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 6 | S(n)= 6715 keV 6 | S(p)= 6246 keV 6 | Q(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 |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCD | 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) | XREF | Jπ(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) | XREF | Jπ(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) | XREF | Jπ(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
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+ |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Conversion Coefficient | Additional Data |
111.137 | 2+ | 0.52 ns 4 | 111.15 3 | E2 | 6.12 | B(E2)(W.u.)=112.8 +96-82, α=6.12 9 |
242.157 | 1- | 9.5 ps +21-16 | 131.01 3 | (E1) | 0.2500 | B(E1)(W.u.)=0.00186 +40-34, α=0.2500 35 |
1- | 9.5 ps +21-16 | 242.13 2 | E1 | 0.0575 | B(E1)(W.u.)=0.00095 +19-17, α=0.0575 8 | |
301.495 | 4+ | 135 ps +17-14 | 190.42 14 | E2 | 0.700 | B(E2)(W.u.)=123 14, α=0.700 10 |
317.330 | (3)- | 4.7 ps +26-14 | 75.13 2 | [E2] | 36.8 | B(E2)(W.u.)=98 +49-40, α=36.8 5 |
(3)- | 4.7 ps +26-14 | 206.22 4 | E1 | 0.0839 | B(E1)(W.u.)=0.0041 +17-14, α=0.0839 12 | |
473.87 | (5-) | 24 ps +5-9 | 156.5 1 | [E2] | 1.480 | B(E2)(W.u.)=109 +30-26, α=1.480 21 |
(5-) | 24 ps +5-9 | 172.37 2 | [E1] | 0.1288 | B(E1)(W.u.)=0.00123 +60-24, α=0.1288 18 | |
549.97 | (6+) | 34 ps +6-5 | 77 | [E1] | 0.2211 | B(E1)(W.u.)=0.00211 +44-40, α=0.2211 31 |
(6+) | 34 ps +6-5 | 248.4 2 | [E2] | 0.276 | B(E2)(W.u.)=135 +24-21, α=0.276 4 | |
702.92 | (7-) | 15 ps 5 | 153.1 5 | [E1] | 0.1715 | B(E1)(W.u.)=0.0024 +12-7, α=0.1715 28 |
(7-) | 15 ps 5 | 229.3 5 | [E2] | 0.362 | B(E2)(W.u.)=95 +74-38, α=0.362 6 | |
842.93 | (8+) | 11.1 ps +31-24 | 140.1 2 | [E1] | 0.2126 | B(E1)(W.u.)=0.00265 +75-66, α=0.2126 31 |
(8+) | 11.1 ps +31-24 | 292.9 2 | [E2] | 0.1636 | B(E2)(W.u.)=119 +36-28, α=0.1636 23 | |
992.12 | (9-) | 5.1 ps +17-13 | 149.3 5 | [E1] | 0.1822 | B(E1)(W.u.)=0.0049 +18-14, α=0.1822 30 |
(9-) | 5.1 ps +17-13 | 289.0 5 | [E2] | 0.1705 | B(E2)(W.u.)=2.7E2 +10-7, α=0.1705 26 | |
1173.02 | (10+) | 5.0 ps +24-17 | 180.9 2 | [E1] | 0.1147 | B(E1)(W.u.)=0.0032 +16-11, α=0.1147 16 |
(10+) | 5.0 ps +24-17 | 330.1 2 | [E2] | 0.1147 | B(E2)(W.u.)=139 +76-48, α=0.1147 16 | |
1330.5 | (11-) | 3.6 ps +18-12 | 157.4 5 | [E1] | 0.1604 | B(E1)(W.u.)=0.0046 +24-16, α=0.1604 26 |
(11-) | 3.6 ps +18-12 | 338.3 5 | [E2] | 0.1069 | B(E2)(W.u.)=2.4E2 +13-8, α=0.1069 16 | |
1536.8 | (12+) | 4.6 ps +26-16 | 206.2 5 | [E1] | 0.0839 | B(E1)(W.u.)=0.00164 +93-62, α=0.0839 13 |
(12+) | 4.6 ps +26-16 | 363.9 5 | [E2] | 0.0871 | B(E2)(W.u.)=136 +78-48, α=0.0871 13 | |
1710.0 | (13-) | 173.1 5 | [E1] | 0.1275 | α=0.1275 20 | |
(13-) | 379.6 5 | [E2] | 0.0776 | α=0.0776 11 | ||
1932.9 | (14+) | 396.0 5 | [E2] | 0.0693 | α=0.0693 10 | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Conversion Coefficient | Additional Data |
2125.0 | (15-) | 192.1 5 | [E1] | 0.0993 | α=0.0993 15 | |
(15-) | 415.0 5 | [E2] | 0.0613 | α=0.0613 9 | ||
2358.4 | (16+) | 425.5 5 | [E2] | 0.0575 | α=0.0575 8 | |
2569.8 | (17-) | 444.8 5 | [E2] | 0.0514 | α=0.0514 7 | |
2810.7 | (18+) | 452.3 5 | [E2] | 0.0493 | α=0.0493 7 | |
3040.6 | (19-) | 470.8 5 | [E2] | 0.0447 | α=0.0447 6 | |
3287.4 | (20+) | 476.7 5 | [E2] | 0.0434 | α=0.0434 6 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 0+ | 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. |
111.137 | 2+ | 0.52 ns 4 | Q=-0.75 29 E(level): Kπ=0+ g.s. band. |
242.157 | 1- | 9.5 ps +21-16 | E(level): Kπ=0- octupole vibrational band. |
301.495 | 4+ | 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. |
E(level) | E(gamma) | Comments |
111.137 | 111.15 | E(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 | 131.01 | E(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 | 242.13 | E(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 | 190.42 | E(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 | 206.22 | E(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 | 156.5 | E(γ): from level-energy difference. I(γ): from B(E2,157γ)/B(E1,172γ) ratio in Coulomb excitation; this γ has not been observed. | 172.37 | E(γ): others: 172.3 2 from 226Th α decay and 172.2 5 from (136Xe,Xγ) |
549.97 | 248.4 | E(γ): From 232Th(136Xe,Xγ) I(γ): from Coulomb excitation |
702.92 | 153.1 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) | 229.3 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) |
842.93 | 140.1 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) | 292.9 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) |
914.174 | 802.7 | E(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 | 149.3 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) | 289.0 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) |
1024.920 | 707.54 | E(γ): other: 707.52 9 from 226Th α decay I(γ): other: 100 9 from 226Th α decay | 723.45 | E(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 | 782.77 | E(γ): other: 783.0 5 from 226Th α decay I(γ): other: 112 25 from 226Th α decay | 913.69 | E(γ): other: 913.9 4 from 226Th α decay I(γ): other: 66 33 from 226Th α decay is discrepant |
1170.99 | 696.88 | E(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 | 180.9 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) | 330.1 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) |
1330.5 | 157.4 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) | 338.3 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) |
1360.88 | 1249.1 | E(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 | 1122.41 | E(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 | 206.2 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) | 363.9 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) |
1710.0 | 173.1 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) | 379.6 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) |
1754.36 | 1280.99 | E(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 | 1436.4 | E(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 | 1453.4 | E(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 | 1643.9 | E(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 | 1599.6 | E(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 | 396.0 | E(γ): From 232Th(136Xe,Xγ) |
2125.0 | 192.1 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) | 415.0 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) |
2358.4 | 425.5 | E(γ): From 232Th(136Xe,Xγ) |
2569.8 | 211.4 | E(γ): From 232Th(136Xe,Xγ) | 444.8 | E(γ): From 232Th(136Xe,Xγ) I(γ): From 232Th(136Xe,Xγ) |
2810.7 | 452.3 | E(γ): From 232Th(136Xe,Xγ) |
3040.6 | 470.8 | E(γ): From 232Th(136Xe,Xγ) |
3287.4 | 476.7 | E(γ): From 232Th(136Xe,Xγ) |
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 (β2,β3) 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 (β2,β3) 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)