ADOPTED LEVELS, GAMMAS for 193Po
Author: M. Shamsuzzoha Basunia | Citation: Nucl. Data Sheets 143, 1 (2017) | Cutoff date: 31-Mar-2017
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-8258 keV 26 | S(n)= 8326 keV 18 | S(p)= 2080 keV 30 | Q(α)= 7094 keV 4 | ||
Reference: 2017WA10 |
References: | |||
A | 197Rn α decay (55 MS) | B | 197Rn α decay (24 MS) |
C | 160Dy(36Ar,3nγ) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | Final Levels | |
0.0 | A | (3/2-) | 399 ms 34 % α ≤ 100 | ||||
100 6 | BC | (13/2+) | 245 ms 11 % α ≤ 100 | ||||
351.4 5 | C | (17/2+) | 251.4 5 | 100 | 100 | (13/2+) | |
375.0 5 | C | (15/2+) | 274.9 5 ? | 100 | 100 | (13/2+) | |
712.3 7 | C | (21/2+) | 360.9 5 | 100 | 351.4 | (17/2+) | |
744.3 8 | C | (19/2+) | 369 1 ? 393 1 ? | 100 28 83 22 | 375.0 351.4 | (15/2+) (17/2+) | |
1176.0 9 | C | (25/2+) | 463.7 5 | 100 | 712.3 | (21/2+) | |
1229.7 10 | C | (23/2+) | 485 1 ? 518 1 ? | | 744.3 712.3 | (19/2+) (21/2+) |
E(level): Level energies from a least-squares fit to adopted γ-ray energies, keeping energy of (13/2+) level fixed at 100 keV
Jπ(level): From 160Dy(36Ar,2nγ) unless otherwise noted. The assignments are based on band structures
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | Final Levels | ||
Band 1 - Band based on (13/2+) | |||||||
100 6 | (13/2+) | 245 ms 11 % α ≤ 100 | |||||
351.4 5 | (17/2+) | ||||||
712.3 7 | (21/2+) | 360.9 5 | 100 | 351.4 | (17/2+) | ||
1176.0 9 | (25/2+) | 463.7 5 | 100 | 712.3 | (21/2+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | Final Levels | ||
Band 2 - Band based on (15/2+) | |||||||
375.0 5 | (15/2+) | ||||||
744.3 8 | (19/2+) | ||||||
1229.7 10 | (23/2+) | 485 1 ? 518 1 ? | | 744.3 712.3 | (19/2+) (21/2+) |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | (3/2-) | 399 ms 34 % α ≤ 100 | μ=-0.389 37 (2014Se07), Q=-1.31 30 (2014Se07) δν(193Po,196Po)=-0.59 GHz 15; δ|4r2|5(193Po,210Po)=-0.576 fm2 13 (2013Se03). The uncertainties are statistical only. E(level): δν(193Po,196Po)=-0.59 GHz 15; δ|4r2|5(193Po,210Po)=-0.576 fm2 13 (2013Se03). The uncertainties are statistical only. Jπ(level): From systematics and from shell model two isomers are expected in a n=109 nucleus: high spin 1i13/2, and low spin 3p3/2 (189Hg). |
100 | (13/2+) | 245 ms 11 % α ≤ 100 | μ=-0.742 65 (2014Se07), Q=+1.08 50 (2014Se07) δν(193Po,196Po)=-1.11 GHz 15; δ|4r2|5(193Po,210Po)=-0.532 fm2 13 (2013Se03) The uncertainties are statistical only. E(level): δν(193Po,196Po)=-1.11 GHz 15; δ|4r2|5(193Po,210Po)=-0.532 fm2 13 (2013Se03) The uncertainties are statistical only. Band based on (13/2+). Jπ(level): From systematics and from shell model two isomers are expected in a n=109 nucleus: high spin 1i13/2, and low spin 3p3/2 (189Hg). |
351.4 | (17/2+) | E(level): Band based on (13/2+). | |
375.0 | (15/2+) | E(level): Band based on (15/2+). | |
712.3 | (21/2+) | E(level): Band based on (13/2+). | |
744.3 | (19/2+) | E(level): Band based on (15/2+). | |
1176.0 | (25/2+) | E(level): Band based on (13/2+). | |
1229.7 | (23/2+) | E(level): Band based on (15/2+). |
2013Se03, 2014Se07: beam of 193Po produced at the CERN ISOLDE facility by impinging 1.4 GeV protons on a 50 g/cm2 thick, UCx target. Reaction products diffused out and transferred to the RILIS. Deduced nuclear charge radius from the measured isotope shifts; magnetic dipole and electric quadrupole moments from measured hyperfine structure. Systematic uncertainties in δ|4r2|5 arising from electronic factor and mass-shift calculations are not included. Their magnitude is similar to the quoted experimental uncertainty
2015AnZZ: Measured 193Po production cross section, 5 μ 1, from 56Fe+141Pr fusion-evaporation reaction at E=50 MeV.
Levels: Identification: 185Re(19F,xn) excitation functions (1967Si09); 182W(20Ne,xn) excitation functions (1977De32); natCe(56Fe,xn) and 141Pr(56Fe,p3n) excitation function (1981Le23).
Levels: The level scheme is from 1999He32.