ADOPTED LEVELS, GAMMAS for 185Hg
Author: S. -c. Wu | Citation: Nucl. Data Sheets 106, 619 (2005) | Cutoff date: 1-Nov-2005
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-6.42×103 keV 3 | S(n)= 7898 keV 19 | S(p)= 3.15×103 keV 3 | Q(α)= 5774 keV 5 | ||
Reference: 2012WA38 |
References: | |||
A | 161Dy(28Si,4nγ) | B | 185Hg IT decay (21.6 S) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | AB | 1/2- | 49.1 s 10 % ε = 94 1 % α = 6 1 | |||||
26.1 5 | B | 3/2- | 26.1 5 | 100 | M1+E2 | 0.0 | 1/2- | |
34 8 | AB | (7/2)- | 8 8 S | | 26.1 | 3/2- | ||
96 1 | A | (5/2)- | 96 1 | | (Q) | 0.0 | 1/2- | |
99.3 5 | AB | 13/2+ | 21.6 s 15 % ε = 46 10 % IT = 54 10 % α ≈ 0.03 | 65.3 5 | 100 | E3 | 34 | (7/2)- |
141.0 4 | A | (9/2)- | 107.2 5 | 100 | (D+Q) | 34 | (7/2)- | |
212.7 14 | A | (9/2+) | ||||||
280.7 4 | A | (11/2)- | 139.9 5 246.5 5 | 21 100 | D+Q E2 | 141.0 34 | (9/2)- (7/2)- | |
329.5 11 | A | (9/2)- | 233.5 4 | 100 | Q | 96 | (5/2)- | |
412.7 9 | A | (11/2+) | 200 1 313 1 | | (D+Q) (D+Q) | 212.7 99.3 | (9/2+) 13/2+ | |
435.7 5 | A | (13/2)- | 155 1 294.6 4 | 6 100 | (D+Q) E2 | 280.7 141.0 | (11/2)- (9/2)- | |
479.8 6 | A | (17/2)+ | 380.5 4 | 100 | (Q) | 99.3 | 13/2+ | |
541.2 6 | A | (17/2)+ | 441.9 4 | 100 | E2 | 99.3 | 13/2+ | |
549.6 9 | A | (15/2+) | 136.8 5 | 100 | (Q) | 412.7 | (11/2+) | |
612.7 5 | A | (15/2)- | 177 1 332.1 4 | 6.3 100 | (D+Q) E2 | 435.7 280.7 | (13/2)- (11/2)- | |
633.8 11 | A | (13/2)- | 304.3 4 | 100 | E2 | 329.5 | (9/2)- | |
806.5 6 | A | (17/2)- | 194 1 370.7 4 | 100 | (D+Q) E2 | 612.7 435.7 | (15/2)- (13/2)- | |
906.8 | A | (19/2)+ | 358 1 366 1 428.4 5 | 80 90 100 | (Q) (D+Q) M1+E2 | 549.6 541.2 479.8 | (15/2+) (17/2)+ (17/2)+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1015.3 12 | A | (17/2)- | 381.5 4 | 100 | E2 | 633.8 | (13/2)- | |
1020.0 6 | A | (19/2)- | 213 1 407.4 4 | 100 | (D+Q) E2 | 806.5 612.7 | (17/2)- (15/2)- | |
1030.5 6 | A | (21/2)+ | 489.4 2 | 100 | E2 | 541.2 | (17/2)+ | |
1093 | A | (21/2+) | 614 1 | 100 | (Q) | 479.8 | (17/2)+ | |
1248.4 6 | A | (21/2)- | 228 1 441.9 4 | 100 | (D+Q) (Q) | 1020.0 806.5 | (19/2)- (17/2)- | |
1359.9 7 | A | (23/2)+ | 329 1 452.0 4 | 33 100 | (D+Q) E2 | 1030.5 906.8 | (21/2)+ (19/2)+ | |
1460.6 13 | A | (21/2)- | 445.3 4 | 100 | E2 | 1015.3 | (17/2)- | |
1495.4 7 | A | (23/2)- | 247 1 475.4 4 | 100 | (D+Q) E2 | 1248.4 1020.0 | (21/2)- (19/2)- | |
1514.3 7 | A | (25/2)+ | 152 1 419 1 ? 483.8 2 | 100 | (D+Q) (Q) E2 | 1359.9 1093 1030.5 | (23/2)+ (21/2+) (21/2)+ | |
1752.9 8 | A | (25/2)- | 504.5 4 | 100 | E2 | 1248.4 | (21/2)- | |
1886 | A | (27/2)+ | 373 1 527.3 4 | 17 100 | (D+Q) E2 | 1514.3 1359.9 | (25/2)+ (23/2)+ | |
1954.7 13 | A | (25/2)- | 494.1 4 | 100 | E2 | 1460.6 | (21/2)- | |
2029.2 8 | A | (27/2)- | 533.8 4 | 100 | E2 | 1495.4 | (23/2)- | |
2052.0 7 | A | (29/2)+ | 165 1 ? 537.7 4 | 100 | (D+Q) E2 | 1886 1514.3 | (27/2)+ (25/2)+ | |
2310.1 9 | A | (29/2)- | 557.2 5 | 100 | Q | 1752.9 | (25/2)- | |
2478.9 8 | A | (31/2)+ | 427 1 591.7 5 | 25 100 | (D+Q) (Q) | 2052.0 1886 | (29/2)+ (27/2)+ | |
2480.5 14 | A | (29/2)- | 525.8 5 | 100 | (Q) | 1954.7 | (25/2)- | |
2611.8 9 | A | (31/2)- | 582.6 5 | 100 | E2 | 2029.2 | (27/2)- | |
2648.3 8 | A | (33/2)+ | 596.3 4 | 100 | Q | 2052.0 | (29/2)+ | |
2909.2 10 | A | (33/2)- | 599.1 5 | 100 | Q | 2310.1 | (29/2)- | |
3027.5 17 | A | (33/2)- | 547 1 | 100 | (Q) | 2480.5 | (29/2)- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3123.7 10 | A | (35/2+) | 644.8 5 | 100 | (Q) | 2478.9 | (31/2)+ | |
3236 | A | (35/2)- | 622.8 5 | 100 | Q | 2611.8 | (31/2)- | |
3295.2 10 | A | (37/2)+ | 646.9 5 | 100 | Q | 2648.3 | (33/2)+ | |
3532.7 11 | A | (37/2)- | 623.5 5 | 100 | (Q) | 2909.2 | (33/2)- | |
3617.3 18 | A | 589.8 5 | 100 | 3027.5 | (33/2)- | |||
3810.7 14 | A | 687.0 | 100 | 3123.7 | (35/2+) | |||
3867 | A | 631 1 | 100 | 3236 | (35/2)- | |||
3899 | A | 663.2 5 | 100 | 3236 | (35/2)- | |||
3982.7 11 | A | 687.5 5 | 100 | 3295.2 | (37/2)+ | |||
4176.9 13 | A | 644.2 5 | 100 | 3532.7 | (37/2)- | |||
4581? | A | 682 1 ? | | 3899 | ||||
4702.7 15 ? | A | 720 1 ? | | 3982.7 |
E(level): Deduced by evaluator from a least-squares fit to adopted γ-ray energies. Uncertainties do not include the 8-keV uncertainty in the energy of 21S isomer.
Jπ(level): Assignments from 161Dy(28Si,4nγ) are based on γ-ray multipolarities and decay patterns, angular distributions, linear polarizations, rotational structure, and on the energy systematics of other odd-A Hg isotopes. Ratios of stretched M1 to E2 intraband γ-ray reduced transition probabilities for transitions deexciting members of the 7/2[514] and 9/2[624] rotational bands are consistent with their Nilsson orbital assignments (1988Ha19). Specific arguments are given with the individual levels.
E(γ): Uncertainties have been deduced by evaluator from authors’ estimates of 0.2 keV to 0.5 keV in 161Dy(28Si,4nγ). ΔE=1 keV for for energies quoted to the nearest keV.
I(γ): Relative uncertainties are 10 to 30%.
M(γ): From γ(θ) and linear polarization measurements, and by assuming spin and parities from the level scheme (1988Ha19).
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - 1/2(521) ROTATIONAL band. PROLATE SHAPE. | |||||||
0.0 | 1/2- | 49.1 s 10 % ε = 94 1 % α = 6 1 | |||||
26.1 5 | 3/2- | 26.1 5 | 100 | M1+E2 | 0.0 | 1/2- | |
96 1 | (5/2)- | 96 1 | | (Q) | 0.0 | 1/2- | |
329.5 11 | (9/2)- | 233.5 4 | 100 | Q | 96 | (5/2)- | |
633.8 11 | (13/2)- | 304.3 4 | 100 | E2 | 329.5 | (9/2)- | |
1015.3 12 | (17/2)- | 381.5 4 | 100 | E2 | 633.8 | (13/2)- | |
1460.6 13 | (21/2)- | ||||||
1954.7 13 | (25/2)- | 494.1 4 | 100 | E2 | 1460.6 | (21/2)- | |
2480.5 14 | (29/2)- | 525.8 5 | 100 | (Q) | 1954.7 | (25/2)- | |
3027.5 17 | (33/2)- | 547 1 | 100 | (Q) | 2480.5 | (29/2)- | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=-1/2 | |||||||
34 8 | (7/2)- | ||||||
280.7 4 | (11/2)- | 139.9 5 246.5 5 | 21 100 | D+Q E2 | 141.0 34 | (9/2)- (7/2)- | |
612.7 5 | (15/2)- | 177 1 332.1 4 | 6.3 100 | (D+Q) E2 | 435.7 280.7 | (13/2)- (11/2)- | |
1020.0 6 | (19/2)- | 213 1 407.4 4 | 100 | (D+Q) E2 | 806.5 612.7 | (17/2)- (15/2)- | |
1495.4 7 | (23/2)- | 247 1 475.4 4 | 100 | (D+Q) E2 | 1248.4 1020.0 | (21/2)- (19/2)- | |
2029.2 8 | (27/2)- | 533.8 4 | 100 | E2 | 1495.4 | (23/2)- | |
2611.8 9 | (31/2)- | ||||||
3236 | (35/2)- | 622.8 5 | 100 | Q | 2611.8 | (31/2)- | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - 9/2(624) ROTATIONAL band. PROLATE SHAPE. α=+1/2 | |||||||
212.7 14 | (9/2+) | ||||||
541.2 6 | (17/2)+ | 441.9 4 | 100 | E2 | 99.3 | 13/2+ | |
1030.5 6 | (21/2)+ | 489.4 2 | 100 | E2 | 541.2 | (17/2)+ | |
1514.3 7 | (25/2)+ | 152 1 419 1 ? 483.8 2 | 100 | (D+Q) (Q) E2 | 1359.9 1093 1030.5 | (23/2)+ (21/2+) (21/2)+ | |
2052.0 7 | (29/2)+ | 165 1 ? 537.7 4 | 100 | (D+Q) E2 | 1886 1514.3 | (27/2)+ (25/2)+ | |
2648.3 8 | (33/2)+ | 596.3 4 | 100 | Q | 2052.0 | (29/2)+ | |
3295.2 10 | (37/2)+ | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - Kπ=13/2+, DECOUPLED ROTATIONAL band. Configuration=I13/2. | |||||||
99.3 5 | 13/2+ | 21.6 s 15 % ε = 46 10 % IT = 54 10 % α ≈ 0.03 | |||||
479.8 6 | (17/2)+ | 380.5 4 | 100 | (Q) | 99.3 | 13/2+ | |
1093 | (21/2+) | 614 1 | 100 | (Q) | 479.8 | (17/2)+ |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
26.1 | 3/2- | 26.1 5 | M1+E2 | 1.3 6 | 2.2×103 | α=2.2×103 5 | |
96 | (5/2)- | 96 1 | (Q) | 6.69 | α=6.69 | ||
99.3 | 13/2+ | 21.6 s 15 % ε = 46 10 % IT = 54 10 % α ≈ 0.03 | 65.3 5 | E3 | 1610 | B(E3)(W.u.)=0.0019 4, α=1610 | |
280.7 | (11/2)- | 246.5 5 | E2 | 0.197 | α=0.197 | ||
435.7 | (13/2)- | 294.6 4 | E2 | 0.114 | α=0.114 | ||
541.2 | (17/2)+ | 441.9 4 | E2 | 0.0369 | α=0.0369 | ||
612.7 | (15/2)- | 332.1 4 | E2 | 0.080 | α=0.080 | ||
633.8 | (13/2)- | 304.3 4 | E2 | 0.103 | α=0.103 | ||
806.5 | (17/2)- | 370.7 4 | E2 | 0.0588 | α=0.0588 | ||
1015.3 | (17/2)- | 381.5 4 | E2 | 0.0543 | α=0.0543 | ||
1020.0 | (19/2)- | 407.4 4 | E2 | 0.0456 | α=0.0456 | ||
1030.5 | (21/2)+ | 489.4 2 | E2 | 0.0286 | α=0.0286 | ||
1359.9 | (23/2)+ | 452.0 4 | E2 | 0.0348 | α=0.0348 | ||
1460.6 | (21/2)- | 445.3 4 | E2 | 0.0362 | α=0.0362 | ||
1495.4 | (23/2)- | 475.4 4 | E2 | 0.0307 | α=0.0307 | ||
1514.3 | (25/2)+ | 483.8 2 | E2 | 0.0294 | α=0.0294 | ||
1752.9 | (25/2)- | 504.5 4 | E2 | 0.0266 | α=0.0266 | ||
1886 | (27/2)+ | 527.3 4 | E2 | 0.0239 | α=0.0239 | ||
1954.7 | (25/2)- | 494.1 4 | E2 | 0.0279 | α=0.0279 | ||
2029.2 | (27/2)- | 533.8 4 | E2 | 0.0233 | α=0.0233 | ||
2052.0 | (29/2)+ | 537.7 4 | E2 | 0.0229 | α=0.0229 | ||
2611.8 | (31/2)- | 582.6 5 | E2 | 0.0190 | α=0.0190 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 1/2- | 49.1 s 10 % ε = 94 1 % α = 6 1 | μ=+0.508 3 %α=6 1 adopted by evaluator from data of 1970Ha18. See 185Hg(49 s) α decay. %α=5.5 7 was given by 1970Ha18. E(level): %α=6 1 adopted by evaluator from data of 1970Ha18. See 185Hg(49 s) α decay. %α=5.5 7 was given by 1970Ha18. 1/2(521) ROTATIONAL band. PROLATE SHAPE. |
26.1 | 3/2- | E(level): 1/2(521) ROTATIONAL band. PROLATE SHAPE. From 185Hg IT decay (21 s). | |
34 | (7/2)- | E(level): 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=-1/2. From 185Hg IT decay (21 s). | |
96 | (5/2)- | E(level): 1/2(521) ROTATIONAL band. PROLATE SHAPE. | |
99.3 | 13/2+ | 21.6 s 15 % ε = 46 10 % IT = 54 10 % α ≈ 0.03 | Q=0.20 33, μ=-1.017 9 %IT from 1982Bo27; %α from 1976GrZC, renormalized to %IT=54. E(level): %IT from 1982Bo27; %α from 1976GrZC, renormalized to %IT=54. Kπ=13/2+, DECOUPLED ROTATIONAL band. Configuration=I13/2. From 185Hg IT decay (21 s). |
212.7 | (9/2+) | E(level): 9/2(624) ROTATIONAL band. PROLATE SHAPE. α=+1/2. | |
280.7 | (11/2)- | E(level): 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=-1/2. | |
329.5 | (9/2)- | E(level): 1/2(521) ROTATIONAL band. PROLATE SHAPE. | |
479.8 | (17/2)+ | E(level): Kπ=13/2+, DECOUPLED ROTATIONAL band. Configuration=I13/2. | |
541.2 | (17/2)+ | E(level): 9/2(624) ROTATIONAL band. PROLATE SHAPE. α=+1/2. | |
612.7 | (15/2)- | E(level): 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=-1/2. | |
633.8 | (13/2)- | E(level): 1/2(521) ROTATIONAL band. PROLATE SHAPE. | |
1015.3 | (17/2)- | E(level): 1/2(521) ROTATIONAL band. PROLATE SHAPE. | |
1020.0 | (19/2)- | E(level): 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=-1/2. | |
1030.5 | (21/2)+ | E(level): 9/2(624) ROTATIONAL band. PROLATE SHAPE. α=+1/2. | |
1093 | (21/2+) | E(level): Kπ=13/2+, DECOUPLED ROTATIONAL band. Configuration=I13/2. | |
1460.6 | (21/2)- | E(level): 1/2(521) ROTATIONAL band. PROLATE SHAPE. | |
1495.4 | (23/2)- | E(level): 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=-1/2. | |
1514.3 | (25/2)+ | E(level): 9/2(624) ROTATIONAL band. PROLATE SHAPE. α=+1/2. | |
1954.7 | (25/2)- | E(level): 1/2(521) ROTATIONAL band. PROLATE SHAPE. | |
2029.2 | (27/2)- | E(level): 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=-1/2. | |
2052.0 | (29/2)+ | E(level): 9/2(624) ROTATIONAL band. PROLATE SHAPE. α=+1/2. | |
2480.5 | (29/2)- | E(level): 1/2(521) ROTATIONAL band. PROLATE SHAPE. | |
2611.8 | (31/2)- | E(level): 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=-1/2. | |
2648.3 | (33/2)+ | E(level): 9/2(624) ROTATIONAL band. PROLATE SHAPE. α=+1/2. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
3027.5 | (33/2)- | E(level): 1/2(521) ROTATIONAL band. PROLATE SHAPE. | |
3236 | (35/2)- | E(level): 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=-1/2. | |
3295.2 | (37/2)+ | E(level): 9/2(624) ROTATIONAL band. PROLATE SHAPE. α=+1/2. |
E(level) | E(gamma) | Comments |
26.1 | 26.1 | E(γ): ΔE estimated by evaluator from the conversion electron spectrum of 1982Bo27.. From 185Hg IT decay (21 s). I(γ): From 185Hg IT decay (21 s). |
34 | 8 | E(γ): Eγ<15 keV, from 185Hg IT decay (21 s). |
141.0 | 107.2 | I(γ): Weak. |
435.7 | 155 | I(γ): Complex line, Iγ is from coincidence data. |
541.2 | 441.9 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
612.7 | 177 | I(γ): Complex line, Iγ is from coincidence data. |
806.5 | 194 | I(γ): Weak. |
906.8 | 358 | I(γ): Complex line, Iγ is from coincidence data. | 366 | I(γ): Complex line, Iγ is from coincidence data. |
1020.0 | 213 | I(γ): Weak. |
1093 | 614 | I(γ): Complex line, Iγ is from coincidence data. |
1248.4 | 228 | I(γ): Weak. | 441.9 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1359.9 | 329 | I(γ): Complex line, Iγ is from coincidence data. |
1495.4 | 247 | I(γ): Weak. |
1514.3 | 152 | I(γ): Weak. | 419 | I(γ): Weak. |
1886 | 373 | I(γ): Complex line, Iγ is from coincidence data. |
2052.0 | 165 | I(γ): Weak. |
2478.9 | 427 | I(γ): Complex line, Iγ is from coincidence data. |
3027.5 | 547 | I(γ): Complex line, Iγ is from coincidence data. |
Levels: α significant signature splitting for the 9/2[624] rotational band could be explained in terms of nuclear shape coexistence within the i13/2 subshell: the 9/2[624] rotational band based on a prolate core, and a decoupled rotational band (configuration=i13/2) based on a slightly deformed oblate core. An alternative explanation requires mixing of a K=1/2 configuration with the i13/2 rotational bands, due to a possible hexadecapole deformation and γ asymmetry (1988Ha19). See also 1975Fr08 and 1980Pr01 for theoretical calculations of nuclear deformations, and 1979St04 for a discussion on the odd-particle rotation-aligned coupling scheme.
Levels: band(b) 7/2(514) ROTATIONAL band. PROLATE SHAPE. α=+1/2
Levels: band(d) 9/2(624) ROTATIONAL band. PROLATE SHAPE. α=-1/2
Gammas: From 161Dy(28Si,4nγ), unless otherwise specified.
Q-value: Note: Current evaluation has used the following Q record -6420 60 7898 19 3146 27 5774 5 1993Au05