50MN    50FE EC DECAY (152.0 MS)      2015MO01                  19NDS    201906
 50MN  H TYP=FUL$AUT=Jun Chen and Balraj Singh$CIT=NDS 157, 1 (2019)$
 50MN2 H CUT=15-Apr-2019$
 50MN c  2015Mo01: {+50}Fe ions were produced from fragmentation of
 50MN2c  680 MeV/nucleon {+58}Ni beam with 400 mg/cm{+2} {+9}Be target using
 50MN3c  SIS-18 synchrotron at GSI facility. Reaction fragments were separated
 50MN4c  in-flight using the fragment separator FRS. The identification of
 50MN5c  nuclei was achieved by the measurement of magnetic rigidity and
 50MN6c  velocity of fragments by time-of-flight method. Separated ions were
 50MN7c  implanted in one of the six double-sided silicon strip detectors
 50MN8c  (DSSSDs). The |b-decay signals were detected in the same DSSSD.
 50MN9c  Surrounding the implantation setup was the RISING array of 15 Euroball
 50MNAc  cluster Ge detectors for |g detection. Measured E|g, I|g, |g|g-coin,
 50MNBc  |b|g-coin, and |b-decay half-life. Deduced levels, J, |p, |b feedings,
 50MNCc  log| {Ift} values, Gamow-Teller strengths
 50MN d  2011MoZR is a conference report from authors of 2015Mo01
 50MN c  1997Ko46: {+50}Fe produced in {+40}Ca({+12}C,2n) reaction at the Chalk
 50MN2c  River TASCC Facility. Measured E|g, |g(t) using HPGe, scintillation
 50MN3c  detector, gas counter, and He-jet. Energy of only the 651|g reported
 50MN4c  in this work
 50MN cE TI$From 2015Mo01, based on in-out intensity balance. For the
 50MN2cE ground state, |e+|b{++} feeding is from 100-(summed |e+|b{++}
 50MN3cE feeding to excited states).
 50MN cE LOGFT$Deduced by evaluator using the LOGFT code. Values in
 50MN2cE 2015Mo01 are slightly different
 50MN cG M$From Adopted Gammas
 50MN cL E$From least-squares fit to E|g data
 50MN cL J$From the Adopted Levels.
 50FE  P 0.0         0+                152.0 MS  6              8151      8
 50FE cP T$From {+50}Fe Adopted Levels. Measured value is 152.1 ms {I6} by
 50FE2cP 2015Mo01
 50FE cP QP$From 2017Wa10
 50MN  N 0.225     14           1        1
 50MN cN NR$From determination of number of 651-keV |g rays emitted per
 50MN2cN {+50}Fe decay, using the formula
 50MN3cN I|g(651)=N{+0}(651|g)/[N{+0}{-|b}|e(651|g)], where N{+0}(651|g)
 50MN4cN is the total number of |g events in the implant-|b-|g correlation
 50MN5cN fit, N{+0}{-|b} is the total number of |b events in the implant-|b
 50MN6cN correlation fit, and |e is the detector efficiency for 651|g.
 50MN7cN The |ep decay mode of {+60}Fe is expected to be negligible
 50MN PN                                                                     3
 50MN  L 0.0         0+                283.19 MS 10
 50MN cL T$from Adopted Levels
 50MN  E               74.1  14 0.0710 15  3.49   1             74.2      14
 50MNS E EAV=3358.1 40$CK=0.000853 3$CL=8.94E-5 3$CM+=1.557E-5 6
 50MN cE TI$100-(|b feeding to all the excited states)
 50MN  L 651.00    6  1+
 50MN  E               22.5  14 0.0286 18  3.81   3             22.5      14
 50MNS E EAV=3037.7 40$CK=0.001132 5$CL=0.0001186 5$CM+=2.068E-5 8
 50MN CE $^B(^GT+)=0.589 {I45} (2015Mo01). Other: 0.568 {I16} from ({+3}He,t)
 50MN2cE (2005Fu16) adjusted for new T{-1/2}
 50MN  G 650.99    6   100.0 35 M1
 50MN cG E$from 1997Ko46. Other: 651.0 {I1} (2015Mo01)
 50MN  L 800.01    9  2+
 50MN  G  149.0     1 1.53   14 (M1)
 50MN  G  799.6     2 0.98   12 E2
 50MN  L 2403.84   10 1+
 50MN  E               1.47  10 0.0048 3   4.36   3             1.47      10
 50MNS E EAV=2180.2 39$CK=0.002880 15$CL=0.0003020 1$CM+=5.26E-5 3
 50MN CE $^B(^GT+)=0.167 {I15} (2015Mo01). Other: 0.171 {I5} from ({+3}He,t)
 50MN2cE (2005Fu16) adjusted for new T{-1/2}
 50MN  G 1603.7     2 0.89   11
 50MN  G 2403.8     1 5.54   26
 50MN  L 2684.19   10 1+
 50MN  E               0.70  6  0.0027 2   4.56   4              0.70     6
 50MNS E EAV=2044.0 39$CK=0.003451 19$CL=0.0003620 2$CM+=6.31E-5 4
 50MN CE $^B(^GT+)=0.106 {I11} (2015Mo01). Other: 0.123 {I4} from ({+3}He,t)
 50MN2cE (2005Fu16) adjusted for new T{-1/2}
 50MN  G 1883.8     2  0.28  8
 50MN  G 2684.2     1  2.79  19
 50MN  L 3380.12   10 1+
 50MN  E               0.84  7  0.0055 5   4.14   4             0.85      7
 50MNS E EAV=1707.4 39$CK=0.00572 4$CL=0.000600 4$CM+=0.0001045 7
 50MN CE $^B(^GT+)=0.280 {I31} (2015Mo01). Other: 0.400 {I12} from ({+3}He,t)
 50MN2cE (2005Fu16) adjusted for new T{-1/2}
 50MN  G 3380.0    1  3.75   22
 50MN  L 3643.5     3 1+
 50MN  E               0.15  3  0.0012 2   4.8    1             0.15      3
 50MNS E EAV=1580.8 39$CK=0.00709 5$CL=0.000744 5$CM+=0.0001297 9
 50MN CE $^B(^GT+)=0.069 {I15} (2015Mo01). Other: 0.163 {I5} from ({+3}He,t)
 50MN2cE (2005Fu16) adjusted for new T{-1/2}
 50MN  G 3643.4     3 0.66   12
 50MN  L 4012.9    12 1+
 50MN  E               0.04  2  0.0004 2   5.1   2              0.04      2
 50MNS E EAV=1404.0 39$CK=0.00989 8$CL=0.001038 8$CM+=0.0001809 1
 50MN CE $^B(^GT+)=0.034 {I16} (2015Mo01). Other: 0.076 {I2} from ({+3}He,t)
 50MN2cE (2005Fu16), adjusted for new T{-1/2}
 50MN  G 4012.7    12 0.19   9
 50MN  L 4315.9    14 1+
 50MN  E               0.08  3   0.001 1   4.6   2              0.08      3
 50MNS E EAV=1259.9 39$CK=0.01340 12$CL=0.001407 13$CM+=0.0002451 2
 50MN CE $^B(^GT+)=0.099 {I38} (2015Mo01). Other: 0.119 {I3} from ({+3}He,t)
 50MN2cE (2005Fu16), adjusted for new T{-1/2}
 50MN  G 4315.7    14 0.36   14