ADOPTED LEVELS, GAMMAS for 62Mn
Authors: Balraj Singh, Huang Xiaolong, and Wang Xianghan | Citation: Nucl. Data Sheets 204, 1 (2025) | Cutoff date: 30-Jun-2023
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=10354 keV 7 | S(n)= 4853 keV 7 | S(p)= 13316 keV 7 | Q(α)= -1052×101 keV 10 | ||
Reference: 2021WA16 |
References: | |||
A | 62Cr β- decay (200 MS) | B | NI(86Kr,X) |
C | 238U(64Ni,xγ) | D | 238U(70Zn,xγ) |
E | Coulomb Excitation |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | Final Levels | |
0.0 | A E | 1+ | 92 ms 13 % β- = 100 % β-n = ? | ||||
285.0 17 | A | (0+) | 285 2 | 100 | 0.0 | 1+ | |
343 4 | BCDE | 4+ | 671 ms 5 % β- = 100 % β-n = ? | ||||
418 2 | E | (2+,3+) | 418 2 | 100 | 0.0 | 1+ | |
459.0 3 | BCD | (4) | 95 ns 2 % IT ≈ 100 | 113.8 3 | 100 | 343 | 4+ |
568.0 5 | CD | (5) | 108.6 3 | 100 | 459.0 | (4) | |
640.0 17 | A | (1+) | 355 2 640 2 | 100 68 | 285.0 0.0 | (0+) 1+ | |
764 5 | CD | (6) | 195.8 2 | 100 | 568.0 | (5) | |
988.8 6 | CD | (7) | 224.6 3 | 100 | 764 | (6) | |
1500 3 ? | A | 1215 2 ? | 100 | 285.0 | (0+) | ||
1530.7 12 | CD | (8) | 540.9 10 | 100 | 988.8 | (7) |
E(level): From γ-ray studies when possible, except as noted.
Jπ(level): From systematics of even-A Mn nuclei and decay pattern. See also discussion in 2010Ch51
E(γ): From 238U(70Zn,Xγ), except as noted.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | Final Levels | ||
Band 1 - Band based on (4). | |||||||
459.0 3 | (4) | 95 ns 2 % IT ≈ 100 | |||||
568.0 5 | (5) | 108.6 3 | 100 | 459.0 | (4) | ||
764 5 | (6) | ||||||
988.8 6 | (7) | 224.6 3 | 100 | 764 | (6) | ||
1530.7 12 | (8) | 540.9 10 | 100 | 988.8 | (7) |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 1+ | 92 ms 13 % β- = 100 % β-n = ? | μ=+2.384 7 (2015He28,2019StZV), Q=+0.1 2 (2015He28,2021StZZ) Theoretical T1/2(β)=1.36 s, %β-n=0.016, 0.0 (2021Mi17, two values for a decay mode refer to different fission barriers). E(level): Theoretical T1/2(β)=1.36 s, %β-n=0.016, 0.0 (2021Mi17, two values for a decay mode refer to different fission barriers). |
343 | 4+ | 671 ms 5 % β- = 100 % β-n = ? | μ=+3.170 3 (2015He28,2019StZV), Q=+0.59 13 (2015He28,2021StZZ) δ<r2>(55Mn,62mMn)=+0.640 fm2 9(stat) 61(syst) (2016He14, deduced from isotope shifts for atomic transition). |
459.0 | (4) | 95 ns 2 % IT ≈ 100 | E(level): Band based on (4). |
568.0 | (5) | E(level): Band based on (4). | |
764 | (6) | E(level): Band based on (4). | |
988.8 | (7) | E(level): Band based on (4). | |
1500 | In level-scheme Fig. 9 of 2015Ga38, Jπ=(1+) is assigned for this level, but as the existence of this level remains uncertain, no assignment is recommended here. | ||
1530.7 | (8) | E(level): Band based on (4). |
E(level) | E(gamma) | Comments |
285.0 | 285 | E(γ): From 62Cr β- decay |
418 | 418 | E(γ): from Coulomb excitation. |
640.0 | 355 | E(γ): From 62Cr β- decay | 640 | E(γ): From 62Cr β- decay |
1500 | 1215 | E(γ): From 62Cr β- decay |
1983Ru06: 62Mn identified in W(76Ge,X) at 9 MeV/nucleon; mass separation. Assignment based on the agreement between the energy of the most intense 877-keV γ transition and the energy of the first excited level of 62Fe measured in the 64Ni(14C,16O) and (18O,20Ne) reactions, and the decay of the 877-keV γ and β- rays
Mass measurements: 2012Na15, 2012He13
Hyperfine structure studies: 2016He14, 2015He28 (also 2015He10)
Theoretical structure calculations:
2013Ji04: calculated levels, Jπ, bands, configurations, B(M1), B(E2), moments of inertia, neutron occupation numbers using large-scale shell model; discussed neutron g9/2 excitations.
2012Su07: calculated levels, Jπ, bands, configurations, and moments of inertia using projected shell model and Nilsson model.
2010Sr03: calculated levels, Jπ using large-scale shell model with GXPF1A and KB3G effective interactions; deduced wave functions.
Other theoretical calculations: seven references retrieved from the NSR database are listed in this dataset as ’document’ records.
Q-value: S(2n)=11699 7, S(2p)=30010 180, Q(β-n)=2325 7 (2021Wa16)