ADOPTED LEVELS, GAMMAS for 49V
Author: T. W. Burrows | Citation: Nucl. Data Sheets 109, 1879 (2008) | Cutoff date: 14-Jul-2008
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-2628 keV 3 | S(n)= 11555.5 keV 13 | S(p)= 6758.2 keV 9 | Q(α)= -9314.7 keV 11 | ||
Reference: 2012WA38 |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCDEFGHIJ | 7/2- | 330 d 15 % ε = 100 | |||||
90.6392 17 | ABCDE GHIJ | 5/2- | 228 ps 13 | 90.639 2 | 100 | M1 | 0.0 | 7/2- |
152.9282 17 | A CDEFGHIJ | 3/2- | 19.90 ns 24 | 62.289 2 152.928 2 | 70.5 24 100 3 | (M1) E2 | 90.6392 0.0 | 5/2- 7/2- |
748.27 9 | ABCDE GH J | 3/2+ | 5.3 ps 6 | 595.35 14 657.60 14 | 100.0 15 85.2 15 | (E1(+M2)) (E1(+M2)) | 152.9282 90.6392 | 3/2- 5/2- |
1021.62 11 | ABCDEFGHIJ | 11/2- | 3.4 ps 6 | 1021.63 14 | 100 | E2 | 0.0 | 7/2- |
1140.53 11 | BCDE G J | 5/2+ | 1.3 ps 6 | 392.7 6 987.61 26 1049.79 17 1140.7 3 | 10.5 10 31.4 17 44.5 21 100 4 | M1+E2 (E1(+M2)) E1+M2 E1(+M2) | 748.27 152.9282 90.6392 0.0 | 3/2+ 3/2- 5/2- 7/2- |
1155.32 10 | ABCDEFGHIJ | 9/2- | 1.1 ps 3 | 133.80 17 1064.63 17 1155.33 17 | 3.9 8 30.0 6 100.0 10 | (M1(+E2)) E2 M1+E2 | 1021.62 90.6392 0.0 | 11/2- 5/2- 7/2- |
1183? | H | |||||||
1514.54 7 | A CD GHIJ | 5/2- | 31 fs 12 | 766 1 ? 1361.61 7 1423.6 3 1514.4 4 | 37 11 100.0 22 20.3 11 58 3 | (E1(+M2)) M1+E2 (M1(+E2)) D,E2 | 748.27 152.9282 90.6392 0.0 | 3/2+ 3/2- 5/2- 7/2- |
1602.68 12 | BCD G J | 7/2+ | 0.47 ps 22 | 447.4 3 462.2 2 854.5 3 1512.0 3 1602.6 2 | 1.6 8 13.5 17 15 4 100 8 49.3 20 | (E1) M1(+E2) (E2) (E1) (E1+M2) | 1155.32 1140.53 748.27 90.6392 0.0 | 9/2- 5/2+ 3/2+ 5/2- 7/2- |
1610? | H | (9/2-,11/2-) | ||||||
1643.19 18 | CD G | (3/2-,5/2) | 36 fs 11 | 1490.24 18 1553? | 100 <2.4 | D+Q | 152.9282 90.6392 | 3/2- 5/2- |
1646.43 21 | CD GH J | (1/2+) | 6.6 ps 10 | 898.06 26 1493.6 3 | 87 12 100 12 | D+Q (E1(+M2)) | 748.27 152.9282 | 3/2+ 3/2- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1661.40 13 | A CDEFG IJ | 3/2- | 16 fs 7 | 912.3 10 1508.37 18 1570.83 17 1661.4 10 | 9.6 20 65.4 20 100.0 20 17.3 20 | (E1(+M2)) D,E2 M1(+E2) (E2(+M3)) | 748.27 152.9282 90.6392 0.0 | 3/2+ 3/2- 5/2- 7/2- |
1994.7 4 | CD GH J | 3/2(+) | 0.49 ps 21 | 854.5 4 1246.8 10 1841.0 8 1903.4 8 | 85 21 46 5 100 5 62 5 | (M1+E2) D,E2 (E1+M2) (E1(+M2)) | 1140.53 748.27 152.9282 90.6392 | 5/2+ 3/2+ 3/2- 5/2- |
2178.3 4 | BCD GH J | 9/2+ | 0.56 ps +49-28 | 575.4 9 1023 1 ? 1037.4 5 1157.0 7 2178.3 8 | 11.3 17 33.9 17 16.1 17 100 5 | D(+Q) D,Q E2 D D(+Q) | 1602.68 1155.32 1140.53 1021.62 0.0 | 7/2+ 9/2- 5/2+ 11/2- 7/2- |
2182.0 4 | A CDEFGHIJ | 7/2- | 33 fs 12 | 1026.8 7 2090.7 7 2181.6 11 | 32 3 100 9 8 5 | (M1(+E2)) (M1+E2) D,Q | 1155.32 90.6392 0.0 | 9/2- 5/2- 7/2- |
2204? | EF | (5/2-,7/2-) | ||||||
2234.0 7 | A CD GHIJ | 5/2 | 12 fs 8 | 572.5 25 ? 2081.1 20 ? 2142.9 10 2234.4 15 | 21.9 16 26.6 16 100.0 16 7.8 16 | D,E2 D,E2 D(+Q) D+Q | 1661.40 152.9282 90.6392 0.0 | 3/2- 3/2- 5/2- 7/2- |
2263.30 21 | BC G IJ | 15/2- | 0.65 ps +38-19 | 1241.69 18 | 100 | E2 | 1021.62 | 11/2- |
2265.3 3 | CD GH J | 5/2- | 35 fs 9 | 621? 2112.3 3 | 5.3 100 15 | D D+Q | 1643.19 152.9282 | (3/2-,5/2) 3/2- |
2279? | E | 1/2-,3/2- | ||||||
2309.4 6 | A CDE GHIJ | 3/2- | 14 fs 7 | 1560? 2155.7 12 2218.6 8 2310.6 14 | 19 86 5 100 5 52 5 | (E1(+M2)) D+Q D+Q (E2) | 748.27 152.9282 90.6392 0.0 | 3/2+ 3/2- 5/2- 7/2- |
2353.4 4 | C GHIJ | 9/2- | 33 fs 12 | 1198.9 11 1331.7 7 2262.2 20 ? 2353.2 7 | 8.9 18 57.1 18 10.7 18 100.0 18 | D,E2 (M1+E2) (E2(+M3)) M1+E2 | 1155.32 1021.62 90.6392 0.0 | 9/2- 11/2- 5/2- 7/2- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2388.0 5 | CDE GH J | 5/2+ | 57 fs 20 | 393.6 15 ? 1247.8 12 ? 1639.3 6 2235.5 16 ? 2298.6 15 2388.6 14 | 16.9 17 11.9 17 100 5 <8.5 28.8 17 11.9 17 | (M1(+E2)) D,E2 M1+E2 (E1(+M2)) (E1(+M2)) | 1994.7 1140.53 748.27 152.9282 90.6392 0.0 | 3/2(+) 5/2+ 3/2+ 3/2- 5/2- 7/2- |
2408.3 4 | CD GHIJ | (7/2-) | < 8 fs | 229.2 20 ? 1252.9 8 1268? 1385.7 10 ? 2316.4 20 ? 2408.4 4 | <6.3 18.3 14 33 7.0 14 15.5 14 100.0 14 | D,E2 D D,E2 D,E2 D(+Q) | 2178.3 1155.32 1140.53 1021.62 90.6392 0.0 | 9/2+ 9/2- 5/2+ 11/2- 5/2- 7/2- |
2671.0 3 | BCD IJ | (11/2)- | < 11 fs | 1517 1 1649.2 3 | 33 100 | D,E2 M1+E2 | 1155.32 1021.62 | 9/2- 11/2- |
2671.3 9 ? | D G J | 7/2-,9/2,11/2+ | < 33.3 ps | 1649.3 10 ? 2579.2 20 ? 2672.8 20 ? | 100.0 12 4.4 12 6.7 12 | D,E2 D,Q,E3 | 1021.62 90.6392 0.0 | 11/2- 5/2- 7/2- |
2680.0 15 | D GH J | (7/2,9/2) | 1526 2 ? 1657 2 ? | 100 12 100 12 | 1155.32 1021.62 | 9/2- 11/2- | ||
2727.5 3 | BC GHIJ | 15/2- | 0.10 ps 4 | 464.2 3 1705.5 7 | 100 100 | M1(+E2) (E2) | 2263.30 1021.62 | 15/2- 11/2- |
2741.0 5 | BC | 11/2+ | 0.39 ps +36-17 | 562.5 7 1138.9 9 1585.8 9 1719.0 15 ? | 27.1 21 100 5 81 5 <10 | D,E2 (E2) (E1(+M2)) (E1(+M2)) | 2178.3 1602.68 1155.32 1021.62 | 9/2+ 7/2+ 9/2- 11/2- |
2786.4 3 | C E G IJ | (9/2)- | < 11 fs | 1184.3 10 ? 1631.0 5 1764.5 4 2697.2 20 ? 2786.4 5 | 6.7 23 53.3 23 100.0 23 8.9 23 53.3 23 | D,E2 D+Q D+Q,E2 D,E2 M1+E2,E2 | 1602.68 1155.32 1021.62 90.6392 0.0 | 7/2+ 9/2- 11/2- 5/2- 7/2- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2796.6 15 ? | G J | 1775.0 15 ? 2796 4 ? | 61 10 100 10 | 1021.62 0.0 | 11/2- 7/2- | |||
2808.3 7 | C GH | 5/2+ | 0.32 ps 6 | 1206.6 10 1666.7 10 2058? 2655.7 20 2808.5 20 | 26 5 24 5 54 17 88 8 100 8 | D,E2 D,E2 D,E2 (E1(+M2)) (E1(+M2)) | 1602.68 1140.53 748.27 152.9282 0.0 | 7/2+ 5/2+ 3/2+ 3/2- 7/2- |
2810.9 5 | CDE G IJ | 5/2-,7/2- | < 12 fs | 628.4 10 1673 2 ? 2720.3 19 2810.9 5 | 33 5 25 6 100 5 75 5 | M1 D,E2 D,E2 D,E2 | 2182.0 1140.53 90.6392 0.0 | 7/2- 5/2+ 5/2- 7/2- |
2861.5 5 | BC I | 13/2- | 0.10 ps 6 | 134 1 ? 598.3 7 1706 1 1840 1 ? | 28.2 13 100 6 | (M1(+E2)) (M1(+E2)) E2(+M3) D,E2 | 2727.5 2263.30 1155.32 1021.62 | 15/2- 15/2- 9/2- 11/2- |
3017.3 7 | C G I | < 33.3 ps | 1414.1 10 ? 2865.0 16 2926.5 13 3017.6 14 | 22.5 25 100 5 92 5 35 5 | D,Q | 1602.68 152.9282 90.6392 0.0 | 7/2+ 3/2- 5/2- 7/2- | |
3133.9 5 | C E HIJ | (9/2,11/2,13/2) | 0.22 ps +8-4 | 462.9 3 | 100 | D | 2671.0 | (11/2)- |
3134.0 6 | CDE GHIJ | 7/2,9/2(+) | < 33.3 ps | 1979.5 15 2112.8 16 2385.7 20 ? 3043.5 20 ? 3133.4 10 | 39.0 25 34.1 25 17.1 25 53.7 25 100.0 25 | D,Q D,Q D,Q,E3 D+Q | 1155.32 1021.62 748.27 90.6392 0.0 | 9/2- 11/2- 3/2+ 5/2- 7/2- |
3152.1 10 ? | E G | 2012.0 15 ? 2131.0 15 ? | 100 10 61 10 | 1140.53 1021.62 | 5/2+ 11/2- | |||
3224 1 | D | (1/2,3/2,5/2-) | 1566 3074 | 100 100 | 1661.40 152.9282 | 3/2- 3/2- | ||
3239.5 9 | D G IJ | 7/2- | < 33.3 ps | 1725.2 10 3148.9 20 3238.2 20 | 50.8 17 100.0 17 13.1 17 | D,Q D,Q,E3 | 1514.54 90.6392 0.0 | 5/2- 5/2- 7/2- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3242 2 | D | (3/2,5/2,7/2-) | ||||||
3248 | E H | 1/2+ | ||||||
3259.5 4 | CD | (GE 9/2) | 473.1 2 | 100 | 2786.4 | (9/2)- | ||
3303.2 9 | G | 3/2-,5/2,7/2,9/2 | < 33.3 ps | 1121.0 10 3213.5 20 3302.6 20 | 54 6 40 6 100 4 | D,E2 D,Q,E3 | 2182.0 90.6392 0.0 | 7/2- 5/2- 7/2- |
3305 3 | I | (13/2-) | ||||||
3325 2 | D | (1/2+ TO 7/2+) | ||||||
3325.2 4 | B IJ | (17/2-) | 464 1 597.1 5 1061.9 5 | 36.84 21.05 100 | D,Q D D | 2861.5 2727.5 2263.30 | 13/2- 15/2- 15/2- | |
3340.5 11 | GHIJ | < 33.3 ps | 1106.3 10 3341.2 20 | 37 5 100 3 | D,E2 | 2234.0 0.0 | 5/2 7/2- | |
3341.8 7 | C HIJ | (13/2+) | 601.0 8 670.5 8 1163.0 10 | 72.5 25 78 5 100 5 | D,E2 D,E2 D,Q | 2741.0 2671.0 2178.3 | 11/2+ (11/2)- 9/2+ | |
3342 2 | D | (1/2+ TO 9/2+) | ||||||
3388 1 | D H J | (3/2,5/2-) | 1729 1876 | 67 100 | 1661.40 1514.54 | 3/2- 5/2- | ||
3388.5 9 | GH J | 5/2,7/2 | < 33.3 ps | 602.3 10 1745 2 ? 2233.7 20 2638.9 20 3296 2 ? | 30 7 11.1 24 39 4 100 4 29 13 | D,E2 D,Q D,Q D,Q | 2786.4 1643.19 1155.32 748.27 90.6392 | (9/2)- (3/2-,5/2) 9/2- 3/2+ 5/2- |
3405 | DE IJ | (3/2)- | ||||||
3462.9 17 | DE GH | (3/2+ TO 9/2+) | < 33.3 ps | 1862.0 15 ? 3462.8 17 | | 1602.68 0.0 | 7/2+ 7/2- | |
3479 3 ? | I | (7/2-) | ||||||
3500.6 10 | G J | < 33.3 ps | 1092.2 10 3500.9 20 | 82 15 100 8 | D,E2 | 2408.3 0.0 | (7/2-) 7/2- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3516 2 | D | (3/2- TO 9/2) | ||||||
3521 2 | D | (LE 9/2) | ||||||
3531 2 ? | D IJ | (LE 7/2-) | 1870? 1887? 3378? | 25 42 100 | 1661.40 1643.19 152.9282 | 3/2- (3/2-,5/2) 3/2- | ||
3531.1 6 | G IJ | 5/2-,7/2,9/2+ | < 33.3 ps | 1178.4 10 1348.4 10 2015.6 20 2375.7 20 3378.5 20 3531.0 20 | 74 3 41 3 38 3 15 3 100 3 26 3 | D,E2 D,E2 D,Q D,Q,E3 | 2353.4 2182.0 1514.54 1155.32 152.9282 0.0 | 9/2- 7/2- 5/2- 9/2- 3/2- 7/2- |
3603 2 | D | |||||||
3609 3 | I | (7/2-) | ||||||
3612 6 ? | IJ | (GE 11/2-) | ||||||
3623.9 20 | G I | LE 9/2 | < 33.3 ps | 2483.3 20 | 100 | D,Q | 1140.53 | 5/2+ |
3639.8 8 | D G IJ | (7/2-) | < 33.3 ps | 1461.5 10 2123.8 20 2618.1 20 3640.8 20 | 13 4 50 6 100 6 22.2 19 | D,Q D,Q D,Q | 2178.3 1514.54 1021.62 0.0 | 9/2+ 5/2- 11/2- 7/2- |
3665.9 7 | G | 11/2 | < 33.3 ps | 1312.1 10 1402.7 10 3666.7 20 | 35 3 17 3 100 3 | D,E2 D,Q D,Q,E3 | 2353.4 2263.30 0.0 | 9/2- 15/2- 7/2- |
3671 2 | D J | (1/2+ TO 9/2+) | ||||||
3678 2 | DE IJ | (7/2)- | ||||||
3694 6 | E H J | 3/2+,5/2+ | ||||||
3721 2 | D I | (LE 7/2)- | ||||||
3741 2 | DE | 1/2-,3/2- | 2230 3591 3653 | 67 100 100 | 1514.54 152.9282 90.6392 | 5/2- 3/2- 5/2- | ||
3742.4 6 | B IJ | (19/2-) | 416.9 5 1479.1 9 | 100 93 | D+Q D,Q | 3325.2 2263.30 | (17/2-) 15/2- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3757 2 | DE H | 5/2-,7/2- | ||||||
3771 2 | D | (1/2+ TO 9/2+) | ||||||
3782 2 | D | (GE 9/2) | ||||||
3795 3 | I | (-) | ||||||
3816 2 | D | (LE 7/2-) | 3725 | 100 | 90.6392 | 5/2- | ||
3825 3 | I | (-) | ||||||
3841 2 | D J | 1/2(+),3/2,5/2- | 2180 2197 | 100 67 | 1661.40 1643.19 | 3/2- (3/2-,5/2) | ||
3885.2 27 | IJ | |||||||
3912 2 | DE HI | (3/2)- | 1650 2270 3761 | 50 83 100 | D(+Q) | 2265.3 1643.19 152.9282 | 5/2- (3/2-,5/2) 3/2- | |
3927 2 | D H J | (1/2+ TO 9/2+) | ||||||
3960 2 | D J | (3/2-,5/2,7/2-) | ||||||
3975 3 | HIJ | (-) | ||||||
4002 2 | DE H J | (3/2)- | 1693 2358 | 67 100 | 2309.4 1643.19 | 3/2- (3/2-,5/2) | ||
4035 2 | D | (3/2- TO 9/2+) | ||||||
4048 3 | HI | |||||||
4064 6 | J | |||||||
4088 2 | D H | 3/2(-),5/2,7/2- | 1855 2576 3937 4090 | 33 100 83 67 | 2234.0 1514.54 152.9282 0.0 | 5/2 5/2- 3/2- 7/2- | ||
4098 2 | D I | (LE 7/2-) | ||||||
4129 2 | DE | (5/2)- | 3380 | 100 | 748.27 | 3/2+ | ||
4152 2 | D H J | |||||||
4165 3 ? | I | |||||||
4218 2 | DE I | (3/2)- | ||||||
4253 2 | DE IJ | 1/2-,3/2- | 2589 2606 | 100 100 | 1661.40 1646.43 | 3/2- (1/2+) | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4259 2 | D I | (3/2,5/2,7/2) | ||||||
4270 2 | D I | |||||||
4289 2 | D HI | 3/2+,5/2+ | ||||||
4316 11 | IJ | |||||||
4359 2 | D | |||||||
4373 2 | DE J | 1/2-,3/2- | 2064 2138 2712 | 60 60 100 | 2309.4 2234.0 1661.40 | 3/2- 5/2 3/2- | ||
4397 2 | D H J | 5/2-,7/2- | ||||||
4422 2 | D | |||||||
4436 6 | E J | |||||||
4470 6 | J | |||||||
4498 2 | D J | 5/2(-),7/2(-) | 3343 4345 | 43 100 | 1155.32 152.9282 | 9/2- 3/2- | ||
4502 | E H J | 1/2-,3/2- | ||||||
4540 2 | D H J | |||||||
4590 2 | DE J | 2355 | 100 | 2234.0 | 5/2 | |||
4599 | E | |||||||
4635 2 | DE H J | (5/2)- | 4548 4639 | 100 60 | 90.6392 0.0 | 5/2- 7/2- | ||
4662 6 | H J | 3/2+,5/2+ | ||||||
4740 2 | D H J | 3/2+,5/2+ | ||||||
4796 6 | J | (GE 11/2) | ||||||
4840 2 | DE H J | 1/2-,3/2- | ||||||
4863 6 | H J | |||||||
4885 6 | E J | |||||||
4947 2 | DE J | 1/2-,3/2- | 4853 | 100 | 90.6392 | 5/2- | ||
4959 | H J | 1/2+ | ||||||
4988 6 | J | |||||||
5010 6 | E H J | 5/2-,7/2- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5042 2 | D | |||||||
5057 | E | 1/2-,3/2- | ||||||
5072 | H | 3/2+,5/2+ | ||||||
5134 6 | E H J | |||||||
5212 2 | DE J | 1/2-,3/2- | 2903 | 100 | 2309.4 | 3/2- | ||
5230 2 | D H | |||||||
5257 | E | 1/2-,3/2- | ||||||
5292 6 | H J | 1/2+ | ||||||
5347 6 | H J | (3/2+,5/2+) | ||||||
5387 6 | E H J | 1/2-,3/2- | ||||||
5411 6 | E J | 5/2-,7/2- | ||||||
5522 | H | 1/2+ | ||||||
5529.7 7 | B | (21/2-) | 1787 1 2204 1 | 100 43 | D | 3742.4 3325.2 | (19/2-) (17/2-) | |
5554 | H | |||||||
5597 | E H | 1/2-,3/2- | ||||||
5631? | H | (3/2+,5/2+) | ||||||
5676 | E | 1/2-,3/2- | ||||||
5689.9 8 | B | (23/2-) | 160 1 1947 1 | 2.7 100 | D,Q | 5529.7 3742.4 | (21/2-) (19/2-) | |
5718 | E | 1/2-,3/2- | ||||||
5826 | E | 5/2-,7/2- | ||||||
5889 | E H | 1/2-,3/2- | ||||||
5931? | H | (3/2+,5/2+) | ||||||
5947 | E | 5/2-,7/2- | ||||||
5987 | E H | 1/2-,3/2- | ||||||
6045 | E | 1/2-,3/2- | ||||||
6058? | H | (3/2+,5/2+) | ||||||
6146 | E | 1/2-,3/2- | ||||||
6184 | E H | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
6220 | E H | 1/2-,3/2- | ||||||
6258 | E | |||||||
6286? | H | |||||||
6333 | E H | 1/2-,3/2- | ||||||
6368 | E H | |||||||
6392 | E H | |||||||
6430 | E H J | |||||||
6474 | E H J | |||||||
6521 | E H | |||||||
6555 | E | 1/2-,3/2- | ||||||
6563? | H | (3/2+,5/2+) | ||||||
6603 | E | 1/2-,3/2- | ||||||
6661 30 | E | |||||||
6683 30 | E | |||||||
6711 30 | E | |||||||
6816 30 | E | |||||||
6844.9 8 | B | (23/2-) | 1155 1 1315 1 3102 1 | 100 6.2 12.5 | D | 5689.9 5529.7 3742.4 | (23/2-) (21/2-) (19/2-) | |
6856 30 | E | |||||||
6892 30 | E | |||||||
6943 30 | E | |||||||
6978 30 | E | |||||||
7054 30 | E | |||||||
7099 30 | E | |||||||
7137 30 | E | |||||||
7240 30 | E | |||||||
7290 30 | E | |||||||
7365 30 | E | |||||||
7430 30 | E | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7478 30 | E | |||||||
7554 30 | E | |||||||
7605 30 | E | |||||||
7645 30 | E | |||||||
7745.0 | DE | 3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 3111 3249? 3620 3658 3741 3830 3931? 3999 4355 5363 5443 5486 5516 6089 6104 6995? 7592 7654 7745 | 22.2 5.6 27.8 94.4 11.1 55.6 5.6 50 11.1 5.6 16.7 5.6 11.1 27.8 38.9 5.6 100 72.2 5.6 | D,E2 D,E2 D,E2 D(+Q) D,E2 D(+Q) D,E2 D(+Q) D,E2 (E1(+M2)) D+Q D,E2 D+Q D+Q D+Q (E1(+M2)) (M1+E2) (M1(+E2)) E2+M3 | 4635 4498 4129 4088 4002 3912 3816 3741 3388 2388.0 2309.4 2265.3 2234.0 1661.40 1643.19 748.27 152.9282 90.6392 0.0 | (5/2)- 5/2(-),7/2(-) (5/2)- 3/2(-),5/2,7/2- (3/2)- (3/2)- (LE 7/2-) 1/2-,3/2- (3/2,5/2-) 5/2+ 3/2- 5/2- 5/2 3/2- (3/2-,5/2) 3/2+ 3/2- 5/2- 7/2- |
7750 | DE | 3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 3116 3627 3664 3746 3836 3993 4005 4343 4360 5448 5491 6095 6111 6235 6611 7001 7596 7660 7752 | 6.7 6.7 30 33.3 23.3 6.7 30 10 6.7 16.7 3.3 10 36.7 3.3 3.3 3.3 3.3 100 3.3 | D,E2 D,E2 D(+Q) (M1(+E2)) (M1(+E2)) D,E2 (M1(+E2)) D,E2 D,E2 (M1+E2) D,E2 D+Q (E1(+M2)) D+Q (E1) (E1(+M2)) D+Q (M1+E2) E2(+M3) | 4635 4129 4088 4002 3912 3757 3741 3405 3388 2309.4 2265.3 1661.40 1646.43 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (5/2)- (5/2)- 3/2(-),5/2,7/2- (3/2)- (3/2)- 5/2-,7/2- 1/2-,3/2- (3/2)- (3/2,5/2-) 3/2- 5/2- 3/2- (1/2+) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7801.4 8 | B | (25/2-) | 956 1 2111 1 2271 1 | 88.9 100 8.9 | D D | 6844.9 5689.9 5529.7 | (23/2-) (23/2-) (21/2-) | |
7838.7 21 | DE | (1/2-) | 4098 4451 5574 6177 6196 7090 7685 | 9 21 12 47 100 26 19 | 3741 3388 2265.3 1661.40 1643.19 748.27 152.9282 | 1/2-,3/2- (3/2,5/2-) 5/2- 3/2- (3/2-,5/2) 3/2+ 3/2- | ||
7910.2 21 | DE | (1/2-) | 4522 5600 5645 5915 6248 6264 7161 7756 | 29 62 25 46 62 29 62 100 | 3388 2309.4 2265.3 1994.7 1661.40 1646.43 748.27 152.9282 | (3/2,5/2-) 3/2- 5/2- 3/2(+) 3/2- (1/2+) 3/2+ 3/2- | ||
7943.5 21 | DE | (3/2-) | 3690 3725 4031 4127 4265 4412 4555 5132 5633 5678 5708 5948 6281 6802 7194 7789 7851 7942 | 6 6 6 6 28 6 17 17 50 100 11 28 83 22 11 72 78 11 | 4253 4218 3912 3816 3678 3531 3388 2810.9 2309.4 2265.3 2234.0 1994.7 1661.40 1140.53 748.27 152.9282 90.6392 0.0 | 1/2-,3/2- (3/2)- (3/2)- (LE 7/2-) (7/2)- (LE 7/2-) (3/2,5/2-) 5/2-,7/2- 3/2- 5/2- 5/2 3/2(+) 3/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8013.0 21 | DE | (3/2-) | 4789 5703 6351 6872 7264 7859 7921 8012 | 2 6 6 5 100 15 5 23 | 3224 2309.4 1661.40 1140.53 748.27 152.9282 90.6392 0.0 | (1/2,3/2,5/2-) 3/2- 3/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8058.1 21 | DE | (3/2,5/2+) | 4317 4670 4799 4816 4834 5670 5748 5793 5823 6063 6412 6543 6917 7309 7904 7966 | 35 9 4 13 4 9 17 17 43 9 26 57 43 30 100 17 | 3741 3388 3259.5 3242 3224 2388.0 2309.4 2265.3 2234.0 1994.7 1646.43 1514.54 1140.53 748.27 152.9282 90.6392 | 1/2-,3/2- (3/2,5/2-) (GE 9/2) (3/2,5/2,7/2-) (1/2,3/2,5/2-) 5/2+ 3/2- 5/2- 5/2 3/2(+) (1/2+) 5/2- 5/2+ 3/2+ 3/2- 5/2- | ||
8071.8 21 | DE | (5/2) | 5806 6428 7322 7917 7979 8070 | 22 37 5 100 32 49 | 2265.3 1643.19 748.27 152.9282 90.6392 0.0 | 5/2- (3/2-,5/2) 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8092.6 | DE | (1/2-) | 53 eV 15 % IT = 4.8 19 % p = 95.2 19 | 3456 3718 4089 4179 4249 4349 4851 4866 6429 6447 7341 7936 7999 | 3.1 7.8 4.7 4.7 6.2 6.2 1.6 6.2 1.6 9.4 1.6 100 1.6 | (E2(+M3)) D,E2 D,E2 D,E2 D,E2 D,E2 D,E2 D,E2 D,E2 (E1) (E1) D,E2 (E2+(M3)) | 4635 4373 4002 3912 3841 3741 3242 3224 1661.40 1646.43 748.27 152.9282 90.6392 | (5/2)- 1/2-,3/2- (3/2)- (3/2)- 1/2(+),3/2,5/2- 1/2-,3/2- (3/2,5/2,7/2-) (1/2,3/2,5/2-) 3/2- (1/2+) 3/2+ 3/2- 5/2- |
8104.2 | D | 3/2(-),5/2 | 4263 4716 4880 5716 5796 6443 6460 6589 6963 7355 7950 8012 8103? | 24 12 16 16 28 28 100 76 16 36 16 8 4 | 3841 3388 3224 2388.0 2309.4 1661.40 1643.19 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | 1/2(+),3/2,5/2- (3/2,5/2-) (1/2,3/2,5/2-) 5/2+ 3/2- 3/2- (3/2-,5/2) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8117.5 | D | 3/2 | 3743 4114 4728 4892 5730 5808 5853 5884 6121 6456 6473 6601 6978 7370 7966 8027 8118 | 13.6 18.2 22.7 13.6 13.6 13.6 13.6 13.6 59.1 22.7 31.8 9.1 45.4 36.4 100 18.2 9.1 | D,E2 D,E2 D,E2 D,E2 D,E2 D,E2 D,E2 D,E2 D+Q D+Q D+Q D,E2 D+Q D+Q D+Q D(+Q) Q+O | 4373 4002 3388 3224 2388.0 2309.4 2265.3 2234.0 1994.7 1661.40 1643.19 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | 1/2-,3/2- (3/2)- (3/2,5/2-) (1/2,3/2,5/2-) 5/2+ 3/2- 5/2- 5/2 3/2(+) 3/2- (3/2-,5/2) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8131.5 21 | D | (3/2-) | 4528 4600 4743 4889 5743 6136 6469 6488 6616 6990 7382 7977 8039 8130 | 8.4 12 8.4 2.4 11 14 20 29 24 100 14 20 6.0 2.4 | 3603 3531 3388 3242 2388.0 1994.7 1661.40 1643.19 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (LE 7/2-) (3/2,5/2-) (3/2,5/2,7/2-) 5/2+ 3/2(+) 3/2- (3/2-,5/2) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8192 30 | E | |||||||
8246 30 | E | |||||||
8290.3 | DE | 3/2(-) | 4287 4548 5980 6295 6627 6645 6773 7148 7540 8137 8197 8288 | 5.1 5.1 12.8 5.1 5.1 20.5 2.6 51.3 100 18 7.7 10.3 | D+Q D+Q D+Q D+Q D+Q D+Q Q+O | 4002 3741 2309.4 1994.7 1661.40 1646.43 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2)- 1/2-,3/2- 3/2- 3/2(+) 3/2- (1/2+) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | |
8371 30 | E | |||||||
8405 30 | E | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8416.1 9 | B | (27/2-) | 613 1 5690 1 | 100 45 | D (Q) | 7801.4 2727.5 | (25/2-) 15/2- | |
8444 30 | E | |||||||
8525.3 21 | DE | (5/2) | 4566 4923 6118 6531 6863 6922 7010 7385 7777 8372 8434 8525 | 14 14 3 5 57 3 5 24 19 24 100 3 | 3960 3603 2408.3 1994.7 1661.40 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2-,5/2,7/2-) (7/2-) 3/2(+) 3/2- 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8628.2 21 | DE | (3/2-) | 5817 6363 6633 6965 6981 7487 7879 8474 8536 8627 | 26 15 37 22 48 100 100 15 4 4 | 2810.9 2265.3 1994.7 1661.40 1646.43 1140.53 748.27 152.9282 90.6392 0.0 | 5/2-,7/2- 5/2- 3/2(+) 3/2- (1/2+) 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8633.1 21 | DE | (5/2) | 4504 4673 5117 5245 6245 6323 6398 6450 6638 6970 6989 7029 7117 7492 7884 8479 8541 8632 | 17 12 8 8 8 29 12 17 12 12 17 12 42 38 29 100 38 4 | 4129 3960 3516 3388 2388.0 2309.4 2234.0 2182.0 1994.7 1661.40 1643.19 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (5/2)- (3/2-,5/2,7/2-) (3/2- TO 9/2) (3/2,5/2-) 5/2+ 3/2- 5/2 7/2- 3/2(+) 3/2- (3/2-,5/2) 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8640.9 21 | DE | (3/2-) | 4422 4639 4680 4728 4799 4899 4919 5002 5401 5623 5834 6330 6996 7124 7891 8486 8548 8639 | 3 3 3 6 3 3 9 3 6 3 3 3 17 11 66 100 43 3 | 4218 4002 3960 3912 3841 3741 3721 3639.8 3239.5 3017.3 2808.3 2309.4 1643.19 1514.54 748.27 152.9282 90.6392 0.0 | (3/2)- (3/2)- (3/2-,5/2,7/2-) (3/2)- 1/2(+),3/2,5/2- 1/2-,3/2- (LE 7/2)- (7/2-) 7/2- 5/2+ 3/2- (3/2-,5/2) 5/2- 3/2+ 3/2- 5/2- 7/2- | ||
8642.9 21 | DE | (3/2-,5/2) | 4383 4389 4640 4682 5254 5317 5400 5508 5625 5831 6254 6332 6377 6407 6647 6979 6995 7126 7501 7893 8488 8550 8641 | 6 6 11 6 6 6 6 6 22 6 6 6 6 17 17 56 39 17 50 100 44 100 11 | 4259 4253 4002 3960 3388 3325 3242 3134.0 3017.3 2810.9 2388.0 2309.4 2265.3 2234.0 1994.7 1661.40 1646.43 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2,5/2,7/2) 1/2-,3/2- (3/2)- (3/2-,5/2,7/2-) (3/2,5/2-) (1/2+ TO 7/2+) (3/2,5/2,7/2-) 7/2,9/2(+) 5/2-,7/2- 5/2+ 3/2- 5/2- 5/2 3/2(+) 3/2- (1/2+) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8682.0 21 | DE | (5/2) | 5011 5044 5357 5458 6274 6294 6417 6447 6687 7019 7035 7166 7541 7933 8528 8590 8681 | 2 2 5 2 2 2 5 2 5 9 7 11 2 9 100 7 50 | 3671 3639.8 3325 3224 2408.3 2388.0 2265.3 2234.0 1994.7 1661.40 1646.43 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (1/2+ TO 9/2+) (7/2-) (1/2+ TO 7/2+) (1/2,3/2,5/2-) (7/2-) 5/2+ 5/2- 5/2 3/2(+) 3/2- (1/2+) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8784.9 21 | D | (5/2) | 6377 6397 6789 7122 7269 7644 8036 8631 8693 8784 | 6 6 16 29 16 16 26 19 71 100 | 2408.3 2388.0 1994.7 1661.40 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (7/2-) 5/2+ 3/2(+) 3/2- 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8788.8 21 | D | (5/2-) | 5401 5547 5565 5772 6109 6381 6401 6479 6606 7185 7273 7633 7648 8040 8635 8697 8788 | 8 3 5 8 5 5 5 5 5 3 5 11 5 16 100 38 32 | 3388 3242 3224 3017.3 2680.0 2408.3 2388.0 2309.4 2182.0 1602.68 1514.54 1155.32 1140.53 748.27 152.9282 90.6392 0.0 | (3/2,5/2-) (3/2,5/2,7/2-) (1/2,3/2,5/2-) (7/2,9/2) (7/2-) 5/2+ 3/2- 7/2- 7/2+ 5/2- 9/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8851.5 21 | DE | (5/2-,7/2-) | 4723 4940 5464 5628 5835 6046 6444 6464 6617 7248 7336 7696 7711 8698 8760 8851 | 6 6 16 6 9 12 6 25 25 3 9 3 41 100 3 22 | 4129 3912 3388 3224 3017.3 2808.3 2408.3 2388.0 2234.0 1602.68 1514.54 1155.32 1140.53 152.9282 90.6392 0.0 | (5/2)- (3/2)- (3/2,5/2-) (1/2,3/2,5/2-) 5/2+ (7/2-) 5/2+ 5/2 7/2+ 5/2- 9/2- 5/2+ 3/2- 5/2- 7/2- | ||
8867.2 21 | DE | (5/2) | 4955 5026 5126 5229 5403 5479 5625 5733 5850 6459 6479 6557 6602 6632 6871 7204 7263 7351 7726 8118 8713 8775 8866 | 9 9 9 4 4 4 4 13 4 4 4 22 9 9 4 48 4 17 35 52 100 22 35 | 3912 3841 3741 3639.8 3462.9 3388 3242 3134.0 3017.3 2408.3 2388.0 2309.4 2265.3 2234.0 1994.7 1661.40 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2)- 1/2(+),3/2,5/2- 1/2-,3/2- (7/2-) (3/2+ TO 9/2+) (3/2,5/2-) (3/2,5/2,7/2-) 7/2,9/2(+) (7/2-) 5/2+ 3/2- 5/2- 5/2 3/2(+) 3/2- 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8877.0 21 | DE | (5/2) | 5489 5552 5638 5653 5743 5860 6066 6489 6567 6642 7214 7361 7736 8128 8723 8785 8876 | 3 3 3 3 3 3 3 12 3 12 6 6 64 33 18 27 100 | 3388 3325 3239.5 3224 3134.0 3017.3 2810.9 2388.0 2309.4 2234.0 1661.40 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2,5/2-) (1/2+ TO 7/2+) 7/2- (1/2,3/2,5/2-) 7/2,9/2(+) 5/2-,7/2- 5/2+ 3/2- 5/2 3/2- 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8880.9 21 | DE | (5/2) | 4879 4969 5040 5065 5187 5417 5493 5864 6473 6571 6646 6698 6885 7234 7277 7365 7740 8789 8880 | 4 4 4 4 4 13 9 22 4 13 13 22 22 17 9 13 13 100 52 | 4002 3912 3841 3816 3694 3462.9 3388 3017.3 2408.3 2309.4 2234.0 2182.0 1994.7 1646.43 1602.68 1514.54 1140.53 90.6392 0.0 | (3/2)- (3/2)- 1/2(+),3/2,5/2- (LE 7/2-) 3/2+,5/2+ (3/2+ TO 9/2+) (3/2,5/2-) (7/2-) 3/2- 5/2 7/2- 3/2(+) (1/2+) 7/2+ 5/2- 5/2+ 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8890.7 21 | DE | (3/2-) | 4256 4518 4621 4638 4793 4931 5050 5075 5150 5197 5503 6581 6626 6656 6895 7228 7244 8142 8737 8799 8890 | 7 7 7 3 3 3 3 3 10 3 7 10 13 7 10 13 43 100 50 23 7 | 4635 4373 4270 4253 4098 3960 3841 3816 3741 3694 3388 2309.4 2265.3 2234.0 1994.7 1661.40 1646.43 748.27 152.9282 90.6392 0.0 | (5/2)- 1/2-,3/2- 1/2-,3/2- (LE 7/2-) (3/2-,5/2,7/2-) 1/2(+),3/2,5/2- (LE 7/2-) 1/2-,3/2- 3/2+,5/2+ (3/2,5/2-) 3/2- 5/2- 5/2 3/2(+) 3/2- (1/2+) 3/2+ 3/2- 5/2- 7/2- | ||
8893.6 21 | DE | (5/2-) | 4496 4634 4764 4981 5152 5255 6082 6087 6583 6628 6658 6710 6897 7230 7289 7377 7737 7752 8144 8739 8801 8892 | 3 3 3 6 3 3 3 3 6 9 18 6 9 12 9 9 3 18 12 21 38 100 | 4397 4259 4129 3912 3741 3639.8 2810.9 2808.3 2309.4 2265.3 2234.0 2182.0 1994.7 1661.40 1602.68 1514.54 1155.32 1140.53 748.27 152.9282 90.6392 0.0 | 5/2-,7/2- (3/2,5/2,7/2) (5/2)- (3/2)- 1/2-,3/2- (7/2-) 5/2-,7/2- 5/2+ 3/2- 5/2- 5/2 7/2- 3/2(+) 3/2- 7/2+ 5/2- 9/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8895.6 21 | DE | (5/2) | 4636 5507 5653 6630 6899 7232 7291 7379 7754 8146 8741 8803 8894 | 7 7 7 10 7 31 7 14 41 100 59 41 14 | 4259 3388 3242 2265.3 1994.7 1661.40 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2,5/2,7/2) (3/2,5/2-) (3/2,5/2,7/2-) 5/2- 3/2(+) 3/2- 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8902.5 21 | DE | (5/2) | 4614 5664 5886 6593 6668 6907 7256 7259 7387 7762 8154 8749 8811 8902 | 5 20 10 15 30 20 10 35 10 30 65 95 55 100 | 4289 3239.5 3017.3 2309.4 2234.0 1994.7 1646.43 1643.19 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | 3/2+,5/2+ 7/2- 3/2- 5/2 3/2(+) (1/2+) (3/2-,5/2) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8912.2 21 | DE | (5/2) | 4515 4783 5000 5218 5309 5524 5673 6101 6504 6602 6647 6677 6916 7249 7265 7396 7771 8163 8758 8820 8911 | 5 3 5 3 3 3 3 10 5 5 5 8 8 8 3 3 8 13 21 49 100 | 4397 4129 3912 3694 3603 3388 3239.5 2810.9 2408.3 2309.4 2265.3 2234.0 1994.7 1661.40 1646.43 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | 5/2-,7/2- (5/2)- (3/2)- 3/2+,5/2+ (3/2,5/2-) 7/2- 5/2-,7/2- (7/2-) 3/2- 5/2- 5/2 3/2(+) 3/2- (1/2+) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8921.1 21 | D | (5/2+) | 6612 6739 6743 6926 7275 7318 7406 7781 8173 8768 8831 8921 | 42 16 16 21 42 53 21 16 42 100 68 89 | 2309.4 2182.0 2178.3 1994.7 1646.43 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | 3/2- 7/2- 9/2+ 3/2(+) (1/2+) 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8925.0 21 | D | (7/2-) | 4290 4890 5143 5537 6690 7262 7321 7409 7784 8771 8833 8924 | 2 2 4 4 4 4 15 4 6 49 13 100 | 4635 4035 3782 3388 2234.0 1661.40 1602.68 1514.54 1140.53 152.9282 90.6392 0.0 | (5/2)- (3/2- TO 9/2+) (GE 9/2) (3/2,5/2-) 5/2 3/2- 7/2+ 5/2- 5/2+ 3/2- 5/2- 7/2- | ||
8927.9 21 | DE | (5/2) | 5540 5911 6618 6693 6932 7265 7281 7324 7412 7787 8179 8774 8836 8927 | 22 33 22 39 11 56 83 11 11 56 22 50 39 100 | 3388 3017.3 2309.4 2234.0 1994.7 1661.40 1646.43 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2,5/2-) 3/2- 5/2 3/2(+) 3/2- (1/2+) 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8942.6 21 | D | (5/2) | 5249 5926 6555 6633 6708 6947 7280 7296 7339 7427 7802 8194 8789 8851 8942 | 14 10 14 29 5 14 62 62 14 14 10 29 48 52 100 | 3694 3017.3 2388.0 2309.4 2234.0 1994.7 1661.40 1646.43 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | 3/2+,5/2+ 5/2+ 3/2- 5/2 3/2(+) 3/2- (1/2+) 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
8945 25 | J | (1/2+) | ||||||
8965.1 21 | D | (5/2+) | 4712 4747 4877 5005 5038 5053 5149 5224 5577 5741 5831 5948 6285 6557 6785 7449 7824 8216 8811 8873 8964 | 4 4 4 8 8 8 8 17 12 4 8 12 8 8 8 38 100 42 42 50 21 | 4253 4218 4088 3960 3927 3912 3816 3741 3388 3224 3134.0 3017.3 2680.0 2408.3 2178.3 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | 1/2-,3/2- (3/2)- 3/2(-),5/2,7/2- (3/2-,5/2,7/2-) (1/2+ TO 9/2+) (3/2)- (LE 7/2-) 1/2-,3/2- (3/2,5/2-) (1/2,3/2,5/2-) 7/2,9/2(+) (7/2,9/2) (7/2-) 9/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8998.5 21 | D | (1/2-) | 6733 7351 8249 8844 | 27 11 19 100 | 2265.3 1646.43 748.27 152.9282 | 5/2- (1/2+) 3/2+ 3/2- | ||
9008.2 21 | D | (5/2+) | 4920 5006 5096 5237 5267 5330 5337 5666 5991 6600 6620 6698 7012 7361 7404 7867 8259 8854 8916 9007 | 6 9 14 6 9 9 9 9 11 6 29 11 14 3 3 14 14 100 9 9 | 4088 4002 3912 3771 3741 3678 3671 3342 3017.3 2408.3 2388.0 2309.4 1994.7 1646.43 1602.68 1140.53 748.27 152.9282 90.6392 0.0 | 3/2(-),5/2,7/2- (3/2)- (3/2)- (1/2+ TO 9/2+) 1/2-,3/2- (7/2)- (1/2+ TO 9/2+) (1/2+ TO 9/2+) (7/2-) 5/2+ 3/2- 3/2(+) (1/2+) 7/2+ 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
9029.8 21 | D | (5/2) | 4490 5359 5427 5642 5791 5896 6013 6622 6642 6720 6794 7034 7367 7386 7426 7889 8281 8876 8938 9029 | 4 2 2 2 9 2 7 2 4 2 7 11 7 16 2 4 7 11 9 100 | 4540 3671 3603 3388 3239.5 3134.0 3017.3 2408.3 2388.0 2309.4 2234.0 1994.7 1661.40 1643.19 1602.68 1140.53 748.27 152.9282 90.6392 0.0 | (1/2+ TO 9/2+) (3/2,5/2-) 7/2- 7/2,9/2(+) (7/2-) 5/2+ 3/2- 5/2 3/2(+) 3/2- (3/2-,5/2) 7/2+ 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
9037.6 21 | D | (5/2) | 7897 8289 8884 8946 9037 | 96 22 93 100 59 | 1140.53 748.27 152.9282 90.6392 0.0 | 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
9044.5 21 | D | (7/2-) | 5084 5132 5528 5785 6373? 6373? 6734 6808 6860 7528 7903 8890 8952 9043 | 13 13 13 25 19 19 69 44 69 19 81 94 69 100 | 3960 3912 3516 3259.5 2671.3 2671.0 2309.4 2234.0 2182.0 1514.54 1140.53 152.9282 90.6392 0.0 | (3/2-,5/2,7/2-) (3/2)- (3/2- TO 9/2) (GE 9/2) 7/2-,9/2,11/2+ (11/2)- 3/2- 5/2 7/2- 5/2- 5/2+ 3/2- 5/2- 7/2- | ||
9056.2 21 | D | (5/2) | 6747 7061 7394 7541 7916 8308 8903 8965 9056 | 23 20 10 10 7 27 100 53 83 | 2309.4 1994.7 1661.40 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | 3/2- 3/2(+) 3/2- 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
9071.9 21 | D | (5/2) | 5551 5684 6055 6261 6684 6761 6836 6888 7076 7409 7425 7468 7556 7931 8323 8918 8980 9071 | 14 5 10 5 10 48 5 10 19 24 29 10 10 19 24 81 100 57 | 3516 3388 3017.3 2810.9 2388.0 2309.4 2234.0 2182.0 1994.7 1661.40 1646.43 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2- TO 9/2) (3/2,5/2-) 5/2-,7/2- 5/2+ 3/2- 5/2 7/2- 3/2(+) 3/2- (1/2+) 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
9075.8 21 | D | (5/2) | 5116 5164 5355 5382 5751 6059 6668 6765 6892 7080 7413 7432 7472 7560 7935 8327 8922 8984 9075 | 5 11 5 5 11 16 11 32 11 32 32 32 26 37 37 11 53 63 100 | 3960 3912 3721 3694 3325 3017.3 2408.3 2309.4 2182.0 1994.7 1661.40 1643.19 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2-,5/2,7/2-) (3/2)- (LE 7/2)- 3/2+,5/2+ (1/2+ TO 7/2+) (7/2-) 3/2- 7/2- 3/2(+) 3/2- (3/2-,5/2) 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
9078.8 21 | D | (3/2-) | 6062 6691 7416 7435 7563 8330 8925 8987 9078 | 5 10 7 7 10 100 16 9 9 | 3017.3 2388.0 1661.40 1643.19 1514.54 748.27 152.9282 90.6392 0.0 | 5/2+ 3/2- (3/2-,5/2) 5/2- 3/2+ 3/2- 5/2- 7/2- | ||
9082.7 21 | D J | (3/2+) | 7420 7439 7942 8334 8929 8993 | 27 43 57 53 13 100 | 1661.40 1643.19 1140.53 748.27 152.9282 90.6392 | 3/2- (3/2-,5/2) 5/2+ 3/2+ 3/2- 5/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
9089.5 21 | D | (3/2-,5/2) | 6702 7443 8341 8936 8998 9089 | 7 3 10 100 33 5 | 2388.0 1646.43 748.27 152.9282 90.6392 0.0 | 5/2+ (1/2+) 3/2+ 3/2- 5/2- 7/2- | ||
9094.4 21 | D | (5/2) | 5183 5354 5401 6078 6784 6859 7448 7579 7954 8346 8941 9003 9094 | 7 7 7 14 7 11 36 21 36 100 25 82 4 | 3912 3741 3694 3017.3 2309.4 2234.0 1643.19 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2)- 1/2-,3/2- 3/2+,5/2+ 3/2- 5/2 (3/2-,5/2) 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
9118.0 21 | D | (5/2) | 5730 6101 6312 6807 6882 7122 7514 7602 7977 8369 8964 9026 9117 | 5 33 24 10 52 48 14 100 29 24 29 81 29 | 3388 3017.3 2808.3 2309.4 2234.0 1994.7 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (3/2,5/2-) 5/2+ 3/2- 5/2 3/2(+) 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
9131.7 21 | D | (5/2) | 6821 6866 7469 7485 7528 8383 8978 9040 9131 | 9 13 9 24 17 11 100 24 11 | 2309.4 2265.3 1661.40 1646.43 1602.68 748.27 152.9282 90.6392 0.0 | 3/2- 5/2- 3/2- (1/2+) 7/2+ 3/2+ 3/2- 5/2- 7/2- | ||
9135.6 21 | D | (5/2) | 7472 7488 8386 8981 9043 9134 | 38 21 28 100 21 49 | 1661.40 1646.43 748.27 152.9282 90.6392 0.0 | 3/2- (1/2+) 3/2+ 3/2- 5/2- 7/2- | ||
9148.3 21 | D | (5/2) | 5618 6760 6965 7153 7545 7633 8400 8995 9057 9148 | 25 35 35 65 60 50 100 45 65 20 | 3531 2388.0 2182.0 1994.7 1602.68 1514.54 748.27 152.9282 90.6392 0.0 | (LE 7/2-) 5/2+ 7/2- 3/2(+) 7/2+ 5/2- 3/2+ 3/2- 5/2- 7/2- | ||
9154.2 21 | D | (5/2+) | 5915 5930 6348 6843 6888 6974 7491 7507 7638 8405 9000 9062 9153 | 9 5 14 59 23 14 36 23 59 100 50 41 23 | 3239.5 3224 2808.3 2309.4 2265.3 2178.3 1661.40 1646.43 1514.54 748.27 152.9282 90.6392 0.0 | 7/2- (1/2,3/2,5/2-) 5/2+ 3/2- 5/2- 9/2+ 3/2- (1/2+) 5/2- 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
9161.1 21 | D | (1/2-,3/2) | 5937 6895 6925 7517 8412 9007 9069 | 5 7 16 19 9 100 19 | 3224 2265.3 2234.0 1643.19 748.27 152.9282 90.6392 | (1/2,3/2,5/2-) 5/2- 5/2 (3/2-,5/2) 3/2+ 3/2- 5/2- | ||
9167.9 21 | D | (5/2) | 4533 4746 4809 5133 5208 5427 5474 5490 5565 5780 5926 6151 6362 6759 6779 6857 6902 6932 7172 7505 7524 7564 7652 8027 8419 9014 9076 9167 | 8 8 15 8 15 8 8 8 8 15 15 15 23 15 15 62 15 8 8 69 62 54 46 31 23 77 31 100 | 4635 4422 4359 4035 3960 3741 3694 3678 3603 3388 3242 3017.3 2808.3 2408.3 2388.0 2309.4 2265.3 2234.0 1994.7 1661.40 1643.19 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (5/2)- (3/2- TO 9/2+) (3/2-,5/2,7/2-) 1/2-,3/2- 3/2+,5/2+ (7/2)- (3/2,5/2-) (3/2,5/2,7/2-) 5/2+ (7/2-) 5/2+ 3/2- 5/2- 5/2 3/2(+) 3/2- (3/2-,5/2) 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
9168.9 21 | D | (3/2-) | 5428 5781 5945 6858 7173 7506 7525 7565 7653 9015 9077 9168 | 2 2 3 5 7 5 12 3 3 100 3 7 | 3741 3388 3224 2309.4 1994.7 1661.40 1643.19 1602.68 1514.54 152.9282 90.6392 0.0 | 1/2-,3/2- (3/2,5/2-) (1/2,3/2,5/2-) 3/2- 3/2(+) 3/2- (3/2-,5/2) 7/2+ 5/2- 3/2- 5/2- 7/2- | ||
9174.8 21 | D | (5/2) | 6157 6863 7511 7570 8033 8425 9020 9082 9173 | 14 9 23 11 23 40 49 17 100 | 3017.3 2309.4 1661.40 1602.68 1140.53 748.27 152.9282 90.6392 0.0 | 3/2- 3/2- 7/2+ 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
9182.6 21 | D | (5/2) | 7667 8042 8434 9091 9182 | 7 100 74 47 5 | 1514.54 1140.53 748.27 90.6392 0.0 | 5/2- 5/2+ 3/2+ 5/2- 7/2- | ||
9193.4 21 | D | (5/2,7/2+) | 7197 7546 8444 9101 9192 | 100 42 100 92 83 | 1994.7 1646.43 748.27 90.6392 0.0 | 3/2(+) (1/2+) 3/2+ 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
9195.3 21 | D | (5/2) | 5674 6178 6786 6806 6884 7532 7591 7679 8054 8446 9041 9103 9194 | 14 14 14 14 14 38 19 38 76 90 19 24 100 | 3521 3017.3 2408.3 2388.0 2309.4 1661.40 1602.68 1514.54 1140.53 748.27 152.9282 90.6392 0.0 | (LE 9/2) (7/2-) 5/2+ 3/2- 3/2- 7/2+ 5/2- 5/2+ 3/2+ 3/2- 5/2- 7/2- | ||
9568 10 | E | (1/2-) | ||||||
9662 10 | E | 3/2- | ||||||
10230 10 | E | (5/2)- | ||||||
10925 7 | E | (5/2)+ | ||||||
11150 7 | E | (9/2+) |
E(level): From a least-squares fit to Eγ except as noted in the XREF column, comments, or footnotes. Resonance E(level)=(0.97955873 4)E(p)+S(p) with S(p)=6758.2 8 (2003Au03)
Jπ(level): From angular momentum transfer in (3He,d), except as noted
T1/2(level): From (α,pγ), except as noted; see discussion of discrepancies there and in (p,nγ). Γ’s from Γp and Γγ in (p,γ)
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - 7/2- GS yrast band | |||||||
0.0 | 7/2- | 330 d 15 % ε = 100 | |||||
90.6392 17 | 5/2- | 228 ps 13 | 90.639 2 | 100 | M1 | 0.0 | 7/2- |
1021.62 11 | 11/2- | 3.4 ps 6 | 1021.63 14 | 100 | E2 | 0.0 | 7/2- |
1155.32 10 | 9/2- | 1.1 ps 3 | 133.80 17 1064.63 17 1155.33 17 | 3.9 8 30.0 6 100.0 10 | (M1(+E2)) E2 M1+E2 | 1021.62 90.6392 0.0 | 11/2- 5/2- 7/2- |
2263.30 21 | 15/2- | 0.65 ps +38-19 | 1241.69 18 | 100 | E2 | 1021.62 | 11/2- |
2861.5 5 | 13/2- | 0.10 ps 6 | 134 1 ? 598.3 7 1706 1 1840 1 ? | 28.2 13 100 6 | (M1(+E2)) (M1(+E2)) E2(+M3) D,E2 | 2727.5 2263.30 1155.32 1021.62 | 15/2- 15/2- 9/2- 11/2- |
3325.2 4 | (17/2-) | 464 1 597.1 5 1061.9 5 | 36.84 21.05 100 | D,Q D D | 2861.5 2727.5 2263.30 | 13/2- 15/2- 15/2- | |
3742.4 6 | (19/2-) | ||||||
5529.7 7 | (21/2-) | 1787 1 2204 1 | 100 43 | D | 3742.4 3325.2 | (19/2-) (17/2-) | |
5689.9 8 | (23/2-) | 160 1 1947 1 | 2.7 100 | D,Q | 5529.7 3742.4 | (21/2-) (19/2-) | |
7801.4 8 | (25/2-) | ||||||
8416.1 9 | (27/2-) | 613 1 5690 1 | 100 45 | D (Q) | 7801.4 2727.5 | (25/2-) 15/2- | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - Kπ=3/2+ ROTATIONAL band | |||||||
748.27 9 | 3/2+ | 5.3 ps 6 | |||||
1140.53 11 | 5/2+ | 1.3 ps 6 | 392.7 6 987.61 26 1049.79 17 1140.7 3 | 10.5 10 31.4 17 44.5 21 100 4 | M1+E2 (E1(+M2)) E1+M2 E1(+M2) | 748.27 152.9282 90.6392 0.0 | 3/2+ 3/2- 5/2- 7/2- |
1602.68 12 | 7/2+ | 0.47 ps 22 | 447.4 3 462.2 2 854.5 3 1512.0 3 1602.6 2 | 1.6 8 13.5 17 15 4 100 8 49.3 20 | (E1) M1(+E2) (E2) (E1) (E1+M2) | 1155.32 1140.53 748.27 90.6392 0.0 | 9/2- 5/2+ 3/2+ 5/2- 7/2- |
2178.3 4 | 9/2+ | 0.56 ps +49-28 | 575.4 9 1023 1 ? 1037.4 5 1157.0 7 2178.3 8 | 11.3 17 33.9 17 16.1 17 100 5 | D(+Q) D,Q E2 D D(+Q) | 1602.68 1155.32 1140.53 1021.62 0.0 | 7/2+ 9/2- 5/2+ 11/2- 7/2- |
2741.0 5 | 11/2+ | 0.39 ps +36-17 | 562.5 7 1138.9 9 1585.8 9 1719.0 15 ? | 27.1 21 100 5 81 5 <10 | D,E2 (E2) (E1(+M2)) (E1(+M2)) | 2178.3 1602.68 1155.32 1021.62 | 9/2+ 7/2+ 9/2- 11/2- |
3341.8 7 | (13/2+) | 601.0 8 670.5 8 1163.0 10 | 72.5 25 78 5 100 5 | D,E2 D,E2 D,Q | 2741.0 2671.0 2178.3 | 11/2+ (11/2)- 9/2+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - Kπ=1/2+ ROTATIONAL BAND? | |||||||
1646.43 21 | (1/2+) | 6.6 ps 10 | |||||
1994.7 4 | 3/2(+) | 0.49 ps 21 | 854.5 4 1246.8 10 1841.0 8 1903.4 8 | 85 21 46 5 100 5 62 5 | (M1+E2) D,E2 (E1+M2) (E1(+M2)) | 1140.53 748.27 152.9282 90.6392 | 5/2+ 3/2+ 3/2- 5/2- |
2388.0 5 | 5/2+ | 57 fs 20 | 393.6 15 ? 1247.8 12 ? 1639.3 6 2235.5 16 ? 2298.6 15 2388.6 14 | 16.9 17 11.9 17 100 5 <8.5 28.8 17 11.9 17 | (M1(+E2)) D,E2 M1+E2 (E1(+M2)) (E1(+M2)) | 1994.7 1140.53 748.27 152.9282 90.6392 0.0 | 3/2(+) 5/2+ 3/2+ 3/2- 5/2- 7/2- |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - NEGATIVE-PARITY SIDE band | |||||||
2671.0 3 | (11/2)- | < 11 fs | |||||
2727.5 3 | 15/2- | 0.10 ps 4 | 464.2 3 1705.5 7 | 100 100 | M1(+E2) (E2) | 2263.30 1021.62 | 15/2- 11/2- |
2810.9 5 | 5/2-,7/2- | < 12 fs | 628.4 10 1673 2 ? 2720.3 19 2810.9 5 | 33 5 25 6 100 5 75 5 | M1 D,E2 D,E2 D,E2 | 2182.0 1140.53 90.6392 0.0 | 7/2- 5/2+ 5/2- 7/2- |
6844.9 8 | (23/2-) | 1155 1 1315 1 3102 1 | 100 6.2 12.5 | D | 5689.9 5529.7 3742.4 | (23/2-) (21/2-) (19/2-) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
90.6392 | 5/2- | 228 ps 13 | 90.639 2 | M1 | 0.0287 | B(M1)(W.u.)=0.126 8, α=0.0287, α(K)=0.0259 4, α(L)=0.00245 4, α(M)=0.000320 5, α(N)=1.629×10-5 23, α(N+)=1.629E-5 23 | |
152.9282 | 3/2- | 19.90 ns 24 | 62.289 2 | (M1) | 0.0787 | B(M1)(W.u.)=0.00176 8, α=0.0787, α(K)=0.0710 10, α(L)=0.00676 10, α(M)=0.000885 13, α(N)=4.47×10-5 7, α(N+)=4.47E-5 7 | |
3/2- | 19.90 ns 24 | 152.928 2 | E2 | 0.0725 | B(E2)(W.u.)=17.4 7, α=0.0725, α(K)=0.0654 10, α(L)=0.00623 9, α(M)=0.000808 12, α(N)=3.91E-5 6, α(N+)=3.91E-5 6 | ||
748.27 | 3/2+ | 5.3 ps 6 | 595.35 14 | (E1(+M2)) | -0.02 2 | 0.000184 | B(E1)(W.u.)=0.00024 3, B(M2)(W.u.)=1.3 +26-13, α=0.000184 3, α(K)=0.0001664 25, α(L)=1.514E-5 23, α(M)=1.98E-6 3, α(N)=1.030E-7 16, α(N+)=1.030E-7 16 |
3/2+ | 5.3 ps 6 | 657.60 14 | (E1(+M2)) | -0.01 2 | 0.0001450 | B(E1)(W.u.)=0.000154 18, B(M2)(W.u.)=0.16 +66-16, α=0.0001450 21, α(K)=0.0001317 19, α(L)=1.197E-5 18, α(M)=1.567E-6 23, α(N)=8.15E-8 12, α(N+)=8.15E-8 12 | |
1021.62 | 11/2- | 3.4 ps 6 | 1021.63 14 | E2 | 0.0001310 | B(E2)(W.u.)=14.0 25, α=0.0001310 19, α(K)=0.0001184 17, α(L)=1.079E-5 16, α(M)=1.413E-6 20, α(N)=7.35E-8 11, α(N+)=7.35E-8 11 | |
1140.53 | 5/2+ | 1.3 ps 6 | 392.7 6 | M1+E2 | 0.0015 | α=0.0015 8, α(K)=0.0013 7, α(L)=0.00012 6, α(M)=1.6×10-5 8, α(N)=8.E-7 4, α(N+)=8.E-7 4 | |
5/2+ | 1.3 ps 6 | 987.61 26 | (E1(+M2)) | -0.04 8 | 6.16×10-5 | B(E1)(W.u.)=7.E-5 4, B(M2)(W.u.)=0.5 +21-5, α=6.16E-5 25, α(K)=5.59E-5 22, α(L)=5.07E-6 21, α(M)=6.6E-7 3, α(N)=3.46E-8 14, α(N+)=3.46E-8 14 | |
5/2+ | 1.3 ps 6 | 1049.79 17 | E1+M2 | 0.00013 | B(E1)(W.u.)=8.E-5 4, α=0.00013 8, α(K)=0.00012 7, α(L)=1.1E-5 7, α(M)=1.4E-6 9, α(N)=7.E-8 5, α(N+)=7.E-8 5 | ||
5/2+ | 1.3 ps 6 | 1140.7 3 | E1(+M2) | -0.05 6 | 7.00×10-5 | B(E1)(W.u.)=0.00014 7, B(M2)(W.u.)=1.2 +30-12, α=7.00E-5 14, α(K)=4.27E-5 13, α(L)=3.87E-6 12, α(M)=5.07E-7 15, α(N)=2.65E-8 8, α(N+)=2.30E-5 4 | |
1155.32 | 9/2- | 1.1 ps 3 | 133.80 17 | (M1(+E2)) | -0.15 15 | 0.013 | B(E2)(W.u.)=7.×102 +15-7, B(M1)(W.u.)=0.24 9, α=0.013 7, α(K)=0.012 6, α(L)=0.0011 6, α(M)=0.00014 8, α(N)=7.E-6 4, α(N+)=7.E-6 4 |
9/2- | 1.1 ps 3 | 1064.63 17 | E2 | 0.0001180 | B(E2)(W.u.)=7.9 22, α=0.0001180 17, α(K)=0.0001073 15, α(L)=9.77E-6 14, α(M)=1.280E-6 18, α(N)=6.66E-8 10, α(N+)=6.66E-8 10 | ||
9/2- | 1.1 ps 3 | 1155.33 17 | M1+E2 | +0.70 7 | 8.89×10-5 | B(E2)(W.u.)=5.8 18, B(M1)(W.u.)=0.0065 19, α=8.89E-5 16, α(K)=7.78E-5 14, α(L)=7.07E-6 12, α(M)=9.26E-7 16, α(N)=4.84E-8 9, α(N+)=3.11E-6 8 | |
1514.54 | 5/2- | 31 fs 12 | 766 1 | (E1(+M2)) | 0.0045 LT | 0.00028 | B(E1)(W.u.)=0.006 3, α=0.00028 18, α(K)=0.00025 16, α(L)=2.3E-5 15, α(M)=3.0E-6 20, α(N)=1.6E-7 10, α(N+)=1.6E-7 10 |
5/2- | 31 fs 12 | 1361.61 7 | M1+E2 | -0.57 5 | 9.57×10-5 | B(E2)(W.u.)=42 18, B(M1)(W.u.)=0.10 4, α=9.57E-5 16, α(K)=5.53E-5 9, α(L)=5.02E-6 8, α(M)=6.58E-7 10, α(N)=3.44E-8 6, α(N+)=3.47E-5 7 | |
5/2- | 31 fs 12 | 1423.6 3 | (M1(+E2)) | -0.6 +6-21 | 1.06×10-4 | B(E2)(W.u.)=7 +12-7, B(M1)(W.u.)=0.017 12, α=1.06E-4 16, α(K)=5.1E-5 5, α(L)=4.6E-6 5, α(M)=6.1E-7 6, α(N)=3.2E-8 3, α(N+)=4.9E-5 11 | |
1602.68 | 7/2+ | 0.47 ps 22 | 447.4 3 | (E1) | 0.000376 | B(E1)(W.u.)=0.00011 8, α=0.000376 6, α(K)=0.000340 5, α(L)=3.10E-5 5, α(M)=4.05E-6 6, α(N)=2.10E-7 3, α(N+)=2.10E-7 3 | |
7/2+ | 0.47 ps 22 | 462.2 2 | M1(+E2) | -0.05 21 | 0.00053 | B(E2)(W.u.)=1.0 +85-10, B(M1)(W.u.)=0.036 18, α=0.00053 5, α(K)=0.00048 4, α(L)=4.4E-5 4, α(M)=5.8E-6 5, α(N)=3.01E-7 25, α(N+)=3.01E-7 25 | |
7/2+ | 0.47 ps 22 | 854.5 3 | (E2) | 0.000205 | B(E2)(W.u.)=21 12, α=0.000205 3, α(K)=0.000185 3, α(L)=1.692E-5 24, α(M)=2.22E-6 4, α(N)=1.149E-7 17, α(N+)=1.149E-7 17 | ||
7/2+ | 0.47 ps 22 | 1512.0 3 | (E1) | 0.000300 | B(E1)(W.u.)=0.00017 9, α=0.000300 5, α(K)=2.61E-5 4, α(L)=2.36E-6 4, α(M)=3.10E-7 5, α(N)=1.620E-8 23, α(N+)=0.000271 4 | ||
7/2+ | 0.47 ps 22 | 1602.6 2 | (E1+M2) | +0.29 11 | 3.50×10-4 | B(E1)(W.u.)=7.E-5 4, B(M2)(W.u.)=10 9, α=3.50E-4 16, α(K)=2.8E-5 3, α(L)=2.5E-6 3, α(M)=3.3E-7 4, α(N)=1.71E-8 19, α(N+)=0.000320 19 | |
1646.43 | (1/2+) | 6.6 ps 10 | 1493.6 3 | (E1(+M2)) | 0.204 LT | 0.00020 | B(E1)(W.u.)=1.2E-5 3, α=0.00020 9, α(K)=6.E-5 3, α(L)=5.E-6 3, α(M)=7.E-7 4, α(N)=3.5E-8 18, α(N+)=0.00014 12 |
1661.40 | 3/2- | 16 fs 7 | 912.3 10 | (E1(+M2)) | 0.0095 LT | 0.00018 | B(E1)(W.u.)=0.0021 10, α=0.00018 11, α(K)=0.00016 10, α(L)=1.5E-5 10, α(M)=2.0E-6 12, α(N)=1.0E-7 7, α(N+)=1.0E-7 7 |
3/2- | 16 fs 7 | 1570.83 17 | M1(+E2) | -0.04 9 | 1.33×10-4 | B(E2)(W.u.)=0.3 +13-3, B(M1)(W.u.)=0.18 8, α=1.33E-4 2, α(K)=4.11E-5 6, α(L)=3.72E-6 6, α(M)=4.88E-7 7, α(N)=2.56E-8 4, α(N+)=8.74E-5 13 | |
3/2- | 16 fs 7 | 1661.4 10 | (E2(+M3)) | 0.00041 LT | 0.00018 | B(E2)(W.u.)=24 11, α=0.00018 3, α(K)=8.E-5 4, α(L)=7.E-6 4, α(M)=9.E-7 5, α(N)=4.9E-8 23, α(N+)=9.E-5 7 | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
1994.7 | 3/2(+) | 0.49 ps 21 | 854.5 4 | (M1+E2) | -0.22 16 | 1.47×10-4 | B(E2)(W.u.)=3 +5-3, B(M1)(W.u.)=0.020 10, α=1.47E-4 6, α(K)=0.000133 5, α(L)=1.21E-5 5, α(M)=1.59E-6 6, α(N)=8.3E-8 3, α(N+)=8.3E-8 3 |
3/2(+) | 0.49 ps 21 | 1841.0 8 | (E1+M2) | -0.17 9 | 5.35×10-4 | B(E1)(W.u.)=5.5E-5 24, B(M2)(W.u.)=2.1 +24-2, α=5.35E-4 16, α(K)=2.02E-5 13, α(L)=1.83E-6 12, α(M)=2.39E-7 15, α(N)=1.25E-8 8, α(N+)=0.000512 17 | |
3/2(+) | 0.49 ps 21 | 1903.4 8 | (E1(+M2)) | 0.16 LT | 0.00038 | B(E1)(W.u.)=3.2E-5 14, α=0.00038 22, α(K)=3.4E-5 17, α(L)=3.1E-6 15, α(M)=4.1E-7 20, α(N)=2.1E-8 10, α(N+)=0.00034 24 | |
2178.3 | 9/2+ | 0.56 ps +49-28 | 575.4 9 | D(+Q) | -0.07 15 | ||
9/2+ | 0.56 ps +49-28 | 1037.4 5 | E2 | 0.0001260 | B(E2)(W.u.)=17 +9-15, α=0.0001260 18, α(K)=0.0001141 16, α(L)=1.040E-5 15, α(M)=1.361E-6 20, α(N)=7.08E-8 10, α(N+)=7.08E-8 10 | ||
9/2+ | 0.56 ps +49-28 | 2178.3 8 | D(+Q) | -0.02 5 | |||
2182.0 | 7/2- | 33 fs 12 | 1026.8 7 | (M1(+E2)) | 0.0084 LT | 1.00×10-4 | B(M1)(W.u.)=0.14 6, α=1.00×10-4 2, α(K)=9.09E-5 13, α(L)=8.26E-6 12, α(M)=1.083E-6 16, α(N)=5.66E-8 8, α(N+)=5.66E-8 8 |
7/2- | 33 fs 12 | 2090.7 7 | (M1+E2) | -0.09 4 | 0.000318 | B(E2)(W.u.)=0.23 23, B(M1)(W.u.)=0.052 20, α=0.000318 5, α(K)=2.50E-5 4, α(L)=2.26E-6 4, α(M)=2.97E-7 5, α(N)=1.556E-8 22, α(N+)=0.000290 5 | |
2234.0 | 5/2 | 12 fs 8 | 2142.9 10 | D(+Q) | +0.04 14 | ||
2263.30 | 15/2- | 0.65 ps +38-19 | 1241.69 18 | E2 | 9.96×10-5 | B(E2)(W.u.)=28 +8-17, α=9.96E-5 14, α(K)=7.55E-5 11, α(L)=6.86E-6 10, α(M)=8.99E-7 13, α(N)=4.69E-8 7, α(N+)=1.637E-5 24 | |
2309.4 | 3/2- | 14 fs 7 | 1560 | (E1(+M2)) | 0.028 LT | 0.00023 | B(E1)(W.u.)=0.0007 4, α=0.00023 11, α(K)=5.E-5 3, α(L)=4.6E-6 24, α(M)=6.E-7 4, α(N)=3.2E-8 17, α(N+)=0.00017 14 |
3/2- | 14 fs 7 | 2310.6 14 | (E2) | 0.000490 | B(E2)(W.u.)=12 6, α=0.000490 7, α(K)=2.24E-5 4, α(L)=2.03E-6 3, α(M)=2.66E-7 4, α(N)=1.393E-8 20, α(N+)=0.000465 7 | ||
2353.4 | 9/2- | 33 fs 12 | 1331.7 7 | (M1+E2) | -0.19 16 | 8.79×10-5 | B(E2)(W.u.)=4 +8-4, B(M1)(W.u.)=0.09 4, α=8.79E-5 20, α(K)=5.58E-5 11, α(L)=5.06E-6 10, α(M)=6.64E-7 13, α(N)=3.47E-8 7, α(N+)=2.64E-5 9 |
9/2- | 33 fs 12 | 2262.2 20 | (E2(+M3)) | 0.00213 LT | 0.00033 | B(E2)(W.u.)=1.6 7, α=0.00033 14, α(K)=3.9E-5 16, α(L)=3.6E-6 15, α(M)=4.7E-7 20, α(N)=2.4E-8 10, α(N+)=0.00029 16 | |
9/2- | 33 fs 12 | 2353.2 7 | M1+E2 | -0.54 23 | 4.44×10-4 | B(E2)(W.u.)=2.9 22, B(M1)(W.u.)=0.022 10, α=4.44E-4 14, α(K)=2.08E-5 4, α(L)=1.88E-6 3, α(M)=2.47E-7 4, α(N)=1.294E-8 21, α(N+)=0.000421 14 | |
2388.0 | 5/2+ | 57 fs 20 | 393.6 15 | (M1(+E2)) | -0.0 4 | 0.00076 | B(M1)(W.u.)=0.62 23, α=0.00076 20, α(K)=0.00069 18, α(L)=6.3×10-5 17, α(M)=8.3E-6 22, α(N)=4.3E-7 11, α(N+)=4.3E-7 11 |
5/2+ | 57 fs 20 | 1639.3 6 | M1+E2 | -0.36 15 | 1.57×10-4 | B(E2)(W.u.)=5 5, B(M1)(W.u.)=0.045 17, α=1.57E-4 5, α(K)=3.86E-5 7, α(L)=3.49E-6 6, α(M)=4.58E-7 8, α(N)=2.40E-8 5, α(N+)=0.000115 4 | |
5/2+ | 57 fs 20 | 2298.6 15 | (E1(+M2)) | 0.096 LT | 0.0006 | B(E1)(W.u.)=0.00012 5, α=0.0006 3, α(K)=2.4E-5 11, α(L)=2.2E-6 10, α(M)=2.9E-7 13, α(N)=1.5E-8 7, α(N+)=0.0005 3 | |
5/2+ | 57 fs 20 | 2388.6 14 | (E1(+M2)) | 0.17 LT | 0.0006 | B(E1)(W.u.)=4.5E-5 17, α=0.0006 4, α(K)=2.3E-5 10, α(L)=2.0E-6 9, α(M)=2.7E-7 12, α(N)=1.4E-8 6, α(N+)=0.0006 4 | |
2408.3 | (7/2-) | < 8 fs | 2408.4 4 | D(+Q) | +0.02 15 | ||
2671.0 | (11/2)- | < 11 fs | 1649.2 3 | M1+E2 | -0.41 6 | 1.61×10-4 | B(E2)(W.u.)>32, B(M1)(W.u.)>0.28, α=1.61E-4 3, α(K)=3.83E-5 6, α(L)=3.47E-6 5, α(M)=4.54E-7 7, α(N)=2.38E-8 4, α(N+)=0.0001193 22 |
2727.5 | 15/2- | 0.10 ps 4 | 464.2 3 | M1(+E2) | 0.0009 | B(E2)(W.u.)<1.2×102 5, B(M1)(W.u.)=1.1 5, α=0.0009 4, α(K)=0.0008 4, α(L)=7.E-5 3, α(M)=1.0E-5 4, α(N)=5.0E-7 20, α(N+)=5.0E-7 20 | |
15/2- | 0.10 ps 4 | 1705.5 7 | (E2) | 0.000218 | B(E2)(W.u.)=18 8, α=0.000218 4, α(K)=3.91E-5 6, α(L)=3.55E-6 5, α(M)=4.65E-7 7, α(N)=2.43E-8 4, α(N+)=0.0001749 25 | ||
2741.0 | 11/2+ | 0.39 ps +36-17 | 1138.9 9 | (E2) | 0.0001040 | B(E2)(W.u.)=33 +15-33, α=0.0001040 15, α(K)=9.17E-5 13, α(L)=8.34E-6 12, α(M)=1.093E-6 16, α(N)=5.69E-8 8, α(N+)=2.73E-6 7 | |
11/2+ | 0.39 ps +36-17 | 1585.8 9 | (E1(+M2)) | 0.00024 | B(E1)(W.u.)=0.00012 +6-12, α=0.00024 12, α(K)=4.9E-5 25, α(L)=4.5E-6 23, α(M)=6.E-7 3, α(N)=3.1E-8 16, α(N+)=0.00018 15 | ||
11/2+ | 0.39 ps +36-17 | 1719.0 15 | (E1(+M2)) | 0.00029 | B(E1)(W.u.)=6.E-6 +7-6, α=0.00029 17, α(K)=4.2E-5 21, α(L)=3.8E-6 19, α(M)=5.0E-7 25, α(N)=2.6E-8 13, α(N+)=0.00025 19 | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
2808.3 | 5/2+ | 0.32 ps 6 | 2655.7 20 | (E1(+M2)) | 0.25 LT | 0.0007 | B(E1)(W.u.)=2.5E-5 6, α=0.0007 4, α(K)=1.9E-5 8, α(L)=1.7E-6 7, α(M)=2.2E-7 9, α(N)=1.2E-8 5, α(N+)=0.0007 4 |
5/2+ | 0.32 ps 6 | 2808.5 20 | (E1(+M2)) | 0.28 LT | 0.0008 | B(E1)(W.u.)=2.4E-5 6, α=0.0008 4, α(K)=1.7E-5 7, α(L)=1.5E-6 6, α(M)=2.0E-7 8, α(N)=1.1E-8 4, α(N+)=0.0008 4 | |
2810.9 | 5/2-,7/2- | < 12 fs | 628.4 10 | M1 | 0.000273 | B(M1)(W.u.)>1.0, α=0.000273 4, α(K)=0.000247 4, α(L)=2.25×10-5 4, α(M)=2.95E-6 5, α(N)=1.540E-7 23, α(N+)=1.540E-7 23 | |
2861.5 | 13/2- | 0.10 ps 6 | 134 1 | (M1(+E2)) | 0.49 LT | 0.07 | α=0.07 6, α(K)=0.06 5, α(L)=0.006 5, α(M)=0.0007 7, α(N)=4.E-5 3, α(N+)=4.E-5 3 |
13/2- | 0.10 ps 6 | 598.3 7 | (M1(+E2)) | 0.5 LT | 0.00043 | B(M1)(W.u.)=0.22 17, α=0.00043 13, α(K)=0.00039 12, α(L)=3.6×10-5 11, α(M)=4.7E-6 14, α(N)=2.4E-7 7, α(N+)=2.4E-7 7 | |
13/2- | 0.10 ps 6 | 1706 1 | E2(+M3) | -0.09 17 | 2.18×10-4 | B(E2)(W.u.)=28 18, B(M3)(W.u.)=6.×105 +21-6, α=2.18E-4 5, α(K)=4.0E-5 4, α(L)=3.6E-6 4, α(M)=4.7E-7 5, α(N)=2.46E-8 24, α(N+)=0.000174 9 | |
3134.0 | 7/2,9/2(+) | < 33.3 ps | 3133.4 10 | D+Q | +0.26 12 | ||
3742.4 | (19/2-) | 416.9 5 | D+Q | -2.0 4 | |||
3912 | (3/2)- | 3761 | D(+Q) | -1.3 20 | |||
7745.0 | 3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 3658 | D(+Q) | 0.00 3 | ||
3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 3830 | D(+Q) | +0.01 2 | |||
3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 3999 | D(+Q) | -0.01 2 | |||
3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 5363 | (E1(+M2)) | 0.10 LT | 0.0016 | B(E1)(W.u.)=0.00062, α=0.0016 5, α(K)=6.3E-6 16, α(L)=5.7E-7 14, α(M)=7.4E-8 19, α(N)=3.9E-9 10, α(N+)=0.0016 5 | |
3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 6104 | D+Q | +0.038 25 | |||
3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 6995 | (E1(+M2)) | 0.19 LT | B(E1)(W.u.)=0.00028 | ||
3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 7592 | (M1+E2) | -0.023 14 | B(E2)(W.u.)=0.0004 +5-4, B(M1)(W.u.)=0.017 5 | ||
3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 7654 | (M1(+E2)) | -0.01 2 | B(E2)(W.u.)=5.E-5 +20-5, B(M1)(W.u.)=0.012 4 | ||
3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | 7745 | E2+M3 | -0.02 1 | B(E2)(W.u.)=0.036 11, B(M3)(W.u.)=1.7 +18-17 | ||
7750 | 3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 3664 | D(+Q) | +0.01 3 | ||
3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 3746 | (M1(+E2)) | -0.01 2 | 0.000967 | B(E2)(W.u.)=0.0011 +44-11, B(M1)(W.u.)=0.064 19, α=0.000967 14, α(K)=9.96E-6 14, α(L)=9.00E-7 13, α(M)=1.179E-7 17, α(N)=6.19E-9 9, α(N+)=0.000956 14 | |
3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 3836 | (M1(+E2)) | -0.01 2 | 0.001000 | B(E2)(W.u.)=0.0007 +28-7, B(M1)(W.u.)=0.041 12, α=0.001000 14, α(K)=9.62E-6 14, α(L)=8.69E-7 13, α(M)=1.139E-7 16, α(N)=5.98E-9 9, α(N+)=0.000990 14 | |
3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 4005 | (M1(+E2)) | +0.01 2 | 0.001060 | B(E2)(W.u.)=0.0007 +29-7, B(M1)(W.u.)=0.047 14, α=0.001060 15, α(K)=9.03E-6 13, α(L)=8.16E-7 12, α(M)=1.069E-7 15, α(N)=5.61E-9 8, α(N+)=0.001050 15 | |
3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 5448 | (M1+E2) | -0.09 6 | 0.001480 | B(E2)(W.u.)=0.007 +10-7, B(M1)(W.u.)=0.010 3, α=0.001480 21, α(K)=5.85E-6 9, α(L)=5.28E-7 8, α(M)=6.92E-8 10, α(N)=3.64E-9 5, α(N+)=0.001473 21 | |
3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 6111 | (E1(+M2)) | +0.02 3 | B(E1)(W.u.)=0.00037 11, B(M2)(W.u.)=0.018 +55-18 | ||
3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 6611 | (E1) | B(E1)(W.u.)=2.6E-5 8 | |||
3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 7001 | (E1(+M2)) | +0.07 25 | B(E1)(W.u.)=2.2E-5 7, B(M2)(W.u.)=0.010 +72-10 | ||
3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 7660 | (M1+E2) | +0.03 2 | B(E2)(W.u.)=0.0008 +12-8, B(M1)(W.u.)=0.022 7 | ||
3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | 7752 | E2(+M3) | -0.03 38 | B(E2)(W.u.)=0.029 9, B(M3)(W.u.)=3 +76-3 | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
8092.6 | (1/2-) | 53 eV 15 % IT = 4.8 19 % p = 95.2 19 | 3456 | (E2(+M3)) | 0.0012 LT | 0.00074 | B(E2)(W.u.)=12, α=0.00074 25, α(K)=1.7E-5 6, α(L)=1.5E-6 5, α(M)=2.0E-7 7, α(N)=1.1E-8 4, α(N+)=0.0007 3 |
(1/2-) | 53 eV 15 % IT = 4.8 19 % p = 95.2 19 | 6447 | (E1) | B(E1)(W.u.)=0.00063 18 | |||
(1/2-) | 53 eV 15 % IT = 4.8 19 % p = 95.2 19 | 7341 | (E1) | B(E1)(W.u.)=7.2E-5 21 | |||
(1/2-) | 53 eV 15 % IT = 4.8 19 % p = 95.2 19 | 7999 | (E2+(M3)) | 0.032 LT | B(E2)(W.u.)=0.092 | ||
8117.5 | 3/2 | 6978 | D+Q | -0.11 8 | |||
3/2 | 7370 | D+Q | +0.10 4 | ||||
3/2 | 8027 | D(+Q) | +0.14 15 | ||||
3/2 | 8118 | Q+O | -0.29 15 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 7/2- | 330 d 15 % ε = 100 | μ=4.47 5 (2005St24,1957We17), T=3/2 E(level): 7/2- GS yrast band. From β+ decay. |
90.6392 | 5/2- | 228 ps 13 | E(level): 7/2- GS yrast band. From β+ decay. |
748.27 | 3/2+ | 5.3 ps 6 | T=3/2 E(level): Kπ=3/2+ ROTATIONAL band. |
1021.62 | 11/2- | 3.4 ps 6 | E(level): 7/2- GS yrast band. From β+ decay. |
1140.53 | 5/2+ | 1.3 ps 6 | E(level): Kπ=3/2+ ROTATIONAL band. |
1155.32 | 9/2- | 1.1 ps 3 | E(level): 7/2- GS yrast band. From β+ decay. |
1602.68 | 7/2+ | 0.47 ps 22 | E(level): Kπ=3/2+ ROTATIONAL band. |
1610 | (9/2-,11/2-) | Jπ(level): From angular momentum transfer in (t,α). | |
1646.43 | (1/2+) | 6.6 ps 10 | E(level): Kπ=1/2+ ROTATIONAL BAND?. |
1994.7 | 3/2(+) | 0.49 ps 21 | E(level): Kπ=1/2+ ROTATIONAL BAND?. |
2178.3 | 9/2+ | 0.56 ps +49-28 | E(level): Kπ=3/2+ ROTATIONAL band. |
2182.0 | 7/2- | 33 fs 12 | Jπ(level): From angular momentum transfer in (p,t). |
2263.30 | 15/2- | 0.65 ps +38-19 | E(level): 7/2- GS yrast band. From β+ decay. |
2388.0 | 5/2+ | 57 fs 20 | E(level): Kπ=1/2+ ROTATIONAL BAND?. |
2671.0 | (11/2)- | < 11 fs | E(level): NEGATIVE-PARITY SIDE band. |
2671.3 | 7/2-,9/2,11/2+ | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
2727.5 | 15/2- | 0.10 ps 4 | E(level): NEGATIVE-PARITY SIDE band. |
2741.0 | 11/2+ | 0.39 ps +36-17 | E(level): Kπ=3/2+ ROTATIONAL band. |
2810.9 | 5/2-,7/2- | < 12 fs | E(level): NEGATIVE-PARITY SIDE band. |
2861.5 | 13/2- | 0.10 ps 6 | E(level): 7/2- GS yrast band. From β+ decay. |
3017.3 | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. | |
3134.0 | 7/2,9/2(+) | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
3224 | (1/2,3/2,5/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3239.5 | 7/2- | < 33.3 ps | Jπ(level): From angular momentum transfer in (p,t). T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
3242 | (3/2,5/2,7/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
3248 | 1/2+ | Jπ(level): From angular momentum transfer in (t,α). | |
3259.5 | (GE 9/2) | T1/2>2 ps,T1/2<0.7 ns. | |
3303.2 | 3/2-,5/2,7/2,9/2 | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
3325 | (1/2+ TO 7/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
3325.2 | (17/2-) | E(level): 7/2- GS yrast band. From β+ decay. | |
3340.5 | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. | |
3341.8 | (13/2+) | T1/2>3.5 ps, T1/2<0.7 ns. E(level): Kπ=3/2+ ROTATIONAL band. | |
3342 | (1/2+ TO 9/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3388 | (3/2,5/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3388.5 | 5/2,7/2 | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
3405 | (3/2)- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3462.9 | (3/2+ TO 9/2+) | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
3479 | (7/2-) | Jπ(level): From angular momentum transfer in (p,t). | |
3500.6 | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. | |
3516 | (3/2- TO 9/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
3521 | (LE 9/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
3531 | (LE 7/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
3531.1 | 5/2-,7/2,9/2+ | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
3603 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | ||
3609 | (7/2-) | Jπ(level): From angular momentum transfer in (p,t). | |
3623.9 | LE 9/2 | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
3639.8 | (7/2-) | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
3665.9 | 11/2 | < 33.3 ps | T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps. |
3671 | (1/2+ TO 9/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3678 | (7/2)- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
3694 | 3/2+,5/2+ | E(level): From (p,α). Jπ(level): From angular momentum transfer in (t,α). | |
3721 | (LE 7/2)- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3741 | 1/2-,3/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3742.4 | (19/2-) | E(level): 7/2- GS yrast band. From β+ decay. | |
3757 | 5/2-,7/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3771 | (1/2+ TO 9/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
3782 | (GE 9/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3795 | (-) | Jπ(level): From angular momentum transfer in (p,t). | |
3816 | (LE 7/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3825 | (-) | Jπ(level): From angular momentum transfer in (p,t). | |
3841 | 1/2(+),3/2,5/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
3912 | (3/2)- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): L(3He,d)=1; 3/2 from deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
3927 | (1/2+ TO 9/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
3960 | (3/2-,5/2,7/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
3975 | (-) | Jπ(level): From angular momentum transfer in (p,t). | |
4002 | (3/2)- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): L(3He,d)=1; 3/2 from deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
4035 | (3/2- TO 9/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
4088 | 3/2(-),5/2,7/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
4098 | (LE 7/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
4129 | (5/2)- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
4152 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | ||
4218 | (3/2)- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): L(3He,d)=1; 3/2 from deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
4253 | 1/2-,3/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
4259 | (3/2,5/2,7/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis. | |
4270 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
4289 | 3/2+,5/2+ | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From angular momentum transfer in (t,α). | |
4359 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | ||
4373 | 1/2-,3/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
4397 | 5/2-,7/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From angular momentum transfer in (t,α). | |
4422 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | ||
4436 | E(level): From (p,α). | ||
4498 | 5/2(-),7/2(-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
4502 | 1/2-,3/2- | E(level): From (3He,d). | |
4540 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | ||
4590 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | ||
4635 | (5/2)- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
4662 | 3/2+,5/2+ | E(level): From (p,α). Jπ(level): From angular momentum transfer in (t,α). | |
4740 | 3/2+,5/2+ | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): From angular momentum transfer in (t,α). | |
4840 | 1/2-,3/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
4863 | E(level): From (p,α). | ||
4885 | E(level): From (p,α). | ||
4947 | 1/2-,3/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
4959 | 1/2+ | Jπ(level): From angular momentum transfer in (t,α). | |
5010 | 5/2-,7/2- | E(level): From (p,α). Jπ(level): From angular momentum transfer in (t,α). | |
5042 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | ||
5072 | 3/2+,5/2+ | Jπ(level): From angular momentum transfer in (t,α). | |
5134 | E(level): From (p,α). | ||
5212 | 1/2-,3/2- | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
5230 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | ||
5292 | 1/2+ | E(level): From (p,α). Jπ(level): From angular momentum transfer in (t,α). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
5347 | (3/2+,5/2+) | E(level): From (p,α). Jπ(level): From angular momentum transfer in (t,α). | |
5387 | 1/2-,3/2- | E(level): From (p,α). Jπ(level): From angular momentum transfer in (t,α). | |
5411 | 5/2-,7/2- | E(level): From (p,α). | |
5522 | 1/2+ | Jπ(level): From angular momentum transfer in (t,α). | |
5529.7 | (21/2-) | E(level): 7/2- GS yrast band. From β+ decay. Jπ(level): From stretched (ΔJ=1) dipole or stretched (ΔJ=2) quadrupole cascade and membership in 7/2- g.s. yrast band. | |
5597 | 1/2-,3/2- | E(level): From (3He,d). | |
5631 | (3/2+,5/2+) | Jπ(level): From angular momentum transfer in (t,α). | |
5689.9 | (23/2-) | E(level): 7/2- GS yrast band. From β+ decay. Jπ(level): From stretched (ΔJ=1) dipole or stretched (ΔJ=2) quadrupole cascade and membership in 7/2- g.s. yrast band. | |
5889 | 1/2-,3/2- | E(level): From (3He,d). | |
5931 | (3/2+,5/2+) | Jπ(level): From angular momentum transfer in (t,α). | |
5987 | 1/2-,3/2- | E(level): From (3He,d). | |
6058 | (3/2+,5/2+) | Jπ(level): From angular momentum transfer in (t,α). | |
6184 | E(level): From (3He,d). | ||
6220 | 1/2-,3/2- | E(level): From (3He,d). | |
6333 | 1/2-,3/2- | E(level): From (3He,d). | |
6368 | E(level): From (3He,d). | ||
6430 | E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. Jπ(level): Jp=7/2-, t=5/2, IAS(49Ti g.s.) for 6446 25 in (p,|A). | ||
6474 | E(level): From (3He,d). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. Jπ(level): Jp=7/2-, t=5/2, IAS(49Ti g.s.) for 6446 25 in (p,|A). | ||
6521 | E(level): From (3He,d). | ||
6563 | (3/2+,5/2+) | Jπ(level): From angular momentum transfer in (t,α). | |
6844.9 | (23/2-) | E(level): NEGATIVE-PARITY SIDE band. | |
7745.0 | 3/2- | 8.9 eV 30 % IT = 10 4 % p = 90 4 | T=5/2, Γγ=0.88 25, Γp=8 3 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. |
7750 | 3/2- | 6.7 eV 20 % IT = 10 4 % p = 90 4 | T=5/2, Γγ=0.70 20, Γp=6 2 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. |
7801.4 | (25/2-) | E(level): 7/2- GS yrast band. From β+ decay. Jπ(level): From stretched (ΔJ=1) dipole or stretched (ΔJ=2) quadrupole cascade and membership in 7/2- g.s. yrast band. | |
7838.7 | (1/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 1/2-,3/2,5/2 from γ’s to 3/2-, 3/2+, and 5/2- assuming d,E2; 1/2,3/2 from multidimensional nonmetric scaling analysis. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
7910.2 | (1/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 1/2-,3/2,5/2 from γ’s to 3/2-, 3/2+, and 5/2- assuming d,E2; 1/2,3/2 from multidimensional nonmetric scaling analysis. | |
7943.5 | (3/2-) | T=5/2 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis. | |
8013.0 | (3/2-) | T=5/2 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis. | |
8058.1 | (3/2,5/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
8071.8 | (5/2) | T=5/2 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8092.6 | (1/2-) | 53 eV 15 % IT = 4.8 19 % p = 95.2 19 | T=5/2, Γγ=2.5 7, Γp=50 15 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. |
8104.2 | 3/2(-),5/2 | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
8117.5 | 3/2 | Γγ=0.33 9 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
8131.5 | (3/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis. | |
8290.3 | 3/2(-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
8416.1 | (27/2-) | E(level): 7/2- GS yrast band. From β+ decay. Jπ(level): From stretched (ΔJ=1) dipole or stretched (ΔJ=2) quadrupole cascade and membership in 7/2- g.s. yrast band. | |
8525.3 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8628.2 | (3/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis. | |
8633.1 | (5/2) | T=5/2 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8640.9 | (3/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis. | |
8642.9 | (3/2-,5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
8682.0 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8784.9 | (5/2) | T=5/2 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8788.8 | (5/2-) | T=5/2 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. | |
8851.5 | (5/2-,7/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
8867.2 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8877.0 | (5/2) | T=5/2 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8880.9 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
8890.7 | (3/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis. | |
8893.6 | (5/2-) | T=5/2 E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
8895.6 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
8902.5 | (5/2) | T=(5/2) E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. Jp=5/2-, t=5/2 from IAS identification in (3He,pd). | |
8912.2 | (5/2) | T=(5/2) E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. Jp=5/2-, t=5/2 from IAS identification in (3He,pd). | |
8921.1 | (5/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (α,pγ). Jπ(level): 5/2+ from γ’s to 3/2-, 3/2+, and 9/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8925.0 | (7/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
8927.9 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. Jp=5/2-, t=5/2 from IAS identification in (3He,pd). | |
8942.6 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8945 | (1/2+) | T=(5/2) E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. | |
8965.1 | (5/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (α,pγ). Jπ(level): 5/2+ from γ’s to 3/2-, 3/2+, and 9/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
8998.5 | (1/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
9008.2 | (5/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9029.8 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9037.6 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9044.5 | (7/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
9056.2 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9071.9 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9075.8 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9078.8 | (3/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis. | |
9082.7 | (3/2+) | T=(5/2) E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. | |
9089.5 | (3/2-,5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
9094.4 | (5/2) | E(level): From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9118.0 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9131.7 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9135.6 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (p,γ) E=960-2488 keV res. Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9148.3 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
9154.2 | (5/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (α,pγ). Jπ(level): 5/2+ from γ’s to 3/2-, 3/2+, and 9/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9161.1 | (1/2-,3/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 1/2-,3/2,5/2 from γ’s to 3/2-, 3/2+, and 5/2- assuming d,E2; 1/2,3/2 from multidimensional nonmetric scaling analysis. | |
9167.9 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9168.9 | (3/2-) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
9174.8 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9182.6 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
9193.4 | (5/2,7/2+) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. | |
9195.3 | (5/2) | E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. | |
9568 | (1/2-) | T=(5/2) E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. | |
9662 | 3/2- | T=5/2 E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. | |
10230 | (5/2)- | T=5/2 E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. | |
10925 | (5/2)+ | T=5/2 E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. | |
11150 | (9/2+) | T=5/2 E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. |
E(level) | E(gamma) | Comments |
90.6392 | 90.639 | E(γ): From β+ decay M(γ): from α(exp) in (p,nγ) and comparison to RUL. Δπ=1 d γ from recoil-γ(θ) in (40C,3pγ) |
152.9282 | 62.289 | E(γ): From β+ decay I(γ): weighted av of Iγ(62γ)/Iγ(153γ)=72.4 35/100.0 52 from (α,pγ) and 68.9 32/100.0 32 from (p,nγ). Iγ(62γ)/Iγ(153γ)=54.0 7/100.0 4 from B=decay and 100/92 from (p,γ) discrepant M(γ): d from comparison to RUL. Δπ=no from the level scheme | 152.928 | E(γ): From β+ decay I(γ): From β+ decay M(γ): from α(exp) in (p,nγ) and comparison to RUL |
748.27 | 595.35 | M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme | 657.60 | M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme |
1021.62 | 1021.63 | M(γ): Q(+O) from pγ(θ) in (α,pγ). Ne M2(+E3) from comparison to RUL. ΔJ=2 Q or ΔJ=0 d γ from recoil-γ(θ) in (40Ca,3pγ) |
1140.53 | 392.7 | E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies M(γ): D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL | 987.61 | M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme | 1049.79 | M(γ): from α(exp) and γ(θ) in (p,nγ) | 1140.7 | E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies M(γ): from α(exp) in (p,nγ) and pγ(θ) in (α,pγ) |
1155.32 | 133.80 | E(γ): From (p,α) M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme | 1064.63 | M(γ): Q from pγ(θ) in (α,pγ). Ne M2 from comparison to RUL | 1155.33 | M(γ): ΔJ=1 d γ from recoil-γ(θ) in (40Ca,3pγ). D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL |
1514.54 | 766 | M(γ): d from comparison to RUL. Δπ=yes from level scheme | 1361.61 | E(γ): From β+ decay M(γ): D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL | 1423.6 | E(γ): From (p,α). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme | 1514.4 | E(γ): From (3He,d). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents M(γ): From comparison to RUL |
1602.68 | 447.4 | I(γ): Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ. M(γ): d,E2 from α(exp) in (p,nγ). Δπ=yes from level scheme | 462.2 | I(γ): Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ. M(γ): d(+Q) from pγ(θ) in (α,pγ). Ne E1+M2 from α(exp) in (p,nγ) | 854.5 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided. Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ. M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme | 1512.0 | I(γ): Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ. M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 1602.6 | I(γ): Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ. M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme |
1643.19 | 1490.24 | I(γ): From (p,γ) E=960-2488 keV res M(γ): from pγ(θ) in (α,pγ) | 1553 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
1646.43 | 898.06 | I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ) | 1493.6 | E(γ): From (α,pγ) I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ) M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme |
E(level) | E(gamma) | Comments |
1661.40 | 912.3 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 1508.37 | E(γ): From (3He,d) M(γ): From comparison to RUL | 1570.83 | E(γ): From (p,α) M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme | 1661.4 | M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme |
1994.7 | 854.5 | E(γ): Multiply placed with intensity suitably divided. From (p,α) I(γ): Multiply placed with intensity suitably divided M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme | 1246.8 | E(γ): Multiply placed with intensity suitably divided. From (3He,d) I(γ): Multiply placed with intensity suitably divided M(γ): From comparison to RUL | 1841.0 | M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme | 1903.4 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme |
2178.3 | 575.4 | I(γ): From (α,pγ) | 1023 | E(γ): From (3He,d). From (40Ca,3pγ) M(γ): From comparison to RUL | 1037.4 | I(γ): From (α,pγ) M(γ): from pγ(θ) in (α,pγ) and α(exp) in (p,nγ) | 1157.0 | I(γ): From (α,pγ) M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ) | 2178.3 | I(γ): From (α,pγ) |
2182.0 | 1026.8 | I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ) M(γ): d,E2 from comparison to RUL. Δπ=no from level scheme. d,E2 from comparison to RUL. Δπ=yes from level scheme | 2090.7 | E(γ): From (p,α). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ) M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme | 2181.6 | E(γ): From (3He,d) I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ) M(γ): From comparison to RUL |
2234.0 | 572.5 | E(γ): From (3He,d). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents I(γ): Note that Iγ(572γ) from (p,nγ) may have an unresolved component from 2178 state and that Iγ(2233γ) from (α,pγ) may have an unresolved component from the 3388 state discrepant. M(γ): From comparison to RUL | 2142.9 | E(γ): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents | 2234.4 | E(γ): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents I(γ): Note that Iγ(572γ) from (p,nγ) may have an unresolved component from 2178 state and that Iγ(2233γ) from (α,pγ) may have an unresolved component from the 3388 state discrepant. |
2263.30 | 1241.69 | M(γ): from α(exp) in (p,nγ) and comparison to RUL. ΔJ=2 Q or ΔJ=0 d from recoil-γ(θ) in (40Ca,3pγ) |
2265.3 | 621 | E(γ): From (3He,d). From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res M(γ): From comparison to RUL | 2112.3 | E(γ): From (α,pγ) I(γ): From (p,γ) E=960-2488 keV res |
2309.4 | 1560 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 2310.6 | M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme |
2353.4 | 1198.9 | E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (3He,d) M(γ): From comparison to RUL | 1331.7 | E(γ): From (p,α) M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme | 2262.2 | M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme | 2353.2 | E(γ): From (α,pγ) M(γ): D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL |
E(level) | E(gamma) | Comments |
2388.0 | 393.6 | E(γ): From (p,α). From (α,pγ) I(γ): From (α,pγ) M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme | 1247.8 | E(γ): Multiply placed with intensity suitably divided. From (3He,d). From (α,pγ) I(γ): Multiply placed with intensity suitably divided. From (α,pγ) M(γ): From comparison to RUL | 1639.3 | I(γ): From (α,pγ) M(γ): D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL | 2235.5 | I(γ): From (α,pγ) | 2298.6 | I(γ): From (α,pγ) M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 2388.6 | I(γ): From (α,pγ) M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme |
2408.3 | 229.2 | E(γ): From (α,pγ) I(γ): From (α,pγ) | 1252.9 | E(γ): From (3He,d) M(γ): From comparison to RUL | 1268 | E(γ): From (3He,d). From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res M(γ): From comparison to RUL | 1385.7 | E(γ): From (3He,d) M(γ): From comparison to RUL | 2408.4 | E(γ): From (α,pγ) |
2671.0 | 1517 | E(γ): From (3He,d). From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): From comparison to RUL | 1649.2 | E(γ): From (α,pγ) I(γ): From (40Ca,3pγ) M(γ): D+Q from pγ(θ) in (α,pγ). δ(9/2,11/2,13/2) and comparison to RUL exclude E1+M2 |
2671.3 | 1649.3 | E(γ): From (3He,d) M(γ): From comparison to RUL | 2579.2 | E(γ): From (3He,d) M(γ): From comparison to RUL |
2727.5 | 464.2 | E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies I(γ): From (40Ca,3pγ) M(γ): d(+Q) from pγ(θ) in (α,pγ). Ne E1 from comparison to RUL. ΔJ=2 Q or ΔJ=0 d γ from recoil-γ(θ) in (40Ca,3pγ) | 1705.5 | I(γ): From (40Ca,3pγ) M(γ): d,E2 from comparison to RUL. ΔJ=2 Q or ΔJ=0 d from recoil-γ(θ) in (40Ca,3pγ). ΔJπ=2,no from level scheme |
2741.0 | 562.5 | E(γ): From (3He,d) I(γ): From (α,pγ) M(γ): From comparison to RUL | 1138.9 | E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies I(γ): From (α,pγ) M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme | 1585.8 | I(γ): From (α,pγ) M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 1719.0 | E(γ): From (α,pγ) I(γ): From (α,pγ) M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme |
2786.4 | 1184.3 | E(γ): From (3He,d) M(γ): From comparison to RUL | 1764.5 | M(γ): D+Q,Q from pγ(θ) in (α,pγ). Ne M2 from comparison to RUL | 2697.2 | E(γ): From (3He,d) M(γ): From comparison to RUL | 2786.4 | E(γ): From (α,pγ) M(γ): D+Q,Q from pγ(θ) in (α,pγ). δ(9/2) and comparison to RUL exclude E1+M2; Ne M2 from comparison to RUL |
E(level) | E(gamma) | Comments |
2808.3 | 1206.6 | E(γ): From (3He,d) M(γ): From comparison to RUL | 1666.7 | E(γ): From (3He,d) M(γ): From comparison to RUL | 2058 | E(γ): From (3He,d). From (α,pγ) I(γ): From (α,pγ) M(γ): From comparison to RUL | 2655.7 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 2808.5 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme |
2810.9 | 628.4 | E(γ): From (3He,d) M(γ): From comparison to RUL | 1673 | E(γ): From (3He,d) M(γ): From comparison to RUL | 2720.3 | E(γ): From (3He,d). From (α,pγ) M(γ): From comparison to RUL | 2810.9 | E(γ): From (3He,d). From (α,pγ) M(γ): From comparison to RUL |
2861.5 | 134 | E(γ): From (40Ca,3pγ) M(γ): d from comparison to RUL. Δπ=no from the level scheme | 598.3 | E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies M(γ): ΔJ=1 d transition from recoil-γ(θ) in (40Ca,3pγ). Δπ=no from level scheme | 1706 | E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies M(γ): Q+O from pγ(θ) in (α,pγ). Ne M2+E3 from comparison to RUL. ΔJ=2 Q or ΔJ=0 d from recoil-γ(θ) in (40Ca,3pγ) | 1840 | E(γ): From (3He,d). From (40Ca,3pγ) M(γ): From comparison to RUL |
3017.3 | 1414.1 | E(γ): From (3He,d) M(γ): From comparison to RUL |
3133.9 | 462.9 | E(γ): From (3He,d). From (α,pγ) I(γ): From (α,pγ) M(γ): From comparison to RUL |
3134.0 | 1979.5 | E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (3He,d) M(γ): From comparison to RUL | 2112.8 | E(γ): From (3He,d) M(γ): From comparison to RUL | 2385.7 | E(γ): From (3He,d) M(γ): From comparison to RUL |
3224 | 1566 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 3074 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
3239.5 | 1725.2 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3238.2 | E(γ): From (3He,d) M(γ): From comparison to RUL |
3259.5 | 473.1 | E(γ): From (α,pγ) I(γ): From (α,pγ) |
3303.2 | 1121.0 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3213.5 | E(γ): From (3He,d) M(γ): From comparison to RUL |
E(level) | E(gamma) | Comments |
3325.2 | 464 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=2) quadrupole or ΔJ=0 dipole transition from recoil-γ(θ) in (40Ca,3pγ) | 597.1 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ) | 1061.9 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ) |
3341.8 | 601.0 | E(γ): From (3He,d). From (α,pγ) I(γ): From (α,pγ) M(γ): From comparison to RUL | 670.5 | E(γ): From (3He,d). From (α,pγ) I(γ): From (α,pγ) M(γ): From comparison to RUL | 1163.0 | E(γ): From (3He,d). From (α,pγ) I(γ): From (α,pγ) M(γ): From comparison to RUL |
3388 | 1729 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 1876 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
3531 | 1870 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 1887 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 3378 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
3531.1 | 1178.4 | E(γ): From (3He,d) M(γ): From comparison to RUL | 1348.4 | E(γ): From (3He,d) M(γ): From comparison to RUL | 2015.6 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3378.5 | E(γ): From (3He,d) M(γ): From comparison to RUL |
3623.9 | 2483.3 | E(γ): From (3He,d) M(γ): From comparison to RUL |
3639.8 | 1461.5 | E(γ): From (3He,d) M(γ): From comparison to RUL | 2123.8 | E(γ): From (3He,d) M(γ): From comparison to RUL | 2618.1 | E(γ): From (3He,d) M(γ): From comparison to RUL |
3665.9 | 1312.1 | E(γ): From (3He,d) M(γ): From comparison to RUL | 1402.7 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3666.7 | E(γ): From (3He,d) M(γ): From comparison to RUL |
3741 | 2230 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 3591 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 3653 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
E(level) | E(gamma) | Comments |
3742.4 | 416.9 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) | 1479.1 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=2) quadrupole or ΔJ=0 dipole transition from recoil-γ(θ) in (40Ca,3pγ) |
3816 | 3725 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
3841 | 2180 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 2197 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
3912 | 1650 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 2270 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 3761 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
4002 | 1693 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 2358 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
4088 | 1855 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 2576 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 3937 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 4090 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
4129 | 3380 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
4253 | 2589 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 2606 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
4373 | 2064 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 2138 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 2712 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
4498 | 3343 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 4345 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
4590 | 2355 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
4635 | 4548 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res | 4639 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
E(level) | E(gamma) | Comments |
4947 | 4853 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
5212 | 2903 | E(γ): From (p,γ) E=960-2488 keV res I(γ): From (p,γ) E=960-2488 keV res |
5529.7 | 1787 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): from recoil-γ(θ) in (40Ca,3pγ) | 2204 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) |
5689.9 | 160 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) | 1947 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=2) quadrupole or ΔJ=0 dipole transition from recoil-γ(θ) in (40Ca,3pγ) |
6844.9 | 1155 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ) | 1315 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) | 3102 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) |
7745.0 | 3111 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3249 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3620 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3741 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3931 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4355 | E(γ): From (3He,d) M(γ): From comparison to RUL | 5363 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 5486 | E(γ): From (3He,d) M(γ): From comparison to RUL | 6995 | E(γ): From (3He,d) M(γ): From comparison to RUL. d,E2 from comparison to RUL. Δπ=yes from level scheme | 7592 | M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme | 7654 | M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme | 7745 | M(γ): Q+O from γ(θ) in (p,γ). Ne M2+E3 from comparison to RUL |
7750 | 3116 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3627 | E(γ): From (3He,d) M(γ): From comparison to RUL | 3746 | M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme | 3836 | M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme | 3993 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4005 | M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme | 4343 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4360 | E(γ): From (3He,d) M(γ): From comparison to RUL | 5448 | M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme | 5491 | E(γ): From (3He,d) M(γ): From comparison to RUL | 6111 | M(γ): d(+Q) from γ(θ) in (p,γ). Δπ=yes from level scheme | 6611 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 7001 | M(γ): d(+Q) from γ(θ) in (p,γ). Δπ=yes from level scheme | 7660 | M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme | 7752 | M(γ): Q(+O) from γ(θ) in (p,γ). Ne M2 from comparison to RUL |
E(level) | E(gamma) | Comments |
7801.4 | 956 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ) | 2111 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ) | 2271 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) |
8092.6 | 3456 | M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme | 3718 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4089 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4179 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4249 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4349 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4851 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4866 | E(γ): From (3He,d) M(γ): From comparison to RUL | 6429 | E(γ): From (3He,d) M(γ): From comparison to RUL | 6447 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 7341 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 7936 | M(γ): from comparison to RUL. γ(θ) isotropic in (p,γ) | 7999 | M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme |
8117.5 | 3743 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4114 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4728 | E(γ): From (3He,d) M(γ): From comparison to RUL | 4892 | E(γ): From (3He,d) M(γ): From comparison to RUL | 5730 | E(γ): From (3He,d) M(γ): From comparison to RUL | 5808 | E(γ): From (3He,d) M(γ): From comparison to RUL | 5853 | E(γ): From (3He,d) M(γ): From comparison to RUL | 5884 | E(γ): From (3He,d) M(γ): From comparison to RUL | 6601 | E(γ): From (3He,d) M(γ): From comparison to RUL |
E(level) | E(gamma) | Comments |
8416.1 | 613 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ) | 5690 | E(γ): From (40Ca,3pγ) I(γ): From (40Ca,3pγ) M(γ): Stretched (ΔJ=2) quadrupole or ΔJ=0 dipole transition from recoil-γ(θ) in (40Ca,3pγ) |
9044.5 | 6373 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity | 6373 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
Levels: Resonances: see 1978Ha15 and the references cited below for additional resonance states and more information on the resonance parameters. Others: see 1995Bu23
Levels: Bound-state t’s: from 50Cr(3He,α) in 49Cr
Levels: Γp, Γγ: from (p,γ)
Levels: %p,%γ: from Γp and Γγ
Levels: Multidimensional nonmetric scaling analysis: see 47V adopted levels, gammas and 46Ti(p,γ) E=0.4-1.8 MeV res (1991Bu05) for a comparison of results from multidimensional nonmetric scaling analysis of the data from 1986De13 by 1993Ca12 to an average-spin method analysis by 1988Va08 and 1991Ki11 of the data and results using the Nuclear Data Sheets "Strong " arguments for spin and parity assignments.
Gammas: Γγ: from (p,γ)
Q-value: Note: Current evaluation has used the following Q record -2626.5 2611552.9 266758.2 8 -9084 3 2003Au03