ADOPTED LEVELS, GAMMAS for 195Pt
Authors: Huang Xiaolong and Kang Mengxiao | Citation: Nucl. Data Sheets 121, 395 (2014) | Cutoff date: 1-Mar-2014
Full ENSDF file | Adopted Levels (PDF version)
| Q(β-)=-226.8 keV 10 | S(n)= 6105.06 keV 12 | S(p)= 7551.5 keV 21 | Q(α)= 1175.6 keV 18 | ||
| Reference: 2012Wa38 |
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 0.0 | ABCDEFGHIJKLMNO | 1/2- | STABLE | |||||
| 98.880 2 | ABCDEFGHIJKL NO | 3/2- | 0.170 ns 19 | 98.857 10 | 100 | M1+E2 | 0.0 | 1/2- |
| 129.772 3 | ABCDEFGHI KLMNO | 5/2- | 0.67 ns 3 | 30.876 6 129.735 10 | 92 4 100 3 | M1+E2 E2 | 98.880 0.0 | 3/2- 1/2- |
| 199.532 2 | B DEFG I KL NO | 3/2- | 0.66 ns 14 | 100.652 3 199.533 2 | 49 5 100 10 | M1(+E2) M1+E2 | 98.880 0.0 | 3/2- 1/2- |
| 211.406 2 | ABCDEFG IJKL NO | 3/2- | 49 ps 8 | 211.407 2 | 100 | M1+E2 | 0.0 | 1/2- |
| 222.230 4 | E G IJ | 1/2- | 123.337 10 222.230 5 | 100 10 49 6 | M1(+E2) M1 | 98.880 0.0 | 3/2- 1/2- | |
| 239.264 4 | BC EFG I KL NO | 5/2- | 70 ps 9 | 28S 140.385 9 239.261 5 | 2.5 1 55 3 100 5 | M1+E2 E2 | 98.880 0.0 | 3/2- 1/2- |
| 259.077 23 | BC E G KLM O | 13/2+ | 4.010 d 5 % IT = 100 | 19.8S 129.5 2 | 0.24 1 100 5 | [M4] M4 | 239.264 129.772 | 5/2- 5/2- |
| 389.132 4 | B E G I | 5/2- | 9 ps 4 | 150.11 15 259.351 6 290.254 3 389 1 | 9 2 40 5 100 5 2.7 12 | [M1] M1(+E2) M1(+E2) E2 | 239.264 129.772 98.880 0.0 | 5/2- 5/2- 3/2- 1/2- |
| 419.702 3 | E G I | 3/2- | 54 ps 8 | 197.479 14 320.819 3 419.705 4 | 10.3 19 16.3 19 100 10 | M1(+E2) M1(+E2) M1(+E2) | 222.230 98.880 0.0 | 1/2- 3/2- 1/2- |
| 431.98 2 | B EFG I KL | 9/2+ | 172.906 3 | 100 | E2 | 259.077 | 13/2+ | |
| 432 | M | (17/2+) | ||||||
| 449.65 5 | B I L | (7/2)- | 60.4 211.3 239.21 319.90 7 350.90 10 | <15 2.7 1.3 100 5 10.6 15 | [M1,E2] [E2] M1+E2 [E2] | 389.132 239.264 129.772 98.880 | 5/2- 5/2- 5/2- 3/2- | |
| 455.272 7 | B E G I KL | 5/2- | > 10.5 ps | 216.012 9 243.855 14 255.741 30 325.18 10 ? 356.395 14 | 47 5 42 3 47 5 42 5 100 10 | M1(+E2) M1 (M1+E2) M1 | 239.264 211.406 199.532 129.772 98.880 | 5/2- 3/2- 3/2- 5/2- 3/2- |
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 507.917 6 | B E G I KLM | 5/2-,7/2- | 9.5 ps 22 | 119.12 10 296.5 378.129 9 409.049 11 | ≤27 4.6 10 87 11 100 11 | [M1,E2] [E2] M1 E2 | 389.132 129.772 | 5/2- 5/2- |
| 524.846 3 | EFG IJ | 3/2- | 285.578 4 313.449 6 395.071 3 425.978 7 524.846 4 | 33 4 18 2 72 8 39 4 100 10 | M1+E2 M1(+E2) M1+E2 M1+E2 | 239.264 211.406 129.772 98.880 0.0 | 5/2- 3/2- 5/2- 3/2- 1/2- | |
| 539 3 ? | F | |||||||
| 544.1 5 | G I | (5/2-) | > 2.8 ps | 305? 333 414 445.2 544.2 | 56.25 100 | 239.264 211.406 129.772 98.880 0.0 | 5/2- 3/2- 5/2- 3/2- 1/2- | |
| 547.16 10 | B FG K M | (11/2+) | 115.0 5 287.80 15 | 10 3 100 30 | (M1+E2) | 259.077 | 13/2+ | |
| 562.80 5 | B G I K M | 9/2- | 14 ps 3 | 130.3 5 324 432.86 7 | 0.8 5 8.9 11 100 | [E1] E2 | 239.264 129.772 | 5/2- 5/2- |
| 590.902 4 | E G | 3/2- | 368.671 3 379.503 8 391.377 10 590.895 7 | 92 9 29 4 16 3 100 10 | M1(+E2) M1(+E2) M1(+E2) | 222.230 211.406 199.532 0.0 | 1/2- 3/2- 3/2- 1/2- | |
| 612.72 8 | B FG I KLM | (7/2)- | 6 ps 3 | 223.7 3 373.39 15 401.30 15 513.6 3 | ≈0.91 100 27 27 9 2.7 9 | M1(+E2) [E2] | 389.132 239.264 211.406 98.880 | 5/2- 5/2- 3/2- 3/2- |
| 627.8 5 | O | 17/2+ | 368.8 5 | 100 | 259.077 | 13/2+ | ||
| 630.147 6 | E G | 1/2-,3/2- | 407.910 12 418.741 8 430.620 10 531.263 23 629.86 25 | 91 11 100 15 95 11 61 18 17 5 | 222.230 211.406 199.532 98.880 0.0 | 1/2- 3/2- 3/2- 3/2- 1/2- | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 632.1 5 | I | 1/2-,3/2- | 392.8 5 | | 239.264 | 5/2- | ||
| 664.205 6 | E G L | (5/2-,7/2-) | 424.944 18 452.799 16 464.674 7 534.418 15 | 30 8 67 12 100 12 77 15 | 239.264 211.406 199.532 129.772 | 5/2- 3/2- 3/2- 5/2- | ||
| 667.0 7 | I | (9/2-) | 16 ps 4 | 428 537 | 100 19 3 | (E2) | 239.264 129.772 | 5/2- 5/2- |
| 678.3 10 | I K | 5/2-,7/2- | > 72.8 ps | 439 | | 239.264 | 5/2- | |
| 695.30 6 | B G KL | (7/2)- | 306.0 455.94 10 495.8 2 565.48 15 596.48 20 | 100 92 6 60 6 26 6 25 6 | [M1] M1(+E2) [E2] [M1] [E2] | 389.132 239.264 199.532 129.772 98.880 | 5/2- 5/2- 3/2- 5/2- 3/2- | |
| 739.545 5 | E G L | 1/2-,3/2- | 319.843 4 640.33 16 739.74 16 | 100 12 27 4 56 8 | E2(+M1) | 419.702 98.880 0.0 | 3/2- 3/2- 1/2- | |
| 758.3 5 | O | 15/2+ | 499.2 5 | 100 | 259.077 | 13/2+ | ||
| 765.8 9 | KL | (7/2)- | ||||||
| 793 2 | KLM | 11/2+,13/2+ | ||||||
| 793.0 10 | I | 3/2- | 793 | 100 | M1+E2 | 0.0 | 1/2- | |
| 814.50 4 | B G KL | 9/2- | 119.12 10 201.65 15 251.61 5 267.10 15 306.48 10 359.31 15 364.94 7 383.3 3 425.41 20 575.35 10 684.88 7 | ≤4 15 1 19 2 6 1 14.2 48 3 99 3 ≤2.5 7 2 16 3 100 5 | (M1) M1 M1(+E2) (E1) E2 M1+E2 (E2) E2 | 695.30 612.72 562.80 547.16 507.917 455.272 449.65 389.132 239.264 129.772 | (7/2)- (7/2)- 9/2- (11/2+) 5/2-,7/2- 5/2- (7/2)- 5/2- 5/2- 5/2- | |
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 821.79 2 | E G | 5/2+ | 389.803 4 432.647 22 | 100 10 15.3 42 | E2 | 389.132 | 5/2- | |
| 875 1 | KL | 5/2-,7/2- | ||||||
| 895.41 6 | B G M | 9/2- | 283.0 5 333.2 5 387.1 2 440.40 10 445.55 15 506.16 10 | 9 3 12 5 49 5 33 8 73 9 100.0 75 | 612.72 562.80 507.917 455.272 449.65 389.132 | (7/2)- 9/2- 5/2-,7/2- 5/2- (7/2)- 5/2- | ||
| 915 1 ? | L | |||||||
| 925 5 ? | K | (5/2-,7/2-) | ||||||
| 926.89 5 | EF J L | 1/2-,3/2- | 687.686 56 715.11 14 926.85 23 | 100 18 59 9 57 16 | 239.264 211.406 0.0 | 5/2- 3/2- 1/2- | ||
| 930.70 6 | B | (9/2)- | 235.4 3 383.3 3 422.4 3 475.38 15 481.17 10 498.6 2 691.6 3 800.90 10 | 9.6 18 ≤8.93 5.0 7 5.7 11 100 7 4.3 7 1.8 4 39 4 | E2(+M1) | 695.30 547.16 507.917 455.272 449.65 239.264 129.772 | (7/2)- (11/2+) 5/2-,7/2- 5/2- (7/2)- 5/2- 5/2- | |
| 971.3 8 | KLM | 5/2-,7/2- | ||||||
| 1016 5 | J | (5/2-,7/2-) | ||||||
| 1049.3 7 | LM | |||||||
| 1058 5 | K | 5/2-,7/2- | ||||||
| 1092.4 5 | I | (5/2 TO 13/2) | 529.6 5 | | 562.80 | 9/2- | ||
| 1096.2 10 | EFG J LM | 1/2-,3/2- | 1096.2 | | 0.0 | 1/2- | ||
| 1122.60 2 | E G J | 3/2+,5/2+ | 300.811 2 | 100 | E2(+M1) | 821.79 | 5/2+ | |
| 1132.40 2 | E I | 1/2-,3/2- | 392.860 19 892.57 26 1033.13 22 | 62 14 66 17 100 21 | 739.545 239.264 98.880 | 1/2-,3/2- 5/2- 3/2- | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 1151 6 | K | 1/2-,3/2- | ||||||
| 1155.8 5 | I L | |||||||
| 1160.38 3 | EF K | 1/2-,3/2- | 420.711 60 635.589 31 705.07 13 948.70 15 1030.60 22 1061.45 10 | 16 7 45 6 36 6 44 7 31 7 100 12 | 739.545 524.846 455.272 211.406 129.772 98.880 | 1/2-,3/2- 3/2- 5/2- 3/2- 5/2- 3/2- | ||
| 1166.4 6 | E | 1/2+,3/2+ | ||||||
| 1187.3 5 | O | 19/2+ | 429.0 5 559.6 5 | 64 8 100 8 | 758.3 627.8 | 15/2+ 17/2+ | ||
| 1189 6 | H KL | 5/2-,7/2- | ≥ 2.4×10-6 eV | |||||
| 1206.0 6 | O | 21/2+ | 578.1 5 | 100 | 627.8 | 17/2+ | ||
| 1271.0 3 | E | 1/2-,3/2- | ||||||
| 1287.7 4 | E K | 1/2-,3/2- | ||||||
| 1294 1 | F | 1/2-,3/2- | ||||||
| 1306 10 | M | |||||||
| 1312.7 7 | E J | 1/2+,3/2+ | ||||||
| 1320.8 4 | E | 1/2-,3/2- | ||||||
| 1334.7 4 | EF K | 1/2-,3/2- | ||||||
| 1346.9 6 | E | 1/2,3/2 | ||||||
| 1372.7 4 | E | 1/2-,3/2- | ||||||
| 1378 10 | K M | 11/2+,13/2+ | ||||||
| 1391.8 6 | O | 21/2- | 185.7 5 204.5 5 | 62 6 100 13 | 1206.0 1187.3 | 21/2+ 19/2+ | ||
| 1411.1 5 | E | 1/2-,3/2- | ||||||
| 1425.0 5 | EF | 1/2-,3/2- | ||||||
| 1438.3 4 | E | 1/2,3/2 | ||||||
| 1445.3 5 | EF K | 1/2-,3/2- | ||||||
| 1505 10 | M | |||||||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 1535.7 8 | O | 25/2- | 143.9 5 | 100 | 1391.8 | 21/2- | ||
| 1577 2 | F | 1/2-,3/2- | ||||||
| 1590 12 ? | K | |||||||
| 1681 3 | F M | 11/2+,13/2+ | ||||||
| 1766 2 | F | (1/2-,3/2-) | ||||||
| 1785 10 | J M | |||||||
| 1840 2 | F | 1/2-,3/2- | ||||||
| 1872 2 | F | (5/2-,7/2-) | ||||||
| 1899 1 | F | (9/2+) | ||||||
| 1911 10 | M | |||||||
| 1915.6 8 | O | (25/2+) | 709.6 5 | 100 | 1206.0 | 21/2+ | ||
| 1947.3 10 | O | 29/2- | 411.6 5 | 100 | 1535.7 | 25/2- | ||
| 1972 3 | M | 1/2-,3/2- | ||||||
| 2128 10 | M | 11/2+,13/2+ | ||||||
| 2291 10 | M | |||||||
| 2330 20 | J | |||||||
| 2390 20 | J | |||||||
| 2437 10 | M | |||||||
| 2592.6 11 | O | 33/2- | 645.3 5 | 100 | 1947.3 | 29/2- | ||
E(level): For the states connected by γ’s, E(level) are from Eγ using least-squares fit.
I(γ): Relative photon branching ratios renormalized to Iγ=100 for the strongest branching from each level.
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 1 - Kπ=1/2- band. Configuration=1/2-[530]. | |||||||
| 0.0 | 1/2- | STABLE | |||||
| 211.406 2 | 3/2- | 49 ps 8 | 211.407 2 | 100 | M1+E2 | 0.0 | 1/2- |
| 239.264 4 | 5/2- | 70 ps 9 | 28S 140.385 9 239.261 5 | 2.5 1 55 3 100 5 | M1+E2 E2 | 98.880 0.0 | 3/2- 1/2- |
| 695.30 6 | (7/2)- | 306.0 455.94 10 495.8 2 565.48 15 596.48 20 | 100 92 6 60 6 26 6 25 6 | [M1] M1(+E2) [E2] [M1] [E2] | 389.132 239.264 199.532 129.772 98.880 | 5/2- 5/2- 3/2- 5/2- 3/2- | |
| 814.50 4 | 9/2- | 119.12 10 201.65 15 251.61 5 267.10 15 306.48 10 359.31 15 364.94 7 383.3 3 425.41 20 575.35 10 684.88 7 | ≤4 15 1 19 2 6 1 14.2 48 3 99 3 ≤2.5 7 2 16 3 100 5 | (M1) M1 M1(+E2) (E1) E2 M1+E2 (E2) E2 | 695.30 612.72 562.80 547.16 507.917 455.272 449.65 389.132 239.264 129.772 | (7/2)- (7/2)- 9/2- (11/2+) 5/2-,7/2- 5/2- (7/2)- 5/2- 5/2- 5/2- | |
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 2 - Kπ=3/2- band. Configuration=3/2-[532]. | |||||||
| 98.880 2 | 3/2- | 0.170 ns 19 | |||||
| 389.132 4 | 5/2- | 9 ps 4 | 150.11 15 259.351 6 290.254 3 389 1 | 9 2 40 5 100 5 2.7 12 | [M1] M1(+E2) M1(+E2) E2 | 239.264 129.772 98.880 0.0 | 5/2- 5/2- 3/2- 1/2- |
| 612.72 8 | (7/2)- | 6 ps 3 | 223.7 3 373.39 15 401.30 15 513.6 3 | ≈0.91 100 27 27 9 2.7 9 | M1(+E2) [E2] | 389.132 239.264 211.406 98.880 | 5/2- 5/2- 3/2- 3/2- |
| 930.70 6 | (9/2)- | 235.4 3 383.3 3 422.4 3 475.38 15 481.17 10 498.6 2 691.6 3 800.90 10 | 9.6 18 ≤8.93 5.0 7 5.7 11 100 7 4.3 7 1.8 4 39 4 | E2(+M1) | 695.30 547.16 507.917 455.272 449.65 239.264 129.772 | (7/2)- (11/2+) 5/2-,7/2- 5/2- (7/2)- 5/2- 5/2- | |
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 3 - Kπ=5/2- band. Configuration=5/2-[532]. | |||||||
| 129.772 3 | 5/2- | 0.67 ns 3 | |||||
| 449.65 5 | (7/2)- | 60.4 211.3 239.21 319.90 7 350.90 10 | <15 2.7 1.3 100 5 10.6 15 | [M1,E2] [E2] M1+E2 [E2] | 389.132 239.264 129.772 98.880 | 5/2- 5/2- 5/2- 3/2- | |
| 562.80 5 | 9/2- | 14 ps 3 | 130.3 5 324 432.86 7 | 0.8 5 8.9 11 100 | [E1] E2 | 239.264 129.772 | 5/2- 5/2- |
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 4 - Kπ=3/2- band. Configuration=3/2-[541]. | |||||||
| 199.532 2 | 3/2- | 0.66 ns 14 | |||||
| 507.917 6 | 5/2-,7/2- | 9.5 ps 22 | 119.12 10 296.5 378.129 9 409.049 11 | ≤27 4.6 10 87 11 100 11 | [M1,E2] [E2] M1 E2 | 389.132 129.772 | 5/2- 5/2- |
| 765.8 9 | (7/2)- | ||||||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 5 - Kπ=9/2+ band. Configuration=9/2+[615]. | |||||||
| 1899 1 | (9/2+) | ||||||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 6 - νi13/2-1 sequence based on 259 LEVEL,α=+1/2. | |||||||
| 259.077 23 | 13/2+ | 4.010 d 5 % IT = 100 | |||||
| 627.8 5 | 17/2+ | 368.8 5 | 100 | 259.077 | 13/2+ | ||
| 1206.0 6 | 21/2+ | 578.1 5 | 100 | 627.8 | 17/2+ | ||
| 1915.6 8 | (25/2+) | 709.6 5 | 100 | 1206.0 | 21/2+ | ||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 7 - νi13/2-1 sequence based on 759 LEVEL,α=-1/2. | |||||||
| 758.3 5 | 15/2+ | ||||||
| 1187.3 5 | 19/2+ | 429.0 5 559.6 5 | 64 8 100 8 | 758.3 627.8 | 15/2+ 17/2+ | ||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 8 - Sequence on 21/2-. | |||||||
| 1391.8 6 | 21/2- | ||||||
| 1535.7 8 | 25/2- | 143.9 5 | 100 | 1391.8 | 21/2- | ||
| 1947.3 10 | 29/2- | 411.6 5 | 100 | 1535.7 | 25/2- | ||
| 2592.6 11 | 33/2- | 645.3 5 | 100 | 1947.3 | 29/2- | ||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
| 98.880 | 3/2- | 0.170 ns 19 | 98.857 10 | M1+E2 | -0.130 4 | 6.86 | B(E2)(W.u.)=11.1 15, B(M1)(W.u.)=0.0168 19, α=6.86 |
| 129.772 | 5/2- | 0.67 ns 3 | 30.876 6 | M1+E2 | -0.021 4 | 37.6 | B(E2)(W.u.)=4.8 19, B(M1)(W.u.)=0.0269 21, α=37.6 |
| 5/2- | 0.67 ns 3 | 129.735 10 | E2 | 1.732 | B(E2)(W.u.)=8.9 7, α=1.732 | ||
| 199.532 | 3/2- | 0.66 ns 14 | 100.652 3 | M1(+E2) | +0.02 23 | 6.54 | B(E2)(W.u.)=(0.05 +106-5), B(M1)(W.u.)=(0.0030 8), α=6.54 14 |
| 3/2- | 0.66 ns 14 | 199.533 2 | M1+E2 | +1.2 2 | 0.60 | B(E2)(W.u.)=4.5 13, B(M1)(W.u.)=0.00033 11, α=0.60 6 | |
| 211.406 | 3/2- | 49 ps 8 | 211.407 2 | M1+E2 | +0.38 3 | 0.737 | B(E2)(W.u.)=30 7, B(M1)(W.u.)=0.024 4, α=0.737 14 |
| 222.230 | 1/2- | 123.337 10 | M1(+E2) | 0.32 LT | 3.59 | α=3.59 9 | |
| 1/2- | 222.230 5 | M1 | 0.696 | α=0.696, α(K)=0.594, α(L)=0.098, α(M)=0.0225, α(N)=0.0074 | |||
| 239.264 | 5/2- | 70 ps 9 | 140.385 9 | M1+E2 | -0.17 4 | 2.49 | B(E2)(W.u.)=11 6, B(M1)(W.u.)=0.019 3, α=2.49 |
| 5/2- | 70 ps 9 | 239.261 5 | E2 | 0.198 | B(E2)(W.u.)=49 7, α=0.198 | ||
| 259.077 | 13/2+ | 4.010 d 5 % IT = 100 | 19.8 | [M4] | 6.10×108 | B(M4)(W.u.)=6.×101 3, α=6.10×108 21 | |
| 13/2+ | 4.010 d 5 % IT = 100 | 129.5 2 | M4 | 1135 | B(M4)(W.u.)=0.00107 9, α=1135 19 | ||
| 389.132 | 5/2- | 9 ps 4 | 150.11 15 | [M1] | 2.09 | B(M1)(W.u.)=0.030 15, α=2.09 | |
| 5/2- | 9 ps 4 | 259.351 6 | M1(+E2) | +0.01 3 | 0.455 | B(E2)(W.u.)=(0.015 +88-15), B(M1)(W.u.)=(0.026 12), α=0.455 | |
| 5/2- | 9 ps 4 | 290.254 3 | M1(+E2) | -0.47 7 | 0.293 | B(E2)(W.u.)=(38 20), B(M1)(W.u.)=(0.038 17), α=0.293 11 | |
| 5/2- | 9 ps 4 | 389 1 | E2 | 0.0471 | B(E2)(W.u.)=1.3 9, α=0.0471 8 | ||
| 419.702 | 3/2- | 54 ps 8 | 197.479 14 | M1(+E2) | 1.9 LT | 0.74 | B(E2)(W.u.)<37, B(M1)(W.u.)>0.00054, α=0.74 24 |
| 3/2- | 54 ps 8 | 320.819 3 | M1(+E2) | -0.12 5 | 0.252 | B(E2)(W.u.)=(0.07 6), B(M1)(W.u.)=(0.0013 3), α=0.252 5 | |
| 3/2- | 54 ps 8 | 419.705 4 | M1(+E2) | +0.17 2 | 0.1214 | B(E2)(W.u.)=(0.22 7), B(M1)(W.u.)=(0.0036 7), α=0.1214 18 | |
| 431.98 | 9/2+ | 172.906 3 | E2 | 0.596 | α=0.596 | ||
| 449.65 | (7/2)- | 211.3 | [M1,E2] | 0.5 | α=0.5 3 | ||
| (7/2)- | 239.21 | [E2] | 0.199 | α=0.199 | |||
| (7/2)- | 319.90 7 | M1+E2 | 1.5 3 | 0.135 | α=0.135 18 | ||
| (7/2)- | 350.90 10 | [E2] | 0.0626 | α=0.0626 | |||
| 455.272 | 5/2- | > 10.5 ps | 216.012 9 | M1(+E2) | 0.6 LT | 0.69 | B(E2)(W.u.)<60, α=0.69 7 |
| 5/2- | > 10.5 ps | 243.855 14 | M1 | 0.539 | B(M1)(W.u.)<0.017, α=0.539 | ||
| 5/2- | > 10.5 ps | 255.741 30 | (M1+E2) | 0.32 | α=0.32 16 | ||
| 5/2- | > 10.5 ps | 356.395 14 | M1 | 0.192 | B(M1)(W.u.)<0.013, α=0.192 | ||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
| 507.917 | 5/2-,7/2- | 9.5 ps 22 | 119.12 10 | [M1,E2] | 3.2 | B(E2)(W.u.)<3.9×103, B(M1)(W.u.)<0.14, α=3.2 9 | |
| 5/2-,7/2- | 9.5 ps 22 | 296.5 | [E2] | 0.102 | B(E2)(W.u.)=7 3, α=0.102 | ||
| 5/2-,7/2- | 9.5 ps 22 | 378.129 9 | M1 | 0.1635 | B(M1)(W.u.)=0.014 5, α=0.1635 | ||
| 5/2-,7/2- | 9.5 ps 22 | 409.049 11 | E2 | 0.0412 | B(E2)(W.u.)=29 10, α=0.0412 | ||
| 524.846 | 3/2- | 285.578 4 | M1+E2 | +0.14 14 | 0.345 | α=0.345 14 | |
| 3/2- | 395.071 3 | M1(+E2) | 0.49 +60-49 | 0.13 | α=0.13 4 | ||
| 3/2- | 425.978 7 | M1+E2 | -3.27 283 | 0.04 | α=0.04 7 | ||
| 3/2- | 524.846 4 | M1+E2 | +2.25 115 | 0.030 | α=0.030 14 | ||
| 547.16 | (11/2+) | 287.80 15 | (M1+E2) | 0.23 | α=0.23 12 | ||
| 562.80 | 9/2- | 14 ps 3 | 130.3 5 | [E1] | 0.208 | B(E1)(W.u.)=5.E-5 3, α=0.208 4 | |
| 9/2- | 14 ps 3 | 432.86 7 | E2 | 0.0356 | B(E2)(W.u.)=35 8, α=0.0356 | ||
| 590.902 | 3/2- | 368.671 3 | M1(+E2) | 0.14 LT | 0.174 | α=0.174 3 | |
| 3/2- | 391.377 10 | M1(+E2) | 0.14 LT | 0.1481 | α=0.1481 23 | ||
| 3/2- | 590.895 7 | M1(+E2) | 0.32 LT | 0.0488 | α=0.0488 17 | ||
| 612.72 | (7/2)- | 6 ps 3 | 373.39 15 | M1(+E2) | 0.11 | B(E2)(W.u.)<210, B(M1)(W.u.)<0.077, α=0.11 6 | |
| (7/2)- | 6 ps 3 | 401.30 15 | [E2] | 0.0434 | B(E2)(W.u.)=26 17, α=0.0434 | ||
| 667.0 | (9/2-) | 16 ps 4 | 428 | (E2) | 0.0366 | B(E2)(W.u.)=30 8, α=0.0366 | |
| 695.30 | (7/2)- | 306.0 | [M1] | 0.289 | α=0.289 | ||
| (7/2)- | 455.94 10 | M1(+E2) | 0.07 | α=0.07 4 | |||
| (7/2)- | 495.8 2 | [E2] | 0.0253 | α=0.0253 | |||
| (7/2)- | 565.48 15 | [M1] | 0.0565 | α=0.0565 | |||
| (7/2)- | 596.48 20 | [E2] | 0.01632 | α=0.01632 | |||
| 739.545 | 1/2-,3/2- | 319.843 4 | E2(+M1) | 1.23 GE | 0.12 | α=0.12 4 | |
| 793.0 | 3/2- | 793 | M1+E2 | 0.016 | B(E2)(W.u.)=1.1 2, B(M1)(W.u.)=0.0036 6, α=0.016 8 | ||
| 814.50 | 9/2- | 119.12 10 | (M1) | 4.04 | α=4.04 | ||
| 9/2- | 201.65 15 | M1 | 0.912 | α=0.912 | |||
| 9/2- | 251.61 5 | M1(+E2) | 0.33 | α=0.33 17 | |||
| 9/2- | 267.10 15 | (E1) | 0.0344 | α=0.0344 | |||
| 9/2- | 359.31 15 | E2 | 0.0586 | α=0.0586 | |||
| 9/2- | 364.94 7 | M1+E2 | 1.5 +5-3 | 0.094 | α=0.094 14 | ||
| 9/2- | 575.35 10 | (E2) | 0.01773 | α=0.01773 | |||
| 9/2- | 684.88 7 | E2 | 0.01198 | α=0.01198 | |||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
| 821.79 | 5/2+ | 389.803 4 | E2 | 0.0469 | α=0.0469 | ||
| 930.70 | (9/2)- | 481.17 10 | E2(+M1) | 0.06 | α=0.06 3 | ||
| 1122.60 | 3/2+,5/2+ | 300.811 2 | E2(+M1) | 2.1 +17-4 | 0.136 | α=0.136 25 |
Additional Level Data and Comments:
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 0.0 | 1/2- | STABLE | μ=+0.60952 6 (1951Pr02,2011StZZ) Change of the mean-square charge radius (rel to 198Pt) Δ<r2>≈-0.1 (fm)2 (1988Ro20). E(level): Kπ=1/2- band. Configuration=1/2-[530]. Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 98.880 | 3/2- | 0.170 ns 19 | μ=-0.62 6 (1967Ag01,2011StZZ) E(level): Kπ=3/2- band. Configuration=3/2-[532]. Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 129.772 | 5/2- | 0.67 ns 3 | μ=+0.90 6 (1974Ru03,2011StZZ) E(level): Kπ=5/2- band. Configuration=5/2-[532]. Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 199.532 | 3/2- | 0.66 ns 14 | E(level): Kπ=3/2- band. Configuration=3/2-[541]. Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 211.406 | 3/2- | 49 ps 8 | μ=+0.16 3 (1972Va16,2011StZZ) E(level): Kπ=1/2- band. Configuration=1/2-[530]. Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 222.230 | 1/2- | XREF: J(220). Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. | |
| 239.264 | 5/2- | 70 ps 9 | μ=+0.52 5 (1973Ga31,2011StZZ), +0.64 9 (1994La02,2011StZZ). E(level): μ=+0.52 5 (1973Ga31,2011StZZ), +0.64 9 (1994La02,2011StZZ). Kπ=1/2- band. Configuration=1/2-[530]. Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 259.077 | 13/2+ | 4.010 d 5 % IT = 100 | μ=-0.606 15 (1972Ba22,2011StZZ), Q=+1.4 6 (1985Ed05,2011StZZ) μ=- from 1991Sc28. E(level): μ=- from 1991Sc28. νi13/2-1 sequence based on 259 LEVEL,α=+1/2. |
| 389.132 | 5/2- | 9 ps 4 | μ=+0.39 10 (1994La02,2011StZZ). E(level): μ=+0.39 10 (1994La02,2011StZZ). Kπ=3/2- band. Configuration=3/2-[532]. Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 419.702 | 3/2- | 54 ps 8 | Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 449.65 | (7/2)- | E(level): Kπ=5/2- band. Configuration=5/2-[532]. | |
| 455.272 | 5/2- | > 10.5 ps | μ=+1.6 6 (1994La02,2011StZZ). E(level): μ=+1.6 6 (1994La02,2011StZZ). Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 507.917 | 5/2-,7/2- | 9.5 ps 22 | μ=+0.55 8 (1994La02,2011StZZ). E(level): μ=+0.55 8 (1994La02,2011StZZ). Kπ=3/2- band. Configuration=3/2-[541]. |
| 524.846 | 3/2- | XREF: J(524). Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. | |
| 544.1 | (5/2-) | > 2.8 ps | μ=+1.5 4 (1994La02,2011StZZ). E(level): μ=+1.5 4 (1994La02,2011StZZ). Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. |
| 562.80 | 9/2- | 14 ps 3 | μ=+1.55 12 (1994La02,2011StZZ). E(level): μ=+1.55 12 (1994La02,2011StZZ). Kπ=5/2- band. Configuration=5/2-[532]. |
| 590.902 | 3/2- | Jπ(level): Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) supports given values. | |
| 612.72 | (7/2)- | 6 ps 3 | μ=+1.4 4 (1994La02,2011StZZ). E(level): μ=+1.4 4 (1994La02,2011StZZ). Kπ=3/2- band. Configuration=3/2-[532]. |
| 627.8 | 17/2+ | E(level): νi13/2-1 sequence based on 259 LEVEL,α=+1/2. | |
| 630.147 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) favors Jπ=1/2-. | |
| 667.0 | (9/2-) | 16 ps 4 | μ=+1.52 16 (1994La02,2011StZZ). E(level): μ=+1.52 16 (1994La02,2011StZZ). |
| 678.3 | 5/2-,7/2- | > 72.8 ps | μ=+1.23 28 (1994La02,2011StZZ). E(level): μ=+1.23 28 (1994La02,2011StZZ). |
| 695.30 | (7/2)- | E(level): Kπ=1/2- band. Configuration=1/2-[530]. | |
| 758.3 | 15/2+ | E(level): νi13/2-1 sequence based on 759 LEVEL,α=-1/2. | |
| 765.8 | (7/2)- | E(level): Kπ=3/2- band. Configuration=3/2-[541]. | |
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 814.50 | 9/2- | XREF: K(817)L(816). E(level): Kπ=1/2- band. Configuration=1/2-[530]. | |
| 875 | 5/2-,7/2- | XREF: K(883). | |
| 926.89 | 1/2-,3/2- | XREF: F(930). Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). Analysis for multi-J supersymmetry scheme of interacting boson-fermion model (1987Ve09) favors Jπ=1/2-. | |
| 930.70 | (9/2)- | E(level): Kπ=3/2- band. Configuration=3/2-[532]. | |
| 971.3 | 5/2-,7/2- | XREF: K(980). | |
| 1049.3 | XREF: M(1043). | ||
| 1096.2 | 1/2-,3/2- | XREF: F(1100)J(1106)L(1098)M(1107). Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1132.40 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1155.8 | XREF: L(1156). | ||
| 1160.38 | 1/2-,3/2- | XREF: K(1151). | |
| 1166.4 | 1/2+,3/2+ | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1187.3 | 19/2+ | E(level): νi13/2-1 sequence based on 759 LEVEL,α=-1/2. | |
| 1189 | 5/2-,7/2- | ≥ 2.4×10-6 eV | XREF: H(1180). |
| 1206.0 | 21/2+ | E(level): νi13/2-1 sequence based on 259 LEVEL,α=+1/2. | |
| 1271.0 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1287.7 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1312.7 | 1/2+,3/2+ | XREF: J(1300). Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1320.8 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1334.7 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1346.9 | 1/2,3/2 | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1372.7 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1391.8 | 21/2- | E(level): Sequence on 21/2-. | |
| 1411.1 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1425.0 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1438.3 | 1/2,3/2 | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 1445.3 | 1/2-,3/2- | Jπ(level): From average resonance neutron capture measurements: ratios of reduced primary γ-ray intensities observed in 2- and 24-keV average neutron energy in 194Pt(n,γ). | |
| 1535.7 | 25/2- | E(level): Sequence on 21/2-. | |
| 1899 | (9/2+) | E(level): Kπ=9/2+ band. Configuration=9/2+[615]. | |
| 1915.6 | (25/2+) | E(level): νi13/2-1 sequence based on 259 LEVEL,α=+1/2. | |
| 1947.3 | 29/2- | E(level): Sequence on 21/2-. | |
| 2592.6 | 33/2- | E(level): Sequence on 21/2-. |
| E(level) | E(gamma) | Comments |
| 98.880 | 98.857 | E(γ): from 1972HsZX in 195Au ε decay (186.01 d) |
| 129.772 | 30.876 | E(γ): from 1972HsZX in 195Au ε decay (186.01 d) I(γ): from 195Au ε decay (186.01 d). | 129.735 | E(γ): from 1972HsZX in 195Au ε decay (186.01 d) I(γ): from 195Au ε decay (186.01 d). |
| 199.532 | 100.652 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). | 199.533 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| 211.406 | 211.407 | E(γ): From 194Pt(n,γ). |
| 222.230 | 123.337 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). | 222.230 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| 239.264 | 28 | E(γ): From Coulomb excitation. I(γ): From 195Pt IT decay (4.010 d). | 140.385 | E(γ): From 194Pt(n,γ). I(γ): From 195Pt IT decay (4.010 d). M(γ): From 195Pt IT decay (4.010 d). | 239.261 | E(γ): From 194Pt(n,γ). I(γ): From 195Pt IT decay (4.010 d). M(γ): From Coulomb excitation. |
| 259.077 | 19.8 | I(γ): From 195Pt IT decay (4.010 d). M(γ): From ΔJ and Δπ between γ-ray transition levels. | 129.5 | E(γ): from E(level) difference. From 195Pt IT decay (4.010 d). I(γ): From 195Pt IT decay (4.010 d). M(γ): From 195Pt IT decay (4.010 d). |
| 389.132 | 150.11 | M(γ): From ΔJ and Δπ between γ-ray transition levels. | 259.351 | E(γ): From 194Pt(n,γ). | 290.254 | E(γ): From 194Pt(n,γ). | 389 | E(γ): From Coulomb excitation. I(γ): from Iγ(389γ)/Iγ(290γ)=0.027 12 in Coul. ex. M(γ): From Coulomb excitation. |
| 419.702 | 197.479 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). | 320.819 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). | 419.705 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). |
| 431.98 | 172.906 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). |
| 449.65 | 60.4 | E(γ): from E(level) difference | 211.3 | M(γ): From ΔJ and Δπ between γ-ray transition levels. | 239.21 | M(γ): From ΔJ and Δπ between γ-ray transition levels. | 350.90 | M(γ): From ΔJ and Δπ between γ-ray transition levels. |
| E(level) | E(gamma) | Comments |
| 455.272 | 216.012 | E(γ): From 194Pt(n,γ). | 243.855 | E(γ): From 194Pt(n,γ). | 255.741 | E(γ): From 194Pt(n,γ). | 325.18 | E(γ): seen in (n,γ), but energy is not consistent with placement from 455 level; no 325γ seen in (n,n’γ). Placement in β- decay may be wrong. | 356.395 | E(γ): From 194Pt(n,γ). |
| 507.917 | 119.12 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 296.5 | E(γ): from E(level) difference I(γ): from Coul. ex. | 378.129 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 409.049 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| 524.846 | 285.578 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From Coulomb excitation. | 313.449 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 395.071 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). | 425.978 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From Coulomb excitation. | 524.846 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From Coulomb excitation. |
| 544.1 | 305 | E(γ): a 305γ deexcites the 695 level in β- decay and (n,n’γ).. From Coulomb excitation. | 333 | E(γ): From Coulomb excitation. | 414 | E(γ): From Coulomb excitation. | 445.2 | E(γ): From 195Pt(n,n’γ). I(γ): From 195Pt(n,n’γ). | 544.2 | E(γ): From 195Pt(n,n’γ). I(γ): From 195Pt(n,n’γ). |
| 562.80 | 130.3 | M(γ): From ΔJ and Δπ between γ-ray transition levels. | 324 | E(γ): From Coulomb excitation. I(γ): from Iγ(324γ)/Iγ(432γ)=0.089 11 in Coul. ex. |
| 590.902 | 368.671 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). | 379.503 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 391.377 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 590.895 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). |
| E(level) | E(gamma) | Comments |
| 630.147 | 407.910 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 418.741 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 430.620 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 531.263 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 629.86 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| 632.1 | 392.8 | E(γ): From Coulomb excitation. |
| 664.205 | 424.944 | E(γ): From 194Pt(n,γ). I(γ): Iγ(425γ):Iγ(453γ):Iγ(465γ):Iγ(534γ)=26:17:24:33 reported in (n,n’γ). From 194Pt(n,γ). | 452.799 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 464.674 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 534.418 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| 667.0 | 428 | E(γ): From Coulomb excitation. M(γ): From Coulomb excitation. | 537 | E(γ): From Coulomb excitation. I(γ): from Iγ(537γ)/Iγ(428γ)=0.19 3 (Coul. ex.) |
| 678.3 | 439 | E(γ): From Coulomb excitation. |
| 695.30 | 306.0 | I(γ): Iγ(306γ):Iγ(456γ):Iγ(496γ):Iγ(565γ)=100:73:32:65 in (n,n’γ) suggest that perhaps too much of the 306γ intensity in β- decay is assigned to this level. M(γ): From ΔJ and Δπ between γ-ray transition levels. | 495.8 | M(γ): From ΔJ and Δπ between γ-ray transition levels. | 565.48 | M(γ): From ΔJ and Δπ between γ-ray transition levels. | 596.48 | M(γ): From ΔJ and Δπ between γ-ray transition levels. |
| 739.545 | 319.843 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). | 640.33 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 739.74 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| 758.3 | 499.2 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) |
| 793.0 | 793 | E(γ): From Coulomb excitation. M(γ): From Coulomb excitation. |
| 814.50 | 119.12 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 383.3 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
| 821.79 | 389.803 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). | 432.647 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| E(level) | E(gamma) | Comments |
| 926.89 | 687.686 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 715.11 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 926.85 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| 930.70 | 383.3 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
| 1092.4 | 529.6 | E(γ): From Coulomb excitation. |
| 1096.2 | 1096.2 | E(γ): From 195Pt(n,n’γ). |
| 1122.60 | 300.811 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). M(γ): From 194Pt(n,γ). |
| 1132.40 | 392.860 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 892.57 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 1033.13 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| 1160.38 | 420.711 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 635.589 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 705.07 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 948.70 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 1030.60 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). | 1061.45 | E(γ): From 194Pt(n,γ). I(γ): From 194Pt(n,γ). |
| 1187.3 | 429.0 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) | 559.6 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) |
| 1206.0 | 578.1 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) |
| 1391.8 | 185.7 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) | 204.5 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) |
| 1535.7 | 143.9 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) |
| 1915.6 | 709.6 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) |
| 1947.3 | 411.6 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) |
| 2592.6 | 645.3 | E(γ): From 192Os(7Li,p3nγ) I(γ): From 192Os(7Li,p3nγ) |
Levels: For multi-J supersymmetry scheme of interacting boson-fermion model, see 1986Ma57, 1983Ve02, and 1987Ve09.
Levels: For Nilsson model configuration, see 1978Be09 and 1976Ya07.
Gammas: All data are from 195Ir β- decay (3.67 h), except as noted.