195PT    195IR B- DECAY (2.29 H)       1973JA10                  14NDS    201408
195PT  H TYP=FUL$AUT=Huang Xiaolong and Kang Mengxiao$CIT=NDS 121, 395 (2014)$
195PT2 H CUT=1-Mar-2014$
195PT c  Others: 1968Ho01, 1968Ja06.
195PT c  1973Ja10: measured E|g, I|g, E(ce), and |b|g-coin with Ge(Li) and
195PTxc  Si(Li).
195PT c  Sources produced by {+195}Pt(n,p) (1954Bu02,1968Ja06), {+198}Pt(p,|a)
195PT2c  (1973Ja10), {+198}Pt(d,|an) (1968Ja06), and {+192}Os(|a,p) (1968Ho01).
195PT cL E         From decay scheme and E|g using least-squares fit to data
195PT cL J,T       From adopted levels.
195PT cL           All data are shown in the drawing.
195PT cB IB        From photon intensity imbalance, except for I|b(g.s.)=13
195PTxcB {I9}.
195PT cG E         Adopted value in 1973Ja10.
195PT cG RI$I|g(3.67 h component), deduced from 3.67-h {+195}Ir |b{+-}
195PT2cG decay scheme by evaluator.
195PT c  Energy balance: total decay energy of 1089 keV {I222} deduced
195PT2c  (using RADLIST code) from proposed decay scheme is in agreement with
195PT3c  the expected value of 1102.0 keV {I21} (2012Wa38),
195PT4c  suggesting that the decay scheme is reasonably complete.
195IR  P 0.0         3/2+              2.29 H    17             1102.0    21
195PT  N 0.099     25          1.0       1.0
195PT cN NR        Assuming %I|b(to g.s.)=13 {I9} (1973Ja10)
195PT PN                                                                     3
195PT cG           For |g-ray properties, see {+195}Au |e decay.
195PT2cG Other possible photons: see unplaced |g's in 3.67-h {+195}Ir decay
195PT cG RI        From I|g(2.29 h + 3.67 h) minus I|g(3.67 h). Relative photon
195PT2cG intensity normalized to I|g(E|g=98.85)=101
195PT cG M,MR      From |a(K)exp
195PT  L 0.0         1/2-              STABLE
195PT  B             13      9              7.0   3
195PTS B EAV=370.50 83
195PT cB E         1150 {I100} (1973Ja10); 1160 {I100} (1968Ja06) mixed
195PTxcB {+195}Ir+{+196}Ir |b's
195PT cB IB        I|b(1150|b)/I|b(980|b)=0.15 {I10} (1973Ja10).
195PT  L 98.830    103/2-
195PT  B             25      18             6.5   4
195PTS B EAV=332.07 81
195PT  G 98.83     1 101     11M1+E2     -0.130  4     6.86
195PTS G KC=5.58 8$LC=0.983 14$MC=0.229 4$NC+=0.0673 10
195PT cG RI        from I|g(2.29 h and 3.67 h components)=210 {I10} and
195PT2cG I|g(3.67 h component)=109.3 {I18}
195PT  L 129.71     35/2-
195PT  B             57      22            6.13  17
195PTS B EAV=320.23 81
195PT cB E         980 {I40} (1973Ja10) |b(99|g)-coin; doublet to 99+130 states
195PT  G 30.88     4 14      4 M1+E2     -0.021  4     37.7
195PTS G LC=29.0 5$MC=6.73 11$NC+=1.98 3
195PT cG RI        from I|g(2.29 h and 3.67 h components)=33 {I4} and
195PT2cG I|g(3.67 h component)=19.3 {I3}
195PT  G 129.71    4 14      3 E2                      1.732
195PTS G KC=0.468 7$LC=0.950 14$MC=0.245 4$NC+=0.0692 10
195PT cG RI        from I|g(2.29 h and 3.67 h components)=31 {I2} and
195PT2cG I|g(3.67 h component)=17.4 {I15}
195PT  L   211.30  103/2-
195PT  B             4.3     11            7.12  12
195PTS B EAV=289.19 80
195PT  G 211.30    1025      3 M1+E2     +0.38   3     0.738  14
195PT cG E$from 1973Ja10
195PTS G KC=0.596 13$LC=0.1091 16$MC=0.0255 4$NC+=0.00750 11
195PT cG RI        from I|g(2.29 h and 3.67 h components)=45 {I2} and
195PT2cG I|g(3.67 h component)=20.1 {I23}