115SN 115SB EC DECAY (32.1 M) 1975WIZX,1976WI10 12NDS 201210
115SN H TYP=FUL$AUT=JEAN BLACHOT$CIT=NDS 113, 2391 (2012)$CUT=1-Sep-2012$
115SN c Others: 1961Se08, 1962Se03, 1968Ra27, 1969Ki16, 1974Ki07, 1993BaZJ
115SN cE Q(|e)=3030 {I20} from E(|b{++})=1510 {I20} to 497 state
115SN cG E(A) From Coul. ex. (1977Da12)
115SN cG MR Deduced from |g-ray angular distributions via Coul. ex.
115SB P 0.0 5/2+ 32.1 M 3 3030 16
115SN N 0.0979 4 1.0 1.0
115SN cN NR |SI(|g+ce) to g.s.=100 decays; (|e+|b{++})|?0 to g.s. from
115SN2cN unobserved |b{++} (1962Se03) (|DJ=2,no)
115SN PN 5
115SN G 1097.3 2 0.29 4
115SN G 1471.3 4 0.16 3
115SN G 1476.4 4 0.10 2
115SN G 1543.1 4 0.10 2
115SN cG E$placed from a 2440 level in (p,n|g)
115SN G 1658.3 4 0.05 2
115SN G 1717.5 5 0.05 2
115SN G 1817.3 5 0.15 2
115SN G 1854.7 6 0.05 2
115SN G 1938.0 5 0.09 2
115SN G 1990.0 9 0.08 2
115SN G 2589.8 100.02 1
115SN L 0.0 1/2+ STABLE
115SN L 497.3 3/2+
115SN E 2530 20 33.3 19 63 4 4.741 25
115SNS E EAV=675 9 $CK=0.561 9 $CL=0.0727 11 $CM+=0.0187 3
115SN cE E E(|b{++})=1510 {I20} (1961Se08) s, 1500 {I50} (1969Ki16) scin
115SN cE Allowed log| {Ift} to low-lying 3/2+ states
115SN2cE characterize (|e+|b{++})-decays of odd-mass {+111}Sb-{+119}Sb
115SN cE |eK/|b{++}=1.62 theory, 1.22 {I6} exp (1969Ki16)
115SN G 497.31 8 1000 M1+E2 +0.21 2 C
115SNS G KC=0.00699 $LC=0.00085 $MC=0.00017
115SN L 612.9 7/2+ 3.26 US 8
115SN E 0.052 0.13 7.4
115SNS E EAV=623 9 $CK=0.609 9 $CL=0.0790 11 $CM+=0.0203 3
115SN G 115.6 1 2.4 2 E2 0.954 C
115SNS G KC=0.719 11$LC=0.190 3$MC=0.0385 6$NC+=0.00718 11
115SNS G NC=0.00686 10$OC=0.000325 5
115SN cG HF(E2,115|g)=7.8; analogs: HF(E2,553|g,{+117}Sn)=3.1,
115SN2cG HF(E2,763|g,{+119}Sn)=3.0
115SN L 986.5 5/2+
115SN E 0.18 4 1.2 3 6.27 10
115SNS E EAV=457 9 $CK=0.750 7 $CL=0.0977 9 $CM+=0.02510 23
115SN G 373.8 2 0.42 10M1+E2 -0.26 6 0.0163924
115SNS G KC=0.01420 21$LC=0.00177 3$MC=0.000346 6$NC+=7.07E-5 11
115SNS G NC=6.50E-5 10$OC=5.63E-6 8
115SN G 489.3 7 13 3 M1+E2 +0.040 23 C
115SNS G KC=0.00730 $LC=0.00089 $MC=0.00017
115SN G 986.4 2 3.6 2 E2 C
115SNS G KC=0.00115 $LC=0.00014
115SN L 1280.2 3/2+
115SN cL Branching: I|g(1280|g):I|g(783|g):I|g(668|g):I|g(294|g)=86.2
115SN2cL {I12}:7.8 {I7}:3.0 7:3.0 {I4} (1977Da12) Coul. ex.
115SN E 0.01 0.3 6.8
115SNS E EAV=329 9 $CK=0.822 4 $CL=0.1075 5 $CM+=0.02765 13
115SN G 293.60 29 0.10 CA A S
115SN G 668.13 34 0.10 CA A S
115SN G 782.99 9 0.26 CA A S
115SN G 1279.9 2 2.9 2 M1+E2 -2.2 2
115SNS G KC=0.00068
115SN L 1416.9 5/2+
115SN cL $Branching: I|g(1417|g):I|g(920|g):I|g(804|g):I|g(430|g):I|g(137|g)
115SN2cL =72.1 28:21.0 {I19}:5.1 {I7}:0.6 {I4}:1.2 {I5} (1977Da12) Coul.
115SNxcL ex.
115SN E 0.001 0.06 7.4
115SNS E EAV=269 9 $CK=0.8410 22 $CL=0.1102 4 $CM+=0.02836 9
115SN G 136.70 15 0.007 CA A S
115SN G 430.27 30 0.0034 CA A S
115SN G 804.04 25 0.029 CA A S
115SN G 919.79 17 0.12 CA A S
115SN G 1416.8 3 0.41 4 E2
115SNS G KC=0.00054
115SN L 1633.8 3/2(+)
115SN E 0.002 0.5 6.3
115SNS E EAV=175 9 $CK=0.8549 $CL=0.11260 15 $CM+=0.02899 4
115SN G 1021.1 2 0.44 5
115SN G 1136.3 2 1.3 1 C
115SN G 1633.8 2 3.6 2 (M1)
115SN L 1734.0 5/2+
115SN E 1.0 1 5.95 5
115SNS E CK=0.8567 $CL=0.1132 $CM+=0.02914
115SN G 747.7 2 2.0 2 E2,M1 C
115SNS G KC=0.002
115SN G 1121.3 2 1.6 1
115SN G 1236.6 2 5.9 3 C
115SN G 1734.0 7 0.56 17
115SN L 1825.0
115SN E 0.08 7.0
115SNS E CK=0.8570 $CL=0.1135 $CM+=0.02925
115SN G 1212.1 100.09 3
115SN G 1327.4 3 0.24 3
115SN G 1825.2 3 0.52 4
115SN L 1857.4
115SN E 0.07 7.0
115SNS E CK=0.8570 $CL=0.1137 $CM+=0.02929
115SN G 1360.1 3 0.63 5 C
115SN G 1857 1 0.10 CA S
115SN cG E from 1975Ma38 in-beam reaction
115SN cG RI from I|g(1857|g)/I|g(1360|g)=0.15 (1975Ma38) via (|a,n|g)
115SN L 2060.2
115SN G 1562.6 3 0.19 4
115SN G 2060.7 5 0.06 2
115SN L 2193.2 (3/2+,5/2+)
115SN E 0.16 6.4
115SNS E CK=0.8548 $CL=0.11538 15 $CM+=0.02980 5
115SN G 1207.0 100.41 4
115SN G 1579.9 3 0.09 3
115SN G 1696.1 3 0.92 6 C
115SN G 2194.0 6 0.19 3
115SN L 2230.0 3/2+,5/2+
115SN cL J based on |g-decays to 1/2+,3/2+,5/2+ states and log|
115SNxcL {Ift}=6.2
115SN E 0.22 6.2
115SNS E CK=0.8545 $CL=0.11566 17 $CM+=0.02989 5
115SN G 1243.7 3 0.45 4 C
115SN cG E$placed from a 1857 level in (p,n|g)
115SN G 1732.6 4 0.50 15 C
115SN G 2229.5 5 1.3 1
115SN L 2364.6 3/2+,5/2+
115SN cL E may correspond with L=2, 2355-keV (d,t) and 2360-keV
115SN2cL (p,d) excitations
115SN cL J based on |g-decays to 1/2+,3/2+,5/2+ states and log|
115SNxcL {Ift}=6.4
115SN cL Branching: I|g(1378|g)/I|g(1867|g)/I|g(2365|g)=14
115SN2cL {I2}/100/23 {I9} (1974Ki07), 7 {I3}/100/21 {I5} (1975WiZX); I|g-ratios
115SN3cL via in-beam (1975Ma38) are different
115SN E 0.09 6.4
115SNS E CK=0.8528 $CL=0.11695 25 $CM+=0.03028 8
115SN G 1377.8 4 0.13 3
115SN G 1867.4 4 0.61 4 C
115SN G 2364.8 5 0.04 2