1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
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1 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 and is 1,0006. The values given here are the nuclides in equibium. Le Sn- se désintègre par capture électronique conduisant principalement à l isomère In-m ayant 99 min de période. Lorsque In-m et Sn- sont à l équilibre le rapport des activités de ces deux radionucléides est : 1,0006. Les valeurs sont données ici à l équilibre. 2 Nuclear Data T 1/2 ( Sn ) : 115,09 (3) d T 1/2 ( m In ) : 1,6579 (38) h Q ( Sn ) : 1036,0 (28) kev 2.1 Electron Capture Transitions Probability (%) Nature lg ft P K P L P M ɛ 0,3 6 (3) 0,00103 (4) Allowed 6,5 0,3 (3) 0,54 (20) ɛ 0,2 389 (3) 2,21 (8) 1st Forbidden 8,2 0,8490 (14) 0,121 (1) 0,0254 (5) ɛ 0,1 644 (3) 97,79 (8) 1st Forbidden 7,01 0,855 (1) 0,116 (1) 0,0241 (5) 2.2 Gamma Transitions and Internal Conversion Coefficients P γce α Multipolarity K α L α M α N α T (%) (10 2 ) (10 2 ) (10 3 ) γ 2,1(In) 255,134 (10) 2,21 (8) M133%E2 0,0396 (12) 0,549 (16) 0,1078 (32) 0,211 (6) 0,0464 (14) γ 3,2(In) 382,90 (8) 0, (3) γ 1,0(In) 391,698 (3) 100,00 (17) M4 0,437 (4) 8,58 (26) 1,70 (5) 3,77 (11) 0,540 (4) γ 3,1(In) 638,03 (8) 0,00097 (4) γ 2,0(In) 646,83 (1) 0, (2) [E3] INEEL / R.G. Helmer 1 14/07/ /10/2017
2 3 Atomic Data 3.1 In ω K : 0,851 (4) ω L : 0,0684 (20) n KL : 0,944 (4) X Radiations Relative probability X K Kα 2 24, ,3 Kα 1 24, Kβ 3 27,238 Kβ 1 27, ,8 Kβ 5 27,495 Kβ 2 27,861 Kβ 4 27,928 5,4 KO 2,3 27,939 L Ll 2,9 Lα 3,28-3,29 Lη 3,11 Lβ 3,49-3,79 Lγ 3,82-4, Auger Electrons Relative probability Auger K KLL 19,34-20, KLX 22,83-24,19 43,6 KXY 26,25-27,90 5,7 Auger L 2,0-4,2 INEEL / R.G. Helmer 2 14/07/ /10/2017
3 4 Electron Emissions Electrons (per 100 disint.) e AL (In) 2,0-4,2 116,3 (6) e AK (In) KLL 19,34-20,35 KLX 22,83-24,19 KXY 26,25-27,90 17,0 (5) ec 2,1 K (In) 227,194 (10) 0,0836 (41) ec 2,1 L (In) 250, ,404 0,0116 (6) ec 1,0 K (In) 363,758 (3) 28,39 (27) ec 1,0 L (In) 387, ,968 5,57 (17) ec 1,0 M (In) 390, ,255 1,104 (33) ec 1,0 N (In) 391, ,682 0,245 (7) ec 1,0 T (In) 363, ,682 35,31 (28) 5 Photon Emissions 5.1 X-Ray Emissions Photons (per 100 disint.) XL (In) 2,9-4,16 8,48 (19) } XKα 2 (In) 24, ,69 (21) Kα XKα 1 (In) 24,21 51,9 (3) XKβ 3 (In) 27,238 XKβ 1 (In) 27, ,58 (17) K β 1 XKβ 5 (In) 27,495 XKβ 2 (In) 27,861 XKβ 4 (In) 27,928 2,77 (10) K β 2 XKO 2,3 (In) 27, Gamma Emissions Photons (per 100 disint.) γ 2,1 (In) 255,134 (10) 2,11 (8) γ 3,2 (In) 382,90 (8) 0, (3) γ 1,0 (In) 391,698 (3) 64,97 (17) γ 3,1 (In) 638,03 (8) 0,00097 (4) γ 2,0 (In) 646,83 (1) 0, (2) INEEL / R.G. Helmer 3 14/07/ /10/2017
4 6 Main Production Modes Sn 112(n,γ)Sn m σ : 0,30 (4) barns Sn m(it)sn T 1/2 : 20 min { Sn 112(n,γ)Sn σ : 0,71 (10) barns Possible impurities: Sn 119m, Sn 121m, Sn 117m, Sn 123, Sn 125m 7 References - S.W.Barnes. Phys. Rev. 56 (1939) J.L.Lawson, J.M.Cork. Phys. Rev. 57 (1940) R.K.Girgis, R.Van Lieshout. Physica 24 (1958) S.B.Burson, H.A.Grench, L.C.Schmid. Phys. Rev. 115 (1959) R.C.Greenwood, E.Brannen. Phys. Rev. 122 (1961) 1849 (Gamma ray emission intensities) - R.C.Catura. Nucl. Instrum. Methods 32 (1965) H.E.Bosch, M.C.Simon, E.Szichman, L.Gatto, S.M.Abecasis. Phys. Rev. 159 (1967) H.Okamura, M.Ogawa, A.Mito. J. Inorg. Nucl. Chem. 29 (1967) B.Fogelberg, A.Bäcklin. Institute of Physics, University of Uppsala and Swedish Research Councils Laboratory Studsvik NP (1968) - E.Der Mateosian, M.Goldhaber. Phys. Rev. 186 (1969) H.van den Berg, M.McDonnell, M.K.Ramaswamy. Can. J. Phys. 47 (1969) E.Der Mateosian, M.Goldhaber. Phys. Rev. C2 (1970) I.W.Goodier, F.H.Hughes, M.J.Woods. Int. J. Appl. Radiat. Isotop. 21 (1970) J.Legrand, F.Lagoutine, J.P.Brethon. Int. J. Appl. Radiat. Isotop. 21 (1970) M.K.Ramaswamy. Phys. Rev. C1 (1970) R.J.Rousselin, Cl.Gauthier. Int. J. Appl. Radiat. Isotop. 21 (1970) J.M.Oottukulam, M.K.Ramaswamy. J. Am. Phys. 39 (1971) H.H.Hansen, E.De Roost, D.Mouchel, R.Vaninbroukx. Int. J. Appl. Radiat. Isotop. 22 (1971) 1 - F.Lagoutine, J.Legrand, C.Perrot, J.P.Brethon, J.Morel. Int. J. Appl. Radiat. Isotop. 23 (1972) J.F.Emery, S.A.Reynolds, E.I.Wyatt, G.I.Gleason. Nucl. Sci. Eng. 48 (1972) M.Ramaswamy. Conf. Vanderbilt Vol. 2 (1972) H.Inoue, Y.Yoshizawa, T.Morii. J. Phys. Soc. Jap. 34 (1973) S.Raman, N.B.Gove. Phys. Rev. C7 (1973) 1995 (lg ft) - H.J.Kim, R.L.Robinson. Phys. Rev. C9 (1974) 767 INEEL / R.G. Helmer 4 14/07/ /10/2017
5 - B.Bulow, M.Eriksson, G.G.Jonsson, Hagebo. Z Physik A275 (1975) V.Z.Kuttemperoor, R.A.Kobiske. Int. J. Appl. Radiat. Isotop. 26 (1975) A.A.Delucchi, R.A.Meyer. J. Inorg. Nucl. Chem. 38 (1976) 2135 (Gamma ray energies and emission probabilities) - W.Dietrich, A.Bäcklin. Z. Physik A276 (1976) F.Rösel, H.M.Fries, K.Alder, H.C.Pauli. At. Data. Nucl. Data Tables 21 (1978) 92 (Theoretical Internal Conversion Coefficients) - K.Heyde, M.Waroquier, R.A.Meyer. Phys. Rev. C17 (1978) 1219 (Gamma ray energies and emission probabilities) - H.Houtermans, O.Milosevic, F.Reichel. Int. J. Appl. Radiat. Isotop. 31 (1980) A.R.Rutledge, L.V.Smith, J.S.Merritt. NBS-SP-626 (1982) 5 - D.D.Hoppes, J.M.R.Hutchinson, F.J.Schima, M.P.Unterweger. NBS-SP-626 (1982) 85 - Y.Iwata, I.Yamamoto, Y.Yoshizawa. Int. J. Appl. Radiat. Isotop. 35 (1984) Zs.Nemeth, L.Lakosi, I.Pavlicsek, A.Veres. Int. J. Appl. Radiat. Isotop. 38 (1987) 63 - J.Blachot. Nucl. Data Sheets 59 (1990) 729 (Spin, multipolarities) - M.P.Unterweger, D.D.Hoppes, F.J.Schima. Nucl. Instrum. Methods A312 (1992) A.Mukherjee, S.Bhattacharya, B.Dasmahapatra. Appl. Rad. Isotopes 44 (1993) 731 (Gamma-ray emission intensities) - K.Debertin. Private Communication (1994) (Gamma-ray emission intensities) - G.Audi, A.H.Wapstra. Nucl. Phys. A595 (1995) 409 (Q) - X.Wen, K.Shizuma, S.Hamanaka, K.Iwatani, H.Hasai. Nucl. Instrum. Methods A397 (1997) R.G.Helmer, C.Van der Leun. Nucl. Instrum. Methods A450 (2000) 35 (Gamma ray energies) INEEL / R.G. Helmer 5 14/07/ /10/2017
6 LNE-LNHB/CEA - Table de Radionucléides Sn γ Emission intensities per 100 disintegrations 0 ε Sn /2 ; 0 115,09 (3) d 0,33 ns ,000 0,000 1/2,3/2 ; 1029,73 0, ,11 0, /2- ; 646,833 2,21 1,6579 h 1 6 4,97-1/2 ; 391,699 97,79 Stable 0 In Q = 1036 kev % ε = 100 9/2 ; 0 INEEL / R.G. Helmer Scheme page : 1/1 14/07/ /02/2004
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 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 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 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- 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
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 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. 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 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 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Co decays 100% by electron capture to the excited levels of 706.42 kev (0.183%) and 136.47 kev (99.80%) in Fe. Le cobalt se désintègre par capture électronique vers des niveaux excités du
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Eu- disintegrates 100 % via beta minus disintegration to excited levels and to the ground state in Gd-. L europium se désintègre par émission bêta moins vers des niveaux excités et le niveau
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 β + Transitions. 2.2 Electron Capture Transitions
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
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 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. 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 α Transitions
1 Decay Scheme U- disintegrates by alpha emission mainly to the ground and 49- states in Th-232, and by 9,3 10 8 % spontaneous fission. L uranium se désintègre par émission alpha et par fission spontanée
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Pu- decays approximately 100 % by beta minus emission to the ground state of Am- and 0,00244 % by alpha emission to levels of U-237. The spontaneous fission decay branching is less than
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 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Pb- disintegrates by electron capture to Tl- via excited levels. Le plomb se désintègre par capture électronique vers des niveaux excités du thallium. 2 Nuclear Data T 1/2 ( Pb ) : 51,929
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Am decays by emission of alpha particles to Np239, with a minute branch of 3.8 (7) 10 9 % by spontaneous fission. L américium se désintègre par émission alpha vers le neptunium 239. Un faible
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
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
1 Decay Scheme Cm decays 1% by alpha transitions to Pu38 and by spontaneous fission with branching fraction of 6.36 (14) E6 %. Le curium se désintègre à 1% par transition alpha vers le plutonium 38 et
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
1 Decay Scheme Cm- decays 100% by alpha transitions to Pu-240 and by spontaneous fission with branching fraction of 1.36 (1) E-4 %. Le curium se désintègre par émission alpha et par fission spontanée dans
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
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme L iode se désintègre par émission bêta moins vers les niveaux excités de xénon, incluant l isomère xénon m de 11,962 (20) jours de période. L état d équilibre idéal, c est à dire l activité
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
1 Decay Scheme Ba disintegrates by electron capture mainly to two Cs excited levels of 437 kev (85.4%) and of 383 kev (14.5%) with three very minor branches to the 160 kev, 81 kev excited levels and the
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.
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