196PT 196AU EC DECAY (6.1669 D) 1967JA02,1963IK01 07NDS 200706
196PT H TYP=FUL$AUT=Huang Xiaolong$CIT=NDS 108, 1093 (2007)$CUT=1-Jan-2006$
196PT c Source prepared by {+196}Pt(d,2n), enriched target, chem, |g's semi
196PT2c (1967Ja02); natural Pt(p,n) and {+197}Au(|g,n), chem, cryst |g, s ce
196PT3c (1963Ik01).
196PT c The adopted level scheme is essentially that given by 1967Ja02.
196PT cL E From least-squares fit to E|g's
196PT cL J From adopted levels, except as noted.
196PT cE IE From intensity balance at each level
196PT N 0.935 28 0.930 3 1.075269
196PT cN NR From |e+|b{++}(g.s.)|<0.9% and |b{+-}(g.s.)|<0.3%
196PT2cN (systematics of log| {Ift} in neighboring nuclei) and [I(|g+ce)(356|g,
196PT3cN with |e decay)+I(|g+ce) (426|g, with |b{+-}
196PTxcN decay)]=100%-|e+|b{++}(g.s.)-|b{+-}(g.s.)=100-0.6 {I6}=99.4 % {I6}.
196PT PN 1.0
196AU P 0.0 2- 6.1669 D 6 1507 3
196PT L 0.0 0+ STABLE
196PT E 0.9 LT 10.4 GT 1U
196PTS E CK=0.7907$CL=0.15782 5$CM+=0.05138 2
196PT cE IE <0.9 estimated from |b{+-} systematics (calculated and
196PT2cE observed |e/|b{++})
196PT L 355.73 5 2+ 32 PS 2
196PT cL E$from 1961Be14
196PT cL J$supported by E2 transition, Coul. ex.
196PT cL T$weighted av of 30.2 ps {I21}, delayed coin (1972Be53);
196PT2cL 35.4 ps {I35}, recoil-distance Doppler shift (1971NoZT)
196PT E 67.0 21 7.392 14
196PTS E CK=0.8026$CL=0.14939 4$CM+=0.04806 2
196PT cE IE I|e/I|b=2.0|*10{+6} {I4} (1963Ik01)
196PT G 355.73 5 100 E2 0.0603 C
196PT cG E from 1961Be14, 1976HeZF; also 355.68 {I6} (1960De17,
196PT2cG calibration correction by evaluators)
196PT cG M supported by |a(K)exp: 0.0395 {I22} (1962Ja10), 0.041 {I3}
196PT2cG and 0.042 {I3} (1962Ge07), 0.0367 {I24} (1960De17), 0.042 {I3}
196PT3cG (1956Th10). Theory: |a(K)(E2)=0.0404, |a(K)(M1)=0.165
196PTS G KC=0.0402 6$LC=0.01519 22$MC=0.00377 6$NC+=0.001081 16
196PT L 688.76 7 2+ 38 PS 4
196PT cL E from 1961Be14
196PT cL J supported by E0+M1+E2 transition to 356 level
196PT cL T from delayed coin, renormalized to T{-1/2}(356)=32 ps
196PTxcL (1972Be53)
196PT E 24.6 10 7.509 18
196PTS E CK=0.7941 2$CL=0.15547 8$CM+=0.05040 3
196PT G 333.03 5 26.3 6E0+M1+E2 5.2 5 0.0782 17 C
196PT cG |a(K)=0.051, |a(L)=0.021 (from |a(K)exp and K/L/M+N+O from
196PTxcG E2 theory)
196PT cG E from 1961Be14
196PT cG RI from 1967Ja02
196PT cG M based upon angular correlation; see comment under |d. Also
196PT2cG from |a(K)exp: 0.059 {I4} (1956Th10), 0.056 {I3} (1962Ge07), 0.048 {I5}
196PT3cG (1967Ja02,1963Ik01); also 1961Be14, theory: |a(K)(E2)=0.050,
196PTxcG |a(K)(M1)=0.253.
196PT cG M theory predicts that monopole internal conversion
196PT2cG transitions between states of equal J|p can compete with E2
196PT3cG transitions. Although conversion coefficients may be too insensitive to
196PT4cG detect E0 admixtures, angular correlations have been so used. Two
196PT5cG solutions have been identified. Q, |l: -0.22 {I7}, 2 {I6}, and +0.39
196PT6cG {I5}, 68 {I12} (1965Pe06); -0.25 {I11}, 2 {I7}, and +0.42 {I6}, 62
196PT7cG {I15} (1968IkZZ); -0.23 +16-20, 6 {I9}, and +0.44 {I+9-10}, 67 {I11}
196PT8cG (1971Do12). Q**2=(E0 ce)/(E2 ce) and |l=penetration factor. See also
196PT9cG 1955Ch65, 1956Ch21, 1958Ch48, 1958Ge37, 1962Ge07
196PT cG MR 5.2 adopted.
196PT cG MR from angular correlation measurements: |d=-5 {I1} (1953St05),
196PT2cG |d=-5.0 {I5} (1963Ik01), |d=-4.9 {I2} (1965Pe06), |d=-4.03 {I12}
196PT3cG (1969Ha43), |d=-5.7 {I3} (1971Kr01)
196PTS G KC=0.0523 14$LC=0.0196 3$MC=0.00487 7$NC+=0.001398 21
196PT G 688.76 0.007 2(E2) 0.01184 C
196PT cG RI from 1967Ja02; also |a(K)exp(689)/|a(K)exp(356)<2|*10{+-5}
196PT2cG (1963Ik01), |a(K)exp(689)/|a(K)exp(333)<1/12000 (1957Al45), I|g=0.003
196PT3cG {I2} (1962Wa16), I|g(688.7)/ I|g(333.0)|<6.|*10{+-5} (1972Be53)
196PT cG M |a(K)exp=0.006 {I6} (1967Ja02,1963Ik01)
196PTS G KC=0.00924 13$LC=0.00199 3$MC=0.000473 7$NC+=0.0001375 20
196PT L 877.0 2 4+
196PT cL E from coin observation of 521.4 and 355.7 |g's
196PTxcL (1962Wa16,1963Ik01)
196PT cL J supported by E2 character of 521.4|g, E1 character of 571|g,
196PT2cL as well as log| {Ift}. See also {+196}Ir |b{+-} decay.
196PT E 0.380 15 9.167 20 1U
196PTS E CK=0.7319 6$CL=0.1998 5$CM+=0.06828 17
196PT G 521.4 2 0.447 10E2 0.0224 C
196PT cG E from 1967Ja02, also 521.3 {I7} (1962Wa16)
196PT cG RI from 1967Ja02, also 1963Ik01
196PT cG M supported by |a(K)exp=0.015 {I2} (Ice(K) from 1963Ik01, I|g
196PT2cG from 1967Ja02). |a(K)(theory)=0.017; see also {+196}Ir(1.4-h) |b{+-}
196PTxcG decay.
196PTS G KC=0.01666 24$LC=0.00435 7$MC=0.001054 15$NC+=0.000305 5
196PT L 1015.2 3(2+,3+)
196PT cL E supported by coin between 326, 333 and 356 |g's.
196PT cL J if 659 |g is M1
196PT E 0.057 15 9.65 12
196PTS E CK=0.7726 4$CL=0.1710 3$CM+=0.05643 11
196PT G 326.2 4 0.057 13[M1] 0.243 C
196PT cG E|g,I|g: from 1967Ja02, seen in |g|g-coin
196PTS G KC=0.201 3$LC=0.0327 5$MC=0.00755 11$NC+=0.00223 4
196PT G 659.5 3 0.0042 3(M1) 0.0379 C
196PT cG E|g,I|g: from 1967Ja02
196PT cG M |a(K)exp=0.029 {I10} (if the 645 K-line of 1963Ik01 may be
196PT2cG identified with the 659.5|g)
196PTS G KC=0.0314 5$LC=0.00501 7$MC=0.001153 17$NC+=0.000340 5
196PT L 1270.4 105- ?
196PT E 0.0102 7 9.61 4
196PTS E CK=0.693 3$CL=0.2277 19$CM+=0.0789 8
196PT G 393.4 4 0.0116 6E1 0.01395 C
196PT cG E placement based upon observation of coin with 356|g and
196PT2cG absence of coin with either 333 or 326 |g. See also {+196}Ir |b{+-}
196PTxcG decay.
196PTS G KC=0.01159 17$LC=0.00182 3$MC=0.000419 6$NC+=0.0001220 18
196PT L 1361.5 5(1+,2+)
196PT E 0.0059 5 9.22 5
196PTS E CK=0.534 12$CL=0.340 9$CM+=0.125 4
196PT G 673.5 7 0.0031 3(M1+E2) 0.024 12 C
196PT cG E|g,I|g: from 1967Ja02
196PTS G KC=0.020 10$LC=0.0034 14$MC=0.0008 3$NC+=0.00023 9
196PT G 1005.7 3 0.0031 3 C
196PT cG E|g,I|g: from 1967Ja02; also 1962Wa16,1963Ik01
196PT G 1361.0 10 0.0005 2[E2] 0.00305
196PT cG E|g,I|g: from 1967Ja02
196PTS G KC=0.00249 4$LC=0.000410 6$MC=9.48E-5 14$NC+=5.61E-5 8
196PT L 1447.3 8(3)-
196PT cL E from 1091.4 and 355.7 |g's
196PT cL J supported by E1 character of 1091 and 759 |g's.
196PT E 0.210 9 6.45 6
196PTS E CL=0.677 6$CM+=0.323 6
196PT G 432.0 3 0.0077 7[E1,M2] 0.19 18 C
196PT cG E|g,I|g: from 1967Ja02, seen in |g|g-coin
196PTS G KC=0.15 14$LC=0.03 3$MC=0.007 7$NC+=0.0021 21
196PT G 570.8 4 0.0079 6(E1+M2) 0.08 8 C
196PTS G KC=0.07 7$LC=0.013 12
196PT cG E|g,I|g: from 1967Ja02
196PT cG M |a(K)exp=0.016 {I6} (1967Ja02), |a(K)exp=0.0061 (1963Ik01)
196PT G 759.1 3 0.051 2(E1) 0.00355 C
196PT cG E|g,I|g: from 1967Ja02
196PT cG M supported by |a(K)exp=0.0032 {I8}, theory: |a(K)(E1)=0.0030
196PTS G KC=0.00297 5$LC=0.000444 7$MC=0.0001014 15$NC+=2.97E-5 5
196PT G 1091.4 2 0.171 7E1 0.00181 C
196PT cG E|g,I|g: from 1967Ja02; also 1963Ik01,1962Wa16
196PT cG M supported by |a(K)exp=0.0016 {I2} (1967Ja02,1963Ik01), also
196PT2cG 1961Be14; theory: |a(K)(E1)=0.0015
196PTS G KC=0.001521 22$LC=0.000222 4$MC=5.06E-5 7$NC+=1.486E-5 21
196PT G 1446.3 7 .0009 2[E3] 0.00555
196PT cG E|g,I|g: from 1967Ja02
196PTS G KC=0.00442 7$LC=0.000849 12$MC=0.000200 3$NC+=7.99E-5 12