1 Decay Scheme. 2 Nuclear Data. 2.1 β + Transitions. 2.2 Electron Capture Transitions
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1 1 Decay Scheme Ni disintegrates by electron capture (56.6 %) and positron emission (43.4 %) to excited levels in Co. The transition to the ground state has not been observed. Le nickel se désintègre par capture électronique (56,6%) et émission de positrons (43,4%) vers des niveaux excités de cobalt. La transition vers le niveau fondamental n a pas été observée. 2 Nuclear Data T 1/2 ( Ni ) : 35,9 (3) h T 1/2 ( Co ) : 271,80 (5) d Q + ( Ni ) : 3264,2 (26) 2.1 β + Transitions Probability Nature 100 β 0, ,6 (3) 0,45 (3) Allowed β 0, ,6 (3) 0,85 (6) Allowed β 0, ,4 (3) 6,8 (3) Allowed β 0, ,6 (3) 35,3 (5) Allowed 2.2 Electron Capture Transitions Probability Nature lg ft P K P L P M 100 ɛ 0,11 87 (3) 0,025 (5) Allowed 6 0,8706 (19) 0,1103 (15) 0,0181 (6) ɛ 0, (3) 0,063 (4) Allowed 6,1 0,8790 (17) 0,1033 (14) 0,0168 (5) ɛ 0,9 460 (3) 0,308 (23) Allowed 6,4 0,8853 (16) 0,0980 (13) 0,0158 (5) ɛ 0,8 533 (3) 0,020 (3) Allowed 7,7 0,88 (16) 0,0977 (13) 0,0158 (5) Tsing Hua Univ. /S. C. Wu 1 12/02/02 27/5/2004
2 Probability Nature lg ft P K P L P M 100 ɛ 0, (3) 0,039 (5) Allowed 8,1 0,8871 (16) 0,0965 (13) 0,0156 (5) ɛ 0, (3) 12,1 (6) Allowed 5,7 0,8873 (16) 0,0964 (13) 0,0155 (5) ɛ 0, (3) 5,2 (3) Allowed 6,2 0,8874 (16) 0,0963 (13) 0,0155 (5) ɛ 0, (3) 9,6 (4) Allowed 6,1 0,8875 (16) 0,0962 (13) 0,0155 (5) ɛ 0, (3) 29,3 (5) Allowed 5,6 0,8876 (16) 0,0961 (13) 0,0155 (5) 2.3 Gamma Transitions and Internal Conversion Coefficients P γ+ce Multipolarity α K α L α T 100 γ 3,2(Co) 127,164 (3) 16,4 (5) M1+0,0064%E2 0,0193 (6) 0,00191 (6) 0,0215 (6) γ 6,4(Co) 161,86 (3) 0,0204 (24) M1 0,0104 (3) 0,00102 (3) 0,0115 (3) γ 10,9(Co) 304,1 (1) 0,0020 (6) γ 4,2(Co) 379,941 (20) 0,072 (6) [M1] 0,00129 (4) 0, (4) 0,00143 (4) γ 6,2(Co) 541,9 (1) 0,0036 (5) [E2] 0,00105 (3) 0, (3) 0,00116 (3) γ 5,1(Co) 673,44 (4) 0,0483 (15) M1+0,04%E2 0,00036 (1) 0, (1) 0,00040 (1) γ 6,1(Co) 696,0 (4) 0,0009 (6) [E2] 0,00050 (2) 0, (1) 0,00056 (2) γ 7,2(Co) 755,31 (10) 0,0054 (6) M1+10,9%E2 0, (9) 0, (8) 0,00033 (1) γ 9,5(Co) 906,99 (5) 0,075 (14) γ 9,4(Co) 1046,55 (14) 0,132 (3) γ 1,0(Co) 1223,8 (3) 0,076 (13) M1+6,3%E2 0, (3) 0, (3) 0, (4) γ 11,5(Co) 1280,01 (6) 0,0096 (7) γ 10,4(Co) 1350,54 (6) 0,002 (1) γ 2,0(Co) 1377,64 (4) 81,2 (6) E2 0, (3) 0, (3) 0, (3) γ 10,3(Co) 1603,30 (6) 0,0039 (6) γ 10,2(Co) 1730,48 (6) 0,055 (3) γ 4,0(Co) 17,58 (3) 6,1 (4) E2 γ 5,0(Co) 1897,0 (5) 0,0252 (25) M1+0,16%E2 γ 6,0(Co) 1919,65 (14) 12,5 (5) M1+5,0%E2 γ 7,0(Co) 2133,08 (5) 0,033 (5) M1 γ 8,0(Co) 2730,83 (14) 0,020 (3) γ 9,0(Co) 2804,15 (15) 0,102 (17) E2 γ 11,0(Co) 3177,37 (5) 0,015 (4) Tsing Hua Univ. /S. C. Wu 2 12/02/02 27/5/2004
3 3 Atomic Data 3.1 Co ω K : 0,388 (4) ω L : 0,0072 (5) n KL : 1,418 (4) X Radiations Relative probability K Kα 2 6, ,16 Kα 1 6, Kβ 1 7,6495 } Kβ 5 7,706 } 20,74 L Ll 0,678 Lγ 0, Auger Electrons Relative probability Auger K KLL 5,81 6, KLX 6,67 6,86 27,3 KXY 7,50 7,58 1,88 Auger L 0,564 0, Tsing Hua Univ. /S. C. Wu 3 12/02/02 27/5/2004
4 4 Electron Emissions Electrons per 100 disint. e AL (Co) 0,564 0,653 76,7 (12) e AK (Co) 31,0 (6) KLL 5,81 6,10 } KLX 6,67 6,86 } KXY 7,50 7,58 } ec 3,2 K (Co) 119,46 (3) 0,310 (14) ec 6,4 K (Co) 154,15 (3) 0,00021 (3) β 0,6 + max: 320,6 (3) 0,45 (3) β 0,6 + avg: 138,6 β 0,4 + max: 482,6 (3) 0,85 (6) β 0,4 + avg: 206,1 β 0,3 + max: 735,4 (3) 6,8 (3) β 0,3 + avg: 313,4 β 0,2 + max: 862,6 (3) 35,3 (5) β 0,2 + avg: 368,3 5 Photon Emissions 5.1 XRay Emissions Photons per 100 disint. XL (Co) 0,678 0,870 0,56 (4) XKα 2 (Co) 6,9153 5,84 (12) } Kα XKα 1 (Co) 6, ,42 (23) } XKβ 1 (Co) 7,6495 } 2,37 (6) K β 1 XKβ 5 (Co) 7,706 } Tsing Hua Univ. /S. C. Wu 4 12/02/02 27/5/2004
5 5.2 Gamma Emissions Photons per 100 disint. γ 3,2 (Co) 127,164 (3) 16,0 (5) γ 6,4 (Co) 161,86 (3) 0,0202 (24) γ 10,9 (Co) 304,1 (1) 0,0020 (6) γ 4,2 (Co) 379,94 (2) 0,072 (6) γ ± ,8 (12) γ 6,2 (Co) 541,9 (1) 0,0036 (5) γ 5,1 (Co) 673,44 (4) 0,0483 (15) γ 6,1 (Co) 696,0 (4) 0,0009 (6) γ 7,2 (Co) 755,3 (1) 0,0054 (6) γ 9,5 (Co) 906,98 (5) 0,075 (14) γ 9,4 (Co) 1046,68 (14) 0,132 (3) γ 1,0 (Co) 1223,8 (3) 0,076 (13) γ 11,5 (Co) 1279,99 (6) 0,0096 (7) γ 10,4 (Co) 1350,52 (6) 0,002 (1) γ 2,0 (Co) 1377,62 (4) 81,2 (6) γ 10,3 (Co) 1603,28 (6) 0,0039 (6) γ 10,2 (Co) 1730,45 (6) 0,055 (3) γ 4,0 (Co) 17,55 (3) 6,1 (4) γ 5,0 (Co) 1897,0 (5) 0,0252 (25) γ 6,0 (Co) 1919,62 (14) 12,5 (5) γ 7,0 (Co) 2133,04 (5) 0,033 (5) γ 8,0 (Co) 2730,76 (14) 0,020 (3) γ 9,0 (Co) 2804,08 (15) 0,102 (17) γ 11,0 (Co) 3177,27 (5) 0,015 (4) 6 Main Production Modes Ni 58(γ,n)Ni Ni 58(n,2n)Ni Ni 58(d,dn)Ni Fe 56(p,γ)Ni Fe 56(d,n)Ni Mn 55(α,2n)Ni 7 References F. Maienschein, J.L. Meem Jr. Phys. Rev. 76 (1949) 899 (Halflife) G. Friedlander, M.L.Perlman, D. Alburger, A. W. Sunyar. Phys. Rev. 80 (1950) 30 (Halflife) P.F. Zweifel. Phys. Rev. 96 (1954) 12 G. Rudstam. Thesis, University of Uppsala (1956) (Halflife) Tsing Hua Univ. /S. C. Wu 5 12/02/02 27/5/2004
6 P.F. Zweifel. Phys. Rev. 107 (19) 329 J. Konijn, H. L. Hagedoorn, B. van Nooijen. Physica 24 (1958) 129 L.A. Rayburn. Phys. Rev. 122 (1961) 168 (Halflife) G. Chilosi, S. Monaro, R. A. Ricci. Nuovo Cim. 26 (1962) 440 G. Rudstam. Nucl. Phys. 56 (1964) 593 (Halflife, Electron Capture/Beta plus ratio) T.G. Ebrey, P.R. Gray. Nucl. Phys. 61 (1965) 479 (Halflife) C.J. Piluso, D.O. Wells, D.K. McDaniels. Nucl. Phys. 77 (1966) 193 (Gamma ray energies) E.W.A. Lingeman, J. Konijn, F. Diederix, B. J. Meijer. Nucl. Phys. A100 (1967) 136 (Gamma ray energies, Electron Capture/Beta plus ratio) C. Gatrousis, R.A. Meyer, L.G. Mann, J.B. McGrory. Phys. Rev. 180 (1969) 1052 (Gamma ray energies) S.J. Rothman, N.L. Peterson, W.K. Chen, J.J. Hines, R. Bastar, L.C. Robinson, L.J. Nowicki, J.B. Anderso. Phys. Rev. C9 (1974) 2272 (Halflife) I.M. Band, M.B. Trzhaskovskaya, M. A. Listengarten. At. Data. Nucl. Data Tables 18 (1976) 433 (ICC) W. Bambynek, H. Behrens, M.H. Chen, B. Crasemann, M.L. Fitzpatrick, K.W.D. Ledingham, H. Genz, M. Mutterer, R.L. Intemann. Rev. Mod. Phys. 49 (1977) 77 A. Grutter. Int. J. Appl. Radiat. Isotop. 33 (1982) 533 (Halflife) J.K. Dickens. J. Radioanal. Nucl. Chem. 103 (1986) 273 (Halflife) A.M.S. Scardino, O. Helene, P. R. Pascholati, V. R. Vanin. Z. Physik A336 (1990) 313 (Gamma ray energies, Gammaray emission probabilities) M.R.Bhat. Nucl. Data Sheets 67 (1992) 195 (Gammaray emission probabilities) NNDC. The Program LOGFT (1993) (lg ft) G.Audi, A.H. Wapstra. Nucl. Phys. A595 (1995) 409 (Q) E.Schönfeld, H.Janssen. Nucl. Instrum. Methods Phys. Res. A369 (1996) 527 (Atomic Data) H.Janssen, E.Schönfeld. PTB (1997) (EMISSION, a computer program to calculate Xray and Auger electron emission probabilities.) E.Schönfeld, F.Chu, E.Browne. PTB, LBNL (1997) (ECCapture, a computer program to calculate electroncapture probabilities for allowed and firstforbidden nonunique transitions) Tsing Hua Univ. /S. C. Wu 6 12/02/02 27/5/2004
7 BNM LNHB/CEA Table de Radionucléides Ni γ Emission probabilities per 100 disintegrations ε β + 0 Ni /2 ; 0 35,9 (3) h 152 fs 54 fs ,00 0,01 0,00 0,00 0,00 0,05 5/2,7/2 ; 3177,31 (3/2) ; 3108,14 0,025 0, fs 91 fs ,07 0,13 0,10 0,02 (3/2,5/2) ; 2804,18 3/2,5/2 ; 2730,83 0,308 0,02 0,34 ps 22 fs 110 fs 0,27 ps 0,21 ns 19 ps 54 fs ,005 0, ,020 0,003 0, , ,04 0,02 2 0,07 6,1 5/2 ; 2133,06 5/2 ; 1919,47 7/2 ; 1897,24 3/2 ; 17,596 1/2 ; 1504,82 3/2 ; 1377,65 9/2 ; 1223,79 0,039 12,1 5,2 9,6 29,3 0,45 0,85 6,8 35,3 271,80 (5) d 0 Co Q = 3264,2 % β + + % ε = 100 7/2 ; 0 Tsing Hua Univ. / S. C. Wu Scheme page : 1/2 12/02/ /02/2002
8 BNM LNHB/CEA Table de Radionucléides Ni ε β + 0 Ni /2 ; 0 35,9 (3) h γ Emission probabilities per 100 disintegrations 0,21 ns 19 ps 54 fs ,2 0,07 1/2 ; 1504,82 3/2 ; 1377,65 9/2 ; 1223,79 9,6 29,3 6,8 35,3 271,80 (5) d 0 Co Q = 3264,2 % β + + % ε = 100 7/2 ; 0 Tsing Hua Univ. / S. C. Wu Scheme page : 2/2 12/02/ /02/2002
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Cf- disintegrates by alpha emissions mainly to the Cm-248 ground state level, and by spontaneous fission for 3,086(8) %. The average number of neutrons emitted by spontaneous fission is:
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 β Transitions
1 Decay Scheme Le césium se désintègre essentiellement par émission bêta moins vers des niveaux excités du baryum. Cs- desintegrates mainly by beta minus emissions to excited levels in Ba-. 2 Nuclear Data
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Np decays 87,8 (6) % by electron capture to U, 12,0 (6) % by beta minus emission to Pu, a possible alpha emission of 0,16 (6)% to Pa232 has not been observed. Le neptunium se désintègre
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Pa is a member of the natural U235 decay chain. Pa disintegrates by alpha emission to various excited levels and the ground state of Ac227. Le protactinium se désintègre par émissions alpha
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Bi- disintegrates 97.91(3) % by beta minus emission to the levels in Po- and 2.09(3) % through alpha decay to Tl-209. Le bismuth se désintègre principalement par émissions bêta vers le polonium
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Pb disintegrates by beta minus emission to excited levels and to the ground state level of Bi. Le plomb se désintègre par émission bêta moins vers des niveaux excités et le niveau fondamental
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
1 Decay Scheme I- disintegrates by electron capture mainly via the 159 level of Te- (97%). L iode se désintègre par capture électronique principalement vers le niveau excité de 159 du tellure, avec une
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Se disintegrates 100% by electron capture to excited levels and to the ground state of As. Le Se se désintègre à 100% par capture électronique vers des niveaux excités et le niveau fondamental
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Pb ground state (J π = 9/2 + ) decays by 100 % beta minus to Bi. The strongest branch (91.28 (12) %) decays directly to the ground state (J π = 9/2 ). Le plomb se désintègre par émissions
1 Decay Scheme. 2 Nuclear Data. 236m. 2.1 Electron Capture Transitions. 2.2 β Transitions
1 Decay Scheme Np- (isomer state of Np-236, J=1, E1 =60 ) decays 53(1) % by electron capture to U-236 and 47(1) % by beta minus emission to Pu-236. Le neptunium 236 isomère se désintègre par capture électronique
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Rh- disintegrates by beta minus emission to the ground state and excited levels of Pd-. Le rhodium se désintègre par émission bêta principalement vers le niveau fondamental et les niveaux
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Bi- undergoes beta decay to Po- (64.07(7)%), and alpha decay to Tl-208 (35.93(7)%). 0.014(1)% of the beta branch undergoes prompt long-range alpha decay to Pb-208. Le bismuth se désintègre
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme In- disintegrates by > 99.99% electron capture via the excited level of 416.6 in Cd- and by < 0.01% electron capture via the isomer level in Cd- (T 1/2 = 48.5 min) at 396.2. Transitions
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Sn- decays by electron capture mainly to the In-m isomer which has a half-life of 99 minutes. After a sufficient time, the ratio of the In-m (99 min) and Sn- activities remains constant
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
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1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
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1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Co disintegrates by 100% electron capture to the excited levels of 706.42 (0.18%), and 136.47 (99.82%) in Fe. Le cobalt se désintègre à 100 % par capture électronique principalement vers
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 β + Transitions
1 Decay Scheme Zr- (half-life of 78.42 h) undergoes 100% EC/positron decay (Q EC of 2832.8(28) kev) to various nuclear levels, including the metastable and ground states of Y-. Le zirconium se désintègre
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
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1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
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
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
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1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
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1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
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1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
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1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Uranium decays primarily by alpha decay to excited states in Th-228. A small branching of exotic decay via Ne-24 emission and a smaller branching of spontaneous fission have been reported.
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Nd- disintegrates by beta minus emission to excited levels of Pm-. If a transition to the ground state level exists, it is less than 0.15 %. Le néodyme se désintègre par émission bêta moins
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
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1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
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1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Pu- decays 100% by alpha transitions to U-234. Most of the alpha decay populates the U-234 ground state (71.04 %) and the U-234 first excited level with energy of 43.50 (28.85 %). Branching
Th, Ra, Rn, Po, Pb, Bi, & Tl K x-rays. Rn Kα1. Rn Kα2. 93( 227 Th)/Rn Kβ3. Ra Kα2. Po Kα2 /Bi K α1 79( 227 Th)/Po Kα1. Ra Kα1 /Bi K β1.
Page -1-10 8 10 7 10 6 10 5 10 4 334 ( Th) Counts/Channel 10 3 10 2 10 1 49 ( Th)/ 50 ( Th)/ 50 ( Fr) 0 100 200 300 400 500 600 700 800 900 1000 1000 1100 1200 1300 1400 1500 1600 1700 1800 1900 2000 Channel
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