ADOPTED LEVELS, GAMMAS for 42Cl

Authors: Jun Chen and Balraj Singh |  Citation: Nucl. Data Sheets 135, 1 (2016) |  Cutoff date: 31-May-2016 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=9.51×103 keV 14S(n)= 5.68×103 keV 16S(p)= 13.19×103 keV 14Q(α)= -12.67×103 keV 17
Reference: 2012WA38

References:
  A  42S β- decay (1.016 S)  B  43S β-n decay (265 MS)
  C  208Pb(40Ar,xγ) 

General Comments:

1971Ar32: 42Cl produced and identified in 232Th(40Ar,X) reaction at 290 MeV, measured fragment yield.

1981Vo04: 42Cl produced in U,Nb(p,X) at 600 MeV, measured half-life

1998WiZX, 1998WiZV, 1989Mi03, 1981HuZT: studies of 42Cl β decay

Mass measurements: 2015Xu14, 1991Zh24, 1990Tu01

Cross-section and radius measurements: 2006Kh08, 2006Ro34, 1999Ai02

1991Wa19: shell-model calculations, levels, binding energy, β-decay rates.

Q-value: S(2n)=13500 150, S(2p)=31420 180, Q(β-n)=80 140 (2012Wa38)










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
     0A C (2-) 6.8 s 3 
% β- = 100
     
   118.19 6 A   (3-)      118.25 10 
  100

     0
(2-)
   522 1 ?  C (4-)      522 1 
  100

     0
(2-)
   588.97 6 A   (1-,2,3+)      470.78 6 
   588.78 9 
  100 4 
    0.75 15 


   118.19
     0
(3-)
(2-)
   639.44 9 A   (1-,2,3+)      521.26 10 
   638.9 4 
  100 20 
   28 5 


   118.19
     0
(3-)
(2-)
   841.91 6 A   (1-,2,3+)      202.42 11 
   252.6 4 ?
   723.72 7 
   841.95 8 
    2.6 3 
    0.93 24 
  100 3 
   25 3 




   639.44
   588.97
   118.19
     0
(1-,2,3+)
(1-,2,3+)
(3-)
(2-)
  1025.82 23 A   (1-,2,3+)      907.5 5 
  1025.9 4 ?
   71 33 
  100 31 


   118.19
     0
(3-)
(2-)
  1267.49 7 A   1+      425.61 6 
   678.43 7 
  1149.42 13 
  1268.8 7 ?
   44 3 
  100 6 
   13 3 
   12.8 19 



[M2]
   841.91
   588.97
   118.19
     0
(1-,2,3+)
(1-,2,3+)
(3-)
(2-)
  1385.69 18 A        796.80 20 
  100

   588.97
(1-,2,3+)
  1550.42 9 A       1550.52 14 
  100

     0
(2-)
  1576.65 20 ?A       1458.53 23 ?
  100

   118.19
(3-)
  1684.22 11 ?A       1684.1 3 ?
  100

     0
(2-)
  1710.92 8 A        160.60 9 
   685.1 3 
   868.94 14 
  1071.6 3 
  1121.97 13 
  1592.55 18 
   52 5 
   41 4 
   66 7 
   43 10 
  100 20 
   65 7 






  1550.42
  1025.82
   841.91
   639.44
   588.97
   118.19

(1-,2,3+)
(1-,2,3+)
(1-,2,3+)
(1-,2,3+)
(3-)
  1834.87 13 ?A       1245.93 24 ?
  100

   588.97
(1-,2,3+)
  2123.31 8 A   1+      288.49 12 ?
   439.09 8 ?
   737.8 3 
  1281.44 12 
  1534.26 11 
  2004.93 16 
  2123.9 5 
    1.93 24 
    5.4 5 
    1.2 4 
  100 4 
   34.0 16 
   52.0 19 
    3.9 5 






[M2]
  1834.87
  1684.22
  1385.69
   841.91
   588.97
   118.19
     0



(1-,2,3+)
(1-,2,3+)
(3-)
(2-)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  2221.03 12 ?A        670.55 10 ?
  100

  1550.42

  2241.17 25 A   (1+)     1399.1 3 
  1652.4 4 
  100 11 
   45 15 


   841.91
   588.97
(1-,2,3+)
(1-,2,3+)
  2403.2 4 ?A       1814.2 4 ?
  100

   588.97
(1-,2,3+)
  3029.71 11 A   1+      808.55 15 ?
  1193.1 9 ?
  1318.88 11 
  1453.2 3 ?
  2187.2 4 
  2440.6 3 
  2911.7 5 
   16.3 26 
   18 3 
  100 4 
   14.4 19 
   29 3 
   26 3 
   20 3 







  2221.03
  1834.87
  1710.92
  1576.65
   841.91
   588.97
   118.19




(1-,2,3+)
(1-,2,3+)
(3-)

E(level): From least-squares fit to Eγ data.

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0(2-) 6.8 s 3 
% β- = 100
Mean radius r20=1.304 fm2 54 (2006Kh08).
E(level): Mean radius r20=1.304 fm2 54 (2006Kh08).
Jπ(level): From shell-model calculations (2013Sz02).
   118.19(3-)   Jπ(level): From shell-model calculations (2013Sz02).
   522(4-)   Jπ(level): From shell-model calculations (2013Sz02).
   588.97(1-,2,3+)   Jπ(level): Inferred from a comparison with the decay scheme of 40S (2006Wi10).
   639.44(1-,2,3+)   Jπ(level): Inferred from a comparison with the decay scheme of 40S (2006Wi10).
   841.91(1-,2,3+)   Jπ(level): Inferred from a comparison with the decay scheme of 40S (2006Wi10).
  1025.82(1-,2,3+)   Jπ(level): Inferred from a comparison with the decay scheme of 40S (2006Wi10).

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