198AU    198AU IT DECAY (2.272 D)      1972CU06,1973PA08,1975MA3016NDS    201603
198AU  H TYP=FUL$AUT=Huang Xiaolong and Kang Mengxiao$CIT=NDS 133, 221 (2016)$
198AU2 H CUT=1-Dec-2015$
198AU c  Sources produced by {+200}Hg(d,|a) (1972Cu06), {+197}Au(d,p)
198AU2c  (1968Bo30,1973Pa08), {+198}Hg(n,p) (1973Pa08), {+196}Pt(|a,pn)
198AU3c  (1975Ma30), {+198}Pt(d,2n) (1975Ma30), and
198AU4c  {+197}Au(n,|g) (1990Pi08). {+200}Hg(d,|a) E=18 MeV (1972Cu06), chem.;
198AU5c  {+197}Au(d,p) E=12.5 MeV (1968Bo30,1973Pa08);
198AU6c  {+198}Hg(n,p) E=14.5 MeV (1973Pa08), chem.;
198AU7c  {+196}Pt(|a,pn) E=35 MeV, {+198}Pt(d,2n) E=18 MeV (1975Ma30), chem.
198AU c  {+197}Au(d,p|g) |g(t) (1968Bo30) prompt and delayed |g spectra
198AU cG E$From 1972Cu06 (semi), except as noted.
198AU c  Level scheme is consistent with |g|g(t) spectra (1972Cu06,1973Pa08)
198AU tG
198AU tG             K  x-ray  Intensities   (1990Pi08)
198AU tG $-----------------------------------------------------
198AU tG
198AU tG $  Radiations          E,keV{+a}         Intensities{+b}
198AU tG $ ------------        ----------         -------------
198AU tG $    K|a{-1}| x-ray         68.8037 {I8}             47
198AU tG $    K|a{-2}| x-ray         66.9895 {I8}             28
198AU tG $    K|b| x-ray          78.00                 21.4
198AU tG
198AU tG $ a  Calculated values
198AU tG $ b  Measured values per 100 decays (1990Pi08)
198AU tG
198AU  P 811.7     15(12-)             2.272 D   16
198AU  N 0.773     3 0.773   3 1.0
198AU cN NR        No |b{+-} or |e decay observed and I(|g+ce)(to g.s.)=100
198AU PN 0.77      1 0.77    1                                               3
198AU cL E         From decay scheme, using least-squares fit to E|g values
198AU cL J         From Adopted Levels, except as noted.
198AU cL J(A)      From analogy with {+196}Au
198AU cL T         From Adopted Levels.
198AU cG RI        Relative intensity normalized to I|g(214.89|g)=100.
198AU2cG Values are from 1973Pa08.
198AU cG M         Deduced from |a(K)exp=ce(K)/I|g (1973Pa08) normalized to
198AU2cG |a(K)(215|g)=0.142 (E2 theory), except as noted.
198AU cG M(M)      From Adopted Gamma radiations.
198AU  L 0.0         2-                2.6941 D  2
198AU  L     214.89 54-
198AU  G 214.89    5 100       E2                      0.294                 C
198AUS G KC=0.1421 20$LC=0.1140 16$MC=0.0292 4$NC+=0.00839 12
198AU cG M         From K:L1:L2:L3:M=100 {I5}:7 {I3}:45 {I4}:23 {I5}:18 {I3}
198AU2cG (1966Eg01) in (n,|g)
198AU  L     312.10 75+                124 NS    4
198AU  G 97.21     5 89      6 E1                      0.445                 C
198AUS G KC=0.356 5$LC=0.0684 10$MC=0.01594 23$NC+=0.00460 7
198AU3 G FLAG=M$
198AU  L     516.2010 6+                                                       ?
198AU2 L FLAG=A$
198AU cL E         Order of 180|g-204|g cascade is tentative;
198AU2cL alternatively, E(level)=492.4, J|p=(7+)
198AU  G 204.10    6 50      6 M1                      0.959                 C
198AUS G KC=0.789 11$LC=0.1311 19$MC=0.0304 5$NC+=0.00906 13
198AU3 G FLAG=M$
198AU cG           |a(K)exp=0.83 {I15}
198AU cG M         M1+(E2) from |g anisotropy I|g(|q,t) in Ni (1975Ma30)
198AU2cG with |d=-0.10 5
198AU  L     645.9217                                                          S
198AU cL E         Possible a proposed 646 level could resolve intensity
198AU2cL imbalance at the 312 level. It could be fed directly from the isomer,
198AU3cL or via a low-energy transition from 696-level. The latter is more
198AU4cL likely, and would suggest I(|g+ce)(115.2|g)=100. Neither author would
198AU5cL have seen a highly converted 50|g connecting the 696 and the possible
198AU6cL 646 level. Unplaced 333.82|g could be placed between 646 and 312
198AUxcL levels.
198AU  G 333.82    1523      5 M1                      0.248
198AUS G KC=0.205 3$LC=0.0337 5$MC=0.0078 1$NC+=0.0019 3
198AU cG           |a(K)exp<0.3
198AU cG M         Dipole with |DJ=+1 from |g anisotropy  I|g(|q,t) (1975Ma30).
198AU  L     696.5111 8+
198AU2 L FLAG=A$
198AU  G 50.5                                                   29        6    S
198AU cG           50.5|g would not have been seen experimentally since it is
198AU2cG expected to have a large conversion coefficient
198AU cG TI        From I(|g+ce) value of 333.82|g
198AU  G 180.31    5 64      6 E2                      0.537                 C
198AUS G KC=0.219 3$LC=0.239 4$MC=0.0616 9$NC+=0.01767 25
198AU cG           |a(K)exp=0.20 {I7}; also |g anisotropy I|g(|q,t) (1975Ma30)
198AU  L      811.715(12-)             2.272 D   16                          M
198AU2 L FLAG=A$MOMM1=(+)5.85 9 (2005St24)
198AU3 L %IT=100$
198AU CL           MOMM1 from NMR/^ON (2005ST24)
198AU cL           No |b{+-} or |e branching observed (1972Cu06,1973Pa08)
198AU  G 115.2     150.052   5 (M4)                    2.49E3 22             C
198AUS G KC=185 5$LC=1620 150$MC=530 50$NC+=160 15
198AU cG E         From 1973Pa08
198AU cG RI        From I(|g+ce) and |a
198AU cG           I|g(exp)<1.5 (1973Pa08)
198AU cG           ce(L)=99 {I14}, |a(L)=1670 (1973Pa08).
198AU cG M         M3, M4, E4 from |a(L)exp>56; M3 ruled out from no evidence
198AU2cG of ce(K); B(M4)(W.u.)=0.31 is consistent with B(M4)(W.u.)=0.24
198AU3cG ({+196}Au), 0.48 ({+195}Au), 0.25 ({+198}Tl)