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1 Decay Scheme - disintegrates 19.58 (11) % by beta plus emission and 8.2 (11) % by electron capture to Fe-. - emits gamma rays with energies up to 612 and the energies and emission probabilities for many of these transitions are useful for the calibration of Ge detectors. Le cobalt se désintègre à 19,58 (11) % par émission bêta plus et à 8,2 (11) % par capture électronique vers des niveaux excités du fer. Le cobalt émets des rayonnements gamma d énergie allant jusqu à 612, ce qui le rend utile pour l étalonnage des détecteurs germanium. 2 Nuclear Data T 1/2 ( ) : 77,26 (26) d Q ( ) : 6 (2) 2.1 Electron Capture Transitions Probability Nature lg ft P K P L P M 1 ɛ,15 17,7 (2),29 (7) Allowed 6,91,8766 (17),155 (1),171 (6) ɛ,1 118, (2),167 (5) 8,1,8779 (17),1 (1),169 (6) ɛ,1 171,2 (2),2159 (18) Allowed 7,2,8816 (17),11 (1),16 (6) ɛ,12 268 (2),688 (1) Allowed 6,9,885 (16),989 (1),159 (5) ɛ,11 6,1 (2) 9,9 (18) Allowed 6,51,886 (16),972 (1),1 (5) ɛ,1 65,7 (2) 12,66 () Allowed 6,,8866 (16),971 (1),1 (5) ɛ,9 517,2 (2),965 (15) Allowed 7,,8868 (16),969 (1),155 (5) ɛ,8 79,5 (2) 16,86 (5) Allowed 6,69,8875 (16),96 (1),15 (5) ɛ,7 112,7 (2) 21, (5) Allowed 6,98,8882 (16),957 (1),15 (5) ɛ,6 1195,9 (2),15 (5) 2nd Forbidden 1,2,888 (16),957 (1),15 (5) ɛ,5 1,1 (2) 8,99 (6) Allowed 7,58,888 (16),955 (1),15 (5) ɛ, 166,1 (2),2 (6) 2nd Forbidden 1,26,8885 (16),955 (1),15 (5) ɛ,2 28,9 (2) 2, () Allowed 8,62,8888 (16),952 (1),152 (5) ɛ,1 719,2 (2),5 () 2nd Forbidden 11,6,889 (16),951 (1),152 (5) LBNL, NPL /C.M. Baglin and T.D. MacMahon 1 9/9/2 9/2/25

2.2 β Transitions Probability Nature lg f t 1 β,7 98,7 (2),8 (7) Allowed 6,98 β,6 17 (2),6 (2) 2nd Forbidden 1,2 β,5 21,1 (2) 1, (2) Allowed 7,58 β, 58,1 (2),86 (22) 2nd Forbidden 1,26 β,2 158,9 (2) 18,29 (16) Allowed 8,62 β,1 2697,2 (2),25 (17) 2nd Forbidden 11,6 2. Gamma Transitions and Internal nversion efficients P γce Multipolarity α T α π 1 (1 ) (1 ) γ 11,8(Fe) 26, (5),2 (2) γ 8,7(Fe) 11,15 (),269 (2) γ 8,6(Fe) 86,55 (11),58 () γ 1,7(Fe) 655, (5),8 (8) γ 11,7(Fe) 67,579 (5),5 (5) γ 8,5(Fe) 7,51 (),191 () M1E2 γ 7,(Fe) 787,7 (5),1 () M1E2 γ 1,(Fe) 86,77 (2) 99,972 (2) E2, (9) γ 12,7(Fe) 852,72 (),9 () γ 8,(Fe) 896,51 (6),7 (22) γ 1,5(Fe) 977,72 (5) 1,22 (7) M1(E2) γ 11,5(Fe) 996,98 (5),116 (6) M1E2 γ 5,2(Fe) 17,827 (9) 1, (5) M1(E2) γ 9,(Fe) 188,89 (9),5 () M1E2 γ 1,(Fe) 11,68 (6),12 () γ 11,(Fe) 1159,9 (6),88 () M1E2 γ 12,5(Fe) 1175,11 () 2,29 (9) M1E2 γ 8,(Fe) 1198,888 (5), () γ 2,1(Fe) 128,288 (1) 66,1 (16) E2 γ 1,5(Fe) 1271,92 (6),22 (8) γ 15,5(Fe) 15,99 (),1228 (16) γ 7,2(Fe) 16,2117 (9),28 (1) M1E2 γ 1,(Fe) 12,76 (6),18 () γ 11,(Fe) 162,22 (6),778 (9) γ 12,(Fe) 16,75 (5),621 (21) γ 8,2(Fe) 1771,7 (9) 15,5 () M1E2 γ,1(fe) 181,757 (),69 () M1E2 γ 9,2(Fe) 196,71 (8),76 () M1E2 γ 1,2(Fe) 215,217 (7),17 (1) M1E2 γ 11,2(Fe) 2,797 (7) 7,7 (1) M1E2 2,7 γ,1(fe) 211,15 (5),76 () M1E2 γ 12,2(Fe) 2212,97 (9),85 (5) M1E2,1 γ 5,1(Fe) 2276,11 (6),1181 () E2,5 γ 15,2(Fe) 27,22 (),78 (6) γ 6,1(Fe) 252,9 (11),6 () M1E2,8 γ 7,1(Fe) 2598,5 () 16,969 () M1E2 5,2 γ,(fe) 2657,527 (),195 (2) [E2] 6, γ 8,1(Fe) 9,65 () 1,9 (19) M1E2 6,8 γ 9,1(Fe) 22,29 (8),25 (1) M1E2 7,8 LBNL, NPL /C.M. Baglin and T.D. MacMahon 2 9/9/2 9/2/25

P γce Multipolarity α T α π 1 (1 ) (1 ) γ 1,1(Fe) 25,5 () 7,877 () E2 8,9 γ 11,1(Fe) 27,79 () 1,8 (9) M1E2 8 γ 6,(Fe) 69,86 (11),1 (8) E2 9,6 γ 12,1(Fe) 51,22 (),9 (6) E2 9,7 γ 1,1(Fe) 58,5 (6),1958 (16) M1E2 9 γ 1,1(Fe) 6,8 (),167 (5) γ 15,1(Fe) 611,5 (),81 () [E2] 1, Atomic Data.1 Fe ω K :,55 () ω L :,6 (6) n KL : 1,7 ().1.1 X Radiations Relative probability K Kα 2 6,991 51,7 Kα 1 6,91 1 Kβ 1 7,58 } Kβ 5 7,18 } 2,67 L Ll,615 Lβ,792.1.2 Auger Electrons Relative probability Auger K KLL 5,7 5,65 1 KLX 6,158 6, 27, KXY 6,926 7,15 1,87 Auger L,51,59 LBNL, NPL /C.M. Baglin and T.D. MacMahon 9/9/2 9/2/25

Electron Emissions Electrons per 1 disint. e AL (Fe),51 -,59 111,8 (8) e AK (Fe) 6, () KLL 5,7-5,65 } KLX 6,158-6, } KXY 6,926-7,15 } β,2 max: 158,9 (2) 18,29 (16) β,2 avg: 61,2 (9) β, max: 58,1 (2),86 (22) β, avg: 27,1 (9) β,5 max: 21,1 (2) 1, (2) β,5 avg: 178,7 (8) β,6 max: 17 (2),6 (2) β,6 avg: 76,7 (8) β,7 max: 98,7 (2),8 (7) β,7 avg: 5, (9) β,1 max: 2697,2 (2),25 (17) β,1 avg: 125,8 (1) LBNL, NPL /C.M. Baglin and T.D. MacMahon 9/9/2 9/2/25

5 Photon Emissions 5.1 X-Ray Emissions Photons per 1 disint. XL (Fe),615,792,581 (17) XKα 2 (Fe) 6,991 7,5 (1) } Kα XKα 1 (Fe) 6,91 1,75 (17) } XKβ 1 (Fe) 7,58 },5 (5) K β 1 XKβ 5 (Fe) 7,18 } 5.2 Gamma Emissions Photons per 1 disint. γ 11,8 (Fe) 26,1 (1),2 (2) γ 8,7 (Fe) 11,8 (8),269 (2) γ 8,6 (Fe) 86,5 (11),58 () γ ± 511 9,21 (22) γ 1,7 (Fe) 655, (8),8 (8) γ 11,7 (Fe) 67,7 (8),5 (5) γ 8,5 (Fe) 7,585 (2),191 () γ 7, (Fe) 787,791 (2),1 () γ 1, (Fe) 86,768 (19) 99,999 (2) γ 12,7 (Fe) 852,78 (5),9 () γ 8, (Fe) 896,5 (7),7 (22) γ 1,5 (Fe) 977,6 () 1,22 (7) γ 11,5 (Fe) 996,99 (5),116 (6) γ 5,2 (Fe) 17,8 (2) 1, (5) γ 9, (Fe) 189, (2),5 () γ 1, (Fe) 11, (7),12 () γ 11, (Fe) 1159,9 (8),88 () γ 12,5 (Fe) 1175,878 (22) 2,29 (9) γ 8, (Fe) 1198,78 (2), () γ 2,1 (Fe) 128,276 (22) 66,1 (16) γ 1,5 (Fe) 1272,2 (6),22 (8) γ 15,5 (Fe) 15,8 (29),1228 (16) γ 7,2 (Fe) 16,196 (),28 (1) γ 1, (Fe) 12,75 (8),18 () γ 11, (Fe) 162, (12),778 (9) γ 12, (Fe) 16,5 (5),621 (21) γ 8,2 (Fe) 1771,27 () 15,5 () γ,1 (Fe) 181,726 (),69 () γ 9,2 (Fe) 196,7 (11),76 () LBNL, NPL /C.M. Baglin and T.D. MacMahon 5 9/9/2 9/2/25

Photons per 1 disint. γ 1,2 (Fe) 215,176 (5),17 (1) γ 11,2 (Fe) 2,752 (5) 7,71 (1) γ,1 (Fe) 211,92 (6),76 () γ 12,2 (Fe) 2212,898 (),85 (5) γ 5,1 (Fe) 2276,6 (16),118 () γ 15,2 (Fe) 27,7 (),78 (6) γ 6,1 (Fe) 252, (8),6 () γ 7,1 (Fe) 2598,8 () 16,96 () γ, (Fe) 2657, (8),195 (2) γ 8,1 (Fe) 9,559 () 1,8 (19) γ 9,1 (Fe) 21,9 (11),2 (1) γ 1,1 (Fe) 25,2 (5) 7,87 () γ 11,1 (Fe) 272,978 (6) 1,855 (9) γ 6, (Fe) 69,69 (),1 (8) γ 12,1 (Fe) 51,119 (),92 (6) γ 1,1 (Fe) 57,9 (6),19 (16) γ 1,1 (Fe) 6,71 (),167 (5) γ 15,1 (Fe) 611,8 (8),8 () 6 Main Production Modes { Fe (p,n) Possible impurities : 57, 58 7 References - W. H. Burgus, G.A. wan, J.W. Hadley, W. Hess, T. Shull, M.L. Stevenson, H.F. York. Phys. Rev. 95 (195) 75 - H. W. Wright, E.I. Wyatt, S.A. Reynolds, W.S. Lyon, T.H. Handley. Nucl. Sci. Eng. 2 (1957) 27 - H. Pettersson, O. Bergman, C. Bergman. Ark. Fysik 29 (1965) 2 - K. W. Dolan, D.K. McDaniels, D.O. Wells. Phys. Rev. 18 (1966) 1151 - M. Huguet, H. Forest, C. Ythier. mp. Rend. Acad. Sci. (Paris) 26B (1966) 12 - R. Schöneberg, M. Schumacher, A. Flammersfeld. Z. Physik 192 (1966) 5 - P.H. Barker, R.D. nnor. Nucl. Instrum. Methods 57 (1967) 17 - C. Chasman, R.A. Ristinen. Phys. Rev. 159 (1967) 915 - R.L. Auble, W.C. McHarris, W.H. Kelly. Nucl. Phys. A91 (1967) 225 - A.H. Sher, B.D. Pate. Nucl. Phys. A112 (1968) 85 LBNL, NPL /C.M. Baglin and T.D. MacMahon 6 9/9/2 9/2/25

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CEA - LNHB - Table de Radionucléides γ Emission probabilities per 1 disintegrations ε β ; 77,26 (26) d 11 fs 15 1 1 12 11 8 2 8 8,12,7, 8,1 6 7 2 5 6,2,19 9 9 2 1 5 2, 2,2,6,8,9 5 6 8 7 8 1 5,2,,11,8,7 7,7 1,85 ; 58, (2-,,) ; 7,6 ; 9,82 ; 298,2 ; 119,89 ; 8,15,29,167,2159,688 9,9 16,86 7 ; 5,27 21,,8 5 ; 122,91 2 ; 2959,95 8,99,2 1,,86 2 ; 2657,527 2 ; 285,58 2, 18,29 1 2 ; 86,77,5,25 Stable Fe 26 Q = 6 % β % ε = 1 ; LBNL, NPL / C.M. Baglin and T.D. MacMahon Scheme page : 1/ 9/9/2-9/2/25

CEA - LNHB - Table de Radionucléides γ Emission probabilities per 1 disintegrations ε β ; 77,26 (26) d 55 fs 1 9 8,8 1,22,12,18,17 7,87,5,76,2 9,26,58,191,7, 1 5,5 1,8 ; 1,27 ; 8,799 ; 8,15 12,66,965 16,86 7 6,1,28 1 6,96 ; 5,27 2 ; 69,86 21,,15,8,6 5 ; 122,91 2 ; 2959,95 8,99,2 1,,86 2 ; 2657,527 2 ; 285,58 2, 18,29 1 2 ; 86,77,5,25 Stable Fe 26 Q = 6 % β % ε = 1 LBNL, NPL / C.M. Baglin and T.D. MacMahon Scheme page : 2/ 9/9/2-9/2/25 ;

CEA - LNHB - Table de Radionucléides γ Emission probabilities per 1 disintegrations ε β ; 77,26 (26) d 6 5,6,1 1,,118,76 5 2 ; 69,86 ; 122,91 2 ; 2959,95,15 8,99,2,6 1,,86,69,19 2 ; 2657,527 2 6 6,1 ; 285,58 2, 18,29 1 9 9,9 9 9 2 ; 86,77,5,25 Stable Fe 26 Q = 6 % β % ε = 1 ; LBNL, NPL / C.M. Baglin and T.D. MacMahon Scheme page : / 9/9/2-9/2/25