ADOPTED LEVELS, GAMMAS for 93Sr
Author: Coral M. Baglin | Citation: Nucl. Data Sheets 112, 1163 (2011) | Cutoff date: 15-Dec-2010
Full ENSDF file | Adopted Levels (PDF version)
| Q(β-)=4142 keV 12 | S(n)= 5290 keV 9 | S(p)= 12602 keV 10 | Q(α)= -5975 keV 8 | ||
| Reference: 2012WA38 |
| References: | |||
| A | 93Rb β- decay | B | 94Rb β-n decay |
| C | 252Cf SF decay | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 0 | ABC | 5/2+ | 7.43 m 3 % β- = 100 | |||||
| 213.431 11 | AB | (9/2)+ | 4.3 ns 1 | 213.429 11 | 100 | E2 | 0 | 5/2+ |
| 432.604 24 | AB | (5/2,7/2,9/2)+ | < 0.3 ns | 219.16 6 432.61 3 | 15.8 9 100.0 5 | M1,E2 M1,E2 | 213.431 0 | (9/2)+ 5/2+ |
| 986.12 5 | ABC | (9/2+) | 986.05 6 | 100 | 0 | 5/2+ | ||
| 1142.55 4 | AB | (5/2+,7/2,9/2+) | 709.95 5 929.04 9 1142.58 12 | 100 7 7.9 6 5.9 5 | 432.604 213.431 0 | (5/2,7/2,9/2)+ (9/2)+ 5/2+ | ||
| 1148.20 6 | AB | (5/2+,7/2,9/2+) | 934.70 10 1148.18 8 | 20.9 16 100 6 | 213.431 0 | (9/2)+ 5/2+ | ||
| 1238.24 7 | ABC | (7/2+) | 1238.30 8 | 100 | 0 | 5/2+ | ||
| 1385.31 6 | AB | 1385.21 8 | 100 | 0 | 5/2+ | |||
| 1529.32 10 | AB | 1096.71 9 | 100 | 432.604 | (5/2,7/2,9/2)+ | |||
| 1562.96 9 | A | (5/2+,7/2,9/2+) | 1349.67 21 1562.91 11 | 14.0 17 100 7 | 213.431 0 | (9/2)+ 5/2+ | ||
| 1779.79 7 | A C | (11/2-) | 793.65 6 1566.2 9 | 100 5 5.5 26 | 986.12 213.431 | (9/2+) (9/2)+ | ||
| 1808.44 6 | A | (5/2+,7/2,9/2+) | 822.41 22 1808.50 10 | 6.0 11 100 5 | 986.12 0 | (9/2+) 5/2+ | ||
| 1869.64 7 | A | 1437.10 16 1869.69 11 | 22.0 19 100 6 | 432.604 0 | (5/2,7/2,9/2)+ 5/2+ | |||
| 1910.86 9 | A | 768.36 23 1910.72 12 | 10.0 17 100 6 | 1142.55 0 | (5/2+,7/2,9/2+) 5/2+ | |||
| 2045.57 8 | A | 1059.4 3 1612.87 11 | 3.8 7 100 6 | 986.12 432.604 | (9/2+) (5/2,7/2,9/2)+ | |||
| 2054.02 9 | A | 905.6 3 2054.06 12 | 4.9 10 100 5 | 1148.20 0 | (5/2+,7/2,9/2+) 5/2+ | |||
| 2072.2 4 | C | (11/2+) | 292.4 833.9 | 100 55 | 1779.79 1238.24 | (11/2-) (7/2+) | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 2117.46 11 | A | 1684.76 13 | 100 | 432.604 | (5/2,7/2,9/2)+ | |||
| 2141.07 11 | A | (5/2+,7/2,9/2+) | 1927.64 12 | 100 | 213.431 | (9/2)+ | ||
| 2168.6 4 | C | (13/2+) | 388.8 1182.5 | 16 100 | 1779.79 986.12 | (11/2-) (9/2+) | ||
| 2273.00 12 | A | 1035.1 5 1130.12 16 1287.0 5 | 35 11 100 11 58 18 | 1238.24 1142.55 986.12 | (7/2+) (5/2+,7/2,9/2+) (9/2+) | |||
| 2292.87 7 | A | (5/2+,7/2,9/2+) | 1054.7 3 1150.38 13 1306.92 19 2292.80 13 | 11.1 23 87 8 21.5 26 100 6 | 1238.24 1142.55 986.12 0 | (7/2+) (5/2+,7/2,9/2+) (9/2+) 5/2+ | ||
| 2319.10 8 | A | (5/2+,7/2,9/2+) | 1332.97 8 1886.6 3 | 100 10 13.6 21 | 986.12 432.604 | (9/2+) (5/2,7/2,9/2)+ | ||
| 2351.51 11 | A | (5/2+,7/2,9/2+) | 1365.36 11 1919.0 4 | 100 7 33 6 | 986.12 432.604 | (9/2+) (5/2,7/2,9/2)+ | ||
| 2456.44 19 | A | 163.4 3 2023.9 4 | 94 21 100 21 | 2292.87 432.604 | (5/2+,7/2,9/2+) (5/2,7/2,9/2)+ | |||
| 2459.78 13 | A | 1473.2 6 2026.88 25 | 23 8 100 13 | 986.12 432.604 | (9/2+) (5/2,7/2,9/2)+ | |||
| 2530.4 10 | C | 750.6 | 100 | 1779.79 | (11/2-) | |||
| 2553.80 10 | A | 1315.64 10 1405.37 22 | 100 7 26 3 | 1238.24 1148.20 | (7/2+) (5/2+,7/2,9/2+) | |||
| 2621.39 14 | A | (5/2+,7/2,9/2+) | 1479.1 3 1635.20 15 | 16 3 100 8 | 1142.55 986.12 | (5/2+,7/2,9/2+) (9/2+) | ||
| 2737.44 17 | A | 2523.7 5 | 100 | 213.431 | (9/2)+ | |||
| 2770.70 13 | A | (GE7/2) | 901.08 18 990.9 3 2557.5 4 | 89 11 92 18 100 17 | 1869.64 1779.79 213.431 | (11/2-) (9/2)+ | ||
| 2773.99 25 | A | 1388.7 6 | 100 | 1385.31 | ||||
| 2782.21 11 | A | (5/2+,7/2,9/2+) | 1397.7 5 2349.58 17 2568.59 20 | 9 3 100 9 63 5 | 1385.31 432.604 213.431 | (5/2,7/2,9/2)+ (9/2)+ | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 2869.07 11 | A | 595.87 13 1726.3 4 2869.23 18 | 50 7 18 4 100 8 | 2273.00 1142.55 0 | (5/2+,7/2,9/2+) 5/2+ | |||
| 2886.46 9 | A | 1501.18 12 1738.4 9 2886.3 3 | 100 7 30 20 95 10 | 1385.31 1148.20 0 | (5/2+,7/2,9/2+) 5/2+ | |||
| 2954.3 8 | C | (9/2,11/2,13/2) | 882.1 1174.5 | 100 30 | 2072.2 1779.79 | (11/2+) (11/2-) | ||
| 2979.90 10 | A | 3/2,5/2,7/2 | 1594.61 12 2766.48 17 | 100 6 69 5 | 1385.31 213.431 | (9/2)+ | ||
| 3100.2 8 | C | (15/2-) | 931.6 1320.4 | 100 93 | 2168.6 1779.79 | (13/2+) (11/2-) | ||
| 3198.14 15 | A | 1812.76 21 | 100 | 1385.31 | ||||
| 3233.01 14 | A | (7/2-,9/2+) | 776.4 4 1115.77 22 1452.7 7 | 56 19 100 15 54 20 | 2456.44 2117.46 1779.79 | (11/2-) | ||
| 3256.40 12 | A | (5/2+,7/2,9/2+) | 2270.20 12 | 100 | 986.12 | (9/2+) | ||
| 3283.2 12 | C | (17/2+) | 1114.6 | 100 | 2168.6 | (13/2+) | ||
| 3307.7 12 | C | (15/2+) | 1235.5 | 100 | 2072.2 | (11/2+) | ||
| 3404.40 21 | A | (5/2+,7/2) | 1841.6 7 2256.2 9 2418.22 22 | 25 7 21 16 100 10 | 1562.96 1148.20 986.12 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (9/2+) | ||
| 3481.5 12 | C | 1409.3 | 100 | 2072.2 | (11/2+) | |||
| 3603.18 11 | A | (5/2+,7/2) | 404.99 18 1284.0 4 2454.97 22 3389.8 9 | 11.1 18 31 7 100 11 13 4 | 3198.14 2319.10 1148.20 213.431 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (9/2)+ | ||
| 3623.70 16 | A | 1164.36 25 1167.1 5 1578.0 3 1753.6 4 | 59 9 30 8 100 14 61 13 | 2459.78 2456.44 2045.57 1869.64 | ||||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 3772.0 10 | C | 1992.2 | 100 | 1779.79 | (11/2-) | |||
| 3789.19 14 | A | 3/2,5/2,7/2 | 1470.13 22 1743.2 5 2403.5 6 2646.6 6 3789.3 3 | 100 11 59 17 34 8 92 28 80 10 | 2319.10 2045.57 1385.31 1142.55 0 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) 5/2+ | ||
| 3803.73 9 | A | 3/2-,5/2-,7/2- | 1531.1 7 1892.70 24 1933.9 3 2661.08 22 3370.97 16 3803.98 19 | 4.1 12 11.1 13 16.4 26 19.8 19 72 4 100 6 | 2273.00 1910.86 1869.64 1142.55 432.604 0 | (5/2+,7/2,9/2+) (5/2,7/2,9/2)+ 5/2+ | ||
| 3847.62 8 | A | (7/2)- | 867.74 16 1978.28 15 2461.98 19 2704.97 17 2861.34 15 | 6.6 8 72 5 43 4 92 6 100 6 | 2979.90 1869.64 1385.31 1142.55 986.12 | 3/2,5/2,7/2 (5/2+,7/2,9/2+) (9/2+) | ||
| 3866.87 12 | A | (5/2+,7/2) | 610.1 4 1547.78 15 2724.60 25 2880.48 22 | 32 6 51 4 100 16 68 6 | 3256.40 2319.10 1142.55 986.12 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (9/2+) | ||
| 3867.40 8 | A | (7/2)- | 981.1 3 1515.8 3 1574.71 22 1749.61 19 1821.86 13 1956.4 3 1997.8 6 2058.78 17 2087.4 3 3867.60 17 | 5.1 11 3.6 7 4.8 5 9.8 9 22.3 15 6.8 9 2.3 7 13.6 11 6.8 9 100 5 | 2886.46 2351.51 2292.87 2117.46 2045.57 1910.86 1869.64 1808.44 1779.79 0 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (11/2-) 5/2+ | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 3869.9 10 | C | 2090.1 | 100 | 1779.79 | (11/2-) | |||
| 3876.82 10 | A | (5/2+,7/2) | 1736.3 13 1831.10 22 2068.36 24 2491.20 22 2638.1 4 2734.0 10 2890.4 3 3876.7 3 | 26 13 51 6 35 4 96 10 69 9 14 6 100 9 51 6 | 2141.07 2045.57 1808.44 1385.31 1238.24 1142.55 986.12 0 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (7/2+) (5/2+,7/2,9/2+) (9/2+) 5/2+ | ||
| 3880.9 16 | C | (21/2+) | 597.7 | 100 | 3283.2 | (17/2+) | ||
| 3890.64 10 | A | 3/2-,5/2-,7/2- | 1120.0 4 1836.4 6 2327.5 3 2505.20 15 3458.19 16 3890.5 3 | 2.0 6 8 5 3.1 5 22.0 14 100 5 5.6 6 | 2770.70 2054.02 1562.96 1385.31 432.604 0 | (GE7/2) (5/2+,7/2,9/2+) (5/2,7/2,9/2)+ 5/2+ | ||
| 3934.66 12 | A | (5/2+,7/2) | 1793.62 18 3502.6 4 3721.6 4 3934.34 18 | 27.5 25 55 9 15.5 25 100 5 | 2141.07 432.604 213.431 0 | (5/2+,7/2,9/2+) (5/2,7/2,9/2)+ (9/2)+ 5/2+ | ||
| 3954.94 8 | A | 3/2,5/2,7/2 | 351.74 11 721.99 17 1068.51 11 1494.85 15 1662.16 15 1900.94 12 2812.6 5 3954.2 12 | 10.9 11 8.3 11 100 9 38 3 60 5 76 5 18 4 6 3 | 3603.18 3233.01 2886.46 2459.78 2292.87 2054.02 1142.55 0 | (5/2+,7/2) (7/2-,9/2+) (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) 5/2+ | ||
| 4017.60 15 | A | 3/2,5/2,7/2 | 2147.6 3 2875.3 6 3585.4 5 4017.55 21 | 70 9 25 6 26 5 100 7 | 1869.64 1142.55 432.604 0 | (5/2+,7/2,9/2+) (5/2,7/2,9/2)+ 5/2+ | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 4037.86 10 | A | 3/2,5/2,7/2 | 1483.96 24 1983.2 9 1991.8 3 2168.24 14 2229.44 12 2799.9 4 | 9.3 13 7 3 17.8 24 47 3 100 6 16 3 | 2553.80 2054.02 2045.57 1869.64 1808.44 1238.24 | (5/2+,7/2,9/2+) (7/2+) | ||
| 4037.9 10 | C | 2258.1 | 100 | 1779.79 | (11/2-) | |||
| 4041.9 3 | A | 1690.9 7 2262.0 3 | 43 15 100 14 | 2351.51 1779.79 | (5/2+,7/2,9/2+) (11/2-) | |||
| 4097.43 12 | A | (7/2-) | 473.8 6 1359.92 16 1745.7 5 2954.93 24 3664.75 19 3883.95 22 | 5.1 22 37 3 22 6 83 10 100 7 82 6 | 3623.70 2737.44 2351.51 1142.55 432.604 213.431 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (5/2,7/2,9/2)+ (9/2)+ | ||
| 4156.4 10 | C | 2376.6 | 100 | 1779.79 | (11/2-) | |||
| 4336.12 24 | A | 3/2,5/2,7/2 | 1138.0 3 2773.2 4 | 100 16 60 10 | 3198.14 1562.96 | (5/2+,7/2,9/2+) | ||
| 4461.10 15 | A | 3/2,5/2,7/2 | 1204.9 7 2550.06 22 2652.62 22 4461.4 4 | 16 7 86 8 100 10 25 3 | 3256.40 1910.86 1808.44 0 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) 5/2+ | ||
| 4470.8 16 | C | 989.3 | 100 | 3481.5 | ||||
| 4509.26 12 | A | 3/2(-),5/2,7/2 | 661.64 11 3366.6 3 | 100 19 81 10 | 3847.62 1142.55 | (7/2)- (5/2+,7/2,9/2+) | ||
| 4577.6 3 | A | 3/2,5/2,7/2 | 1803.6 3 2258.4 4 | 91 13 100 20 | 2773.99 2319.10 | (5/2+,7/2,9/2+) | ||
| 4596.8 16 | C | (19/2+) | 1289.1 | 100 | 3307.7 | (15/2+) | ||
| 4620.20 16 | A | 3/2-,5/2-,7/2- | 602.6 4 831.2 3 1838.0 4 1882.9 4 3477.39 24 | 37 7 13 3 100 37 22 4 57 5 | 4017.60 3789.19 2782.21 2737.44 1142.55 | 3/2,5/2,7/2 3/2,5/2,7/2 (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 4714.64 13 | A | 3/2,5/2,7/2 | 205.2 6 910.91 14 3572.05 25 4281.9 3 | 35 18 48 5 100 9 57 5 | 4509.26 3803.73 1142.55 432.604 | 3/2(-),5/2,7/2 3/2-,5/2-,7/2- (5/2+,7/2,9/2+) (5/2,7/2,9/2)+ | ||
| 4790.38 25 | A | 3/2,5/2,7/2 | 1533.8 3 2170.4 16 2334.0 5 3642.4 6 | 100 15 37 37 46 10 69 15 | 3256.40 2621.39 2456.44 1148.20 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) | ||
| 4797.0 19 | C | (25/2+) | 916.1 | 100 | 3880.9 | (21/2+) | ||
| 4913.09 13 | A | (7/2)- | 2043.82 17 2359.45 16 2620.2 6 3104.1 8 3133.1 8 3770.4 3 | 94 7 100 7 26 6 22 7 27 8 55 6 | 2869.07 2553.80 2292.87 1808.44 1779.79 1142.55 | (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) (11/2-) (5/2+,7/2,9/2+) | ||
| 4991.28 14 | A | (7/2)- | 1100.63 12 1202.4 7 3211.6 6 3848.7 7 4004.5 8 | 100 9 26 12 62 13 59 13 43 11 | 3890.64 3789.19 1779.79 1142.55 986.12 | 3/2-,5/2-,7/2- 3/2,5/2,7/2 (11/2-) (5/2+,7/2,9/2+) (9/2+) | ||
| 5012.24 14 | A | 3/2,5/2,7/2 | 1077.60 17 1208.55 19 1222.7 4 2958.1 6 | 28 3 96 12 43 10 100 26 | 3934.66 3803.73 3789.19 2054.02 | (5/2+,7/2) 3/2-,5/2-,7/2- 3/2,5/2,7/2 | ||
| 5333.9 19 | C | 863.1 | 100 | 4470.8 | ||||
| 5384.67 12 | A | 3/2-,5/2-,7/2- | 1507.77 14 2602.38 22 2614.1 3 3821.9 4 4242.1 5 | 68 5 100 9 37 5 28 4 22 3 | 3876.82 2782.21 2770.70 1562.96 1142.55 | (5/2+,7/2) (5/2+,7/2,9/2+) (GE7/2) (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 5395.5 4 | A | (5/2-,7/2-) | 2624.8 5 4009.9 12 4156.6 6 5396.7 9 | 96 20 55 20 100 20 31 7 | 2770.70 1385.31 1238.24 0 | (GE7/2) (7/2+) 5/2+ | ||
| 5413.6 3 | A | 3/2(-) TO 7/2(-) | 3296.1 10 3544.0 8 4271.23 19 ? | 21 9 47 16 100 7 | 2117.46 1869.64 1142.55 | (5/2+,7/2,9/2+) | ||
| 5601.3 9 ? | A | 3547.2 9 ? | 100 | 2054.02 | ||||
| 5631.2 9 ? | A | 2398.3 3 ? 3172.1 4 ? 3338.0 4 ? 4645.0 9 | 63 9 100 14 70 12 23 7 | 3233.01 2459.78 2292.87 986.12 | (7/2-,9/2+) (5/2+,7/2,9/2+) (9/2+) | |||
| 5775.5 4 ? | A | 1439.6 5 ? 1908.1 6 ? 4627.0 5 ? | 88 29 95 31 100 14 | 4336.12 3867.40 1148.20 | 3/2,5/2,7/2 (7/2)- (5/2+,7/2,9/2+) | |||
| 6000.51 16 ? | A | 1491.25 24 ? 2377.0 3 ? 3113.85 24 ? 3226.4 3 ? 4615.4 9 ? | 29 4 32 5 100 9 71 7 10 3 | 4509.26 3623.70 2886.46 2773.99 1385.31 | 3/2(-),5/2,7/2 | |||
| 6096.7 3 ? | A | 2206.2 3 ? 4947.5 6 ? 4953.9 11 ? | 100 14 38 7 20 5 | 3890.64 1148.20 1142.55 | 3/2-,5/2-,7/2- (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) | |||
| 6260.73 21 ? | A | 3027.6 11 ? 3486.9 7 ? 3706.6 7 ? 3941.7 4 ? 4481.2 6 ? 4875.1 3 ? | 28 12 39 10 42 10 64 13 34 6 100 8 | 3233.01 2773.99 2553.80 2319.10 1779.79 1385.31 | (7/2-,9/2+) (5/2+,7/2,9/2+) (11/2-) | |||
| 6272.70 21 ? | A | 859.05 18 ? 3403.56 18 ? | 18.3 23 100 6 | 5413.6 2869.07 | 3/2(-) TO 7/2(-) | |||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 6277.40 22 ? | A | 2386.72 23 ? 2674.2 4 ? | 100 11 47 9 | 3890.64 3603.18 | 3/2-,5/2-,7/2- (5/2+,7/2) | |||
| 6707.42 22 ? | A | 2903.6 3 ? 4250.9 7 ? 4387.9 4 ? 4899.4 5 ? | 100 12 22 5 52 6 22 3 | 3803.73 2456.44 2319.10 1808.44 | 3/2-,5/2-,7/2- (5/2+,7/2,9/2+) (5/2+,7/2,9/2+) | |||
E(level): From least-squares fit to Eγ, except as noted; transitions with uncertain placement are omitted from the fit unless all transitions deexciting a given level are of this character, and 1 keV uncertainty is assumed for transitions for which the authors failed to state an uncertainty. Note that additional levels exist in the vicinity of 4250 keV and 5200 keV as evidenced by the β- strength distribution deduced from absorption γ spectrometry (see 93Rb β- decay); these are not included here because specific energies have not been determined. Tentative E(level) values proposed for n-emitting levels in 93Rb β-n decay (E=5300-6600) have also been omitted here.
Jπ(level): Values given without comment are very tentative suggestions from 2003Hw01 in 252Cf SF decay; they are based on the correspondence between level energies in 93Sr and the yrast levels of 94Sr which suggests a weak stretched or ’stretched-minus-one’ coupling of a d5/2 neutron hole to levels in a 94Sr core. Note that a number of Jπ values shown here depend critically on tentative assignments of (9/2)+ and (11/2-) to the 213 and 1780 levels, respectively.
M(γ): From α(K)exp in 93Rb β- decay.
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 1 - 5/2+ yrast band. | |||||||
| 0 | 5/2+ | 7.43 m 3 % β- = 100 | |||||
| 986.12 5 | (9/2+) | 986.05 6 | 100 | 0 | 5/2+ | ||
| 2168.6 4 | (13/2+) | 388.8 1182.5 | 16 100 | 1779.79 986.12 | (11/2-) (9/2+) | ||
| 3283.2 12 | (17/2+) | 1114.6 | 100 | 2168.6 | (13/2+) | ||
| 3880.9 16 | (21/2+) | 597.7 | 100 | 3283.2 | (17/2+) | ||
| 4797.0 19 | (25/2+) | 916.1 | 100 | 3880.9 | (21/2+) | ||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 2 - (11/2-) band. | |||||||
| 1779.79 7 | (11/2-) | ||||||
| 3100.2 8 | (15/2-) | 931.6 1320.4 | 100 93 | 2168.6 1779.79 | (13/2+) (11/2-) | ||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 3 - (7/2+) band. | |||||||
| 1238.24 7 | (7/2+) | ||||||
| 2072.2 4 | (11/2+) | 292.4 833.9 | 100 55 | 1779.79 1238.24 | (11/2-) (7/2+) | ||
| 3307.7 12 | (15/2+) | 1235.5 | 100 | 2072.2 | (11/2+) | ||
| 4596.8 16 | (19/2+) | 1289.1 | 100 | 3307.7 | (15/2+) | ||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Conversion Coefficient | Additional Data |
| 213.431 | (9/2)+ | 4.3 ns 1 | 213.429 11 | E2 | 0.0639 | B(E2)(W.u.)=11.2 3, α=0.0639 |
| 432.604 | (5/2,7/2,9/2)+ | < 0.3 ns | 219.16 6 | M1,E2 | 0.039 | α=0.039 19 |
| (5/2,7/2,9/2)+ | < 0.3 ns | 432.61 3 | M1,E2 | 0.0047 | α=0.0047 11 |
Additional Level Data and Comments:
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 0 | 5/2+ | 7.43 m 3 % β- = 100 | Q=+0.258 11, μ=-0.7926 12 μ: from fast ion beam collinear LASER spectroscopy (1990Bu12 and 1990Li28); value relative to 87Sr. E(level): μ: from fast ion beam collinear LASER spectroscopy (1990Bu12 and 1990Li28); value relative to 87Sr. From 252Cf SF decay. 5/2+ yrast band. |
| 986.12 | (9/2+) | E(level): From 252Cf SF decay. 5/2+ yrast band. | |
| 1238.24 | (7/2+) | E(level): (7/2+) band. | |
| 1779.79 | (11/2-) | E(level): (11/2-) band. | |
| 2072.2 | (11/2+) | E(level): (7/2+) band. | |
| 2168.6 | (13/2+) | E(level): From 252Cf SF decay. 5/2+ yrast band. | |
| 3100.2 | (15/2-) | E(level): (11/2-) band. | |
| 3283.2 | (17/2+) | E(level): From 252Cf SF decay. 5/2+ yrast band. | |
| 3307.7 | (15/2+) | E(level): (7/2+) band. | |
| 3880.9 | (21/2+) | E(level): From 252Cf SF decay. 5/2+ yrast band. | |
| 4596.8 | (19/2+) | 1289γ to (15/2+) 3308. E(level): 1289γ to (15/2+) 3308. (7/2+) band. | |
| 4797.0 | (25/2+) | 916γ to (21/2+) 3881. E(level): 916γ to (21/2+) 3881. From 252Cf SF decay. 5/2+ yrast band. | |
| 5601.3 | E(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. Jπ(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. | ||
| 5631.2 | E(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. Jπ(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. | ||
| 5775.5 | E(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. Jπ(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. | ||
| 6000.51 | E(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. Jπ(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. | ||
| 6096.7 | E(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. Jπ(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. | ||
| 6260.73 | E(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. Jπ(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. | ||
| 6272.70 | E(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. Jπ(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. | ||
| 6277.40 | E(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. Jπ(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. | ||
| 6707.42 | E(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. Jπ(level): Total absorption γ spectrometry data in 93Rb β- decay indicate β- population of level(s) at, or near, this energy. However, the β feeding is very much weaker than implied by the presence of the transitions shown tentatively deexciting this level. Those gammas are probably misplaced; if so, the stated level energy would no longer be meaningful, but some level(s) would exist within maybe 50 keV of this value. Provided only one level is being fed, log f1ut<8.5 so J=3/2,5/2,7/2. |
| E(level) | E(gamma) | Comments |
| 2072.2 | 292.4 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. | 833.9 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 2168.6 | 388.8 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. | 1182.5 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 2530.4 | 750.6 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 2954.3 | 882.1 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. | 1174.5 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 3100.2 | 931.6 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. | 1320.4 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 3283.2 | 1114.6 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 3307.7 | 1235.5 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 3481.5 | 1409.3 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 3772.0 | 1992.2 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 3869.9 | 2090.1 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 3880.9 | 597.7 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 4037.9 | 2258.1 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 4156.4 | 2376.6 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 4470.8 | 989.3 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 4596.8 | 1289.1 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 4797.0 | 916.1 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
| 5333.9 | 863.1 | E(γ): From 252Cf SF decay. I(γ): From 252Cf SF decay. |
For calculation of one-quasiparticle states, see 2010Ro27.
Q-value: Note: Current evaluation has used the following Q record 4140 12 5290 8 12601 10 -5975 8 2003Au03,2009AuZZ
Q-value: Q(β-), S(n), S(p), Q(α): from 2009AuZZ (cf. 4139 12, 5288 8, 12602 10, -5780 50, respectively, from 2003Au03).
Q-value: Q(β-n)=- 3341 12 (2009AuZZ) (cf.-3343 12 (2003Au03)).