ADOPTED LEVELS, GAMMAS for 151Ho

Author: Balraj Singh |  Citation: Nucl. Data Sheets 110, 1 (2009) |  Cutoff date: 20-Nov-2008 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-5356 keV 18S(n)= 9748 keV 16S(p)= 1602 keV 9Q(α)= 4695.0 keV 18
S(2n)= 18119 keV 16S(2p)= 6712 keV 9Q(EC)= 5130 keV 9Q(ECp)= 194 keV 11
Reference: 2017WA10

References:
  A  151Er ε decay (23.5 S)  B  151Er ε decay (0.58 S)
  C  155Tm α decay (21.6 S)  D  155Tm α decay (45 S)
  E  127I(29Si,5nγ)  F  141Pr(16O,6nγ)

General Comments:

Mass measurement (Penning trap): 2000Be42

Nuclear structure calculations (and syst): 2008Al09, 1998Zh23, 1996Zh09, 1993To07, 1993Pa04, 1986Bl14










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
     0.0ABC EF (11/2-) 35.2 s 1 
% ε = 78 3
% α = 22 3
     
    41.0 2 A CD   (1/2+) 47.2 s 13 
% ε = 20 +20-15
% α = 80 +15-20
     
   141.12 22 A      (3/2+)      100.1 1 
  100
M1
    41.0
(1/2+)
   397.60 24 A      (5/2+)      256.5 1 
  100
M1
   141.12
(3/2+)
   638.29 9 A      (7/2-,9/2-)      638.3 1 
  100

     0.0
(11/2-)
   667.18 10 A      (7/2-,9/2-)      667.2 1 
  100

     0.0
(11/2-)
   699.93 24 A      (7/2+)      302.4 2 
   558.8 1 
   52 4 
  100 10 


   397.60
   141.12
(5/2+)
(3/2+)
   789.50 10  B  EF (15/2-)      789.5 1 
  100

     0.0
(11/2-)
   861.7 3 A           720.6 2 
  100

   141.12
(3/2+)
   868.92 10 A           230.7 2 
   868.9 1 
    9.7 12 
  100 9 


   638.29
     0.0
(7/2-,9/2-)
(11/2-)
   910.0 3 A           768.9 2 
  100

   141.12
(3/2+)
   934.6 3 A           537.0 2 
  100

   397.60
(5/2+)
  1001.62 24 A           860.5 1 
  100

   141.12
(3/2+)
  1129.10 16 A           462.0 2 
   987.9 2 
   38 3 
  100 14 


   667.18
   141.12
(7/2-,9/2-)
(3/2+)
  1202.1 5 A          1061.0 4 
  100

   141.12
(3/2+)
  1279.79 12 A           641.5 1 
  100

   638.29
(7/2-,9/2-)
  1377.79 13 A           739.5 1 
  100

   638.29
(7/2-,9/2-)
  1387.10 15  B  EF (19/2-)      597.6 1 
  100

   789.50
(15/2-)
  1541.58 23 A           874.4 2 
  100

   667.18
(7/2-,9/2-)
  1563.32 14 A           694.4 1 
   898.0 2 
  100 11 
   62 10 


   868.92
   667.18

(7/2-,9/2-)
  1684.32 18  B  EF (23/2-)      297.2 1 
  100
(E2)
  1387.10
(19/2-)
  1791.09 22  B  EF (21/2-)      106.6 3 
   404.1 3 
 
 
(M1)

  1684.32
  1387.10
(23/2-)
(19/2-)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  1832.79 12 A      (5/2-,7/2-)      455.0 2 
   553.0 1 
  1194.5 2 
  1435.2 2 
   32.6 22 
   97 8 
  100 7 
   99 7 




  1377.79
  1279.79
   638.29
   397.60


(7/2-,9/2-)
(5/2+)
  1860.92 22 A           992.0 2 
  100

   868.92

  1946.9 4 A          1549.3 3 
  100

   397.60
(5/2+)
  2098.41 20  B  EF (25/2-)      307.3 2 
   414.1 1 
   23 7 
  100 7 

M1+E2
  1791.09
  1684.32
(21/2-)
(23/2-)
  2227.22 21  B  EF (27/2-)      128.8 1 
   542.9 3 
  100 7 
   26
M1(+E2)

  2098.41
  1684.32
(25/2-)
(23/2-)
  2615.40 21     EF (27/2)      517.0 1 
  100

  2098.41
(25/2-)
  2851.4 3 ?    EF (27/2-)      624.2 3 
  100

  2227.22
(27/2-)
  2880.11 23     EF (29/2)      264.7 1 
   653.0 3 
 
 
(M1)

  2615.40
  2227.22
(27/2)
(27/2-)
  3144.33 23     EF (29/2)      529.0 3 
   917.1 1 
 
 


  2615.40
  2227.22
(27/2)
(27/2-)
  3155.37 25     EF (31/2)       11S
   275.3 3 
   540.0 3 
 
  100
   60

(E1)

  3144.33
  2880.11
  2615.40
(29/2)
(29/2)
(27/2)
  3314.5 3     EF (33/2)      159.1 3 
   434.4 3 
 
 


  3155.37
  2880.11
(31/2)
(29/2)
  3522.67 24     EF (33/2)      208.3 3 
   367.3 1 
 
 

(M1)
  3314.5
  3155.37
(33/2)
(31/2)
  3623.94 23     EF (31/2-)      772.6 3 
  1396.7 1 
   14
  100 14 

(E2)
  2851.4
  2227.22
(27/2-)
(27/2-)
  3970.1 4     E  (35/2)      655.6 3 
   814.7 3 
 
 


  3314.5
  3155.37
(33/2)
(31/2)
  4109.86 24     EF (35/2-)      485.9 1 
   587.2 1 
  100 16 
  100 11 


  3623.94
  3522.67
(31/2-)
(33/2)
  4355.9 3     EF (39/2-)      246.0 1 
  100
(E2)
  4109.86
(35/2-)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  4561.7 5     E  (39/2)      591.6 3 
 

  3970.1
(35/2)
  4811.5 3     EF (43/2-) ≈ 1 ns    455.6 1 
  100
(E2)
  4355.9
(39/2-)
  5293.5 4     EF (41/2)      937.6 3 
  100

  4355.9
(39/2-)
  5578.2 4 ?    EF (43/2)      284.6 3 
  100

  5293.5
(41/2)
  5642.5 4     EF (45/2)      831.1 3 
  100
D
  4811.5
(43/2-)
  5835.9 4     EF (45/2)      257.6 3 
  1024.4 2 
   62 12 
  100 15 

D
  5578.2
  4811.5
(43/2)
(43/2-)
  5875.3 4     EF (47/2)       39.3 3 
   232.8 1 
  1063.9 3 
 
 
 

D

  5835.9
  5642.5
  4811.5
(45/2)
(45/2)
(43/2-)
  6184.0 4     EF (49/2)      308.7 1 
  100
D+Q
  5875.3
(47/2)
  6225.4 4     EF       41.4 3 
   350.1 3 
 
 


  6184.0
  5875.3
(49/2)
(47/2)
  6513.7 4     E       329.7 3 
 

  6184.0
(49/2)
  6522.7 5 ?    E       338.7 3 
 

  6184.0
(49/2)
  6534.6 5     EF       21S
   309.1 3 
 
 


  6513.7
  6225.4


  6659.8 4     EF      125.3 3 
   146.1 3 
   434.4 3 
 
 
 



  6534.6
  6513.7
  6225.4



  6805.7 5 ?    E       621.7 3 
 

  6184.0
(49/2)
  6850.5 5 ?    E      1014.6 3 
 

  5835.9
(45/2)
  6907.5 4     E       723.4 3 
  1071.8 3 
 
 


  6184.0
  5835.9
(49/2)
(45/2)
  7071.2 5     EF      887.2 3 
 

  6184.0
(49/2)
  7099.2 5     EF      564.6 3 
  100

  6534.6

  7128.8 5 ?    E       944.8 3 
 

  6184.0
(49/2)
  7192.4 4     EF     1008.4 3 
 

  6184.0
(49/2)
  7326.4 5 ?    E      1142.4 3 
 

  6184.0
(49/2)
  7754.3 4     E       561.9 3 
  1094.5 3 
  1528.9 3 
  1570.3 3 
 
 
 
 




  7192.4
  6659.8
  6225.4
  6184.0



(49/2)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  8025.5 6 ?    E       954.3 3 
 

  7071.2

  8340.9 5     EF (GE 57/2) 9.2 ns 20     586.6 3 
  1241.7 3 
 
 


  7754.3
  7099.2


  8651.7 6     E       310.8 3 
 

  8340.9
(GE 57/2)
  9053.5 6 ?    E       712.6 3 
 

  8340.9
(GE 57/2)
  9531.9 7 ?    EF      478.4 3 
 

  9053.5

  9958.7 7 ?    E      1307.0 3 
 

  8651.7

E(level): From least-squares fit to Eγ’s. The 898γ from 1564 level was was omitted from the least-squares fitting procedure as it resulted in a poor fit with normalized χ2=7.5

Jπ(level): For high-spin (J>11/2) levels, the assignments are mainly based on multipolarities of selected transitions (about 12 in all) from γ(θ), γ(lin pol) and intensity-balance arguments. The shell-model predictions are also used. Ascending spins are assumed as the excitation energy rises.

Back to top

Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - πh11/23~#νf7/22. Multiplet of states with
     0.0 (11/2-) 35.2 s 1 
% ε = 78 3
% α = 22 3
     
   789.50 10  (15/2-)        
  1387.10 15  (19/2-)      597.6 1 
  100

   789.50
(15/2-)
  1684.32 18  (23/2-)      297.2 1 
  100
(E2)
  1387.10
(19/2-)
  1791.09 22  (21/2-)      106.6 3 
   404.1 3 
 
 
(M1)

  1684.32
  1387.10
(23/2-)
(19/2-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - πh11/23~#νf7/22. Multiplet of states with
  2851.4 3  (27/2-)        
  3623.94 23  (31/2-)        
  4109.86 24  (35/2-)      485.9 1 
   587.2 1 
  100 16 
  100 11 


  3623.94
  3522.67
(31/2-)
(33/2)
  4355.9 3  (39/2-)      246.0 1 
  100
(E2)
  4109.86
(35/2-)

Back to top

Additional Gamma Data:













E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityConversion
Coefficient
Additional Data
   141.12 (3/2+)      100.1 1 M12.60α=2.60, α(K)=2.19 4, α(L)=0.325 5, α(M)=0.0718 11, α(N)=0.01667 24, α(O)=0.00242 4, α(P)=0.0001357 20, α(N+)=0.0192 3
   397.60 (5/2+)      256.5 1 M10.187α=0.187, α(K)=0.1577 23, α(L)=0.0230 4, α(M)=0.00508 8, α(N)=0.001179 17, α(O)=0.0001718 25, α(P)=9.70×10-6 14, α(N+)=0.001360 20
  1684.32 (23/2-)      297.2 1 (E2)0.0687α=0.0687, α(K)=0.0508 8, α(L)=0.01385 20, α(M)=0.00322 5, α(N)=0.000733 11, α(O)=9.53×10-5 14, α(P)=2.62E-6 4, α(N+)=0.000831 12
  1791.09 (21/2-)      106.6 3 (M1)2.17α=2.17 4, α(K)=1.83 3, α(L)=0.271 5, α(M)=0.0599 10, α(N)=0.01390 23, α(O)=0.00202 4, α(P)=0.0001133 19, α(N+)=0.0160 3
  2098.41 (25/2-)      414.1 1 M1+E20.039α=0.039 14, α(K)=0.032 12, α(L)=0.0054 10, α(M)=0.00120 20, α(N)=0.00028 5, α(O)=3.9×10-5 9, α(P)=1.9E-6 8, α(N+)=0.00032 6
  2227.22 (27/2-)      128.8 1 M1(+E2)1.19α=1.19 8, α(K)=0.82 25, α(L)=0.29 14, α(M)=0.07 4, α(N)=0.015 8, α(O)=0.0020 8, α(P)=4.5×10-5 21, α(N+)=0.017 9
  2880.11 (29/2)      264.7 1 (M1)0.1719α=0.1719, α(K)=0.1448 21, α(L)=0.0211 3, α(M)=0.00466 7, α(N)=0.001082 16, α(O)=0.0001576 23, α(P)=8.90×10-6 13, α(N+)=0.001248 18
  3155.37 (31/2)      275.3 3 (E1)0.0221α=0.0221, α(K)=0.0187 3, α(L)=0.00268 4, α(M)=0.000589 9, α(N)=0.0001357 20, α(O)=1.92×10-5 3, α(P)=9.68E-7 14, α(N+)=0.0001558 23
  3522.67 (33/2)      367.3 1 (M1)0.0717α=0.0717, α(K)=0.0605 9, α(L)=0.00875 13, α(M)=0.00193 3, α(N)=0.000448 7, α(O)=6.53×10-5 10, α(P)=3.70E-6 6, α(N+)=0.000517 8
  3623.94 (31/2-)     1396.7 1 (E2)1.69×10-3α=1.69×10-3, α(K)=0.001392 20, α(L)=0.000198 3, α(M)=4.34E-5 6, α(N)=1.006E-5 14, α(O)=1.455E-6 21, α(P)=7.99E-8 12, α(N+)=5.29E-5 8
  4355.9 (39/2-)      246.0 1 (E2)0.1241α=0.1241, α(K)=0.0875 13, α(L)=0.0282 4, α(M)=0.00661 10, α(N)=0.001504 22, α(O)=0.000192 3, α(P)=4.35×10-6 7, α(N+)=0.001700 24
  4811.5 (43/2-) ≈ 1 ns    455.6 1 (E2)0.0202B(E2)(W.u.)≈0.6, α=0.0202, α(K)=0.01598 23, α(L)=0.00325 5, α(M)=0.000740 11, α(N)=0.0001698 24, α(O)=2.30E-5 4, α(P)=8.81E-7 13, α(N+)=0.000194 3

Back to top

Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.0(11/2-) 35.2 s 1 
% ε = 78 3
% α = 22 3
%α from weighted average of 28 7 (1991To08), 22 3 (1990Po13), 22 3 (1982Ba75), 18 5 (1974Sc19), 20 5 (1963Ma17).
E(level): πh11/23~#νf7/22. Multiplet of states with.
   789.50(15/2-)   E(level): πh11/23~#νf7/22. Multiplet of states with.
  1387.10(19/2-)   E(level): πh11/23~#νf7/22. Multiplet of states with.
  1684.32(23/2-)   E(level): πh11/23~#νf7/22. Multiplet of states with.
  1791.09(21/2-)   E(level): πh11/23~#νf7/22. Multiplet of states with.
  2098.41(25/2-)   Configuration=(πh11/23)#(νf7/2)(νh9/2); seniority=3.
  2227.22(27/2-)   Configuration=(πh11/23)#(νf7/2)(νh9/2); seniority=1.
  2615.40(27/2)   Configuration=(πh11/23)(150Gd 3-)#(νf7/22) (νf7/2)(νi13/2).
  2851.4(27/2-)   E(level): πh11/23~#νf7/22. Multiplet of states with.
  2880.11(29/2)   Configuration=(πh11/23)(150Gd 3-)#(νf7/22) (νf7/2)(νi13/2).
  3155.37(31/2)   Configuration=(πh11/23)#(νf7/2)(νi13/2).
  3623.94(31/2-)   E(level): πh11/23~#νf7/22. Multiplet of states with.
  3970.1(35/2)   Configuration=(πh11/22)#(νd3/2)(νf7/22).
  4109.86(35/2-)   E(level): πh11/23~#νf7/22. Multiplet of states with.
  4355.9(39/2-)   E(level): πh11/23~#νf7/22. Multiplet of states with.
  4561.7(39/2)   Configuration=(πh11/22)#(νd3/2)(νf7/2)(νh9/2).
  4811.5(43/2-) ≈ 1 ns Configuration=(πh11/23)#(νf7/2)(νh9/2), seniority=3.
  5875.3(47/2)   Configuration=(πh11/23)#(νh9/2)(νi13/2).
  6184.0(49/2)   Configuration=(πh11/23)#(νh9/2)(νi13/2).

Back to top

Additional Gamma Comments:

E(level)E(gamma)Comments
   141.12   100.1M(γ): from α(K)exp and K/L ratio in 151Er ε decay (23.5 s)
   397.60   256.5M(γ): from α(K)exp in 151Er ε decay (23.5 s)
  1563.32   898.0E(γ): poor fit. Level-energy difference=896.1. This γ energy was not included in the least-squares fitting procedure
  1684.32   297.2M(γ): From intensity-balance arguments in 127I(29Si,5nγ)
  1791.09   106.6I(γ): from assumed (by evaluator) intensity balance at 1684 level in 151Er ε decay, I(γ+ce)(106.6γ)/Iγ(404γ)≈100/57
M(γ): From intensity-balance arguments in 127I(29Si,5nγ)
  2098.41   307.3I(γ): from 151Er ε (0.58 s). Other: 42 7 in high spin data
   414.1M(γ): From γ(θ) and linear polarization in 141Pr(16O,6nγ)
  2227.22   128.8M(γ): From γ(θ) and linear polarization in 141Pr(16O,6nγ)
  2880.11   264.7M(γ): From intensity-balance arguments in 127I(29Si,5nγ)
  3155.37   275.3M(γ): From intensity-balance arguments in 127I(29Si,5nγ)
  3623.94  1396.7M(γ): From γ(θ) and linear polarization in 141Pr(16O,6nγ)
  4355.9   246.0M(γ): From γ(θ) and linear polarization in 141Pr(16O,6nγ). From intensity-balance arguments in 127I(29Si,5nγ)
  4811.5   455.6M(γ): From γ(θ) and linear polarization in 141Pr(16O,6nγ)
  5642.5   831.1M(γ): γ(θ) consistent with ΔJ=1
  5835.9  1024.4M(γ): γ(θ) consistent with ΔJ=1
  5875.3   232.8M(γ): γ(θ) consistent with ΔJ=1
  6184.0   308.7M(γ): From γ(θ) and linear polarization in 141Pr(16O,6nγ)

Back to top