ADOPTED LEVELS, GAMMAS for 222Ra

Authors: Balraj Singh, M.S. Basunia, Jun Chen Et Al., |  Citation: Nucl. Data Sheets 192, 315 (2023) |  Cutoff date: 25-Sep-2023 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-2302 keV 6S(n)= 6715 keV 6S(p)= 6246 keV 6Q(α)= 6678 keV 4
Reference: 2021WA16

References:
  A  222Fr β- decay (14.2 M)  B  226Th α decay (30.72 M)
  C  232Th(136Xe,xγ)  D  Coulomb Excitation

General Comments:

Dataset by Balraj Singh, Jun Chen, and IAEA-ICTP-workshop participants: Diwanshu, S. Leblond, α. Rathi, p.S. Rawat, B. Rohila, and V. Vallet.

1948St42: 222Rn identified in 230U |) 226Th |)222Rn α-decay chain; 230U produced in the bombardment of Th with 19-MeV deuterons and 38-MeV He ions at the Berkeley cyclotron facility. Measured half-life of the decay of 222Rn from α decay. Later works on the study of 222Rn decay: 1956As38 (also at Berkeley) and 1958To25 (at Gustaf Werner cyclotron facility in Uppsala).

Theoretical structure calculations:

2023Zh13: calculated T1/2 and branching ratios for α, 2α, and 14C cluster decays, quadrupole, octupole and hexadecupole deformation-energy surfaces using relativistic Hartree-Bogoliubov model with the DD-PC1 functional and a separable pairing force.

2022Ta16: calculated neutron and proton energy gaps, quadrupole and octupole deformation parameters using Hartree-Fock-Bogolyubov approximation with Skyrme forces.

2022Uz01: calculated quadrupole and octupole deformation parameters, rms proton matter radii, the total energy, and 14C cluster decay rate using Skyrme Hartree-Fock+BCS theory with SLy4 and SkM* interactions.

2021Ku31: calculated energy differences, neutron and proton energy gaps, deformation parameters using Hartree-Fock-Bogoliubov theory with an effective Skyrme interaction.

2020No13: calculated potential energy surfaces in (β23) plane using self-consistent mean-field (SCMF), and interacting boson model (IBM), energies of yrast positive-parity and negative-parity states, and relative energy splitting between positive- and negative-parity yrast bands, B(E1), B(E2), B(E3), transition quadrupole and octupole moments using Hartree-Fock-Bogoliubov approximation, based on Gogny-D1M energy density functional, and sdf interacting boson model (IBM) Hamiltonian for quadrupole-octupole coupling and collective excitations

2019Zh50: calculated empirical proton-neutron interaction, B(E2), B(E3), binding energy, contour plot of total energy in (β23) plane, neutron and proton single-particle levels by using the covariant density functional theory and the quadrupole-octupole collective Hamiltonian approach.

2015Bo05: calculated levels, Jπ, B(E1), Be(2), B(E3) using analytic quadrupole octupole axially (AQOA) symmetric model using Davidson potential. Bohr collective Hamiltonian, and quadrupole plus octupole deformation.

2013De12: calculated β2 and deformation parameter, CSM parameter, α-core QQ coupling parameter, Iα to 2+, 4+ and 6+ states from 222Ra decay in daughter nuclei, B(E2), rigidity parameter, E(4+)/E(2+) and E(6+)/E(4+) ratios, effective charge, hindrance factors using coherent state model.

2001Ch02: calculated rotational bands energy vs spin using reflection-asymmetric shell model for octupole-deformed nuclei.

1998Ra05: calculated high-spin levels, Jπ, ground state and Kπ=0- bands using phenomenological model.

1997Bu07, 1997Bu28: calculated levels, Jπ, B(|l), deformation parameters, using mixed Saxon-Woods plus cubed Saxon-Woods cluster-core interaction.

1993Yo02, 1986Le05: calculations of B(E1)/B(E2) transition probabilities from the Kπ=0- band.

1989Eg02: calculated octupole barrier energies, pairing energy, deformation parameters β2, β4 and β6, dipole moment vs constrained quadrupole moment using microscopic model.

1988Ro02, 1987Ro08: calculated E1, E3 transition probabilities and the 0+, 1- energy splitting, barrier heights, single particle and pairing energies vs octupole deformation, dipole vs octupole moments, B(E1)/B(E2) using constrained HF plus BCS method.

1988Ba48: calculated rotational band wave functions, quadrupole, and octupole deformations, energy splitting between the even- and odd-parity rotational bands using a collective Hamiltonian.

1987Na10: calculated levels, Jπ, routhians, rotational bands, B(E1)/B(E2) ratios, shape dependence using cranking model.

1986Bo19: calculated quadrupole-octupole deformation energy surface, nonzero octupole moment using self-consistent Hartree-Fock plus BCS calculations.

Theoretical calculations for decay characteristics:

2023Zh13: calculated T1/2 and branching ratios for α, 2α and 14C cluster decays using relativistic Hartree-Bogoliubov model with the DD-PC1 functional and a separable pairing force, and proximity potential model for deformed nuclei.

2022Ka09: calculated T1/2 for bare nuclei and He-like ions using adiabatic approach.

2020Ni01: calculated α-branching ratio to vibrational states, and α-decay half-life using multichannel cluster model.

2010Ro08: calculated HFB mean-field energies and octupole collective inertial parameters as function of octupole moment, particle-particle correlation energies, B(E1) and B(E3) probabilities, and dipole moments using Hartree-Fock-Bogoliubov approximation, and Barcelona-Catania-Paris energy density functionals.

Consult the NSR database for about 120 references for theoretical structure calculations, and about 230 theory references for α, 2α and 14C decays, and other cluster decay characteristics of 222Ra.

Levels: B(E1)(W.u.) and B(E2)(W.u.) deduced by evaluators from measured matrix elements in Coulomb excitation, except as noted

Levels: The Kπ=0+ g.s. band and the Kπ=0- band at 242.11 keV have been interpreted as octupole parity-doublet bands.

Q-value: S(2n)=12095 9, S(2p)=10870 5 (2021Wa16)










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
     0.0ABCD 0+ 33.6 s 4 
% α = 100
% 14C = 3.0×10-8 10
     
   111.137 20 ABCD 2+ 0.52 ns 4     111.15 3 
  100
E2
     0.0
0+
   242.157 17 AB D 1- 9.5 ps +21-16     131.01 3 
   242.13 2 
   31.2 15 
  100.0 30 
(E1)
E1
   111.137
     0.0
2+
0+
   301.495 34 ABCD 4+ 135 ps +17-14     190.42 14 
  100
E2
   111.137
2+
   317.330 22 AB D (3)- 4.7 ps +26-14      75.13 2 
   206.22 4 
    0.017 4 
  100.0 32 
[E2]
E1
   242.157
   111.137
1-
2+
   473.87 4 ABCD (5-) 24 ps +5-9     156.5 1 S
   172.37 2 
    4.3 23 
  100
[E2]
[E1]
   317.330
   301.495
(3)-
4+
   549.97 19   CD (6+) 34 ps +6-5      77
   248.4 2 
   29 4 
  100
[E1]
[E2]
   473.87
   301.495
(5-)
4+
   702.92 27   CD (7-) 15 ps 5     153.1 5 
   229.3 5 
  100 32 
   18 6 
[E1]
[E2]
   549.97
   473.87
(6+)
(5-)
   842.93 25   CD (8+) 11.1 ps +31-24     140.1 2 
   292.9 2 
  100 18 
   92 8 
[E1]
[E2]
   702.92
   549.97
(7-)
(6+)
   914.174 26  B   (0+)      672.02 2 
   802.7 1 
  100 7 
   13 8 


   242.157
   111.137
1-
2+
   992.12 33   CD (9-) 5.1 ps +17-13     149.3 5 
   289.0 5 
  100 16 
   88 10 
[E1]
[E2]
   842.93
   702.92
(8+)
(7-)
  1024.920 23 AB   (2+)      707.54 3 
   723.45 6 
   782.77 3 
   913.69 5 
  1025.02 8 
  100 5 
    3.4 5 
   98 9 
   16.9 23 
    6.7 11 





   317.330
   301.495
   242.157
   111.137
     0.0
(3)-
4+
1-
2+
0+
  1170.99 4 A    (3-,4+)      696.88 5 
   853.78 8 
   869.6 2 
   29 5 
  100 6 
   81 25 



   473.87
   317.330
   301.495
(5-)
(3)-
4+
  1171.55 4 A    (1,2+)      929.47 8 
  1060.33 5 
  1171.69 8 
   15 2 
  100 8 
   53 6 



   242.157
   111.137
     0.0
1-
2+
0+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  1173.02 30   CD (10+) 5.0 ps +24-17     180.9 2 
   330.1 2 
  100 23 
   75 7 
[E1]
[E2]
   992.12
   842.93
(9-)
(8+)
  1225.23 5 A    (1,2+)      982.90 8 
  1114.26 8 
  1225.24 8 
   97 19 
  100 19 
   38 7 



   242.157
   111.137
     0.0
1-
2+
0+
  1265.05 4 A    (2+,3)      963.61 6 
  1153.87 5 
   26 4 
  100 10 


   301.495
   111.137
4+
2+
  1310.24 8 A    (0+,1,2,3-)     1068.08 8 
 

   242.157
1-
  1330.5 4   CD (11-) 3.6 ps +18-12     157.4 5 
   338.3 5 
   64 10 
  100 10 
[E1]
[E2]
  1173.02
   992.12
(10+)
(9-)
  1360.88 9 A    (1-,2,3)     1043.60 9 
  1249.1 1 
  100 12 
   60 11 


   317.330
   111.137
(3)-
2+
  1375.77 8 A    (1,2,3-)     1133.61 8 
 

   242.157
1-
  1402.596 31 A    (2+,3-)      231.7 2 
   377.64 4 
  1085.20 5 
  1101.09 5 
  1160.52 8 
  1291.61 8 
   15.2 16 
   24 2 
   92 12 
  100 10 
   14.4 14 
    9.6 16 






  1170.99
  1024.920
   317.330
   301.495
   242.157
   111.137
(3-,4+)
(2+)
(3)-
4+
1-
2+
  1432.73 6 A    (1,2,3-)     1190.4 1 
  1321.65 6 
    8.5 15 
  100 8 


   242.157
   111.137
1-
2+
  1439.994 34 A    (3-)      268.99 4 
   415.05 4 
   966.24 9 
  1122.41 9 
  1138.47 5 
  1197.99 8 
   13 3 
   11 2 
   23 5 
   40 7 
  100 10 
   30 5 






  1170.99
  1024.920
   473.87
   317.330
   301.495
   242.157
(3-,4+)
(2+)
(5-)
(3)-
4+
1-
  1499.49 5 A    (1-,2,3-)      474.45 9 
  1182.05 8 
  1257.5 1 
  1388.5 1 
  100 10 
   87 10 
   33 6 
   76 10 




  1024.920
   317.330
   242.157
   111.137
(2+)
(3)-
1-
2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  1536.8 5   CD (12+) 4.6 ps +26-16     206.2 5 
   363.9 5 
   64 12 
  100 10 
[E1]
[E2]
  1330.5
  1173.02
(11-)
(10+)
  1556.04 7 A    (2+)     1238.60 8 
  1254.4 2 
  1445.2 2 
  1556.5 2 
  100 13 
   26 3 
   69 11 
   59 11 




   317.330
   301.495
   111.137
     0.0
(3)-
4+
2+
0+
  1619.62 9 A    (1,2,3-)     1377.4 1 
  1508.7 2 
  100 15 
   24 7 


   242.157
   111.137
1-
2+
  1644.88 4 A    (2+,3-)      619.95 4 
  1327.58 6 
  1343.3 1 
  1402.5 2 
  1534.1 2 
   31 4 
  100 9 
   10.4 17 
   27 3 
   17 3 





  1024.920
   317.330
   301.495
   242.157
   111.137
(2+)
(3)-
4+
1-
2+
  1710.0 5   C  (13-)      173.1 5 
   379.6 5 
   82 12 
  100 9 
[E1]
[E2]
  1536.8
  1330.5
(12+)
(11-)
  1754.36 5 A    (3-)      351.75 4 
  1280.99 9 
  1436.4 1 
  1453.4 1 
  1643.9 2 
   52 11 
   34 7 
  100 10 
   45 9 
   44 11 





  1402.596
   473.87
   317.330
   301.495
   111.137
(2+,3-)
(5-)
(3)-
4+
2+
  1821.56 20 A    (1,2,3-)     1579.4 2 
  100

   242.157
1-
  1841.20 6 A    (1,2,3-)      196.31 4 
  1599.6 2 
  100 13 
   16 5 


  1644.88
   242.157
(2+,3-)
1-
  1932.9 6   C  (14+)      396.0 5 
  100
[E2]
  1536.8
(12+)
  2125.0 6   C  (15-)      192.1 5 
   415.0 5 
   68 30 
  100 12 
[E1]
[E2]
  1932.9
  1710.0
(14+)
(13-)
  2358.4 7   C  (16+)      425.5 5 
  100
[E2]
  1932.9
(14+)
  2569.8 7   C  (17-)      211.4 5 
   444.8 5 
 
  100

[E2]
  2358.4
  2125.0
(16+)
(15-)
  2810.7 9   C  (18+)      452.3 5 
  100
[E2]
  2358.4
(16+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  3040.6 9   C  (19-)      470.8 5 
  100
[E2]
  2569.8
(17-)
  3287.4 10   C  (20+)      476.7 5 
  100
[E2]
  2810.7
(18+)

E(level): From a least-squares fit to Eγ values. Uncertainties of some Eγ values have been increased (as specified under comment at each γ) in the fitting due to poor fit and the resulting reduced χ2=2.2, compared to 4.9 without those ΔEγ adjustments.

T1/2(level): For levels above 111.1, half-lives have been deduced by evaluators from measured matrix elements in Coulomb excitation, and adopted γ-ray branching ratios

M(γ): From ce data in 226Th α decay, unless otherwise noted

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Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - Kπ=0+ g.s. band.
     0.0 0+ 33.6 s 4 
% α = 100
% 14C = 3.0×10-8 10
     
   111.137 20  2+ 0.52 ns 4     111.15 3 
  100
E2
     0.0
0+
   301.495 34  4+ 135 ps +17-14     190.42 14 
  100
E2
   111.137
2+
   549.97 19  (6+) 34 ps +6-5      77
   248.4 2 
   29 4 
  100
[E1]
[E2]
   473.87
   301.495
(5-)
4+
   842.93 25  (8+) 11.1 ps +31-24     140.1 2 
   292.9 2 
  100 18 
   92 8 
[E1]
[E2]
   702.92
   549.97
(7-)
(6+)
  1173.02 30  (10+) 5.0 ps +24-17     180.9 2 
   330.1 2 
  100 23 
   75 7 
[E1]
[E2]
   992.12
   842.93
(9-)
(8+)
  1536.8 5  (12+) 4.6 ps +26-16     206.2 5 
   363.9 5 
   64 12 
  100 10 
[E1]
[E2]
  1330.5
  1173.02
(11-)
(10+)
  1932.9 6  (14+)      396.0 5 
  100
[E2]
  1536.8
(12+)
  2358.4 7  (16+)      425.5 5 
  100
[E2]
  1932.9
(14+)
  2810.7 9  (18+)      452.3 5 
  100
[E2]
  2358.4
(16+)
  3287.4 10  (20+)      476.7 5 
  100
[E2]
  2810.7
(18+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - Kπ=0- octupole vibrational band.
   242.157 17  1- 9.5 ps +21-16       
   317.330 22  (3)- 4.7 ps +26-14      75.13 2 
   206.22 4 
    0.017 4 
  100.0 32 
[E2]
E1
   242.157
   111.137
1-
2+
   473.87 4  (5-) 24 ps +5-9     156.5 1 S
   172.37 2 
    4.3 23 
  100
[E2]
[E1]
   317.330
   301.495
(3)-
4+
   702.92 27  (7-) 15 ps 5     153.1 5 
   229.3 5 
  100 32 
   18 6 
[E1]
[E2]
   549.97
   473.87
(6+)
(5-)
   992.12 33  (9-) 5.1 ps +17-13     149.3 5 
   289.0 5 
  100 16 
   88 10 
[E1]
[E2]
   842.93
   702.92
(8+)
(7-)
  1330.5 4  (11-) 3.6 ps +18-12     157.4 5 
   338.3 5 
   64 10 
  100 10 
[E1]
[E2]
  1173.02
   992.12
(10+)
(9-)
  1710.0 5  (13-)      173.1 5 
   379.6 5 
   82 12 
  100 9 
[E1]
[E2]
  1536.8
  1330.5
(12+)
(11-)
  2125.0 6  (15-)      192.1 5 
   415.0 5 
   68 30 
  100 12 
[E1]
[E2]
  1932.9
  1710.0
(14+)
(13-)
  2569.8 7  (17-)      211.4 5 
   444.8 5 
 
  100

[E2]
  2358.4
  2125.0
(16+)
(15-)
  3040.6 9  (19-)      470.8 5 
  100
[E2]
  2569.8
(17-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - Kπ=(0+) band.
   914.174 26  (0+)        
  1024.920 23  (2+)      707.54 3 
   723.45 6 
   782.77 3 
   913.69 5 
  1025.02 8 
  100 5 
    3.4 5 
   98 9 
   16.9 23 
    6.7 11 





   317.330
   301.495
   242.157
   111.137
     0.0
(3)-
4+
1-
2+
0+

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Additional Gamma Data:













E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityConversion
Coefficient
Additional Data
   111.137 2+ 0.52 ns 4     111.15 3 E26.12B(E2)(W.u.)=112.8 +96-82, α=6.12 9
   242.157 1- 9.5 ps +21-16     131.01 3 (E1)0.2500B(E1)(W.u.)=0.00186 +40-34, α=0.2500 35
1- 9.5 ps +21-16     242.13 2 E10.0575B(E1)(W.u.)=0.00095 +19-17, α=0.0575 8
   301.495 4+ 135 ps +17-14     190.42 14 E20.700B(E2)(W.u.)=123 14, α=0.700 10
   317.330 (3)- 4.7 ps +26-14      75.13 2 [E2]36.8B(E2)(W.u.)=98 +49-40, α=36.8 5
(3)- 4.7 ps +26-14     206.22 4 E10.0839B(E1)(W.u.)=0.0041 +17-14, α=0.0839 12
   473.87 (5-) 24 ps +5-9     156.5 1 [E2]1.480B(E2)(W.u.)=109 +30-26, α=1.480 21
(5-) 24 ps +5-9     172.37 2 [E1]0.1288B(E1)(W.u.)=0.00123 +60-24, α=0.1288 18
   549.97 (6+) 34 ps +6-5      77[E1]0.2211B(E1)(W.u.)=0.00211 +44-40, α=0.2211 31
(6+) 34 ps +6-5     248.4 2 [E2]0.276B(E2)(W.u.)=135 +24-21, α=0.276 4
   702.92 (7-) 15 ps 5     153.1 5 [E1]0.1715B(E1)(W.u.)=0.0024 +12-7, α=0.1715 28
(7-) 15 ps 5     229.3 5 [E2]0.362B(E2)(W.u.)=95 +74-38, α=0.362 6
   842.93 (8+) 11.1 ps +31-24     140.1 2 [E1]0.2126B(E1)(W.u.)=0.00265 +75-66, α=0.2126 31
(8+) 11.1 ps +31-24     292.9 2 [E2]0.1636B(E2)(W.u.)=119 +36-28, α=0.1636 23
   992.12 (9-) 5.1 ps +17-13     149.3 5 [E1]0.1822B(E1)(W.u.)=0.0049 +18-14, α=0.1822 30
(9-) 5.1 ps +17-13     289.0 5 [E2]0.1705B(E2)(W.u.)=2.7E2 +10-7, α=0.1705 26
  1173.02 (10+) 5.0 ps +24-17     180.9 2 [E1]0.1147B(E1)(W.u.)=0.0032 +16-11, α=0.1147 16
(10+) 5.0 ps +24-17     330.1 2 [E2]0.1147B(E2)(W.u.)=139 +76-48, α=0.1147 16
  1330.5 (11-) 3.6 ps +18-12     157.4 5 [E1]0.1604B(E1)(W.u.)=0.0046 +24-16, α=0.1604 26
(11-) 3.6 ps +18-12     338.3 5 [E2]0.1069B(E2)(W.u.)=2.4E2 +13-8, α=0.1069 16
  1536.8 (12+) 4.6 ps +26-16     206.2 5 [E1]0.0839B(E1)(W.u.)=0.00164 +93-62, α=0.0839 13
(12+) 4.6 ps +26-16     363.9 5 [E2]0.0871B(E2)(W.u.)=136 +78-48, α=0.0871 13
  1710.0 (13-)      173.1 5 [E1]0.1275α=0.1275 20
(13-)      379.6 5 [E2]0.0776α=0.0776 11
  1932.9 (14+)      396.0 5 [E2]0.0693α=0.0693 10
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityConversion
Coefficient
Additional Data
  2125.0 (15-)      192.1 5 [E1]0.0993α=0.0993 15
(15-)      415.0 5 [E2]0.0613α=0.0613 9
  2358.4 (16+)      425.5 5 [E2]0.0575α=0.0575 8
  2569.8 (17-)      444.8 5 [E2]0.0514α=0.0514 7
  2810.7 (18+)      452.3 5 [E2]0.0493α=0.0493 7
  3040.6 (19-)      470.8 5 [E2]0.0447α=0.0447 6
  3287.4 (20+)      476.7 5 [E2]0.0434α=0.0434 6

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.00+ 33.6 s 4 
% α = 100
% 14C = 3.0×10-8 10
Evaluated rms charge radius <r2>1/2=5.687 fm 24 (2013An02).
E(level): Evaluated rms charge radius <r2>1/2=5.687 fm 24 (2013An02). Kπ=0+ g.s. band.
   111.1372+ 0.52 ns 4  Q=-0.75 29
E(level): Kπ=0+ g.s. band.
   242.1571- 9.5 ps +21-16  E(level): Kπ=0- octupole vibrational band.
   301.4954+ 135 ps +17-14  Q=-1.59 29
E(level): Kπ=0+ g.s. band.
   317.330(3)- 4.7 ps +26-14  The nuclear electric dipole moment was deduced by 1992Ru01 as 0.036 6 fm from the branching ratio for E1, E2 transitions deexciting the level. The electric quadrupole moment of 6.74 b 28 for both the g.s. and the Kπ=0- band was assumed.
E(level): The nuclear electric dipole moment was deduced by 1992Ru01 as 0.036 6 fm from the branching ratio for E1, E2 transitions deexciting the level. The electric quadrupole moment of 6.74 b 28 for both the g.s. and the Kπ=0- band was assumed. Kπ=0- octupole vibrational band.
   473.87(5-) 24 ps +5-9  E(level): Kπ=0- octupole vibrational band.
   549.97(6+) 34 ps +6-5  E(level): Kπ=0+ g.s. band.
   702.92(7-) 15 ps 5  E(level): Kπ=0- octupole vibrational band.
   842.93(8+) 11.1 ps +31-24  E(level): Kπ=0+ g.s. band.
   914.174(0+)   E(level): Kπ=(0+) band.
   992.12(9-) 5.1 ps +17-13  E(level): Kπ=0- octupole vibrational band.
  1024.920(2+)   E(level): Kπ=(0+) band.
  1173.02(10+) 5.0 ps +24-17  E(level): Kπ=0+ g.s. band.
  1330.5(11-) 3.6 ps +18-12  E(level): Kπ=0- octupole vibrational band.
  1536.8(12+) 4.6 ps +26-16  E(level): Kπ=0+ g.s. band.
  1710.0(13-)   E(level): Kπ=0- octupole vibrational band.
  1932.9(14+)   E(level): Kπ=0+ g.s. band.
  2125.0(15-)   E(level): Kπ=0- octupole vibrational band.
  2358.4(16+)   E(level): Kπ=0+ g.s. band.
  2569.8(17-)   E(level): Kπ=0- octupole vibrational band.
  2810.7(18+)   E(level): Kπ=0+ g.s. band.
  3040.6(19-)   E(level): Kπ=0- octupole vibrational band.
  3287.4(20+)   E(level): Kπ=0+ g.s. band.

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Additional Gamma Comments:

E(level)E(gamma)Comments
   111.137   111.15E(γ): unweighted average of 111.11 1 from 222Fr β- decay, 111.15 1 from 226Th α decay, and 111.2 2 from (136Xe,Xγ)
   242.157   131.01E(γ): unweighted average of 130.98 1 from 222Fr β- decay and 131.04 1 from 226Th α decay
I(γ): from 226Th α decay. Other: 31.8 31 from 222Fr β- decay
M(γ): from intensity balance in 226Th α decay
   242.13E(γ): unweighted average of 242.11 1 from 222Fr β- decay and 242.14 1 from 226Th α decay
I(γ): from 226Th α decay. Other: 100 10 from 222Fr β- decay
   301.495   190.42E(γ): unweighted average of 190.24 2 from 222Fr β- decay, 190.31 1 from 226Th α decay, and 190.7 2 from (136Xe,Xγ)
   317.330   206.22E(γ): unweighted average of 206.18 2 from 222Fr β- decay and 206.25 1 from 226Th α decay
I(γ): from 226Th α decay. Other: 100 10 from 222Fr β- decay
   473.87   156.5E(γ): from level-energy difference.
I(γ): from B(E2,157γ)/B(E1,172γ) ratio in Coulomb excitation; this γ has not been observed.
   172.37E(γ): others: 172.3 2 from 226Th α decay and 172.2 5 from (136Xe,Xγ)
   549.97   248.4E(γ): From 232Th(136Xe,Xγ)
I(γ): from Coulomb excitation
   702.92   153.1E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   229.3E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   842.93   140.1E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   292.9E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   914.174   802.7E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=803.036. Poor fit; uncertainty multiplied by a factor in the fitting
   992.12   149.3E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   289.0E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
  1024.920   707.54E(γ): other: 707.52 9 from 226Th α decay
I(γ): other: 100 9 from 226Th α decay
   723.45E(γ): weighted average of 723.45 4 from 222Fr β- decay and 722.9 4 from 226Th α decay
I(γ): other: 15 6 from 226Th α decay is discrepant
   782.77E(γ): other: 783.0 5 from 226Th α decay
I(γ): other: 112 25 from 226Th α decay
   913.69E(γ): other: 913.9 4 from 226Th α decay
I(γ): other: 66 33 from 226Th α decay is discrepant
  1170.99   696.88E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=697.13. Poor fit; uncertainty multiplied by a factor in the fitting
  1173.02   180.9E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   330.1E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
  1330.5   157.4E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   338.3E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
  1360.88  1249.1E(γ): uncertainty multiplied by a factor of 3 in the fitting; level-energy difference=1249.74. Poor fit; uncertainty multiplied by a factor in the fitting
E(level)E(gamma)Comments
  1439.994  1122.41E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=1122.661. Poor fit; uncertainty multiplied by a factor in the fitting
  1536.8   206.2E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   363.9E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
  1710.0   173.1E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   379.6E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
  1754.36  1280.99E(γ): uncertainty multiplied by a factor of 3 in the fitting; level-energy difference=1280.49. Poor fit; uncertainty multiplied by a factor in the fitting
  1436.4E(γ): uncertainty multiplied by a factor of 3 in the fitting; level-energy difference=1437.03. Poor fit; uncertainty multiplied by a factor in the fitting
  1453.4E(γ): uncertainty multiplied by a factor of 3 in the fitting; level-energy difference=1452.86. Poor fit; uncertainty multiplied by a factor in the fitting
  1643.9E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=1643.22. Poor fit; uncertainty multiplied by a factor in the fitting
  1841.20  1599.6E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=1599.04. Poor fit; uncertainty multiplied by a factor in the fitting
  1932.9   396.0E(γ): From 232Th(136Xe,Xγ)
  2125.0   192.1E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
   415.0E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
  2358.4   425.5E(γ): From 232Th(136Xe,Xγ)
  2569.8   211.4E(γ): From 232Th(136Xe,Xγ)
   444.8E(γ): From 232Th(136Xe,Xγ)
I(γ): From 232Th(136Xe,Xγ)
  2810.7   452.3E(γ): From 232Th(136Xe,Xγ)
  3040.6   470.8E(γ): From 232Th(136Xe,Xγ)
  3287.4   476.7E(γ): From 232Th(136Xe,Xγ)

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