241PU    241NP B- DECAY                1981PA20                  15NDS    201512
241PU  H TYP=FUL$AUT=C.D. NESARAJA$CIT=NDS 130, 183 (2015)$CUT=30-Sep-2015$
241PU c  1981Pa20: {+241}Np produced via {+238}U(|a,p) with E|a=32 MeV and
241PU2c  {+244}Pu(n,p3n) with En=30-160 MeV at the Brookhaven MEIN facility.
241PU3c  Irradiation were followed by chemical separation. Decay of
241PU4c  {+241}Np was studied by |g spectroscopy using a high resolution
241PU5c  Ge(Li) detector and by |b emission by a 4|p proportional counter.
241PU6c  Measured E|g, absolute I|g, and  T{-1/2}.
241PU c  1966Qa02: {+241}Np produced via {+238}U(|a,p) at Nuffield Cyclotron at
241PU2c  Birmingham University with E|a= 40 MeV. Irradiation was followed by
241PU3c  chemical separation. A Geiger counter, anthrracene crystal
241PU4c  scintillation |b spectrometer, Xe proportional counter, NaI(Tl)
241PU5c  detector, and a ZnS-Ag scintillation |a counter were used to measure
241PU6c  |g and |b radiations. The half life from decay curves for {+241}Np
241PU7c  was 16.0 min {I2} with an end-point energy of 1.25 MeV. The 3.4 hour
241PU8c  activity was not detected.
241PU c  1959Va32: {+241}Np produced via {+238}U(|a,p) at Argonne cyclotron
241PU2c  followed by chemical separation and measured with a 2|p and end window
241PU3c  proportional counters. |b and |g spectrum were measured with the
241PU4c  anthracene crystal and a NaI(Tl) detectors. The beta spectrum end
241PU5c  point energy of the 16 minute component was 1.36 MeV {I10} with
241PU6c  log{Ift} of 5.8.
241PU cB IB$From an intensity balance at each level
241PU cG E$From 1981Pa20. Others: 1966Qa02
241PU cG M,MR$From (n,|g) as given in adopted |g's
241PU cG RI(A)$From an intensity balance at the 96 level and
241PU2cG I|g(96|g)/I|g(54|g)=0.15 {I3} from (n,|g)
241PU cG E(B)$Rounded-off value from adopted |g's. Not seen in |b decay
241PU cG E(C),RI(C)$The authors report E|g=518.8 {I1} with I|g=0.44 {I3} for a
241PU2cG transition doubly placed from the 519 and 561 levels. From
241PU3cG I|g/I|g(477|g)=3.09 {I16} for the 519 level, and I|g/I|g(561|g)=1.45
241PU4cG {I13} for the 561 level, both from (n,|g), one gets I|g=0.31 {I3} and
241PU5cG 0.12 {I4} for these two placements, in agreement with the measured
241PU6cG value for the doublet. The energies are rounded-off values from (n,|g)
241PU DG CC$FROM BrIcc v2.3a (30-Jun-2013) 2008Ki07, "Frozen Orbitals" appr.
241PU CG MR$IF NO VALUE GIVEN IT WAS ASSUMED MR=1.00 FOR E2/M1,
241PU2CG MR=1.00 FOR E3/M2 AND MR=0.10 FOR THE OTHER MULTIPOLARITIES
241PU cL E$Rounded-off values from adopted levels, except for the 930
241PU2cL level, whose de excitation transition is seen only in |b decay
241PU cL J$From Adopted Levels
241NP  P 0.0          5/2+             13.9 M    2              1.30E+3   7
241NP cP J$From Adopted Levels in {+241}Np
241NP cP T$From least squares decay analyses of the 175 keV |g.
241NP cP QP$From 2012Wa38
241PU  N 1.0         1.0       1.0        1.0
241PU PN 1.0         1.0                 1.0                                 2
241PU cN NR$I|g(133|g)=0.86 {I5} per 100 disintegrations (4|p proportional
241PU2cN counter 1981Pa20)
241PU  L 0.0          5/2+
241PU  B 1.30E+3    7 70     4             5.87   9
241PUS B EAV=432 27
241PU cB E$From adopted Q(|b{+-}). Measured values are 1360 {I100} (1959Va32)
241PU2cB and 1250 (1966Qa02)
241PU  L 41.97        7/2+
241PU  B
241PU cB IB$The intensity balance gives I|b=-2 {I4}
241PU  G 42.0      1  0.10    3M1+E2     0.186   4     102.2  22
241PUS G  LC=76.0 16$MC=19.4 5
241PUS G  NC=5.29 12$OC=1.29 3$PC=0.231 5$QC=0.01087 17
241PU  L 95.78        9/2+
241PU  G 53.81       0.020   6 M1+E2     0.201   8     44.7   11               S
241PU2 G FLAG=AB$
241PUS G  LC=33.3 8$MC=8.42 21
241PUS G  NC=2.30 6$OC=0.563 14$PC=0.1021 22$QC=0.00519 8
241PU  G 95.79       0.003   1 E2                      19.3                    S
241PU2 G FLAG=AB$
241PUS G  LC=14.00 20$MC=3.92 6
241PUS G  NC=1.077 15$OC=0.254 4$PC=0.0404 6$QC=0.0001375 20
241PU  L 161.69       1/2+
241PU cL E$The feeding of this level has not been established. It cannot
241PU2cL be directly fed by a |b branch, and no transitions feeding the
241PU3cL level have been observed
241PU  G 161.6     2  0.07    1E2                      1.97
241PUS G  KC=0.190 3$LC=1.292 20$MC=0.360 6
241PUS G  NC=0.0991 15$OC=0.0234 4$PC=0.00379 6$QC=2.32E-5 4
241PU  L 175.05       7/2+
241PU  B              30.8   15            6.00  10
241PUS B EAV=366 27
241PU  G 79.26        0.040   4M1+E2     0.65    +25-2222     6                S
241PU2 G FLAG=B$
241PUS G  LC=16 4$MC=4.3 12
241PUS G  NC=1.2 4$OC=0.28 8$PC=0.047 11$QC=0.00129 22
241PU cG RI$From I|g/I|g(133|g+175|g)=0.010 {I1} in |a decay
241PU  G 133.1     1  0.86    5M1+E2     0.222   9     11.35  17
241PUS G  KC=8.79 13$LC=1.92 3$MC=0.472 7
241PUS G  NC=0.1287 19$OC=0.0319 5$PC=0.00599 9$QC=0.000366 6
241PU  G 175.1     1  3.1     2M1+E2     0.217   19    5.20
241PUS G  KC=4.07 7$LC=0.854 12$MC=0.209 3
241PUS G  NC=0.0569 8$OC=0.01413 20$PC=0.00267 4$QC=0.000167 3
241PU  L 404.45       (9/2)-
241PU cL J$See comment on J|p(404 level) in adopted levels
241PU  B              0.27   3             7
241PUS B EAV=282 26
241PU  G 308.8     2  0.07    2E1                      0.0388
241PUS G  KC=0.0307 5$LC=0.00610 9$MC=0.001477 21
241PUS G  NC=0.000399 6$OC=9.75E-5 14$PC=1.761E-5 25$QC=9.22E-7 13
241PU  G 362.4     1  0.19    2E1                      0.0276
241PUS G  KC=0.0220 3$LC=0.00425 6$MC=0.001028 15
241PUS G  NC=0.000278 4$OC=6.81E-5 10$PC=1.238E-5 18$QC=6.70E-7 10
241PU  G 405       AP                                                          ?
241PU cG E$Only a slight indication for its existence was found in the
241PU2cG |g spectrum. One expects E|g=404.453. This transition is not
241PU3cG seen in (n,|g). If one assumes that I|g is smaller than that for the
241PU3cG adjacent 404.707 and 405.90 |g's in (n,|g), one can estimate I|g<0.01
241PU  L 518.81       5/2-
241PU  B              0.42   4             7.32  15
241PUS B EAV=241 25
241PU  G 476.6     2  0.10    1E1+M2     0.104   +20-250.025  4
241PUS G  KC=0.020 3$LC=0.0042 8$MC=0.00104 20
241PUS G  NC=0.00028 6$OC=7.0E-5 14$PC=1.3E-5 3$QC=7.7E-7 16
241PU  G 518.81       0.31    3E1                      0.01340
241PU2 G FLAG=C$
241PUS G  KC=0.01078 15$LC=0.00198 3$MC=0.000477 7
241PUS G  NC=0.0001290 18$OC=3.17E-5 5$PC=5.86E-6 9$QC=3.38E-7 5
241PU  L 561.42       7/2-
241PU  B              0.28    6            7.41  18
241PUS B EAV=226 25
241PU  G 465.65       0.064  17E1+M2     0.088   +21-280.024  4                S
241PU2 G FLAG=B$
241PUS G  KC=0.019 3$LC=0.0039 8$MC=0.00097 20
241PUS G  NC=0.00026 6$OC=6.5E-5 14$PC=1.2E-5 3$QC=7.1E-7 16
241PU cG RI$From I|g/I|g(519|g+562|g)=0.321 {I20} in (n,|g)
241PU  G 519.43       0.12    4E1+M2     0.24    +9-11 0.05   3
241PU2 G FLAG=C$
241PUS G  KC=0.038 22$LC=0.009 6$MC=0.0023 15
241PUS G  NC=0.0006 4$OC=0.00016 10$PC=2.9E-5 19$QC=1.8E-6 12
241PU  G 561.1     2  0.08    3(E1+M2)   0.27    4     0.048  11
241PUS G  KC=0.036 8$LC=0.0087 21$MC=0.0022 6
241PUS G  NC=0.00059 14$OC=0.00015 4$PC=2.8E-5 7$QC=1.7E-6 4
241PU  L 834.84      3/2+,5/2+,7/2+
241PU  B             0.12    AP             7.1  AP
241PUS B EAV=135 23
241PU  G 834.6     2 0.11     3M1+E2     0.94    +25-200.048  7
241PUS G  KC=0.037 6$LC=0.0079 10$MC=0.00192 22
241PUS G  NC=0.00052 6$OC=0.000130 15$PC=2.4E-5 3$QC=1.49E-6 22
241PU  L 929.7     2  3/2,5/2,7/2
241PU  B             0.080   20             7.0   4
241PUS B EAV=105 22
241PU  G 929.7     2 0.08     2