220FR 224AC A DECAY 1992LI31,1968LE17 11NDS 201104
220FR H TYP=FUL$AUT=E. BROWNE, J. K. TULI$CIT=NDS 112, 1115 (2011)$
220FR2 H CUT=31-Oct-2010$
220FR D Modified by E. Browne. Nov. 30, 2010. BRICC, GTOL.
220FR cA E,IA From 1968Le17, unless otherwise noted. These data are also
220FR2cA given in 1969LeZW. Authors' E|a values have been increased by 3.8
220FR3cA keV (see 1991Ry01) to adjust for newer energy calibration values.
220FR cA HF r{-0}({+220}Fr)=1.540 {I6}
220FR DG CC$ FROM BrIcc v2.2 (31-Mar-2008) 2008KiAA, "Frozen Orbitals" appr.
220FR cG E From 1992Li31; others: 1970Br31 (see also 1973ChZH),
220FR2cG 1969Le07, 1969LeZW
220FR cG RI From 1992Li31, I|g/10{+4} |a; others: 1973ChZH, 1969Le07,
220FRxcG 1969LeZW.
220FR cG M From 1992Li31 and 1973ChZH. |a(exp) values are from
220FR2cG 1973ChZH. |g and the ce spectra were normalized through the 261|g
220FR3cG (M1) with |a(K)=0.83 and |a(L)=0.15
220FR cG E(F),M(F)$From 1992Li31. Not listed in the |g-ray table or shown in
220FR2cG the |g-ray or ce spectra; however, |g ray is shown in the level scheme.
220FR3cG E|g and multipolarity probably have been deduced from the level scheme.
220FR cG E(K)$|g ray placed from the 55.8-keV level in 1992Li31; however, the
220FR2cG transition intensity indicates a slight imbalance at this level. The
220FR3cG energy of the |g ray fits also from the 48.4-keV level, and this second
220FR4cG placement would improve the intensity balance at both levels.
220FR cG RI(H) I|g deduced from |a|g coin. In singles spectrum |g ray mixed
220FR2cG or masked by K| x rays or other |g rays of about the same energy
220FR3cG from daughter nuclei.
220FR cG M(B)$From transition-intensity balance in level scheme. With any other
220FR2cG multipolarity, I(|g+ce) would be larger than total feeding from |a
220FR3cG decay to levels above this level.
220FR cG M(G) Deduced from internal conversion data (not given)
220FR2cG (1992Li31). In some cases additional conversion data from other
220FR3cG sources are given.
220FR cG M(J)$From transition-intensity balance in level scheme. Based on the
220FR2cG criterion that |SI(|g+ce) de-exciting the level cannot exceed |SI|a
220FR3cG populating levels with higher energy. From the level scheme the
220FR4cG 55.3|g ray and 81.5|g ray from the 355.2-keV level must
220FR4cG have the same mixing ratio |D|p, therefore, from transition-intensity
220FR5cG balance both must have E1 multipolarity.
220FR cG M(M) The M1(e-) multipolarity given in table 1 in 1992Li31 for the
220FR2cG 271.5|g ray is a misprint, the multipolarity belongs to the next
220FR3cG |g ray, the 273.7|g ray. (Priv. comm. from first author in 1992Li31).
220FR cG TI(L) |g ray not seen; transition intensity estimated from
220FR2cG transition-intensity balance.
220FR cL 1992Li31: measured |g, ce, |a, |a|g, |a(ce), |g|g, |g(ce)
220FR cL 1973ChZH: measured |g, |a|g, |a(ce)
220FR cL 1968Le17, 1969LeZW: measured |g, |a, |a|g
220FR cL Others: 1970Br31, 1969Le07, 1967Br15
220FR cL
220FR cL The decay scheme is that of 1992Li31, based on
220FR2cL |g and ce measurements, and on |a|g, |a(ce) coincidence
220FR3cL results of 1992Li31,
220FR3cL and on |a-particle measurements of 1968Le17.
220FR cL E From least squares fit to E|g. Band assignments are from
220FR2cL 1992Li31. They suggest that the bands with K|p=1|+ and K|p=2|+
220FR3cL form two sets of parity doublets.
220FR cL J From 1992Li31
220FR CL BAND(A) KPI=1+ GS ROTATIONAL BAND
220FR CL BAND(B) KPI=1- BAND
220FR CL BAND(C) KPI=2+ BAND
220FR CL BAND(D) POSSIBLE KPI=2- BAND
220FR CL BAND(E) POSSIBLE KPI=0- BAND
224AC P 0 0- 2.78 H 17 6326.9 7
220FR N 0.1 0.1 0.091 20
220FR cN BR 9.1% {I+20-14} from |e/|a=10 {I2} (1951Me10)
220FR PN 2
220FR G 44.5 2 0.3 1
220FR G 46.0 2 0.3 1
220FR G 70.9 2 0.8 2
220FR G 116.5 5 0.3 2
220FR G 122.3 5 0.4 2
220FR G 123.3 5 0.4 2
220FR G 126.7 4 0.5 2
220FR G 170.2 5 0.4 AP
220FR G 210.0 5 0.2 AP
220FR G 211.5 5 0.2 AP
220FR G 291.2 5 0.3 1
220FR G 376.5 0.3 1
220FR G 382.3 0.5 2
220FR G 409.8 0.3 AP
220FR G 415.8 0.3 AP
220FR G 424.4 0.3 AP
220FR L 0 1+ A
220FR A 6213.8 7 20.4 170 40
220FR cA I|a=25 {I5}, from |g-ray transition-intensity balance.
220FR L 6.92 6 3+ C
220FR A 6207.0 7 11.9 270 60
220FR cA I|a=12.2 {I15}, from |g-ray transition-intensity balance.
220FR G 6.9 215 10L S
220FR L 12.37 5 2+ C
220FR A 6202 0.4 LT 7.7E+3 GT ?
220FR cA IA Not seen. Upper limit given by 1969LeZW.
220FR cA I|a<0.4, from |g-ray transition-intensity balance.
220FR G 12.4 167 14L S
220FR L 19.89 10 4+ C
220FR G 13.0 35 8 L S
220FR L 48.38 4 2+ A
220FR A 6166 0.1 LT 2.1E+4 GT ?
220FR cA IA Not seen. Upper limit given by 1969LeZW
220FR cA I|a<0.2, from |g-ray transition-intensity balance.
220FR G 35.9 1 0.3 2 [M1] 56.5 10 @
220FR2 G FLAG=K
220FRS G LC=42.9 7$MC=10.24 17$NC+=3.39 6
220FRS G NC=2.69 5$OC=0.601 10$PC=0.0963 16$QC=0.00540 9
220FR G 41.5 1 0.4 1 [M1] 36.9
220FRS G LC=28.0 5$MC=6.68 11$NC+=2.21 4
220FRS G NC=1.75 3$OC=0.392 7$PC=0.0628 10$QC=0.00352 6
220FR cG |g ray unplaced in 1992Li31; placement suggested
220FR2cG by evaluators.
220FR G 48.40 5 6.5 5 M1 23.4 G
220FRS G LC=17.8 3$MC=4.24 6$NC+=1.404 21
220FRS G NC=1.113 16$OC=0.249 4$PC=0.0399 6$QC=0.00224 4
220FR L 55.83 13 5+ C
220FR A 6158.9 7 1.03 1.9E+3 4
220FR cA I|a=0.9 {I6}, from |g-ray transition-intensity balance.
220FR G 35.9 1 0.2 1 [M1] 56.5 10 @
220FR2 G FLAG=K
220FRS G LC=42.9 7$MC=10.24 17$NC+=3.39 6
220FRS G NC=2.69 5$OC=0.601 10$PC=0.0963 16$QC=0.00540 9
220FR L 72.99 6 3+ A
220FR A 6141.7 7 25.6 65 15
220FR cA I|a=25.2 {I16}, from |g-ray transition-intensity balance.
220FR G 24.6 1.0 1 [M1] 172.6 181 11
220FRS G L/T=0.754 8$M/T=0.181 4$N+/T=0.0598 12
220FRS G N/T=0.0474 10$O/T=0.01059 21$P/T=0.00170 4$Q/T=9.52E-5 19
220FR cG ce(M) and ce(N) lines seen in ce spectrum. |g ray
220FR2cG marked M1 in level scheme (1992Li31)
220FR cG TI$From |g-ray transition-intensity balance at the 73.0 level.
220FR cG From I(|g+ce)=181 {I11} and |a[M1]=172.6.
220FR G 53.1 1 1.0 2 [M1] 17.9
220FRS G LC=13.56 21$MC=3.23 5$NC+=1.069 17
220FRS G NC=0.848 13$OC=0.190 3$PC=0.0304 5$QC=0.00170 3
220FR G 60.67 5 4.6 2 M1 12.08 G
220FRS G LC=9.17 13$MC=2.19 4$NC+=0.723 11
220FRS G NC=0.574 9$OC=0.1282 19$PC=0.0206 3$QC=0.001151 17
220FR G 66.0 1 2.3 4 [M1] 9.44
220FRS G LC=7.17 11$MC=1.71 3$NC+=0.565 9
220FRS G NC=0.448 7$OC=0.1002 15$PC=0.01608 24$QC=0.000899 14
220FR G 72.9 1 0.5 2 (E2) 39.1 @
220FRS G LC=28.8 5$MC=7.79 12$NC+=2.52 4
220FRS G NC=2.04 4$OC=0.422 7$PC=0.0541 9$QC=9.97E-5 15
220FR cG M$Stated as E2 in 1973ChZH, based on
220FR2cG |a|g results, but no further details are given (1966BrZX).
220FR L 127.31 11 4+ A
220FR G 54.3 1 0.7 1 [M1] 16.7
220FRS G LC=12.70 19$MC=3.03 5$NC+=1.002 15
220FRS G NC=0.794 12$OC=0.178 3$PC=0.0285 5$QC=0.001594 24
220FR L 140.72 6 1- B
220FR G 92.34 5 5.2 5 [E1] 0.1323
220FRS G LC=0.1004 15$MC=0.0242 4$NC+=0.00775 11
220FRS G NC=0.00623 9$OC=0.001324 19$PC=0.000187 3$QC=6.65E-6 10
220FR G 128.4 3 8.1 20E1 0.258
220FRS G KC=0.203 3$LC=0.0420 7$MC=0.01007 16$NC+=0.00325 5
220FRS G NC=0.00260 4$OC=0.000559 9$PC=8.13E-5 13$QC=3.16E-6 5
220FR cG M |a(L)exp<0.14 (1973ChZH); theory: |a(L)(E1)=0.0425,
220FR2cG |a(L)(E2)=2.06, |a(L)(M1)=1.10
220FR G 140.7 1 35.6 30E1 0.207 G
220FRS G KC=0.1630 23$LC=0.0331 5$MC=0.00792 12$NC+=0.00256 4
220FRS G NC=0.00205 3$OC=0.000441 7$PC=6.46E-5 10$QC=2.57E-6 4
220FR cG M |a(L)exp<0.15 (1973ChZH); theory: |a(L)(E1)=0.0334,
220FR2cG |a(L)(E2)=1.36, |a(L)(M1)=0.844
220FR L 156.82 4 2- B
220FR A 6059.8 7 21.9 32 7
220FR cA I|a=21.9 {I13}, from |g-ray transition-intensity balance.
220FR G 16 0.46 10[M1] 159 73 15F S
220FRS G MC=119
220FR cG TI$Deduced from transition-intensity balance at the 156.8-keV level;
220FR2cG I|g from I(|g+ce)=73 {I15} and |a[M1]=159.
220FR G 83.9 2 18.0 10E1 0.171 3 G
220FR2 G FLAG=H
220FRS G LC=0.1295 20$MC=0.0312 5$NC+=0.00999 16
220FRS G NC=0.00804 13$OC=0.00170 3$PC=0.000239 4$QC=8.23E-6 13
220FR G 108.43 5 10.5 10E1 0.387
220FRS G KC=0.301 5$LC=0.0656 10$MC=0.01574 23$NC+=0.00506 8
220FRS G NC=0.00407 6$OC=0.000869 13$PC=0.0001247 18$QC=4.63E-6 7
220FR cG M |a(L)exp<0.65 (1973ChZH); theory: |a(L)(E1)=0.0663,
220FR2cG |a(L)(E2)=4.49, |a(L)(M1)=1.78
220FR G 144.44 5 22.5 20E1 0.194 G
220FRS G KC=0.1531 22$LC=0.0309 5$MC=0.00739 11$NC+=0.00239 4
220FRS G NC=0.00191 3$OC=0.000413 6$PC=6.05E-5 9$QC=2.42E-6 4
220FR cG M |a(L)exp<0.42 (1973ChZH); theory: |a(L)(E1)=0.0312,
220FR2cG |a(L)(E2)=1.21, |a(L)(M1)=0.783
220FR G 149.90 5 12.5 20E1 0.1770
220FRS G KC=0.1401 20$LC=0.0281 4$MC=0.00671 10$NC+=0.00217 3
220FRS G NC=0.001739 25$OC=0.000375 6$PC=5.51E-5 8$QC=2.23E-6 4
220FR cG M |a(L)exp<0.061 (1973ChZH); theory: |a(L)(E1)=0.0284,
220FR2cG |a(L)(E2)=1.03, |a(L)(M1)=0.704
220FR G 156.82 5 81 5 E1 0.1586 G
220FRS G KC=0.1257 18$LC=0.0250 4$MC=0.00597 9$NC+=0.00193 3
220FRS G NC=0.001547 22$OC=0.000334 5$PC=4.93E-5 7$QC=2.01E-6 3
220FR cG RI other: I|g/10|*10{+3} |a's=53 (1969Le07)
220FR cG M |a(L)exp<0.057 (1973ChZH); theory: |a(L)(E1)=0.0252,
220FR2cG |a(L)(E2)=0.841, |a(L)(M1)=0.619
220FR L 177.18 8 3- B
220FR G 20.4 [M1] 299 F S
220FRS G L/T=0.754 8$M/T=0.182 4$N+/T=0.0603 12
220FRS G N/T=0.0478 10$O/T=0.01069 21$P/T=0.00171 4$Q/T=9.61E-5 19
220FR G 49.8 2 0.4 1 [E1] 0.689 13
220FRS G LC=0.522 10$MC=0.1272 23$NC+=0.0402 8
220FRS G NC=0.0326 6$OC=0.00674 12$PC=0.000887 16$QC=2.57E-5 5
220FR G 104.4 2 1.3 3 [E1] 0.422
220FRS G KC=0.327 5$LC=0.0725 11$MC=0.0174 3$NC+=0.00560 9
220FRS G NC=0.00450 7$OC=0.000959 15$PC=0.0001372 21$QC=5.04E-6 8
220FR G 128.9 3 3.6 10[E1] 0.256
220FRS G KC=0.201 3$LC=0.0416 7$MC=0.00996 16$NC+=0.00322 5
220FRS G NC=0.00258 4$OC=0.000554 9$PC=8.05E-5 13$QC=3.13E-6 5
220FR G 164.8 1 5.0 10E1 0.1406
220FRS G KC=0.1117 16$LC=0.0220 3$MC=0.00525 8$NC+=0.001701 24
220FRS G NC=0.001361 20$OC=0.000294 5$PC=4.35E-5 7$QC=1.80E-6 3
220FR cG M |a(L)exp<0.42 (1973ChZH); theory: |a(L)(E1)=0.0222,
220FR2cG |a(L)(E2)=0.675, |a(L)(M1)=0.538
220FR L 200.21 15 5+ A
220FR A 6017.6 14 1.4 310 70
220FR cA I|a=1.09 {I25}, from |g-ray transition-intensity balance.
220FR G 72.9 1 1.4 3 [M1] 7.06 @
220FRS G LC=5.36 8$MC=1.278 19$NC+=0.423 7
220FRS G NC=0.335 5$OC=0.0749 11$PC=0.01202 18$QC=0.000673 10
220FR L 214.43 9 4- B
220FR A 6003.6 14 6.7 56 13
220FR cA I|a=5.0 {I6}, from |g-ray transition-intensity balance.
220FR G 37.3 1 0.6 1 [M1] 50.5 9
220FRS G LC=38.3 7$MC=9.15 15$NC+=3.03 5
220FRS G NC=2.40 4$OC=0.536 9$PC=0.0860 14$QC=0.00482 8
220FR cG M E2 ruled out by intensity balance in the level scheme
220FR G 141.4 1 10.6 20[E1] 0.204
220FRS G KC=0.1611 23$LC=0.0327 5$MC=0.00782 11$NC+=0.00253 4
220FRS G NC=0.00202 3$OC=0.000436 7$PC=6.38E-5 9$QC=2.54E-6 4
220FR G 158.5 2 1.6 4 [E1] 0.1546
220FRS G KC=0.1226 18$LC=0.0243 4$MC=0.00581 9$NC+=0.00188 3
220FRS G NC=0.001505 22$OC=0.000325 5$PC=4.80E-5 7$QC=1.96E-6 3
220FR G 194.5 3 0.7 2 E1 0.0942
220FRS G KC=0.0753 11$LC=0.01441 21$MC=0.00344 5$NC+=0.001115 17
220FRS G NC=0.000892 13$OC=0.000194 3$PC=2.89E-5 5$QC=1.240E-6 18
220FR cG M |a(K)exp<2.9, |a(L)exp<0.15 (1973ChZH); theory: E1:
220FR2cG |a(K)=0.0759, |a(L)=0.0145; E2: |a(K)=0.175, |a(L)=0.329; M1:
220FRxcG |a(K)=1.84, |a(L)=0.336
220FR G 207.6 2 3.6 10E1 0.0806
220FRS G KC=0.0645 10$LC=0.01223 18$MC=0.00291 5$NC+=0.000947 14
220FRS G NC=0.000757 11$OC=0.0001645 24$PC=2.47E-5 4$QC=1.072E-6 16
220FR cG M |a(K)exp<0.62, |a(L)exp<0.03 (1973ChZH); theory: E1:
220FR2cG |a(K)=0.0650, |a(L)=0.0123; E2: |a(K)=0.154, |a(L)=0.249; M1:
220FRxcG |a(K)=1.54, |a(L)=0.280
220FR L 246.8 10
220FR cL E 1968Le17, 1992Li31 give E(level)=237; this is a misprint,
220FR2cL it should read 247 (priv. comm. from first author)
220FR A 5971.5 14 0.18 1.5E+3 3
220FR L 257.0 15
220FR A 5961.5 20 0.03 AP 8.0E+3 AP
220FR L 273.64 11 1+
220FR A 5945.6 14 4.4 45 10
220FR cA I|a=3.4 {I4}, from |g-ray transition-intensity balance.
220FR G 225.3 2 3.2 10M1 1.438 G
220FRS G KC=1.160 17$LC=0.211 3$MC=0.0503 8$NC+=0.01664 24
220FRS G NC=0.01319 19$OC=0.00295 5$PC=0.000473 7$QC=2.64E-5 4
220FR cG M |a(K)exp=1.4, K/L=10 (1973ChZH); theory: E1: |a(K)=0.0537,
220FR2cG K/L=5.34; E2: |a(K)=0.129, K/L=0.73; M1: |a(K)=1.22, K/L=5.48
220FR G 261.3 2 19.0 15M1 0.953 G
220FRS G KC=0.769 11$LC=0.1397 20$MC=0.0332 5$NC+=0.01099 16
220FRS G NC=0.00872 13$OC=0.00195 3$PC=0.000313 5$QC=1.744E-5 25
220FR cG M |a(K)exp=1.06 {I25} from (K| x ray)(|a)/|a|g (1966BrZX),
220FR2cG K/L=4.9 (1973ChZH); theory: E1: |a(K)=0.0380, K/L=5.45; E2:
220FR3cG |a(K)=0.095, K/L=0.98; M1: |a(K)=0.808, K/L=5.48
220FR G 273.7 4 1.1 3 M1 0.838 G
220FR2 G FLAG=M
220FRS G KC=0.676 10$LC=0.1228 18$MC=0.0292 5$NC+=0.00966 14
220FRS G NC=0.00766 12$OC=0.001713 25$PC=0.000275 4$QC=1.533E-5 23
220FR cG M |a(K)exp|<1.13 (1973ChZH); theory: |a(K)(E2)=0.0859,
220FRxcG |a(K)(M1)=0.711
220FR L 276.02 20 (3-) D
220FR G 263.1 5 1.3 4 ?
220FR L 290.8 3 (5-) B
220FR G 163.3 5 0.5 AP[E1] 0.1438 23
220FRS G KC=0.1141 18$LC=0.0225 4$MC=0.00538 9$NC+=0.00174 3
220FRS G NC=0.001394 23$OC=0.000301 5$PC=4.45E-5 8$QC=1.84E-6 3
220FR G 271.5 4 1.0 3 [E1] 0.0430 M
220FRS G KC=0.0346 5$LC=0.00632 10$MC=0.001503 22$NC+=0.000490 7
220FRS G NC=0.000391 6$OC=8.54E-5 13$PC=1.298E-5 19$QC=5.95E-7 9
220FR L 299.91 15 1+
220FR A 5919.6 14 0.96 160 40
220FR cA I|a=0.68 {I18}, from |g-ray transition-intensity balance.
220FR G 251.6 3 2.6 7 M1 1.058 G
220FRS G KC=0.853 13$LC=0.1552 23$MC=0.0369 6$NC+=0.01222 18
220FRS G NC=0.00969 14$OC=0.00217 4$PC=0.000347 5$QC=1.94E-5 3
220FR cG M |a(K)exp=0.85, |a(L)exp<0.24 (1973ChZH): theory: E2:
220FR2cG |a(K)=0.103, |a(L)=0.113; M1: |a(K)=0.90, |a(L)=0.164
220FR G 287.6 5 0.7 3 [M1,E2] 0.4 3 H
220FRS G KC=0.3 3$LC=0.086 21$MC=0.021 5$NC+=0.0070 14
220FRS G NC=0.0056 11$OC=0.0012 3$PC=0.00018 6$QC=8.E-6 6
220FR G 300.0 3 1.7 4 (M1) 0.651
220FRS G KC=0.525 8$LC=0.0952 14$MC=0.0227 4$NC+=0.00749 11
220FRS G NC=0.00594 9$OC=0.001328 19$PC=0.000213 3$QC=1.189E-5 17
220FR cG M |a(K)exp|<1.65, |a(L)exp=0.09 (1973ChZH); theory: E2:
220FR2cG |a(K)=0.0706, |a(L)=0.0565; M1: |a(K)=0.553, |a(L)=0.100
220FR L 306.9 15
220FR A 5912.5 20 0.15 9.3E+2 21
220FR L 314.8 4 (4-) D
220FR A 5905.4 14 0.14 9.1E+2 21
220FR cA I|a=0.07 {I3}, from |g-ray transition-intensity balance.
220FR G 114.7 5 0.3 2 [E1] 0.339 6
220FRS G KC=0.265 5$LC=0.0565 11$MC=0.01356 25$NC+=0.00437 8
220FRS G NC=0.00350 7$OC=0.000750 14$PC=0.0001081 20$QC=4.08E-6 7
220FR G 258.8 5 0.3 AP[E1] 0.0480
220FRS G KC=0.0386 6$LC=0.00710 11$MC=0.001688 25$NC+=0.000550 9
220FRS G NC=0.000439 7$OC=9.58E-5 15$PC=1.453E-5 22$QC=6.60E-7 10
220FR cG |g seen only in |a|g coin
220FR L 340.25 12 0- E
220FR A 5880.3 14 1.7 57 13
220FR cA I|a=1.9 {I4}, from |g-ray transition-intensity balance.
220FR G 40.4 3 0.5 2 (E1) 1.21 3 J
220FR2 G FLAG=H
220FRS G LC=0.912 23$MC=0.224 6$NC+=0.0703 18
220FRS G NC=0.0571 14$OC=0.0117 3$PC=0.00149 4$QC=3.99E-5 9
220FR G 66.6 1 6.0 5 E1 0.316 B
220FRS G LC=0.240 4$MC=0.0581 9$NC+=0.0185 3
220FRS G NC=0.01492 22$OC=0.00313 5$PC=0.000428 7$QC=1.371E-5 20
220FR G 199.5 2 3.0 10M1 2.02 G
220FRS G KC=1.629 24$LC=0.297 5$MC=0.0708 11$NC+=0.0234 4
220FRS G NC=0.0186 3$OC=0.00415 6$PC=0.000666 10$QC=3.72E-5 6
220FR cG M |a(K)exp=2, |a(L)exp<0.4 (1973ChZH); theory: E2:
220FR2cG |a(K)=0.167, |a(L)=0.295; M1: |a(K)=1.72, |a(L)=0.313
220FR G 340.3 3 0.5 2 [E1] 0.0258
220FRS G KC=0.0209 3$LC=0.00371 6$MC=0.000880 13$NC+=0.000287 4
220FRS G NC=0.000229 4$OC=5.02E-5 8$PC=7.72E-6 11$QC=3.68E-7 6
220FR L 347.9 4 (3+)
220FR A 5871.0 10 0.1 8.9E+2 20
220FR cA I|a=0.07 {I3}, from |g-ray transition-intensity balance.
220FR G 328.0 3 0.7 3 &
220FR2 G FLAG=H
220FR L 355.13 19
220FR A 5864.0 14 0.75 109 25
220FR cA I|a=1.4 {I9}, from |g-ray transition-intensity balance.
220FR G 55.3 2 0.4 1 (E1) 0.521 9 J
220FRS G LC=0.394 7$MC=0.0959 17$NC+=0.0304 6
220FRS G NC=0.0246 5$OC=0.00511 9$PC=0.000683 12$QC=2.05E-5 4
220FR G 79.10 5 2.8 3 [M1,E1] 3 3
220FR2 G FLAG=H
220FRS G LC=2.2 21$MC=0.5 5$NC+=0.17 16
220FRS G NC=0.14 13$OC=0.03 3$PC=0.005 5$QC=0.0003 3
220FR G 81.5 3 2.1 2 (E1) 0.184 4 J
220FR2 G FLAG=H
220FRS G LC=0.1399 24$MC=0.0337 6$NC+=0.01080 19
220FRS G NC=0.00869 15$OC=0.00184 4$PC=0.000257 5$QC=8.78E-6 15
220FR G 228 ?
220FR cG |g ray shown only in level scheme of 1992Li31
220FR L 361.0 4
220FR A 5857.7 20 0.25 310 70
220FR G 87.4 3 1.3 5
220FR L 364.16 23 (4-)
220FR A 5854.6 25 0.07 AP1.1E+3 AP
220FR cA I|a=0.15 {I4}, from |g-ray transition-intensity balance.
220FR G 73.6 3 0.6 3
220FR G 186.8 3 0.6 2
220FR G 357.0 5 0.3 AP
220FR L 376.49 20 2- E
220FR A 5844.5 7 0.55 120 30
220FR cA I|a=0.34 {I5}, from |g-ray transition-intensity balance.
220FR G 103.1 4 0.4 AP[E1] 0.433 7 H
220FRS G KC=0.335 6$LC=0.0749 13$MC=0.0180 4$NC+=0.00579 10
220FRS G NC=0.00465 8$OC=0.000991 18$PC=0.0001416 25$QC=5.19E-6 9
220FR G 328.0 3 0.7 3 [E1] 0.0280 &
220FR2 G FLAG=H
220FRS G KC=0.0227 4$LC=0.00404 6$MC=0.000959 14$NC+=0.000313 5
220FRS G NC=0.000249 4$OC=5.47E-5 8$PC=8.39E-6 12$QC=3.98E-7 6
220FR G 364.1 3 2.1 3 [E1] 0.0222
220FRS G KC=0.0181 3$LC=0.00318 5$MC=0.000753 11$NC+=0.000246 4
220FRS G NC=0.000196 3$OC=4.31E-5 6$PC=6.63E-6 10$QC=3.20E-7 5
220FR cG M |a(K)exp|<0.47 (1973ChZH); theory: |a(K)(E1)=0.0181,
220FR2cG |a(K)(E2)=0.0469, |a(K)(M1)=0.326
220FR L 380.1 10
220FR A 5840.6 15 0.26 240 50
220FR L 414.6 20
220FR A 5806.7 25 0.02 AP 2.1E+3 AP
220FR L 442.2 15
220FR A 5779.8 20 0.06 5.1E+2 12
220FR L 452.4 11 (4-) E
220FR cL J alternate assignment J|p=(5+) (1992Li31)
220FR A 5771.8 20 0.24 115 26
220FR G 97.3 ?
220FR cG |g shown only in level scheme of 1992Li31
220FR L 479.6 20
220FR A 5742.8 25 0.05 AP 4.0E+2 AP
220FR L 501.1 4
220FR A 5721.8 20 0.12 130 30
220FR cA I|a=0.12 {I4}, from |g-ray transition-intensity balance.
220FR G 48.6 ?
220FR cG |g shown only in level scheme of 1992Li31
220FR G 201.1 4 0.6 3
220FR G 227.7 5 0.6 2
220FR L 511.1 10
220FR A 5712.8 20 0.12 117 27
220FR cA I|a=0.12, from |g-ray transition-intensity balance.
220FR G 491.2 0.4 AP
220FR L 579.9 20
220FR A 5644.3 25 0.06 105 24