1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
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1 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 du bismuth. 2 Nuclear Data T 1/2 ( Pb ) : 26,916 (44) min T 1/2 ( Bi ) : 19,8 (1) min Q ( Pb ) : 1019 (11) 2.1 β Transitions Probability Nature lg f t 100 β0,9 180 (11) 2,762 (22) Allowed 4,5 β0,8 222 (11) 0,0196 (27) Allowed 6,9 β0,7 485 (11) 1,047 (17) 1st Forbidden 6,2 β0,5 667 (11) 46,52 (37) 1st Forbidden 5,1 β0,4 729 (11) 41,09 (39) 1st Forbidden 5,2 β0, (11) 9,2 (7) 1st Forbidden 6,3 2.2 Gamma Transitions and Internal Conversion Coefficients P γ+ce Multipolarity α K α L α M α T 100 γ 1,0(Bi) 53,2275 (21) 14,71 (42) M1 + E2 9,80 (29) 2,32 (7) 12,88 (39) γ ( 1,0) (Bi) 107,22 (9) 0,0068 (14) γ ( 1,1) (Bi) 137,45 (30) 0,045 (18) γ ( 1,2) (Bi) 141,3 (6) 0,027 (14) LNE LNHB /V. Chisté, M.M. Bé 1 23/02/ /12/2010
2 P γ+ce Multipolarity α K α L α M α T 100 γ ( 1,3) (Bi) 170,07 (6) 0,0146 (27) γ 3,2(Bi) 196,17 (10) 0,069 (9) γ 3,1(Bi) 205,642 (30) 0,0114 (23) γ ( 1,4) (Bi) 216,47 (7) 0,0100 (23) γ 4,1(Bi) 241,997 (3) 13,72 (20) M1(+E2) 0,724 (22) 0,1250 (38) 0,0295 (9) 0,888 (27) γ 3,0(Bi) 258,87 (3) 0,924 (13) M1 0,601 (18) 0,1037 (31) 0,0244 (7) 0,737 (22) γ 7,3(Bi) 274,80 (5) 0,504 (15) M1 + E2 0,295 (9) 0,0731 (22) 0,0179 (5) 0,392 (12) γ 4,0(Bi) 295,224 (2) 27,29 (26) M1 + E2 0,390 (12) 0,0698 (21) 0,0165 (5) 0,482 (14) γ 9,7(Bi) 305,26 (3) 0,0324 (22) [E1] 0,0241 (7) 0,00413 (12) 0, (29) 0,0295 (9) γ 6,2(Bi) 314,32 (7) 0,077 (6) γ 6,1(Bi) 323,83 (4) 0,0287 (32) γ 5,0(Bi) 351,932 (2) 46,96 (37) M1(+ E2) 0,260 (8) 0,0445 (13) 0,01049 (31) 0,319 (10) γ 9,6(Bi) 462,00 (7) 0,213 (6) γ 7,1(Bi) 480,43 (2) 0,3838 (49) M1(+E2) 0,1132 (34) 0,0192 (6) 0,00452 (14) 0,1384 (42) γ 9,5(Bi) 487,09 (7) 0,438 (6) (E1) 0,00871 (26) 0, (43) 0, (10) 0,01058 (32) γ 7,0(Bi) 533,66 (2) 0,192 (10) [M1,E2] 0,05 (3) 0,010 (4) 0,0023 (9) 0,06 (4) γ 8,3(Bi) 538,41 (9) 0,0196 (27) γ 9,4(Bi) 543,81 (7) 0,050 (9) E1 + M2 0,00696 (21) 0, (34) 0, (8) 0,00843 (25) γ 9,3(Bi) 580,13 (3) 0,372 (6) (E1) 0,00611 (18) 0, (29) 0, (7) 0,00740 (22) γ ( 1,5) (Bi) 765,96 (9) 0,053 (8) γ 9,1(Bi) 785,96 (9) 1,068 (13) E1 0,00341 (10) 0, (16) 0, (37) 0,00410 (12) γ 9,0(Bi) 839,00 (4) 0,589 (8) (E1) 0,00302 (9) 0, (14) 0, (33) 0,00363 (11) 3 Atomic Data 3.1 Bi ω K : 0,964 (4) ω L : 0,391 (16) ω M : 0,031 (3) n KL : 0,809 (5) n LM : 1, X Radiations Relative probability K Kα 2 74, ,77 Kα 1 77, Kβ 3 86,835 } Kβ 1 87,344 } Kβ 5 87,862 } 34,25 Kβ 2 89,732 } Kβ 4 90,074 } 10,48 KO 2,3 90,421 } LNE LNHB /V. Chisté, M.M. Bé 2 23/02/ /12/2010
3 Relative probability L Ll 9,42 Lα 10,45 10,55 Lη 11,35 Lβ 12,13 13,38 Lγ 14,31 16, Auger Electrons Relative probability Auger K KLL 57,49 63, KLX 70,02 77,10 56,2 KXY 82,45 90,52 9,2 Auger L 5,3 16,4 4 Electron Emissions Electrons per 100 disint. e AL (Bi) 5,3 16,4 19,8 (3) e AK (Bi) 0,80 (9) KLL 57,49 63,42 } KLX 70,02 77,10 } KXY 82,45 90,52 } ec 1,0 L (Bi) 36, , ,39 (31) ec 1,0 M (Bi) 49, ,6479 2,46 (8) ec 1,0 N (Bi) 52, ,0704 0,641 (20) ec 4,1 K (Bi) 151,471 (3) 5,26 (16) ec 3,0 K (Bi) 168,34 (3) 0,32 (1) ec 4,0 K (Bi) 204,698 (2) 7,22 (23) ec 4,1 L (Bi) 225, ,578 0,908 (28) ec 4,1 M (Bi) 237, ,417 0, (7) ec 4,1 N (Bi) 241, ,840 0,0560 (17) ec 3,0 L (Bi) 242,48 245,45 0,0551 (17) ec 5,0 K (Bi) 261,406 (2) 9,26 (29) ec 4,0 L (Bi) 278, ,805 1,291 (40) ec 4,0 M (Bi) 291, ,644 0,305 (10) LNE LNHB /V. Chisté, M.M. Bé 3 23/02/ /12/2010
4 Electrons per 100 disint. ec 4,0 N (Bi) 294, ,067 0,0797 (25) ec 5,0 L (Bi) 335, ,513 1,584 (46) ec 5,0 M (Bi) 347, ,352 0,373 (11) ec 5,0 N (Bi) 350, ,775 0,0975 (29) β0,9 max: 180 (11) 2,762 (22) β0,9 avg: 50 (3) β0,8 max: 222 (11) 0,0196 (27) β0,8 avg: 62 (3) β0,7 max: 485 (11) 1,047 (17) β0,7 avg: 145 (4) β0,5 max: 667 (11) 46,52 (37) β0,5 avg: 207 (4) β0,4 max: 724 (11) 41,09 (39) β0,4 avg: 227 (4) β0,0 max: 1019 (11) 9,2 (7) β0,0 avg: 337 (4) 5 Photon Emissions 5.1 XRay Emissions Photons per 100 disint. XL (Bi) 9,42 16,36 12,42 (22) XKα 2 (Bi) 74,8157 6,26 (12) } Kα XKα 1 (Bi) 77, ,47 (20) } XKβ 3 (Bi) 86,835 } XKβ 1 (Bi) 87,344 } 3,59 (9) K β 1 XKβ 5 (Bi) 87,862 } XKβ 2 (Bi) 89,732 } XKβ 4 (Bi) 90,074 } 1,10 (4) K β 2 XKO 2,3 (Bi) 90,421 } LNE LNHB /V. Chisté, M.M. Bé 4 23/02/ /12/2010
5 5.2 Gamma Emissions Photons per 100 disint. γ 1,0 (Bi) 53,2275 (21) 1,060 (7) γ ( 1,0) (Bi) 107,22 (9) 0,0068 (14) γ ( 1,1) (Bi) 137,45 (30) 0,045 (18) γ ( 1,2) (Bi) 141,3 (6) 0,027 (14) γ ( 1,3) (Bi) 170,07 (6) 0,0146 (27) γ 3,2 (Bi) 196,20 (5) 0,069 (9) γ 3,1 (Bi) 205,68 (9) 0,0114 (23) γ ( 1,4) (Bi) 216,47 (7) 0,0100 (23) γ 4,1 (Bi) 241,997 (3) 7,268 (22) γ 3,0 (Bi) 258,87 (3) 0,5318 (36) γ 7,3 (Bi) 274,80 (5) 0,362 (10) γ 4,0 (Bi) 295,224 (2) 18,414 (36) γ 9,7 (Bi) 305,26 (3) 0,0315 (21) γ 6,2 (Bi) 314,32 (7) 0,077 (6) γ 6,1 (Bi) 323,83 (4) 0,0287 (32) γ 5,0 (Bi) 351,932 (2) 35,60 (7) γ 9,6 (Bi) 462,00 (7) 0,213 (6) γ 7,1 (Bi) 480,43 (2) 0,3371 (41) γ 9,5 (Bi) 487,09 (7) 0,433 (6) γ 7,0 (Bi) 533,66 (2) 0,182 (6) γ 8,3 (Bi) 538,41 (8) 0,0196 (27) γ 9,4 (Bi) 543,81 (7) 0,050 (9) γ 9,3 (Bi) 580,13 (3) 0,369 (6) γ ( 1,5) (Bi) 765,96 (9) 0,053 (8) γ 9,1 (Bi) 785,96 (9) 1,064 (13) γ 9,0 (Bi) 839,04 (9) 0,587 (8) 6 Main Production Modes { Ra 226 decay chain Possible impurities : Pb References M. Curie, A. Debierne, A.S. Eve, H. Geiger, O. Hahn, S.C. Lind, S. Meyer, E. Rutherford, E. Schweidler. Rev. Mod. Phys. 3 (1931) 427 (Halflife.) E.E. Berlovich. Bull. Acad. Sci. USSR, Phys. Ser. 16 (1952) 314 (Beta emission intensity.) K. Sageyama. J. Phys. Soc. (Japan) 8 (1953) 689 (Beta emission intensity.) H. Daniel, R. Nierhaus. Z. Naturforsch. 11a (1956) 212 (Halflife.) LNE LNHB /V. Chisté, M.M. Bé 5 23/02/ /12/2010
6 K.O. Nielsen, O.B. Nielsen, M.A. Waggoner. Nucl. Phys. 2 (1957) 476 (Beta emission intensity.) H. Daniel. Z. Naturforsch. 11a (1958) 759 (Beta emission intensity.) G.T. Ewan, J. Tavendale. Can. J. Phys. 42 (1964) 2286 E.W.A. Lingeman, J. Konijn, P. Polak, A.H. Wapstra. Nucl. Phys. A133 (1969) 630 G. Wallace, G.E. Coote. Nucl. Instrum. Methods 74 (1969) 353 R.S. Mowatt. Can. J. Phys. 48 (1970) 2606 (Gammaray emission probabilities.) K.Ya. Gromov, B.M. Sabirov, J.J. Urbanets. Bull. Acad. Sci. USSR, Phys. Ser. 33 (1970) 1510 A. Hachem. Comp. Rend. Acad. Sci. (Paris) 281B (1975) 45 V. Zobel, J. Eberth, E. Eube. Nucl. Instrum. Methods 141 (1977) 329 F. Rösel. At. Data. Nucl. Data Tables 21 (1978) 91 (Theoretical ICC.) G. Mouze. Comp. Rend. Acad. Sci. (Paris) 292 (1981) 1243 H. Akcay, G. Mouze, D. Maillard, Ch. Ythier. Radiochem. Radioanal. Lett. 51 (1982) 1 M.A. Farouk, A.M. AlSoraya. Nucl. Instrum. Methods 200 (1982) 593 D.G. Olson. Nucl. Instrum. Methods 206 (1983) 313 U. Schötzig, K. Debertin. Int. J. Appl. Radiat. Isotop. 34 (1983) 533 I. Penev, W. Andrejtscheff, Ch. Protochristow, Zh. Zelev. Z. Physik A318 (1984) 213 (Halflife (E=53 ).) Y.A. Akovali. Nucl. Data Sheets 55 (1988) 665 ( level, spin, parity, multipolariy.) G. Mouze, J.F. Comanducci, C. Ythier. Rev. Roumaine Phys. 35 (1990) 337 G. Mouze, O. Diallo, P. Bechlich, J.F. Comanducci, C. Ythier. Radiochim. Acta 49 (1990) 13 W.J.Lin, G.Harbottle. J. Radioanal. Nucl. Chem. Lett. 153 (1991) 137 D. E. Martz, G. H. Langner Jr., P. R. Johnson. Health Phys. 61 (1991) 511 (Halflife.) O. Diallo, G. Mouze, C. Ythier, J.F. Comanducci. Nuovo Cim. 106A (1993) 1321 Y.A. Akovali. Nucl. Data Sheets 76 (1995) 127 ( level, spin, parity, multipolariy.) E. Schönfeld, H. Janssen. Nucl. Instrum. Meth. Phys. Res. A369 (1996) 527 (Atomic data.) J. Morel, M. Etcheverry, J.L. Picolo. Appl. Rad. Isotopes 49 (1998) 1387 D. Sardari, T.D. MacMahon. J. Radioanal. Nucl. Chem. 244 (2000) 463 J.U. Delgado, J. Morel, M. Etcheverry. Appl. Rad. Isotopes 56 (2002) 137 G.L. Molnar, Z.S. Révay, T. Belgya. 11th Int. Symp. On capture gammaray spectroscopy, 26 sep. 2002, Pruhonice (2002) 522 I.M. Band, M.B. Trzhaskovskaya, C.W. Nestor, Jr., P.O. Tikkanen, S. Raman. At. Data. Nucl. Data Tables 81 (2002) 1 (Theoretical ICC.) LNE LNHB /V. Chisté, M.M. Bé 6 23/02/ /12/2010
7 G. Audi, A.H. Wapstra, C. Thibault. Nucl. Phys. A729 (2003) 129 (Q.) R.G.Helmer. IAEA CRP To be published (2003) J. Morel, S. Speman, M. Rasko, E. Terechtchenko, J.U. Delgado. Appl. Rad. Isotopes 60 (2004) 341 M. Voltaggio, M. Spadoni. Appl. Rad. Isotopes To be published (2011) (Halflife.) LNE LNHB /V. Chisté, M.M. Bé 7 23/02/ /12/2010
8 LNELNHB/CEA Table de Radionucléides Pb Pb ; 0 β 26,916 (44) min γ Emission intensities per 100 disintegrations 2,762 0, ,031 0,213 0,433 0,05 0,369 1,064 0,587 0, ; ,24 1, ,36 0,33 0,18 (1) ; 533,67 46,52 41, ,07 0,02 3 5, ,26 1 8, ,06 0,01 0,53 377,03 (0,1) ; 351,932 1 ; 295,224 (2) ; 258,87 9, Bi Q = 1019 % β = 100 1,06 62,7 (2) ; 53, ; 0 0,52 ns 19,8 (1) min LNE LNHB / V. Chisté, M.M. Bé Scheme page : 1/1 23/02/ /11/2010
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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
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1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
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