33S     33CL EC DECAY (2.5059 S)      1980WI13                  25NDS    202501
 33S   H TYP=FUL$AUT=Jun Chen and Balraj Singh$
 33S 2 H CIT=NDS 199, 1 (2025)$CUT=30-Sep-2024$
 33S  c  1980Wi13: {+33}Cl was produced by {+32}S(d,n){+33}Cl reaction with 11.0
 33S 2c  MeV deuterons from the ONR-CIT tandem accelerator on a natural sulphur
 33S 3c  target. |g rays were detected with a Ge(Li) detector. Measured E|g,
 33S 4c  I|g. Deduced levels, |e-decay branching ratios, log {Ift}. Comparisons
 33S 5c  with available data.
 33S  c  1987Bo21: {+33}Cl was produced from the |b{++}-decay of {+33}Ar at
 33S 2c  ISOLDE facility of CERN. |g rays were detected with a Ge(Li)
 33S 5c  detector. Measured E|g, I|g.
 33S  c  2014Ko17: {+33}Cl was produced from the |b{++}-decay of {+33}Ar at
 33S 2c  ISOLDE facility, CERN. The |g rays were detected with cluster
 33S 3c  detectors. Measured E|g, I|g for 841.3|g, 1966.9|g and 2867|g.
 33S  c  1970Ba65: {+33}Cl source was produced with 2.8 MeV deuteron beam
 33S 2c  on sulfur powder of either natural or enriched {+32}S. |g rays were
 33S 3c  detected with two coaxial Ge(Li) detectors. Measured E|g, I|g, |g(t).
 33S 4c  Deduced levels, parent T{-1/2}, |e-decay branching ratios, log {Ift}.
 33S  c  Half-life measurements: 1958Mu05, 1960Ja12, 1970Sc16, 1972Es02,
 33S 2c  1973Ta04, 1977Az01, 2015Gr14. Others: 1940Ho01, 1941Wh02,
 33S 3c  1948Sc20, 1951Bo56, 1954Ty33, 1960Wa04, 1962Va27, 1970Ba65
 33S  d  Older |g ray measurements: 1953Meyerhof: Phys Rev 93, 949 (1954);
 33S 2d  1953Nahmias: Compt. Rendu 236, 2399 (1953)
 33S  c  |b measurements: 1941Wh02, 1951Bo56, 1960Wa04, 1962Va27
 33S  cE TI$Deduced from measured |g-ray intensities, compared with measured
 33S 2cE intensity of 511-keV radiation produced by the annihilation for
 33S 3cE excited states (1970Ba65,1980Wi13), unless otherwise noted. Quoted
 33S 4cE values are from 1980Wi13.
 33S  cE TI(A)$Reported in 1980Wi13 as weighted average of value measured
 33S 2cE (but not listed) by 1980Wi13 and value from 1970Ba65.
 33S  cG $1987Bo21 report %I|g=0.55 {I6}, 0.42 {I4} and 0.55 {I5} for
 33S 2cG 841|g, 1966|g and 2867|g, respectively, as per 100 {+33}Ar decays,
 33S 3cG but from comparisons with values in 1980Wi13 and 1970Ba65, these
 33S 4cG values are more likely per 100 {+33}Cl decays.
 33S  cG E,RI$From 1980Wi13, unless otherwise noted. Values of intensities are
 33S 2cG relative to I|g(2866.8|g)=100
 33S  cG M,MR$From the Adopted Gammas
 33S  cL E$From a least-squares fit to |g-ray energies, assuming |DE|g=1 keV
 33S 2cL for E|g values without uncertainties.
 33S  cL J,T$From the Adopted Levels.
 33S   N 0.00436   57          1.0       1.0
 33S  PN                                                                     3
 33S  cN NR$Weighted average of 0.00435 {I60}, 0.00436 {I57} and 0.00436 {I58}
 33S 2cN from I|g intensity balance and measured %I|b in 1980Wi13 at 841, 1966,
 33S 3cN and 2867 levels, respectively.
 33CL  P 0.0         3/2+              2.5059 S  23             5582.5    4
 33CL cP J,T$From the Adopted Levels of {+33}Cl
 33CL cP QP$From 2021Wa16
 33S   L 0.0         3/2+               STABLE
 33S   E             98.50   19 0.0755 10 3.753  +2-1           98.58     19
 33S S E EAV=2086.86 19$CK=6.94E-4 9$CL=6.27E-5 9$CM=9.09E-6 17
 33S  cE TI$as given in 1980Wi13, deduced from 100-I|b(excited states) by
 33S 2cE assuming unobserved feedings to higher levels negligible. Other:
 33S 3cE 98.3 {I2} deduced the same way in 1970Ba65, but fewer |g rays are
 33S 4cE observed in that work than 1980Wi13.
 33S   L 840.9     4  1/2+             1.17 PS   7
 33S   E             0.48    6 6.7E-4  8 5.66    6              0.48      6
 33S S E EAV=1681.09 29$CK=0.001262 17$CL=1.140E-4 16$CM=1.654E-5 31
 33S  cE TI$other: 0.54 {I10} (1970Ba65)
 33S   G 840.7     9 118.6   36 M1+E2     0.19   3
 33S 2 G %IG=0.517 70
 33S  cG E$weighted average of 841.3 {I10} (2014Ko17), 840.4 {I9} (1987Bo21),
 33S 2cG and 840.5 {I10} (1970Ba65)
 33S  cG RI$others: 96 {I12} (1970Ba65), 100 {I11} (1987Bo21)
 33S  cG $%I|g=0.55 {I6} in 1987Bo21 gives a relative I|g=100 {I11}
 33S   L 1966.3    4  5/2+             94 FS     14
 33S   E             0.46    6 0.00186 24 4.98   6              0.46      6 A
 33S S E EAV=1144.86 28$CK=0.00367 5$CL=3.312E-4 47$CM=4.80E-5 9
 33S  cE TI$other: 0.56 {I6} (1970Ba65)
 33S   G 1125        1.38    34  E2
 33S 2 G %IG=0.0060 17
 33S   G 1966.4    5 104.2   16  M1+E2    -0.58  4
 33S 2 G %IG=0.454 60
 33S  cG E$weighted average of 1966.9 {I12} (2014Ko17), 1967.3 {I9} (1987Bo21),
 33S 2cG and 1966.1 {I5} (1970Ba65)
 33S  cG RI$others: 100 {I7} (1970Ba65), 76 {I7} (1987Bo21)
 33S  cG $%I|g=0.42 {I4} in 1987Bo21 gives a relative I|g=76 {I7}
 33S   L 2312.6    7  3/2+             117 FS    17
 33S   E             0.0351  48 2.19E-430 5.82   +7-5           0.0353    48
 33S S E EAV=982.31 37$CK=0.00562 8$CL=5.08E-4 7$CM=7.37E-5 14
 33S  cE TI$other: <0.05 (1970Ba65)
 33S   G 1472        5.79    33  M1+E2    -0.32  4
 33S 2 G %IG=0.0252 36
 33S   G 2312        2.31    14  M1+E2    -28    +16-80
 33S 2 G %IG=0.0101 15
 33S   L 2866.9    5  5/2+             12 FS     4
 33S   E             0.43    6 0.0064  9 4.19    +8-5           0.44      6 A
 33S S E EAV=725.91 27$CK=0.01314 18$CL=0.001188 17$CM=1.723E-4 33
 33S  cE TI$other: 0.56 {I6} (1970Ba65)
 33S   G 2026        1.54    19  [E2]
 33S 2 G %IG=0.0067 12
 33S   G 2866.8    5 100.0   18  M1+E2    +0.116 9
 33S 2 G %IG=0.436 58
 33S  cG E$weighted average of 2867 {I3} (2014Ko17), 2867.7 {I9} (1987Bo21),
 33S 2cG and 2866.5 {I5} (1970Ba65)
 33S  cG RI$others: 100 {I7} (1970Ba65), 100 {I9} (1987Bo21)
 33S  cG $%I|g=0.55 {I5} in 1987Bo21 gives a relative I|g=100 {I9}
 33S   L 3832.0    8  5/2+             30 FS     8
 33S   E             7.6E-5  LT 1.6E-5 LT 6.4    GT             9.2E-5    LT
 33S S E EAV=298.10 38$CK=0.1577 22$CL=0.01427 21$CM=0.00207 4
 33S   G 1519        0.52    LT M1+E2    -0.29   9
 33S 2 G %IG LT 0.0023
 33S   G 3832        0.12    LT M1+E2    +0.37   2
 33S 2 G %IG LT 5.2E-4
 33S   L 3935.1    8  3/2+             24 FS     7
 33S   E             5.2E-5  LT 1.8E-5 LT 6.3    GT             7E-5      LT
 33S S E EAV=254.61 38$CK=0.2342 31$CL=0.02119 29$CM=0.00307 6
 33S   G 3094        0.3     LT (M1+E2)  -1.7    GT
 33S 2 G %IG LT 0.0013
 33S   G 3935        0.095   LT M1+E2    -0.23   7
 33S 2 G %IG LT 4.1E-4
 33S   L 4053.2    8  1/2+             12 FS     8
 33S   E             2.8E-5  14 1.9E-5 6 6.57    31             4.7E-5    15
 33S S E EAV=205.50 37$CK=0.3743 42$CL=0.03387 41$CM=0.00491 9
 33S   G 3212        0.13    LT
 33S 2 G %IG LT 5.7E-4
 33S   G 4053        0.11    3
 33S 2 G %IG=0.00048 15
 33S   L 4144.3    10 5/2+             24 FS     7
 33S   E             1.1E-5  LT 1.5E-5 LT 6.3    GT             2.6E-5    LT
 33S S E EAV=168.19 45$CK=0.5265 49$CL=0.04764 49$CM=0.00691 11
 33S   G 4144        0.058   LT (M1+E2)
 33S 2 G %IG LT 2.5E-4
 33S   L 4375.4    8  1/2+             24 FS     10
 33S   E             1.6E-6  LT 4.2E-5 LT 5.7    GT             4.4E-5    LT
 33S S E EAV=75.73 36$CK=0.8722 11$CL=0.07897 37$CM=0.01146 15
 33S   G 2409        0.36    LT
 33S 2 G %IG LT 0.0016
 33S   G 4375        0.099   LT
 33S 2 G %IG LT 4.3E-4
 33S   L 4424.7    8  1/2+,3/2         19 FS     10
 33S   E             6.7E-7  LT 5.6E-5 LT 5.5    GT             5.7E-5    LT
 33S S E EAV=56.29 36$CK=0.8953 7$CL=0.08108 37$CM=0.01176 16
 33S   G 3584        0.09    LT D+Q
 33S 2 G %IG LT 3.9E-4
 33S   G 4424        0.067   LT
 33S 2 G %IG LT 2.9E-4
 33S   L 4746.2    8  1/2+,3/2+,5/2+   7 FS      LT
 33S   E                       4.1E-5  12 5.4    +2-1
 33S S E CK=0.9059 5$CL=0.08215 38$CM=0.01192 16
 33S   G 3905        0.068   LT
 33S 2 G %IG LT 3.0E-4
 33S   G 4746        0.085   23
 33S 2 G %IG=0.00037 11