57MN    57CR B- DECAY                 1978DA04                  98NDS    199812
 57MN  H TYP=FUL$AUT=M. R. BHAT$CIT=NDS 85, 415 (1998)$CUT=24-Sep-1998$
 57CR  P   0.0       3/2-,5/2-,7/2-     21.1 S     10           5.09E+3   9
 57MN c  Measured |g's, |b's, 205.8|g(t), and |g|g- and |b|g-coincidences;
 57MN2c  Ge(Li), scintillator; rabbit and helium-jet systems. 83|g and 850|g
 57MN3c  obscured by contaminants from {+56}Cr and {+56}Mn.
 57MN cL           Decay scheme constructed from |g|g-coincidence and singles
 57MNxcL data
 57MN cG           Identification made by T{-1/2} or coincidence relationships
 57MN DB EAV       CALCULATED BY EVALUATORS
 57MN cL E         Calculated using least-squares adjustment
 57MN2cL procedures; good agreement with 1978Da04.
 57MN DL E$UNCERTAINTY GENERALLY SMALLER THAN THE 0.4 KEV ESTIMATED BY 1978Da04
 57MN2DL FOR THE LOWER STATES AND LARGER FOR THE HIGHER STATES
 57MN cL J         From adopted levels. Assignments suggested by 1978Da04 are
 57MN2cL given under comments. These suggested assignments are based on log|
 57MN3cL {Ift} and existence of |g's with the assumption that
 57MN4cL J|p({+57}Cr)=3/2-. The argument for J|p({+57}Cr)=3/2- depends on the
 57MN5cL transition to the 2186 state. The evaluators do not adopt this
 57MN6cL argument since J(2186)=1/2 is based on a calculation (1978An10) in
 57MN7cL (|a,p) and |D(log ft) does not permit the statement that the
 57MNxcL transition is allowed.
 57MN DB E         ENERGY CALIBRATION BY MEANS OF OTHER KNOWN BETA SPECTRA
 57MN2DB OBTAINED IN THE SAME BG MEASUREMENT
 57MN cB IB        Calculated from intensity balancing at each
 57MN2cB state, except as noted; in good agreement with 1978Da04 although |DI|b
 57MN3cB are generally higher here
 57MN cG RI        Relative intensity. Some I|g's had to be obtained from
 57MN2cG the 83|g coincidence spectrum because of low intensity or interference
 57MN3cG from other lines in the singles spectrum
 57MN  N 0.052     25          1            1
 57MN cN NR        from |SI|g(1+|a) to g.s. and I|b(to g.s.)=74% {i12}
 57MN PN                                                                     5
 57MN cG CC        Calculated using adopted E|g
 57MN DG           KC,LC:  CALCULATED USING ADOPTED EG
 57MN cG M,MR      From adopted gammas
 57MN cG M(A),CC(A)$Added on basis of comment by 1978Da04 that,
 57MN2cG theoretically, there was 5% conversion for this |g.
 57MN cB IB(A)     The ratio of accumulated {+57}Cr to accumulated {+57}Mn
 57MN2cB activity was obtained from the helium-jet run. |s({+57}Mn)/|s({+57}Cr)
 57MN3cB was used to obtain the g.s. feeding. |DI|b also reflects the
 57MN4cB uncertainty in the ratio of production |s's.
 57MN  L   0.0              5/2-
 57MN  B                74   12          5.45    9
 57MNS B EAV AP 2.16E+3
 57MN3 B FLAG=A
 57MN  L    83.39  17 5/2-,7/2-
 57MN cL J         7/2-
 57MN  G    83.4   2   160   32(M1)                     0.0508               C
 57MNS G KC= 0.0449   $LC=0.00443
 57MN3 G FLAG=A
 57MN  L   850.16  23       3/2-
 57MN  B               2.7   23          6.5     4
 57MNS B EAV AP 1.75E+3
 57MN  G   766.5   5   6.7   16
 57MN  G   850.2   6   157   33 E2(+M1)
 57MN cG MR        +0.1 {I+4-1} or |<-5 from adopted gammas
 57MN  L   1055.87 231/2-,3/2-,5/2-
 57MN cL J         (1/2-)
 57MN  B               2.2   11          6.5     2
 57MNS B EAV AP 1.65E+3
 57MN  G   205.8   3   56.2  35 E2(+M1)
 57MN cG MR        |>+0.2 if J=3/2; |>+1 if J=5/2 from adopted gammas
 57MN DG E         NOTE APPARENT MISPRINT IN TABLE I OF 1978Da04 GIVING EG=105.8
 57MN2DG (EVALUATORS)
 57MN  G   1055.8  3   16.3  19
 57MN  L   1375.0  4  -
 57MN cL J         3/2,5/2
 57MN  B               0.4   3           7.1     4
 57MNS B EAV AP 1.49E+3
 57MN  G   1292.2  5   14.6  26
 57MN  L   1492.77 21 -
 57MN cL J         3/2,5/2
 57MN  B               0.8   5           6.7     3
 57MNS B EAV AP 1.44E+3
 57MN  G   1409.3  3   18.0  29
 57MN  G   1492.7  3   18.5  25
 57MN  L   1534.85 25 -
 57MN cL J         |<5/2-
 57MN  B  3.54E+3  13  6.    3           5.8     2                          C
 57MNS B EAV AP 1.42E+3
 57MN  G   479.1   5   3.6   14
 57MN  G   684.1   5   10.5  42
 57MN  G   1535.0  3   94.7  64                                              C
 57MN  L   1725.6  6  -
 57MN cL J         3/2,5/2
 57MN  B               0.22  13          7.2     3
 57MNS B EAV AP 1.33E+3
 57MN  G   1642.2  5   4.2   15
 57MN  L   1835.5  4  -
 57MN  B  3.28E+3  9   7.    4           5.6     3                          C
 57MNS B EAV AP 1.27E+3
 57MN  G   342.9   5   9.5   25
 57MN  G   1752.1  5   100                                                   C
 57MN  G   1835.2  6   26.8  24
 57MN  L   2146.9  9
 57MN cL J         3/2,5/2
 57MN  B               0.22  14          6.9     3
 57MNS B EAV AP 1.12E+3
 57MN  G   2063.5  8   4.3   15
 57MN  L   2185.8  4
 57MN cL J         1/2-
 57MN  B               2.6   14          5.8     2
 57MNS B EAV AP 1.11E+3
 57MN  G   1129.9  3   27.1  25
 57MN  G   1335.7  5   23.   10
 57MN  L   2232.9  6  5/2-,7/2-
 57MN cL J         (3/2-)
 57MN  L   2340.6  4  5/2+,3/2+
 57MN cL J         3/2,5/2
 57MN  B               0.24  22          6.8     4
 57MNS B EAV AP 1.03E+3
 57MN  G   2257.2  9   4.7   34
 57MN  L   2493.3  5
 57MN cL J         3/2-,5/2-
 57MN  B               1.7   9           5.8     2
 57MNS B EAV AP 9.6E+2
 57MN  G   2410.0  7   16.9  19
 57MN  G   2493.1  7   15.6  14
 57MN  L   2702.2  3 1/2- TO 7/2-
 57MN cL J         3/2-,5/2-
 57MN  B               2.6   13          5.5     2
 57MNS B EAV AP 8.6E+2
 57MN  G   1209.2  3   11.3  21
 57MN  G   1327.3  3   6.2   33
 57MN  G   1852.0  4   23.0  28
 57MN  G   2618.3  8   8.6   27