57V     57TI B- DECAY (98 MS)         2005LI53                  ENSDF    201004
 57V   H TYP=FUL$AUT=BALRAJ SINGH$CUT=12-APR-2010$CIT=ENSDF$
 57V  c  2005Li53: {+57}Ti isotope produced in fragmentation of {+86}Kr{+34+}
 57V 2c  beam on a {+9}Be target.  Secondary fragments were selected using the
 57V 3c  A1900 fragment separator.  Fragment identification was performed by a
 57V 4c  combination of multiple energy-loss signals and time of flight method.
 57V 5c  Measured E|g, I|g, |g|g, |g|b(t), lifetime with 12 Ge detectors from
 57V 6c  the MSU segmented Ge array and double-sided Si microstrip detector.
 57V  cB IB$ deduced by the evaluator from |g-ray intensity balances and the
 57V 2cB ground state feeding deduced by 2005Li53 from the total number of
 57V 3cB {+57}Ti nuclei implanted in the Double-sided Si microstrip detector
 57V 4cB (DSSD). The listed |b feedings should be treated as apparent values
 57V  cB LOGFT$ All values are considered as lower limits.
 57V  cL E$ from least-squares fit to E|g's
 57TI  P 0.0           (5/2-)           98 MS    5              10.64E3   51
 57TI cP T$ Deduced from fit of the fragment-|b-decay curve considering the
 57TI2cP exponential decay of the parent, exponential growth, and decay of the
 57TI3cP daughter {+57}V, and a linear background term.  The value obtained
 57TI4cP was compared with that obtained from fragment-|b-|g decay curves for
 57TI5cP each of the transitions assigned to {+57}Ti (2005Li43). See adopted
 57TI6cP levels of {+57}Ti for previous half-life measurements
 57TI cP J$ From {+57}Ti adopted levels
 57TI cP QP$ from 2009AuZZ, 2003Au03.
 57V   N 1                      1          1
 57V  cN NR$ Absolute |g-ray intensities are given in 2005Li43
 57V  PN                                                                     4
 57V   G 2003.7    6  1.8    5
 57V   G 2114.6    5  0.7    3
 57V   L 0.0          (7/2-)
 57V   B              53.8   23            4.7
 57V S B EAV=5.02E3 25
 57V   L 113.2      4
 57V   G 113.1     4  14     1                                               C
 57V   L 174.8      4
 57V   B              5      5              5.7
 57V S B EAV=4.94E3 25
 57V   G 61.7         11     3                                                 S
 57V  cG E$ existence of transition deduced from observed coincidence between
 57V 2cG the 113 and 175 |g rays.  Such a transition is below the
 57V 3cG detection threshold.
 57V   G 174.8     4  31     2                                               C
 57V   L 1731.9     4
 57V   B              1.1    7              6.0
 57V S B EAV=4.18E3 25
 57V   G 1557.3    5  2.2    5                                               C
 57V   G 1732.2    6  1.2    2                                               C
 57V   L 1754.3     5                                                          ?
 57V   B              16     2             4.9                                 ?
 57V S B EAV=4.17E3 25
 57V   G 1579.4    4  16     2                                               C ?
 57V   L 2036.3     4
 57V   B              16.6   21            4.8
 57V S B EAV=4.03E3 25
 57V   G 1861.5    4  14     2                                               C
 57V   G 1922.9    5  2.6    5                                               C
 57V   L 2475.6     5
 57V   B              7.3    7             5.0
 57V S B EAV=3.81E3 25
 57V   G 744.0     4  2.3    4                                               C
 57V   G 2300.4    4  5.0    5                                               C