by β decay.[1] (There is also a significant βn decay mode to75Zn.) However, a 2024 experiment at theUniversity of Jyväskylä discovered that the previously observed 3− state is actually the isomer, whose excitation energy is 64.8(25) keV, and the long-lived ground state probably has spin 1+; Caneteet al. claim that there is a significant isomeric transition to the ground state.[6] However, Olaizolaet al. (2025) found that both the ground state and the isomer have similar half-lives around 656(2) ms, like was found in most previous experiments. Additionally, they find that the non-3− state is probably 6− based on shell model calculations, excluding a significant isomeric transition and preventing identification of the ground state.[7]

See also

[edit]

Daughter products other than copper

References

[edit]
  1. ^abcdefKondev, 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. ^"Standard Atomic Weights: Copper".CIAAW. 1969.
  3. ^Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04)."Standard atomic weights of the elements 2021 (IUPAC Technical Report)".Pure and Applied Chemistry.doi:10.1515/pac-2019-0603.ISSN 1365-3075.
  4. ^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.
  5. ^Zhang, M.; Zhou, X.; Wang, M.; Zhang, Y. H.; Litvinov, Yu. A.; Xu, H. S.; Chen, R. J.; Deng, H. Y.; Fu, C. Y.; Ge, W. W.; Li, H. F.; Liao, T.; Litvinov, S. A.; Shuai, P.; Shi, J. Y.; Sidhu, R. S.; Song, Y. N.; Sun, M. Z.; Suzuki, S.; Wang, Q.; Xing, Y. M.; Xu, X.; Yamaguchi, T.; Yan, X. L.; Yang, J. C.; Yuan, Y. J.; Zeng, Q.; Zhou, X. H. (14 February 2023)."$$B\rho $$-defined isochronous mass spectrometry and mass measurements of $$^{58}$$Ni fragments".The European Physical Journal A.59 (2).doi:10.1140/epja/s10050-023-00928-6.
  6. ^abcCanete, L.; Giraud, S.; Kankainen, A.; Bastin, B.; Nowacki, F.; Ascher, P.; Eronen, T.; Girard Alcindor, V.; Jokinen, A.; Khanam, A.; Moore, I.D.; Nesterenko, D.; De Oliveira, F.; Penttilä, H.; Petrone, C.; Pohjalainen, I.; De Roubin, A.; Rubchenya, V.; Vilen, M.; Äystö, J. (June 2024). "Long-sought isomer turns out to be the ground state of 76Cu".Physics Letters B.853 138663.arXiv:2401.14018.doi:10.1016/j.physletb.2024.138663.
  7. ^abcdOlaizola, B.; Illana, A.; Benito, J.; Suárez-Bustamante, D.P.; Del Piccolo, G.; Algora, A.; Andel, B.; Andreyev, A.N.; Araszkiewicz, M.; Ayyad, Y.; Bark, R.A.; Berry, T.; Borge, M.J.G.; Chrysalidis, K.; Cocolios, T.E.; Costache, C.; Cubiss, J.G.; Van Duppen, P.; Favier, Z.; Fraile, L.M.; Fynbo, H.O.U.; Galtarossa, F.; Georgiev, G.; Greenless, P.T.; Grzywacz, R.; Harkness-Brennan, L.J.; Heinke, R.; Huyse, M.; Ibañez, P.; Johnston, K.; Jones, P.M.; Judson, D.S.; Konki, J.; Korgul, A.; Köster, U.; Kurcewicz, J.; Labiche, M.; Lazarus, I.; Lică, R.; Llanos-Expósito, M.; Madurga, M.; Marginean, N.; Marginean, R.; Marsh, B.A.; Mihai, C.; Mihai, R.E.; Murias, J.R.; Nácher, E.; Neacsu, C.; Negret, A.; Nouvilas, V.M.; Ojala, J.; Orce, J.N.; Page, C.A.A.; Page, R.D.; Pakarinen, J.; Papadakis, J.; Pascu, S.; Perea, A.; Piersa-Siłkowska, M.; Plaza, A.M.; Podolyák, Zs.; Poklepa, W.; Pucknell, V.; Rahkila, P.; Raison, C.; Rapisarda, E.; Rezynkina, K.; Rotaru, F.; Schomacker, K.; Siciliano, M.; Sotty, C.; Stryjczyk, M.; Tengblad, O.; Udías, J.M.; Vedia, V.; Viñals, S.; Wadsworth, R.; Warr, N.; De Witte, H.; Yates, D.; Yue, Z. (July 2025). "The 76Cu conundrum remains unsolved".Physics Letters B.866 139551.arXiv:2505.06400.doi:10.1016/j.physletb.2025.139551.
  8. ^Giraud, S.; Canete, L.; Bastin, B.; Kankainen, A.; Fantina, A.F.; Gulminelli, F.; Ascher, P.; Eronen, T.; Girard-Alcindor, V.; Jokinen, A.; Khanam, A.; Moore, I.D.; Nesterenko, D.A.; de Oliveira Santos, F.; Penttilä, H.; Petrone, C.; Pohjalainen, I.; De Roubin, A.; Rubchenya, V.A.; Vilen, M.; Äystö, J. (October 2022). "Mass measurements towards doubly magic 78Ni: Hydrodynamics versus nuclear mass contribution in core-collapse supernovae".Physics Letters B.833 137309.doi:10.1016/j.physletb.2022.137309.hdl:10138/350386.
  9. ^Pedersen, L. G.; Sahin, E.; Görgen, A.; Bello Garrote, F. L.; Tsunoda, Y.; Otsuka, T.; Niikura, M.; Nishimura, S.; Xu, Z.; Baba, H.; Benzoni, G.; Browne, F.; Bruce, A. M.; Ceruti, S.; Crespi, F. C. L.; Daido, R.; de Angelis, G.; Delattre, M.-C.; Dombradi, Zs.; Doornenbal, P.; Fang, Y.; Franchoo, S.; Gey, G.; Gottardo, A.; Isobe, T.; John, P. R.; Jung, H. S.; Kojouharov, I.; Kubo, T.; Kurz, N.; Kuti, I.; Li, Z.; Lorusso, G.; Matea, I.; Matsui, K.; Mengoni, D.; Miyazaki, T.; Modamio, V.; Momiyama, S.; Morales, A. I.; Morfouace, P.; Napoli, D. R.; Naqvi, F.; Nishibata, H.; Odahara, A.; Orlandi, R.; Patel, Z.; Rice, S.; Sakurai, H.; Schaffner, H.; Sinclair, L.; Söderström, P.-A.; Sohler, D.; Stefan, I. G.; Sumikama, T.; Suzuki, D.; Taniuchi, R.; Taprogge, J.; Vajta, Z.; Valiente-Dobón, J. J.; Watanabe, H.; Werner, V.; Wu, J.; Yagi, A.; Yalcinkaya, M.; Yokoyama, R.; Yoshinaga, K. (3 April 2023). "First spectroscopic study of odd-odd Cu 78".Physical Review C.107 (4) 044301.doi:10.1103/PhysRevC.107.044301.hdl:10852/106240.
  10. ^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) 044313.doi:10.1103/PhysRevC.109.044313.
  11. ^"(Cu) Copper NMR".
  12. ^Harris, M. "Clarity uses a cutting-edge imaging technique to guide drug development".Nature Biotechnology September 2014: 34
  13. ^Winger, J. A.; Hill, John C.; Wohn, F. K.; Warburton, E. K.; Gill, R. L.; Piotrowski, A.; Schuhmann, R. B.; Brenner, D. S. (1 September 1990). "Structure of Zn 76 from Cu 76 decay and systematics of neutron-rich Zn nuclei".Physical Review C.42 (3):954–960.doi:10.1103/PhysRevC.42.954.PMID 9966808.
Group12 3456789101112131415161718
PeriodHydrogen and
alkali metals
Alkaline
earth metals
Pnicto­gensChal­co­gensHalo­gensNoble gases
12
345678910
1112131415161718
192021222324252627282930313233343536
373839404142434445464748495051525354
55561 asterisk71727374757677787980818283848586
87881 asterisk103104105106107108109110111112113114115116117118
119120
1 asterisk5758596061626364656667686970 
1 asterisk8990919293949596979899100101102
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