1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
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- Γιάννης Μητσοτάκης
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1 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 (28.85 %). Branching of Pu- decay by spontaneous fission is 1.85 (5)E-7 %. Le plutonium se désintègre par émission alpha vers les niveaux fondamental (71,04 %) et excité de 43,5 (28,85 %). Le nombre de désintegrations par fission spontanée est de 1,85 (5)E-7 % 2 Nuclear Data T 1/2 ( Pu ) : 87,74 (3) a T 1/2 ( 234 U ) : 2,455 (6) 10 5 a Q α ( Pu ) : 5593,20 (19) 2.1 α Transitions Probability F 100 α 0, ,94 (20) 0, ,5 α 0, ,66 (20) 0, (7) 7,5 α 0, ,43 (20) 0, α 0, ,77 (20) 0, (16) 155 α 0, ,56 (20) 0, α 0,9 4666,48 (20) 0, (5) 53 α 0,8 4741,46 (20) 0, ,5 α 0,7 4743,93 (20) 0, (22) 3400 α 0,6 4783,29 (20) 0, α 0,5 4806,91 (20) 0, (16) 89 α 0,4 5096,16 (20) 0, (23) α 0,3 5297,13 (19) 0,00292 (4) 440 α 0,2 5449,85 (19) 0,104 (3) 102 α 0,1 5549,70 (19) 28,85 (6) 1,39 α 0,0 5593,20 (19) 71,04 (6) 1 KRI /V. Chechev 1 08/06/ /1/2010
2 2.2 Gamma Transitions and Internal Conversion Coefficients P γce Multipolarity α K α L α M α T 100 γ 8,6(U) 41,82 (11) 0, (14) [E2] 630 (13) 174 (4) 863 (18) γ 1,0(U) 43,498 (1) 28,3 (8) E2 520 (11) 143,5 (29) 713 (15) γ 11,9(U) 62,70 (1) 0, (4) E1 0,320 (7) 0,0791 (16) 0,426 (9) γ 2,1(U) 99,852 (3) 0,1060 (23) E2 9,77 (20) 2,71 (6) 13,42 (27) γ 11,7(U) 140,15 (2) 0, (7) M1 63% E2 2,6 (8) 1,79 (5) 0,48 (14) 5,1 (15) γ 3,2(U) 152,719 (2) 0,00292 (4) E2 0,217 (4) 1,404 (28) 0,388 (8) 2,14 (4) γ 13,8(U) 192,91 (7) 0, (4) [E2] 0,1635 (33) 0,505 (10) 0,1391 (28) 0,856 (17) γ 4,3(U) 200,97 (3) 0, (23) E2 0,1534 (31) 0,424 (9) 0,1166 (23) 0,734 (15) γ 11,5(U) 203,12 (3) 0, (5) M1 66% E2 0,90 (17) 0,423 (9) 0,1113 (23) 1,5 (3) γ 14,8(U) 233,6 (2) 0, (E0 E2) γ 13,6(U) 234,6 (2) 0, E0 γ 14,7(U) 235,9 (3) 0, (5) [E1] 0,0532 (11) 0,01067 (21) 0,00258 (5) 0,0673 (14) γ 13,5(U) 258,227 (3) 0, (12) (E1) 0,0434 (9) 0,00859 (17) 0,00207 (4) 0,0548 (11) γ 14,5(U) 299,1 (2) 0, (3) [E1] 0,0314 (6) 0,00608 (12) 0, (29) 0,0395 (8) γ 7,2(U) 705,9 (1) 0, (13) [E1] 0,00568 (12) 0, (20) 0, (5) 0,00698 (14) γ 8,2(U) 708,3 (2) 0, (3) [E2] 0,01537 (31) 0,00489 (10) 0, (25) 0,0219 (5) γ 12,3(U) 727,8 (2) 0, (3) (E2) 0,01464 (29) 0,00454 (9) 0, (23) 0,0207 (4) γ 5,1(U) 742,813 (5) 0, (13) E1 0,00518 (10) 0, (18) 0, (4) 0,00636 (13) γ 6,1(U) 766,38 (2) 0, (5) E2 0,01336 (27) 0,00396 (8) 0, (20) 0,0187 (4) γ 9,2(U) 783,4 (1) 0, (3) [E2] 0,01285 (26) 0,00374 (8) 0, (19) 0,0179 (4) γ 5,0(U) 786,27 (3) 0, (9) E1 0,00467 (9) 0, (16) 0, (4) 0,00573 (12) γ 10,2(U) 804,4 (3) 0, E0 E2 0,57 γ 7,1(U) 805,80 (5) 0, (15) [E1] 0,00447 (9) 0, (16) 0, (4) 0,00549 (11) γ 8,1(U) 808,2 (1) 0, E0 17% E2 3,31 0,94 4,3 γ 6,0(U) 810,0 (5) 0, E0 60 γ 8,0(U) 851,7 (1) 0, (4) [E2] 0,01109 (22) 0,00302 (6) 0, (16) 0,01513 (30) γ 12,2(U) 880,5 (1) 0, (E0 E2) γ 9,1(U) 883,24 (4) 0, (4) E2 0,01040 (21) 0,00276 (6) 0, (14) 0,01409 (28) γ 10,1(U) 904,37 (15) 0, (11) [E2] 0,00998 (20) 0,00260 (5) 0, (13) 0,01346 (27) γ 9,0(U) 926,72 (1) 0, (25) (E2) 0,00956 (20) 0,00245 (5) 0, (12) 0,01284 (26) γ 14,2(U) 941,94 (10) 0, (23) [E2] 0,00929 (20) 0,00236 (5) 0, (12) 0,01244 (25) γ 11,1(U) 946,00 (3) 0, (13) (E1) 0,00337 (7) 0, (12) 0, (27) 0,00412 (8) γ 12,1(U) 980,3 (1) 0, (E2) 0,00866 (18) 0,00214 (4) 0, (11) 0,01152 (23) γ 13,1(U) 1001,03 (3) 0, (4) E2 0,00835 (17) 0,00204 (4) 0, (11) 0,01107 (22) γ 14,1(U) 1041,7 (2) 0, (E0 E2) γ 14,0(U) 1085,4 (2) 0, (9) (E2) 0,00725 (15) 0,00169 (3) 0, (8) 0,00950 (19) 3 Atomic Data 3.1 ω K : 0,970 (4) ω L : 0,500 (19) n KL : 0,794 (5) KRI /V. Chechev 2 08/06/ /1/2010
3 3.1.1 X Radiations Relative probability K Kα 2 94,666 62,47 Kα 1 98, Kβ 3 110,421 } Kβ 1 111,298 } Kβ 5 111,964 } 36,08 Kβ 2 114,407 } Kβ 4 115,012 } 12,34 KO 2,3 115,377 } L Ll 11,619 Lα 13,438 13,615 Lη 15,399 Lβ 15,727 18,206 Lγ 19,507 20, Auger Electrons Relative probability Auger K KLL 71,78 80, KLX 88,15 98,43 59,6 KXY 104,51 115,59 8,88 Auger L 5,9 21,6 4 α Emissions Probability 100 α 0, ,1 (2) 0, α 0, ,1 (2) 0, (7) α 0, ,5 (2) 0, KRI /V. Chechev 3 08/06/ /1/2010
4 Probability 100 α 0, ,3 (2) 0, (16) α 0, ,4 (2) 0, α 0,9 4587,9 (2) 0, (5) α 0,8 4661,7 (2) 0, α 0,7 4664,1 (2) 0, (22) α 0,6 4702,8 (2) 0,0001 α 0,5 4726,0 (2) 0, (16) α 0,4 5010,4 (2) 0, (23) α 0,3 5208,0 (2) 0,00292 (4) α 0,2 5358,1 (2) 0,104 (3) α 0,1 5456,3 (2) 28,85 (6) α 0,0 5499,03 (20) 71,04 (6) 5 Electron Emissions Electrons per 100 disint. e AL (U) 5,9-21,6 10,6 (4) e AK (U) 0, (15) KLL 71,78-80,95 } KLX 88,15-98,43 } KXY 104,51-115,59 } ec 1,0 L (U) 21,74-26,33 20,6 (6) ec 1,0 M (U) 37,95-39,95 5,7 (12) ec 1,0 N (U) 42,057-43,119 1,544 (39) ec 2,1 L (U) 78,095-82,685 0,0718 (17) 6 Photon Emissions 6.1 X-Ray Emissions Photons per 100 disint. XL (U) 11,619 20,714 10,63 (8) KRI /V. Chechev 4 08/06/ /1/2010
5 Photons per 100 disint. XKα 2 (U) 94,666 0, (3) } Kα XKα 1 (U) 98,440 0, (5) } XKβ 3 (U) 110,421 } XKβ 1 (U) 111,298 } 0, (22) K β 1 XKβ 5 (U) 111,964 } XKβ 2 (U) 114,407 } XKβ 4 (U) 115,012 } 0, (6) K β 2 XKO 2,3 (U) 115,377 } 6.2 Gamma Emissions Photons per 100 disint. γ 8,6 (U) 41,82 (11) 0, (16) γ 1,0 (U) 43,498 (1) 0,0397 (8) γ 11,9 (U) 62,70 (1) 0, (3) γ 2,1 (U) 99,852 (3) 0,00735 (8) γ 11,7 (U) 140,15 (2) 0, (7) γ 3,2 (U) 152,719 (2) 0, (7) γ 13,8 (U) 192,91 (7) 0, (20) γ 4,3 (U) 200,97 (3) 0, (13) γ 11,5 (U) 203,12 (3) 0, (15) γ 14,7 (U) 235,9 (3) 0, (5) γ 13,5 (U) 258,227 (3) 0, (11) γ 14,5 (U) 299,1 (2) 0, (3) γ 7,2 (U) 705,9 (1) 0, (13) γ 8,2 (U) 708,3 (2) 0, (3) γ 12,3 (U) 727,8 (2) 0, (3) γ 5,1 (U) 742,813 (5) 0, (13) γ 6,1 (U) 766,38 (2) 0, (5) γ 9,2 (U) 783,4 (1) 0, (3) γ 5,0 (U) 786,27 (3) 0, (9) γ 10,2 (U) 804,4 (3) 0, (5) γ 7,1 (U) 805,80 (5) 0, (15) γ 8,1 (U) 808,2 (1) 0, (25) γ 8,0 (U) 851,7 (1) 0, (4) γ 12,2 (U) 880,5 (1) 0, (4) γ 9,1 (U) 883,24 (4) 0, (4) γ 10,1 (U) 904,37 (15) 0, (11) γ 9,0 (U) 926,72 (1) 0, (25) γ 14,2 (U) 941,94 (10) 0, (23) γ 11,1 (U) 946,00 (3) 0, (13) KRI /V. Chechev 5 08/06/ /1/2010
6 Photons per 100 disint. γ 12,1 (U) 980,3 (1) 0, γ 13,1 (U) 1001,03 (3) 0, (4) γ 14,1 (U) 1041,7 (2) 0, (16) γ 14,0 (U) 1085,4 (2) 0, (9) 7 Main Production Modes Np 237(n,γ)Np Np (β )Pu Cm 242(α)Pu 8 References - A. H. Jaffey, A. Hirsch. Report ANL-4286 (1949) - A. H. Jaffey, J. Lerner. Report ANL-4411 (1950) - A. H. Jaffey, L. B. Magnusson. Paper No National Nuclear Plutonium Project Record Div. IV. 14B (1951) - A. H. Jaffey. Ibid. Paper No (1951) - G. T. Seaborg, R. A. James and A. Giorso. The Transuranium Elements Paper No National Nuclear Series, Plutonium Project Record, Div. IV. 14B.Part II (1951) p E. Segre. Phys. Rev. 86 (1952) 21 - K. W. Jones, R.A. Douglas, M.T. McEllistrem and H.T. Richards. Phys. Rev. 94 (1954) F. Asaro, I. Perlman. Phys. Rev. 94 (1954) E. L. Church, A. W. Sunyar. Phys. Rev. 98 (1955) 1186A (Gamma-ray energies) - J. O. Newton, B. Rose and J. Milsted. Phil. Mag. 1 (1956) 981 (Gamma-ray energies) - D. C. Hoffman, G. P. Ford and F. O. Lawrence. J. Inorg. Nucl. Chem. 5 (1957) 6 - L. N. Kondratev, G. I. Novikova, V. B. Dedov and L. L. Goldin. Izv. Akad. Nauk SSSR, Ser Fiz 21 (1957) V. A. Druin, V. P. Perelygin and G. I. Khlebnikov. Soviet Phys. JETP 13 (1961) C. F. Leang. Compt. Rend. 255 (1962) 3155 KRI /V. Chechev 6 08/06/ /1/2010
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10 LNE-LNHB/CEA - Table de Radionucléides 0,76 ns 1,38 ps γ Emission intensities per 100 disintegrations ,000 0,000 0,000 0,000 0, ,000 0,000 0, ,00 0,00 0, ,00 0,00 0,00 0, ,00 0, ,00 0,00 0, ; 1085,26 0 ; 1044,536 4 ; 1023,77-2 ; 989,43 4 ; 947,64 2 ; 926,72 0 α 0, , , , , , Pu ; 0 Pu ,74 (3) a 1,74 ps ; 851, ; 849,266 0 ; 809,907-1 ; 786,288 0, , ,0001 0, , ; 296,072 0, ; 143,352 0,252 ns 2,455 (6) x10^5 a U α Q = 5593,2 % α = ; 43,4981 KRI / V.P. Chechev Scheme page : 1/2 08/06/ /06/ ; 0 28,85 71,04
11 LNE-LNHB/CEA - Table de Radionucléides Pu γ Emission intensities per 100 disintegrations 0 α Pu ; 0 87,74 (3) a 1,74 ps ,00 0,00 0,00 0,00 0,00 0, , ,00 0,00 2 ; 851, ; 849,266 0 ; 809,907-1 ; 786,288 0, , ,0001 0, , ; 497,04 0, , ; 296,072 0, , ; 143,352 0,104 0,252 ns 1 2,455 (6) x10^5 a 0 0, U α Q = 5593,2 % α = ; 43, ; 0 28,85 71,04 KRI / V.P. Chechev Scheme page : 2/2 08/06/ /06/2009
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 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 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 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 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. 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 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 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 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 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 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 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
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 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 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 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 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 β + Transitions. 2.2 Electron Capture Transitions
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