137LA    137CE EC DECAY (9.0 H)        1975HE20                  07NDS    200709
137LA  H TYP=FUL$AUT=E. BROWNE, J. K. TULI$CIT=NDS 108,2173 (2007)$
137LA2 H CUT=1-Oct-2006$
137LA D  Modified by E. Browne (April 4, 2007).
137LA C  Measured: G, CE (1975He20,1975ArYT), GG, G(THETA,TEMP), GG(THETA)
137LA2C  (1964FrZZ), GG(T) (1963Ru03), B+ (1979BuZZ), CEG (1980ZhZY),
137LA3C  G, GG (1982Ko05)
137LA D  EG, RI, and decay scheme is that proposed by 1975He20
137LA C  EC feedings and decay-scheme normalization was determined based on the
137LA2C  assumption of no ground-state EC branch
137LA C  EKC normalized so that EKC(447G)=0.0136 14 (if KC(254.5G)=5.54 (M4)).
137LA C  1979BuZZ observed B+ with EB+=188.8 15
137LA CG E,RI$From 1975He20.
137CE  P 0.0         3/2+              9.0 H     3              1222.1    16
137LA  N 0.00168    60.00168   1.0       1.0
137LA CN NR        from I(254G)/I(447G)=4.91 15 in a transient equilibrium
137LA2CN G-spectrum of 9.0 H and 34.4 H 137CE. The correction factor for the
137LA3CN G-ray intensities from 137CE(9.0 h) is 34.4 3/[34.4 3 - 9.0 3] =
137LA4CN 1.354 16, where 34.4 h 3 is the half-life of {+137m}Ce,
137LA5CN and 9.0 H 3 the half-life of 137CE ground state.  Thus the
137LA6CN normalization factor becomes RI(447)/[RI(254)x(1+|a)]x
137LA7CN 1/1.354 16 = (1/4.91 15)x(1/(1+7.93 12))x(1/1.354 16) = 0.0168 6,
137LA8CN where |a=7.93 12 is the M4 conversion coefficient of 254G.
137LA9CN However, since in our scale of relative intensities we use
137LAACN RI(447)=1000, then NR=0.00168 6.
137LA PN                                                                     3
137LA  L 0.0         7/2+
137LA  L 10.59      45/2+              89 NS     4
137LA CL T         from 1963Ru03
137LA  E 1210.8    15 0.0085 4   97.83 8   5.37  2              97.84     8
137LAS E EAV=95.8 8 $CK=0.8458 $CL=0.1202 $CM+=0.03391
137LA  G 10.61     5 491     11M1                      117.6  2458232
137LAS G L/T=0.786 10$M/T=0.164 5$N+/T=0.0422 12
137LAS G N/T=0.0359 10$O/T=0.00582 17$P/T=0.000445 13
137LA CG RI        calculated from TI=97.83% 8 and CC=117.6 24.
137LA CG TI$From G-ray intensity balance and assumption of no EC branch to
137LA2CG ground state
137LA CG M         M1:M2:M3=23.4 16:2.87 24:1 (1975Mo12), M1:M2:M3:M4+=
137LA2CG 100:10 1:2.6 7:0.50 15, MR LT 0.008 (1975ArYT)
137LA  L 447.17     65/2+
137LA  E                         1.95  7   6.67  2
137LAS E  CK=0.8416 $CL=0.1234 $CM+=0.03499
137LA  G 436.59    9 149      5E2                      0.01509
137LAS G KC=0.01254 18$LC=0.00201 3$MC=0.000424 6$NC+=0.0001075 15
137LAS G NC=9.21E-5 13$OC=1.444E-5 21$PC=8.78E-7 13
137LA CG M         EKC=0.012 2
137LA  G 447.15    8 1000      M1+E2                   0.0165 25
137LAS G KC=0.0140 23$LC=0.00199 13$MC=0.000416 24$NC+=0.000107 7
137LAS G NC=9.1E-5 6$OC=1.46E-5 12$PC=1.04E-6 22
137LA CG M         EKC=0.0136 14 (if KC(254.5G)=5.54), K:L:M=100 5:12.8 16:2.9 9
137LA  L 493.09    6 (3/2)+
137LA  E                        0.0018 AP   9.6  AP
137LAS E  CK=0.8408 $CL=0.1240 $CM+=0.03518
137LA  G 482.47    1025.7     9
137LA  G 493.03    105.9      3
137LA  L 641.95     71/2+
137LA  E                        0.0134 9   8.57  4
137LAS E  CK=0.8374 $CL=0.1266 $CM+=0.03604
137LA  G 148.83     80.5      2
137LA  G 631.38     67.5      4
137LA  L 709.30     6(3/2)+
137LA  E                         0.027  2  8.15  4
137LAS E  CK=0.8351 $CL=0.1283 $CM+=0.03661
137LA  G 698.72    1117.5     9M1+(E2)                 0.0053 10
137LAS G KC=0.0046 9$LC=0.00061 9$MC=0.000126 18$NC+=3.2E-5 5
137LAS G NC=2.8E-5 4$OC=4.5E-6 7$PC=3.4E-7 8
137LA CG M         EKC=0.0050 10
137LA  G 709.30    110.6      1
137LA  L 781.57     9(7/2)+
137LA  E                        0.0086  6  8.50  4
137LAS E  CK=0.8318 $CL=0.1308 $CM+=0.03744
137LA CE           LOGFT=8.48 is inconsistent with DJ=2 DPI=no transition.
137LA2CE LOGFT GE 12.8 is expected
137LA  G 770.97    103.4      2
137LA  G 781.57    131.7      2
137LA  L 926.33     65/2+
137LA  E                         0.145 6   6.90  2
137LAS E  CK=0.8195 $CL=0.14000 17 $CM+=0.04052 6
137LA  G 217.03     52.2      3
137LA  G 433.22    9 29.1     5E2                      0.01542
137LAS G KC=0.01282 18$LC=0.00206 3$MC=0.000435 6$NC+=0.0001101 16
137LAS G NC=9.44E-5 14$OC=1.479E-5 21$PC=8.97E-7 13
137LA CG M         EKC=0.013 5
137LA  G 479.12    106.7      3
137LA  G 915.80    1328.9    10(M1+E2)                 0.0028 5
137LAS G KC=0.0024 5$LC=0.00031 5$MC=6.5E-5 10$NC+=1.7E-5 3
137LAS G NC=1.43E-5 22$OC=2.3E-6 4$PC=1.8E-7 4
137LA CG M         EKC=0.0025 5
137LA  G 926.35    1319.0     7(M1+E2)                 0.0027 5
137LAS G KC=0.0024 5$LC=0.00031 5$MC=6.3E-5 10$NC+=1.6E-5 3
137LAS G NC=1.39E-5 22$OC=2.3E-6 4$PC=1.8E-7 4
137LA CG M         EKC=0.0023 4
137LA  L 1171.40   11(1/2+,3/2-)
137LA  E                        0.0029  5  6.4   1
137LAS E  CK=0.28 5 $CL=0.54 3 $CM+=0.185 12
137LA  G 529.3      20.2      1                                                ?
137LA  G 678.26    120.5      2
137LA  G 724.4      30.4      2
137LA  G 1160.85   220.84     8