ADOPTED LEVELS, GAMMAS for 162Ta

Author: Balraj Singh |  Citation: ENSDF |  Cutoff date: 31-JUL-2015 

Author: C. W. Reich |  Citation: Nucl. Data Sheets 108,1807 (2007) |  Cutoff date: 1-Mar-2007 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-5780 keV 50S(n)= 9150 keV 60S(p)= 750 keV 60Q(α)= 5010 keV 50
Reference: 2012WA38

References:
  A  166Re α decay (2.25 S)  B  106Cd(60Ni,3PNG)

General Comments:

162Ta produced and identified by 1985Li14 in 175Lu(3He,xn), E=280 MeV reaction; measured half-life. In 1984Sc06, α decay of 166Re was studied which indirectly implied the formation of daughter nuclide of 162Ta.

Q-value: S(2n)=20050 90, S(2p)=4090 80, Q(εp)=5490 60 (2012Wa38)










E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
     0   3.57 s 12 
% ε = 99.926 10
% εp = ?
% α = 0.074 10
     
   0+X B (7-)        
   0+YA         
   275.4+X 1  B (9-)     275.4 1 
  100
(E2)
   0+X
(7-)
   359.4+X 10  B (10-)      84.0 10 
  100

   275.4+X
(9-)
   450.0+X 10  B (11-)      90.6 1 
  100

   359.4+X
(10-)
   692.7+X 11  B (12-)     242.7 1 
  332.6 10 
  100 5 
    4.9 17 
D
(E2)
   450.0+X
   359.4+X
(11-)
(10-)
   877.2+X 11  B (13-)     184.5 1 
  427.2 2 
  100 4 
   23.5 24 
D

   692.7+X
   450.0+X
(12-)
(11-)
  1173.6+X 11  B (14-)     296.4 1 
  481.2 2 
  100 4 
   17.2 18 
D

   877.2+X
   692.7+X
(13-)
(12-)
  1419.1+X 11  B (15-)     245.6 1 
  541.8 1 
  100 4 
   60 4 


  1173.6+X
   877.2+X
(14-)
(13-)
  1731.1+X 11  B (16-)     312.4 1 
  556.7 2 
  100 4 
   34 4 


  1419.1+X
  1173.6+X
(15-)
(14-)
  2020.5+X 11  B (17-)     289.4 1 
  601.3 1 
  100 4 
   45 4 


  1731.1+X
  1419.1+X
(16-)
(15-)
  2359.9+X 11  B (18-)     339.4 1 
  628.8 2 
  100 5 
   52 6 


  2020.5+X
  1731.1+X
(17-)
(16-)
  2667.1+X 11  B (19-)     307.3 1 
  646.7 1 
  100 5 
   58 6 


  2359.9+X
  2020.5+X
(18-)
(17-)
  3036.9+X 11  B (20-)     369.8 1 
  676.8 2 
  100 7 
   54 7 


  2667.1+X
  2359.9+X
(19-)
(18-)
  3347.1+X 11  B (21-)     310.3 1 
  679.9 3 
  100 5 
   29 5 


  3036.9+X
  2667.1+X
(20-)
(19-)
  3759.2+X 11  B (22-)     412.0 1 
  721.3 3 
  100 14 
   56 15 


  3347.1+X
  3036.9+X
(21-)
(20-)
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
  4082.0+X 11  B (23-)     322.8 1 
  735.5 3 
  100 11 
   60 11 


  3759.2+X
  3347.1+X
(22-)
(21-)
  4560.8+X 11  B (24-)     478.8 1 
  800.4 4 
  100 23 
   40 17 


  4082.0+X
  3759.2+X
(23-)
(22-)
  4886.5+X 11  B (25-)     325.7 1 
  804.3 4 
  100 11 
   26 9 


  4560.8+X
  4082.0+X
(24-)
(23-)
  5445.7+X 11  B (26-)     559.3 1 
  883.5 6 
  100 10 
   17 7 


  4886.5+X
  4560.8+X
(25-)
(24-)
  5750.7+X 11  B (27-)     305.0 1 
  862.7 10 
  100 8 
    9 7 


  5445.7+X
  4886.5+X
(26-)
(25-)
  6402.7+X 11  B (28-)     652.0 2 
  956.1 16 
  100 47 
  <29


  5750.7+X
  5445.7+X
(27-)
(26-)
  6668.7+X 11  B (29-)     266.0 2 
  918.0 11 
  100 12 
   33 15 


  6402.7+X
  5750.7+X
(28-)
(27-)
  7631.7+X 15  B (30-)     963.0 10 ?
  100

  6668.7+X
(29-)

E(level): From least-squares fit to Eγ data. Uncertainties for some of the gamma rays as indicated were doubled by the evaluator to get an acceptable fit

Jπ(level): Based on tentative assignment of 9- for the bandhead, and comparison with high-spin structure of 164Ta (2011Gh08). Thus all Jπ assignments are considered here as tentative

M(γ): Assignment by the evaluator from DCO values; in addition, (E2) assigned for two low-energy ΔJ=2, quadrupole transitions from RUL, assuming level half-life less than 20 ns or so from coincidence resolving time. In other cases, where DCO values are given by 2011Gh08, it was not possible to make secure assignments since the values overlap for ΔJ=2, quadrupole and ΔJ=1, dipole transitions

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Band Transitions:

E(level)
(keV)		Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - π9/2[514]~#ν1/2[660],α=0
   359.4+X 10  (10-)        
   692.7+X 11  (12-)        
  1173.6+X 11  (14-)        
  1731.1+X 11  (16-)     312.4 1 
  556.7 2 
  100 4 
   34 4 


  1419.1+X
  1173.6+X
(15-)
(14-)
  2359.9+X 11  (18-)     339.4 1 
  628.8 2 
  100 5 
   52 6 


  2020.5+X
  1731.1+X
(17-)
(16-)
  3036.9+X 11  (20-)     369.8 1 
  676.8 2 
  100 7 
   54 7 


  2667.1+X
  2359.9+X
(19-)
(18-)
  3759.2+X 11  (22-)     412.0 1 
  721.3 3 
  100 14 
   56 15 


  3347.1+X
  3036.9+X
(21-)
(20-)
  4560.8+X 11  (24-)     478.8 1 
  800.4 4 
  100 23 
   40 17 


  4082.0+X
  3759.2+X
(23-)
(22-)
  5445.7+X 11  (26-)     559.3 1 
  883.5 6 
  100 10 
   17 7 


  4886.5+X
  4560.8+X
(25-)
(24-)
  6402.7+X 11  (28-)     652.0 2 
  956.1 16 
  100 47 
  <29


  5750.7+X
  5445.7+X
(27-)
(26-)
  7631.7+X 15  (30-)     963.0 10 ?
  100

  6668.7+X
(29-)
E(level)
(keV)		Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - π9/2[514]~#ν1/2[660],α=1
   275.4+X 1  (9-)        
   450.0+X 10  (11-)        
   877.2+X 11  (13-)        
  1419.1+X 11  (15-)     245.6 1 
  541.8 1 
  100 4 
   60 4 


  1173.6+X
   877.2+X
(14-)
(13-)
  2020.5+X 11  (17-)     289.4 1 
  601.3 1 
  100 4 
   45 4 


  1731.1+X
  1419.1+X
(16-)
(15-)
  2667.1+X 11  (19-)     307.3 1 
  646.7 1 
  100 5 
   58 6 


  2359.9+X
  2020.5+X
(18-)
(17-)
  3347.1+X 11  (21-)     310.3 1 
  679.9 3 
  100 5 
   29 5 


  3036.9+X
  2667.1+X
(20-)
(19-)
  4082.0+X 11  (23-)     322.8 1 
  735.5 3 
  100 11 
   60 11 


  3759.2+X
  3347.1+X
(22-)
(21-)
  4886.5+X 11  (25-)     325.7 1 
  804.3 4 
  100 11 
   26 9 


  4560.8+X
  4082.0+X
(24-)
(23-)
  5750.7+X 11  (27-)     305.0 1 
  862.7 10 
  100 8 
    9 7 


  5445.7+X
  4886.5+X
(26-)
(25-)
  6668.7+X 11  (29-)     266.0 2 
  918.0 11 
  100 12 
   33 15 


  6402.7+X
  5750.7+X
(28-)
(27-)

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
   275.4+X(9-)   E(level): π9/2[514]~#ν1/2[660],α=1.
   359.4+X(10-)   E(level): π9/2[514]~#ν1/2[660],α=0.
   450.0+X(11-)   E(level): π9/2[514]~#ν1/2[660],α=1.
   692.7+X(12-)   E(level): π9/2[514]~#ν1/2[660],α=0.
   877.2+X(13-)   E(level): π9/2[514]~#ν1/2[660],α=1.
  1173.6+X(14-)   E(level): π9/2[514]~#ν1/2[660],α=0.
  1419.1+X(15-)   E(level): π9/2[514]~#ν1/2[660],α=1.
  1731.1+X(16-)   E(level): π9/2[514]~#ν1/2[660],α=0.
  2020.5+X(17-)   E(level): π9/2[514]~#ν1/2[660],α=1.
  2359.9+X(18-)   E(level): π9/2[514]~#ν1/2[660],α=0.
  2667.1+X(19-)   E(level): π9/2[514]~#ν1/2[660],α=1.
  3036.9+X(20-)   E(level): π9/2[514]~#ν1/2[660],α=0.
  3347.1+X(21-)   E(level): π9/2[514]~#ν1/2[660],α=1.
  3759.2+X(22-)   E(level): π9/2[514]~#ν1/2[660],α=0.
  4082.0+X(23-)   E(level): π9/2[514]~#ν1/2[660],α=1.
  4560.8+X(24-)   E(level): π9/2[514]~#ν1/2[660],α=0.
  4886.5+X(25-)   E(level): π9/2[514]~#ν1/2[660],α=1.
  5445.7+X(26-)   E(level): π9/2[514]~#ν1/2[660],α=0.
  5750.7+X(27-)   E(level): π9/2[514]~#ν1/2[660],α=1.
  6402.7+X(28-)   E(level): π9/2[514]~#ν1/2[660],α=0.
  6668.7+X(29-)   E(level): π9/2[514]~#ν1/2[660],α=1.
  7631.7+X(30-)   E(level): π9/2[514]~#ν1/2[660],α=0.

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