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 Be disintegrates by electron capture either directly to the ground state of Li (89.56%) or via the 4 kev of Li (10.44%). Recent experiments have shown that the halflife of Be increases as much as 0.% by embedding this radionuclide in different matrices. The recommended value presented in this evaluation should be adequate for Be and BeO sample. Le Be se désintègre par capture électronique soit directement vers le niveau fondamental de Li, soit via le niveau excité de 4 kev. Des expériences récentes ont montré que la valeur de la période pouvait être affectée jusqu à 0,% par une modification de l environnement extérieur, par exemple la composition chimique. La valeur retenue pour cette évaluation s applique plutôt à des échantillons de Be ou BeO. 2 Nuclear Data T 1/2 ( Be ) : 53,22 (6) d Q + ( Be ) : 861,815 (18) kev 2.1 Electron Capture Transitions Energy Probability Nature lg ft P K P L kev 100 ɛ 0,1 384,194 (18) 10,44 (4) Allowed 3,56 0,908 (12) 0,092 (12) ɛ 0,0 861,815 (18) 89,56 (4) Allowed 3,32 0,908 (12) 0,092 (12) 2.2 Gamma Transitions and Internal Conversion Coefficients Energy P γ+ce Multipolarity α T kev 100 γ 1,0(Li) 4,621 (2) 10,44 (4) M1+4%E2 0, (11) INEEL, PTB /R. G. Helmer, E. Schönfeld 1 03/12/9 12/2/2004
2 3 Atomic Data 3.1 Li ω K : 0,00029 (15) X Radiations Energy kev Relative probability X K Kα 0, Photon Emissions 4.1 Gamma Emissions Energy kev Photons per 100 disint. γ 1,0 (Li) 4,6035 (20) 10,44 (4) 5 Main Production Modes Li 6(d,n)Be Possible impurities : Li B 10(p,α)Be Possible impurities : C 9,C 11 C 12(He 3,2α)Be Possible impurities : C 11,N 13 INEEL, PTB /R. G. Helmer, E. Schönfeld 2 03/12/9 12/2/2004
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4 F.AjzenbergSelove. Nucl. Phys. A490 (1988) 1 (Levels, Elec. Capt. Probabilities) G.Audi, A.H.Wapstra. Nucl. Phys. A565 (1993) 1 (Q) T.Chang, S.Wang, H.Wang. Nucl. Instr. Meth. A325 (1993) 196 J.H.Hubbell, P.N.Trehan, Nirmal Singh, B.Chand, D.Mehta, M.L.Garg, R.R.Garg, Surinder Singh, S.Puri. J.Phys.Chem.Ref.Data 23 (1994) 339 (L fluorescence yield) C.A. Huh, L.G.Liu. J. Radioanal. Nucl. Chem. 246 (2000) 229 R.G.Helmer, C.van der Leun. Nucl. Instr. Meth. A450 (2000) 35 L.G.Liu, C.A. Huh. Earth and Planetary Science Letters 180 (2000) 163 INEEL, PTB /R. G. Helmer, E. Schönfeld 4 03/12/9 12/2/2004
5 BNM LNHB/CEA Table de Radionucléides Be 4 3 γ Emission probabilities per 100 disintegrations 0 ε Be 4 3 3/2 ; 0 53,22 (6) d 105 fs ,4 1/2 ; 4,621 10,44 Stable 0 3/2 ; 0 Li Q = 861,815 kev % ε = ,56 INEEL, PTB \ R. G. Helmer, E. Schönfeld Page number : 1/1 03/12/9 26/03/01
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