ADOPTED LEVELS, GAMMAS for 159Sm
Author: Balraj Singh | Citation: ENSDF | Cutoff date: 07-June-2023
Author: C. W. Reich | Citation: Nucl. Data Sheets 113, 157 (2012) | Cutoff date: 31-Dec-2010
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=3836 keV 7 | S(n)= 5027 keV 8 | S(p)= 10391 keV 6 | Q(α)= -2349 keV 11 | ||
Reference: 2021WA16 |
References: | |||
A | 159Pm β- decay (1.634 S) | B | 159Sm IT decay (115 NS) |
C | 252Cf SF decay |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABC | 5/2- | 11.37 s 15 % β- = 100 | |||||
71.8 5 | A | (7/2-) | 71.8 | 100 | [M1+E2] | 0.0 | 5/2- | |
163.1 9 | C | (9/2-) | 163.1 9 | 100 | [E2] | 0.0 | 5/2- | |
406.3 12 | C | (13/2-) | 243.2 7 | 100 | [E2] | 163.1 | (9/2-) | |
727.3 13 | C | (17/2-) | 321.0 | | [E2] | 406.3 | (13/2-) | |
1123.2 14 | C | (21/2-) | 395.9 | | [E2] | 727.3 | (17/2-) | |
1275.9 14 | C | (11/2-) | 115 ns 10 % IT = 100 | 869.6 8 | 100 | [M1+E2] | 406.3 | (13/2-) |
1418.9 15 | C | (13/2-) | 142.7 | | 1275.9 | (11/2-) | ||
1578.3 15 | C | (15/2-) | 159.2 302.7 | 330 70 100 | 1418.9 1275.9 | (13/2-) (11/2-) | ||
1591.3 15 | C | (25/2-) | 468.1 | | 1123.2 | (21/2-) | ||
1754.0 15 | C | (17/2-) | 175.8 335.1 | 210 40 100 | 1578.3 1418.9 | (15/2-) (13/2-) | ||
1946.0 15 | C | (19/2-) | 191.8 367.5 | | 1754.0 1578.3 | (17/2-) (15/2-) | ||
2128.0 16 | C | (29/2-) | 536.7 | | 1591.3 | (25/2-) | ||
2154.2 15 | C | (21/2-) | 207.9 400.5 | | 1946.0 1754.0 | (19/2-) (17/2-) | ||
2378.0 16 | C | (23/2-) | 223.9 432.0 | | 2154.2 1946.0 | (21/2-) (19/2-) | ||
2616.6 16 | C | (25/2-) | 238.5 462.4 | | 2378.0 2154.2 | (23/2-) (21/2-) | ||
2871.9 16 | C | (27/2-) | 255 494.0 | | 2616.6 2378.0 | (25/2-) (23/2-) | ||
3141.7 17 | C | (29/2-) | 270 525 | | 2871.9 2616.6 | (27/2-) (25/2-) |
E(level): From least-squares fit to Eγ data, assuming ΔEγ=0.5 keV or 1 keV, when not states, the former when Eγ stated to nearest tenth of a keV, the latter when stated to nearest keV
Jπ(level): Based on the observed γ-decay patterns and expected band structure.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - ν5/2[523]. | |||||||
0.0 | 5/2- | 11.37 s 15 % β- = 100 | |||||
71.8 5 | (7/2-) | 71.8 | 100 | [M1+E2] | 0.0 | 5/2- | |
163.1 9 | (9/2-) | 163.1 9 | 100 | [E2] | 0.0 | 5/2- | |
406.3 12 | (13/2-) | 243.2 7 | 100 | [E2] | 163.1 | (9/2-) | |
727.3 13 | (17/2-) | 321.0 | | [E2] | 406.3 | (13/2-) | |
1123.2 14 | (21/2-) | 395.9 | | [E2] | 727.3 | (17/2-) | |
1591.3 15 | (25/2-) | 468.1 | | 1123.2 | (21/2-) | ||
2128.0 16 | (29/2-) | 536.7 | | 1591.3 | (25/2-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - ν11/2[505],α=+1/2. | |||||||
1418.9 15 | (13/2-) | ||||||
1754.0 15 | (17/2-) | 175.8 335.1 | 210 40 100 | 1578.3 1418.9 | (15/2-) (13/2-) | ||
2154.2 15 | (21/2-) | 207.9 400.5 | | 1946.0 1754.0 | (19/2-) (17/2-) | ||
2616.6 16 | (25/2-) | 238.5 462.4 | | 2378.0 2154.2 | (23/2-) (21/2-) | ||
3141.7 17 | (29/2-) | 270 525 | | 2871.9 2616.6 | (27/2-) (25/2-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - ν11/2[505],α=-1/2. | |||||||
1275.9 14 | (11/2-) | 115 ns 10 % IT = 100 | |||||
1578.3 15 | (15/2-) | 159.2 302.7 | 330 70 100 | 1418.9 1275.9 | (13/2-) (11/2-) | ||
1946.0 15 | (19/2-) | 191.8 367.5 | | 1754.0 1578.3 | (17/2-) (15/2-) | ||
2378.0 16 | (23/2-) | 223.9 432.0 | | 2154.2 1946.0 | (21/2-) (19/2-) | ||
2871.9 16 | (27/2-) | 255 494.0 | | 2616.6 2378.0 | (25/2-) (23/2-) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Conversion Coefficient | Additional Data |
71.8 | (7/2-) | 71.8 | [M1+E2] | 6.2 | α=6.2 19 | |
163.1 | (9/2-) | 163.1 9 | [E2] | 0.417 | α=0.417 10 | |
406.3 | (13/2-) | 243.2 7 | [E2] | 0.1095 | α=0.1095 19 | |
727.3 | (17/2-) | 321.0 | [E2] | 0.0456 | α=0.0456 7 | |
1123.2 | (21/2-) | 395.9 | [E2] | 0.0245 | α=0.0245 4 | |
1275.9 | (11/2-) | 115 ns 10 % IT = 100 | 869.6 8 | [M1+E2] | 0.0044 | α=0.0044 11 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 5/2- | 11.37 s 15 % β- = 100 | E(level): ν5/2[523]. |
71.8 | (7/2-) | E(level): ν5/2[523]. | |
163.1 | (9/2-) | E(level): ν5/2[523]. | |
406.3 | (13/2-) | E(level): ν5/2[523]. | |
727.3 | (17/2-) | E(level): ν5/2[523]. | |
1123.2 | (21/2-) | E(level): ν5/2[523]. | |
1275.9 | (11/2-) | 115 ns 10 % IT = 100 | E(level): ν11/2[505],α=-1/2. |
1418.9 | (13/2-) | E(level): ν11/2[505],α=+1/2. | |
1578.3 | (15/2-) | E(level): ν11/2[505],α=-1/2. | |
1591.3 | (25/2-) | E(level): ν5/2[523]. | |
1754.0 | (17/2-) | E(level): ν11/2[505],α=+1/2. | |
1946.0 | (19/2-) | E(level): ν11/2[505],α=-1/2. | |
2128.0 | (29/2-) | E(level): ν5/2[523]. | |
2154.2 | (21/2-) | E(level): ν11/2[505],α=+1/2. | |
2378.0 | (23/2-) | E(level): ν11/2[505],α=-1/2. | |
2616.6 | (25/2-) | E(level): ν11/2[505],α=+1/2. | |
2871.9 | (27/2-) | E(level): ν11/2[505],α=-1/2. | |
3141.7 | (29/2-) | E(level): ν11/2[505],α=+1/2. |
E(level) | E(gamma) | Comments |
71.8 | 71.8 | E(γ): from 159Pm β- decay |
163.1 | 163.1 | E(γ): From 159Sm IT decay I(γ): From 159Sm IT decay |
406.3 | 243.2 | E(γ): From 159Sm IT decay I(γ): From 159Sm IT decay |
1275.9 | 869.6 | E(γ): From 159Sm IT decay I(γ): From 159Sm IT decay |
1578.3 | 302.7 | E(γ): Level-energy difference=301.8 |
1986Ma12: 159Sm produced and identified in 235U(n,F), followed by mass separation of fission fragments at the TRISTAN facility of Brookhaven National Laboratory. Measured half-life of the decay of 159Sm and two γ rays of 114 and 190 keV.
1987Wi14 (also 1986GrZX,1987Gr12,1988GrZY,1990An31): 159Sm produced and identified in SF decay of 252Cf, followed by online mass separation of fission fragments. Measured Eγ, Iγ for 16 γ rays.
2012Va02: measured mass of the g.s. from cyclotron frequency ratios using the Canadian Penning Trap mass spectrometer at the CARIBU-ANL facility.
Theoretical structure calculations:
2022An05: calculated charge radii and odd-even staggering (OES) effects using the relativistic mean field (RMF-BCS) and the modified RMF(BCS) approaches.
2020Li53: calculated energy levels, Jπ, ground-state band, moments of inertia, bandhead energy of isomeric state using modified Nilsson parameters to generate deformed bases for the projected shell model.
2015El05: calculated ground state energy, S(2n) using HFB method with SLy5 Skyrme and Gogny forces.
1984Al30: calculated quadrupole and hexadecapole moments, g.s. energy.
Q-value: S(2n)=11673 7, S(2p)=20292 6 (2021Wa16)