**ADOPTED LEVELS, GAMMAS for ^{189}Pt**

__Authors:__ T.D. Johnson, Balraj Singh **|** __Citation:__ Nucl. Data Sheets 142, 1 (2017) **|** __Cutoff date:__ 15-Apr-2017

Full ENSDF file | Adopted Levels (PDF version)

Q(β-)=-2887 keV 22 | S(n)= 6720 keV 11 | S(p)= 5413 keV 14 | Q(α)= 3912 keV 10 | ||

Reference: 2017WA10 |

References: | |||

A | ^{189}Au ε decay (28.7 M) | B | ^{189}Au ε decay (4.59 M) |

C | ^{176}Yb(^{18}O,5nγ) | D | ^{188}Os(α,3nγ),^{191}Ir(p,3nγ) |

E | ^{190}Pt(p,d) |

E(level) (keV) | XREF | J^{π}(level) | T_{1/2}(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |

0.0 | ABCDE | 3/2- | 10.87 h 12 % ε = 100 | |||||

6.40 3 | ABCD | 5/2- | 6.40 4 S | 100 | [M1] | 0.0 | 3/2- | |

45.78 25 | A E | (1/2)- | 39.47 3 45.69 3 | 14.4 23 100 25 | E2 M1+E2 | 6.40 0.0 | 5/2- 3/2- | |

88.30 3 | A E | 3/2- | 42.75 5 ?82.2 5 88.41 3 | | M1+E2 M1+E2 M1+E2 | 45.78 6.40 0.0 | (1/2)- 5/2- 3/2- | |

172.79 6 | BCDE | 9/2- | 464 ns 25 % IT = 100 | 166.40 5 | 100 | E2 | 6.40 | 5/2- |

191.4 2 | BCDE | (13/2+) | 143 µs 5 % IT = 100 | 18.7 9 S | 100 | [M2] | 172.79 | 9/2- |

202.2 5 | D | (11/2+) | 11.3S | | 191.4 | (13/2+) | ||

222.30 4 | A | (3/2,5/2)- | 134.26 4 176.1 5 215.68 5 221.95 16 | 24 4 62 9 100 12 | M1+E2 M1+E2 E2 | 88.30 45.78 6.40 0.0 | 3/2- (1/2)- 5/2- 3/2- | |

237.4 1 | A CD | (9/2)- | 231.0 1 | 100 | E2 | 6.40 | 5/2- | |

261 5 | E | 1/2-,3/2- | ||||||

285 5 | E | |||||||

348.45 5 | A E | (5/2,3/2)- | 110.8 5 ?126.31 5 259.68 10 302.4 5 ?342.0 5 348.15 15 | 4 1 8.8 12 13 4 20 4 100 7 | (E2) M1+E2 M1+E2 M1(+E2) | 237.4 222.30 88.30 45.78 6.40 0.0 | (9/2)- (3/2,5/2)- 3/2- (1/2)- 5/2- 3/2- | |

356.72 23 | CD | (9/2-) | 350.3 3 | 100 | 6.40 | 5/2- | ||

447.67 8 | A E | (3/2,5/2)- | 225.7 5 359.4 5 441.04 14 447.77 9 | 20 4 8 3 69 8 100 13 | M1(+E2) M1+E2 M1(+E2) | 222.30 88.30 6.40 0.0 | (3/2,5/2)- 3/2- 5/2- 3/2- | |

E(level) (keV) | XREF | J^{π}(level) | T_{1/2}(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |

493.3 4 | B DE | 11/2- | 321.1 5 | 100 | M1+E2 | 172.79 | 9/2- | |

499.2 2 | CD | (17/2+) | 211.4 ps 55 | 307.8 1 | 100 | E2 | 191.4 | (13/2+) |

529.62 11 | A | (1/2,3/2,5/2)- | 484.2 5 523.4 5 529.59 11 | 13 4 13 7 100 18 | M1(+E2) | 45.78 6.40 0.0 | (1/2)- 5/2- 3/2- | |

531.3 3 | CD | (15/2+) | 329.2 5 339.9 1 | 100 | D+Q | 202.2 191.4 | (11/2+) (13/2+) | |

574 5 | E | 1/2-,3/2- | ||||||

608.6 2 | CD | (13/2-) | 251.9 3 371.2 1 | 11 4 100 5 | (E2) | 356.72 237.4 | (9/2-) (9/2)- | |

653.8 2 | CD | (15/2+) | 462.4 1 | 100 | D+Q | 191.4 | (13/2+) | |

712.0 2 | CD | (13/2-) | 539.5 3 | 100 | (E2) | 172.79 | 9/2- | |

843.7 6 | D | (13/2-) | 487.0 5 | 100 | 356.72 | (9/2-) | ||

902.9 7 | D | 409.6 5 | | 493.3 | 11/2- | |||

944.0 2 | CD | (17/2+) | 290.2 5 412.7 1 444.8 5 | 100 15 30 9 | D+Q (E2) | 653.8 531.3 499.2 | (15/2+) (15/2+) (17/2+) | |

955.0 2 | CD | (21/2+) | 175.4 ps 49 | 455.8 1 | 100 | (E2) | 499.2 | (17/2+) |

983.5 3 | CD | (19/2+) | 452.2 1 484.3 3 | 100 15 51 8 | (E2) D+Q | 531.3 499.2 | (15/2+) (17/2+) | |

1048.5 7 | D | (15/2-) | 555.2 5 | 100 | 493.3 | 11/2- | ||

1081.1 2 | CD | (17/2-) | 472.4 1 | 100 | (E2) | 608.6 | (13/2-) | |

1160.87 14 | A | (3/2+) | 631.2 9 713.24 17 812.8 3 1071.5 6 1160.6 3 | 12.1 23 100 14 63 9 27 5 35 5 | E1 E1 E1 E1 E1 | 529.62 447.67 348.45 88.30 0.0 | (1/2,3/2,5/2)- (3/2,5/2)- (5/2,3/2)- 3/2- 3/2- | |

1185.31 20 | CD | (19/2+) | 531.5 1 686.1 1 | 40 6 100 5 | (E2) D+Q | 653.8 499.2 | (15/2+) (17/2+) | |

1361.5 2 | CD | (17/2-) | 280.4 3 649.5 1 707.7 1 862.3 1 | 17 5 56 9 64 10 100 15 | (E2) Q D D | 1081.1 712.0 653.8 499.2 | (17/2-) (13/2-) (15/2+) (17/2+) | |

E(level) (keV) | XREF | J^{π}(level) | T_{1/2}(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |

1414.0 6 | D | 470.0 5 | | 944.0 | (17/2+) | |||

1415.9 8 | D | (17/2-) | 572.2 5 | | 843.7 | (13/2-) | ||

1444.0 3 | CD | (21/2+) | 460.5 3 500.0 1 944.8 5 | 30 10 100 16 10 4 | D+Q (E2) Q | 983.5 944.0 499.2 | (19/2+) (17/2+) (17/2+) | |

1490.4 2 | CD | (19/2-) | 128.9 1 409.3 1 536 1 | 35 6 100 5 | (E2) (E2) | 1361.5 1081.1 955.0 | (17/2-) (17/2-) (21/2+) | |

1512.1 2 | CD | (21/2-) | 21.7S 150.6 3 326.8 1 557.1 1 | 10 4 84 5 100 5 | (E2) D D | 1490.4 1361.5 1185.31 955.0 | (19/2-) (17/2-) (19/2+) (21/2+) | |

1529.3 3 | CD | (25/2+) | 574.3 1 | 100 | (E2) | 955.0 | (21/2+) | |

1555.7 3 | CD | (23/2+) | 572.2 3 600.7 5 | 100 16 22 7 | (E2) D+Q | 983.5 955.0 | (19/2+) (21/2+) | |

1695.7 3 | C | (23/2-) | 183.6 1 740.7 3 | 100 6 4 2 | D+Q | 1512.1 955.0 | (21/2-) (21/2+) | |

1714.3 3 | CD | (25/2-) | 18.6S 202.2 1 | 100 | (E2) | 1695.7 1512.1 | (23/2-) (21/2-) | |

1727.4 4 | D | (23/2+) | 542.1 5 772.4 5 | | 1185.31 955.0 | (19/2+) (21/2+) | ||

2009.5 3 | C | (25/2+) | 565.5 1 1054.5 5 | <100 14 5 | Q | 1444.0 955.0 | (21/2+) (21/2+) | |

2055.2 3 | CD | (27/2-) | 340.9 1 | 100 | D+Q | 1714.3 | (25/2-) | |

2189.5 3 | CD | (29/2+) | 660.2 1 | 100 | Q | 1529.3 | (25/2+) | |

2219.4 4 | CD | (27/2+) | 663.7 3 | 100 | Q | 1555.7 | (23/2+) | |

2291.4 3 | CD | (29/2-) | 236.2 3 577.1 1 | 15 3 100 6 | D+Q (E2) | 2055.2 1714.3 | (27/2-) (25/2-) | |

2303.7 3 | C | (29/2-) | 248.5 3 589.4 1 | 22 4 100 6 | D+Q (E2) | 2055.2 1714.3 | (27/2-) (25/2-) | |

E(level) (keV) | XREF | J^{π}(level) | T_{1/2}(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |

2539.7 4 | C | (27/2+) | 1010.4 5 | 100 | D+Q | 1529.3 | (25/2+) | |

2620.4 3 | C | (31/2-) | 316.7 1 329.0 3 565.2 1 | 100 15 42 7 87 13 | D+Q D+Q (E2) | 2303.7 2291.4 2055.2 | (29/2-) (29/2-) (27/2-) | |

2635.5 3 | C | (29/2+) | 626.0 1 1106.2 3 | 100 5 17 6 | Q Q | 2009.5 1529.3 | (25/2+) (25/2+) | |

2688.4 3 | CD | (31/2-) | 397.0 3 633.2 1 | 63 10 100 15 | D+Q Q | 2291.4 2055.2 | (29/2-) (27/2-) | |

2729.4 3 | C | (29/2+) | 189.7 5 539.9 3 1200.1 5 | 100 32 41 14 | (E2) Q | 2539.7 2189.5 1529.3 | (27/2+) (29/2+) (25/2+) | |

2818.6 5 | C | 763.4 5 | 100 | 2055.2 | (27/2-) | |||

2839.8 3 | C | (33/2-) | 536.1 1 548.4 3 | 100 15 46 8 | (E2) (E2) | 2303.7 2291.4 | (29/2-) (29/2-) | |

2864.7 3 | CD | (33/2+) | 675.2 1 | 100 | Q | 2189.5 | (29/2+) | |

2874.2 3 | C | (33/2-) | 582.8 1 | 100 | (E2) | 2291.4 | (29/2-) | |

2931.6 4 | C | (31/2+) | 712.2 3 | 100 | Q | 2219.4 | (27/2+) | |

2979.3 3 | C | (31/2+) | 249.9 3 439.6 5 759.9 5 | <100 19 6 | Q | 2729.4 2539.7 2219.4 | (29/2+) (27/2+) (27/2+) | |

3066.2 4 | C | (33/2+) | 876.7 3 | 100 | Q | 2189.5 | (29/2+) | |

3201.0 3 | C | (33/2+) | 134.8 5 565.5 1 | 100 | (E2) | 3066.2 2635.5 | (33/2+) (29/2+) | |

3292.4 3 | C | (35/2-) | 91.4 3 418.2 3 452.6 3 473.8 5 604.0 1 672.0 1 | 15 5 15 5 20 7 54 8 100 5 | D D+Q D+Q Q Q | 3201.0 2874.2 2839.8 2818.6 2688.4 2620.4 | (33/2+) (33/2-) (33/2-) (31/2-) (31/2-) | |

3376.4 4 | C | (37/2+) | 511.7 3 | 100 | (E2) | 2864.7 | (33/2+) | |

E(level) (keV) | XREF | J^{π}(level) | T_{1/2}(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |

3420.1 3 | C | (35/2+) | 219.1 3 353.9 5 440.8 5 580.3 3 | 100 16 42 14 74 23 | D+Q D | 3201.0 3066.2 2979.3 2839.8 | (33/2+) (33/2+) (31/2+) (33/2-) | |

3452.7 4 | C | (37/2-) | 612.9 3 | 100 | Q | 2839.8 | (33/2-) | |

3455.4 3 | C | (35/2+) | 163.0 5 254.4 3 476.1 3 523.8 5 | 37 11 55 16 100 15 27 8 | D+Q (E2) | 3292.4 3201.0 2979.3 2931.6 | (35/2-) (33/2+) (31/2+) (31/2+) | |

3574.1 4 | C | (37/2-) | 699.9 3 | 100 | Q | 2874.2 | (33/2-) | |

3582.3 3 | C | (37/2+) | 381.3 1 717.6 3 | 100 16 41 13 | (E2) | 3201.0 2864.7 | (33/2+) (33/2+) | |

3640.7 3 | C | (39/2+) | 58.4S 185.3 1 188.0 3 220.6 1 | 100 15 25 8 67 11 | (E2) D (E2) | 3582.3 3455.4 3452.7 3420.1 | (37/2+) (35/2+) (37/2-) (35/2+) | |

3648.7 3 | C | (39/2-) | 356.3 1 | 100 | (E2) | 3292.4 | (35/2-) | |

3672.9 6 | C | 808.2 5 | | 2864.7 | (33/2+) | |||

3809.3 3 | C | (41/2-) | 160.6 1 | 100 | D+Q | 3648.7 | (39/2-) | |

3848.6 3 | C | (43/2+) | 207.9 1 | 100 | (E2) | 3640.7 | (39/2+) | |

3947.0 5 | C | (41/2+) | 570.6 3 | 100 | (E2) | 3376.4 | (37/2+) | |

3976.0 6 | C | 393.7 5 | | 3582.3 | (37/2+) | |||

4168.6 6 | C | (41/2-) | 715.9 5 | 100 | Q | 3452.7 | (37/2-) | |

4367.8 3 | C | (47/2+) | 519.2 1 | 100 | (E2) | 3848.6 | (43/2+) | |

4437.2 3 | C | (43/2-) | 627.9 1 788.5 5 | 100 15 16 5 | D+Q Q | 3809.3 3648.7 | (41/2-) (39/2-) | |

4647.4 7 | C | (45/2+) | 700.4 5 | 100 | Q | 3947.0 | (41/2+) | |

4686.2 3 | C | (45/2+) | 318.4 3 837.6 1 | 19 6 100 15 | D+Q | 4367.8 3848.6 | (47/2+) (43/2+) | |

4688.1 3 | C | (45/2-) | 250.9 1 | 100 | D+Q | 4437.2 | (43/2-) | |

E(level) (keV) | XREF | J^{π}(level) | T_{1/2}(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |

4708.4 3 | C | (47/2+) | 340.6 3 859.8 1 | 49 8 100 16 | Q | 4367.8 3848.6 | (47/2+) (43/2+) | |

4795.3 3 | C | (45/2-) | 986.0 1 | 100 | Q | 3809.3 | (41/2-) | |

4848.7 4 | C | (45/2-) | 1039.4 3 | 100 | Q | 3809.3 | (41/2-) | |

4879.3 3 | C | (49/2+) | 170.9 3 193.1 1 511.5 3 | 41 13 100 16 58 9 | D+Q (E2) D+Q | 4708.4 4686.2 4367.8 | (47/2+) (45/2+) (47/2+) | |

5042.3 3 | C | (49/2-) | 193.6 5 247.0 3 333.9 3 354.2 3 | 23 7 100 15 90 14 98 15 | (E2) (E2) D (E2) | 4848.7 4795.3 4708.4 4688.1 | (45/2-) (45/2-) (47/2+) (45/2-) | |

5353.7 3 | C | (53/2+) | 474.4 1 | 100 | (E2) | 4879.3 | (49/2+) | |

5464.5 9 | C | (49/2+) | 817.1 5 | 100 | Q | 4647.4 | (45/2+) | |

5502.1 4 | C | (53/2-) | 459.8 1 | 100 | (E2) | 5042.3 | (49/2-) | |

6474.8 5 | C | (57/2-) | 972.7 3 | 100 | Q | 5502.1 | (53/2-) | |

6476.5 4 | C | (55/2+) | 1122.8 1 | 100 | D+Q | 5353.7 | (53/2+) | |

6761.9 7 | C | 287.1 5 | 100 | 6474.8 | (57/2-) | |||

6841.6 5 | C | (57/2+) | 365.1 3 | 100 | D+Q | 6476.5 | (55/2+) | |

7272.3 7 | C | 430.7 5 | 100 | 6841.6 | (57/2+) | |||

7358.0 9 | C | 596.1 5 | | 6761.9 | ||||

7582.5 7 | C | 740.9 5 | | 6841.6 | (57/2+) | |||

7764.8 9 | C | 492.5 5 | | 7272.3 | ||||

8135.3 10 | C | 777.3 5 | | 7358.0 | ||||

8843.1 11 | C | 707.8 5 | | 8135.3 |

E(level): From least square fit to Eγ values

J^{π}(level): Suggested values from ^{188}Os(α,3nγ),^{191}Ir(p,3nγ), up to 2865 keV, except where noted. These values are derived from γγ(θ), excitation functions, and Nilsson model assumptions. These are in general agreement with Jπ values suggested from multipolarity assignments and yrast arguments from (^{18}O,5nγ), which were used for Jπ assignments beyond 2865 keV.

E(γ): From (^{18}O,5nγ) (2009Hu12) except where noted

I(γ): From ^{176}Yb(^{18}O,5nγ) unless otherwise noted

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) | I(γ) | M(γ) | Final Levels | |

Band 1 - γ cascade based on (39/2^{+}). | |||||||

3640.7 3 | (39/2+) | ||||||

3848.6 3 | (43/2+) | 207.9 1 | 100 | (E2) | 3640.7 | (39/2+) | |

4367.8 3 | (47/2+) | 519.2 1 | 100 | (E2) | 3848.6 | (43/2+) | |

4879.3 3 | (49/2+) | 170.9 3 193.1 1 511.5 3 | 41 13 100 16 58 9 | D+Q (E2) D+Q | 4708.4 4686.2 4367.8 | (47/2+) (45/2+) (47/2+) | |

5353.7 3 | (53/2+) | 474.4 1 | 100 | (E2) | 4879.3 | (49/2+) | |

6476.5 4 | (55/2+) | 1122.8 1 | 100 | D+Q | 5353.7 | (53/2+) | |

6841.6 5 | (57/2+) | 365.1 3 | 100 | D+Q | 6476.5 | (55/2+) | |

7272.3 7 | 430.7 5 | 100 | 6841.6 | (57/2+) | |||

7764.8 9 | 492.5 5 | | 7272.3 | ||||

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) | I(γ) | M(γ) | Final Levels | |

Band 2 - 13/2^{+} band, α=+1/2 | |||||||

191.4 2 | (13/2+) | 143 µs 5 % IT = 100 | |||||

499.2 2 | (17/2+) | 211.4 ps 55 | 307.8 1 | 100 | E2 | 191.4 | (13/2+) |

955.0 2 | (21/2+) | 175.4 ps 49 | 455.8 1 | 100 | (E2) | 499.2 | (17/2+) |

1529.3 3 | (25/2+) | 574.3 1 | 100 | (E2) | 955.0 | (21/2+) | |

2189.5 3 | (29/2+) | 660.2 1 | 100 | Q | 1529.3 | (25/2+) | |

2864.7 3 | (33/2+) | 675.2 1 | 100 | Q | 2189.5 | (29/2+) | |

3376.4 4 | (37/2+) | 511.7 3 | 100 | (E2) | 2864.7 | (33/2+) | |

3947.0 5 | (41/2+) | 570.6 3 | 100 | (E2) | 3376.4 | (37/2+) | |

4647.4 7 | (45/2+) | 700.4 5 | 100 | Q | 3947.0 | (41/2+) | |

5464.5 9 | (49/2+) | ||||||

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) | I(γ) | M(γ) | Final Levels | |

Band 3 - 13/2^{+} band, α=-1/2 | |||||||

531.3 3 | (15/2+) | ||||||

983.5 3 | (19/2+) | 452.2 1 484.3 3 | 100 15 51 8 | (E2) D+Q | 531.3 499.2 | (15/2+) (17/2+) | |

1555.7 3 | (23/2+) | 572.2 3 600.7 5 | 100 16 22 7 | (E2) D+Q | 983.5 955.0 | (19/2+) (21/2+) | |

2219.4 4 | (27/2+) | 663.7 3 | 100 | Q | 1555.7 | (23/2+) | |

2931.6 4 | (31/2+) | 712.2 3 | 100 | Q | 2219.4 | (27/2+) | |

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) | I(γ) | M(γ) | Final Levels | |

Band 4 - Band based on (17/2^{+}). | |||||||

944.0 2 | (17/2+) | ||||||

1444.0 3 | (21/2+) | 460.5 3 500.0 1 944.8 5 | 30 10 100 16 10 4 | D+Q (E2) Q | 983.5 944.0 499.2 | (19/2+) (17/2+) (17/2+) | |

2009.5 3 | (25/2+) | 565.5 1 1054.5 5 | <100 14 5 | Q | 1444.0 955.0 | (21/2+) (21/2+) | |

2635.5 3 | (29/2+) | 626.0 1 1106.2 3 | 100 5 17 6 | Q Q | 2009.5 1529.3 | (25/2+) (25/2+) | |

3201.0 3 | (33/2+) | 134.8 5 565.5 1 | 100 | (E2) | 3066.2 2635.5 | (33/2+) (29/2+) | |

3582.3 3 | (37/2+) | 381.3 1 717.6 3 | 100 16 41 13 | (E2) | 3201.0 2864.7 | (33/2+) (33/2+) | |

3976.0 6 | 393.7 5 | | 3582.3 | (37/2+) | |||

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) | I(γ) | M(γ) | Final Levels | |

Band 5 - γ cascade based on (49/2-). | |||||||

5042.3 3 | (49/2-) | ||||||

5502.1 4 | (53/2-) | 459.8 1 | 100 | (E2) | 5042.3 | (49/2-) | |

6474.8 5 | (57/2-) | 972.7 3 | 100 | Q | 5502.1 | (53/2-) | |

6761.9 7 | 287.1 5 | 100 | 6474.8 | (57/2-) | |||

7358.0 9 | 596.1 5 | | 6761.9 | ||||

8135.3 10 | 777.3 5 | | 7358.0 | ||||

8843.1 11 | 707.8 5 | | 8135.3 | ||||

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) | I(γ) | M(γ) | Final Levels | |

Band 6 - The g.s. band | |||||||

0.0 | 3/2- | 10.87 h 12 % ε = 100 | |||||

6.40 3 | 5/2- | 6.40 4 S | 100 | [M1] | 0.0 | 3/2- | |

237.4 1 | (9/2)- | 231.0 1 | 100 | E2 | 6.40 | 5/2- | |

608.6 2 | (13/2-) | 251.9 3 371.2 1 | 11 4 100 5 | (E2) | 356.72 237.4 | (9/2-) (9/2)- | |

1081.1 2 | (17/2-) | 472.4 1 | 100 | (E2) | 608.6 | (13/2-) | |

1490.4 2 | (19/2-) | 128.9 1 409.3 1 536 1 | 35 6 100 5 | (E2) (E2) | 1361.5 1081.1 955.0 | (17/2-) (17/2-) (21/2+) | |

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) | I(γ) | M(γ) | Final Levels | |

Band 7 - ΔJ=2 band based on (25/2-). | |||||||

1714.3 3 | (25/2-) | ||||||

2303.7 3 | (29/2-) | 248.5 3 589.4 1 | 22 4 100 6 | D+Q (E2) | 2055.2 1714.3 | (27/2-) (25/2-) | |

2839.8 3 | (33/2-) | 536.1 1 548.4 3 | 100 15 46 8 | (E2) (E2) | 2303.7 2291.4 | (29/2-) (29/2-) | |

3452.7 4 | (37/2-) | 612.9 3 | 100 | Q | 2839.8 | (33/2-) | |

4168.6 6 | (41/2-) | 715.9 5 | 100 | Q | 3452.7 | (37/2-) | |

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) | I(γ) | M(γ) | Final Levels | |

Band 8 - ΔJ=2 band based on (29/2-). | |||||||

2291.4 3 | (29/2-) | ||||||

2874.2 3 | (33/2-) | 582.8 1 | 100 | (E2) | 2291.4 | (29/2-) | |

3574.1 4 | (37/2-) | 699.9 3 | 100 | Q | 2874.2 | (33/2-) |

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |

6.40 | 5/2- | 6.40 4 | [M1] | 924 | α=924 22, α(M)=714 17, α(N)=177 5, α(O)=31.8 8, α(P)=2.13 5 | ||

45.78 | (1/2)- | 39.47 3 | E2 | 369 | α=369, α(L)=277 4, α(M)=71.2 11, α(N)=17.3 3, α(O)=2.67 4, α(P)=0.00221 4 | ||

(1/2)- | 45.69 3 | M1+E2 | 0.32 3 | 27 | α=27 3, α(L)=20.7 21, α(M)=5.1 6, α(N)=1.25 13, α(O)=0.205 20, α(P)=0.00575 12 | ||

88.30 | 3/2- | 42.75 5 | M1+E2 | 0.14 2 | 18.7 | α=18.7 14, α(L)=14.3 11, α(M)=3.4 3, α(N)=0.84 7, α(O)=0.145 10, α(P)=0.00745 12 | |

3/2- | 82.2 5 | M1+E2 | 0.21 2 | 11.6 | α=11.6 3, α(K)=9.17 22, α(L)=1.88 7, α(M)=0.443 18, α(N)=0.109 5, α(O)=0.0191 7, α(P)=0.00107 3 | ||

3/2- | 88.41 3 | M1+E2 | 0.21 2 | 9.43 | α=9.43, α(K)=7.49 12, α(L)=1.49 4, α(M)=0.350 11, α(N)=0.086 3, α(O)=0.0152 4, α(P)=0.000870 14 | ||

172.79 | 9/2- | 464 ns 25 % IT = 100 | 166.40 5 | E2 | 0.684 | B(E2)(W.u.)=0.088 5, α=0.684, α(K)=0.267 4, α(L)=0.314 5, α(M)=0.0805 12, α(N)=0.0197 3, α(O)=0.00310 5, α(P)=2.53E-5 4 | |

191.4 | (13/2+) | 143 µs 5 % IT = 100 | 18.7 9 | [M2] | 3.8×10^{4} | B(M2)(W.u.)=0.08 3, α=3.8×10^{4} 10, α(L)=2.77×10^{+4} 73, α(M)=7.6E+3 21, α(N)=1.92E+3 52, α(O)=3.28E+2 88, α(P)=15.8 42 | |

222.30 | (3/2,5/2)- | 134.26 4 | M1+E2 | 0.8 3 | 2.3 | α=2.3 3, α(K)=1.6 4, α(L)=0.56 8, α(M)=0.137 23, α(N)=0.034 6, α(O)=0.0056 8, α(P)=0.00018 5 | |

(3/2,5/2)- | 215.68 5 | M1+E2 | 0.9 4 | 0.54 | α=0.54 12, α(K)=0.41 12, α(L)=0.1032 15, α(M)=0.0249 8, α(N)=0.00614 18, α(O)=0.001046 16, α(P)=4.5×10^{-5} 15 | ||

(3/2,5/2)- | 221.95 16 | E2 | 0.253 | α=0.253, α(K)=0.1306 19, α(L)=0.0926 14, α(M)=0.0235 4, α(N)=0.00575 9, α(O)=0.000921 14, α(P)=1.263×10^{-5} 18 | |||

237.4 | (9/2)- | 231.0 1 | E2 | 0.222 | α=0.222, α(K)=0.1180 17, α(L)=0.0786 11, α(M)=0.0200 3, α(N)=0.00488 7, α(O)=0.000783 11, α(P)=1.147×10^{-5} 17 | ||

348.45 | (5/2,3/2)- | 110.8 5 | (E2) | 3.22 | α=3.22 8, α(K)=0.622 10, α(L)=1.95 5, α(M)=0.505 13, α(N)=0.123 4, α(O)=0.0192 5, α(P)=6.75×10^{-5} 12 | ||

(5/2,3/2)- | 126.31 5 | M1+E2 | 0.54 9 | 3.08 | α=3.08 10, α(K)=2.29 14, α(L)=0.60 4, α(M)=0.146 10, α(N)=0.0359 25, α(O)=0.0061 4, α(P)=0.000261 17 | ||

(5/2,3/2)- | 259.68 10 | M1+E2 | 1.4 +8-4 | 0.25 | α=0.25 5, α(K)=0.184 48, α(L)=0.0533 22, α(M)=0.0130 4, α(N)=0.00320 9, α(O)=0.000538 25, α(P)=2.01×10^{-5} 57 | ||

(5/2,3/2)- | 348.15 15 | M1(+E2) | 0.7 LT | 0.181 | α=0.181 24, α(K)=0.148 21, α(L)=0.0256 19, α(M)=0.0060 4, α(N)=0.00147 10, α(O)=0.000262 20, α(P)=1.67×10^{-5} 25 | ||

447.67 | (3/2,5/2)- | 225.7 5 | M1(+E2) | 0.8 LT | 0.58 | α=0.58 9, α(K)=0.47 9, α(L)=0.0895 16, α(M)=0.0211 4, α(N)=0.00520 9, α(O)=0.000915 20, α(P)=5.3×10^{-5} 10 | |

(3/2,5/2)- | 441.04 14 | M1+E2 | 1.3 +20-6 | 0.062 | α=0.062 23, α(K)=0.049 20, α(L)=0.0100 22, α(M)=0.0024 5, α(N)=0.00058 12, α(O)=0.000102 23, α(P)=5.3×10^{-6} 23 | ||

(3/2,5/2)- | 447.77 9 | M1(+E2) | 0.7 LT | 0.092 | α=0.092 12, α(K)=0.076 11, α(L)=0.0128 12, α(M)=0.0030 3, α(N)=0.00073 7, α(O)=0.000131 12, α(P)=8.5×10^{-6} 12 | ||

493.3 | 11/2- | 321.1 5 | M1+E2 | -16.2 +17-21 | 0.0817 | α=0.0817, α(K)=0.0525 8, α(L)=0.0222 4, α(M)=0.00553 9, α(N)=0.001356 20, α(O)=0.000222 4, α(P)=5.34×10^{-6} 8 | |

499.2 | (17/2+) | 211.4 ps 55 | 307.8 1 | E2 | 0.0913 | B(E2)(W.u.)=13.8 4, α=0.0913, α(K)=0.0573 8, α(L)=0.0257 4, α(M)=0.00643 9, α(N)=0.001575 23, α(O)=0.000257 4, α(P)=5.79E-6 9 | |

529.62 | (1/2,3/2,5/2)- | 529.59 11 | M1(+E2) | 1.4 LT | 0.052 | α=0.052 15, α(K)=0.042 13, α(L)=0.0073 16, α(M)=0.0017 4, α(N)=0.00042 9, α(O)=7.5×10^{-5} 17, α(P)=4.7E-6 15 | |

608.6 | (13/2-) | 371.2 1 | (E2) | 0.0536 | α=0.0536, α(K)=0.0363 5, α(L)=0.01308 19, α(M)=0.00324 5, α(N)=0.000794 12, α(O)=0.0001313 19, α(P)=3.75×10^{-6} 6 | ||

712.0 | (13/2-) | 539.5 3 | (E2) | 0.0206 | α=0.0206, α(K)=0.01546 22, α(L)=0.00393 6, α(M)=0.000950 14, α(N)=0.000234 4, α(O)=3.97×10^{-5} 6, α(P)=1.632E-6 23 | ||

944.0 | (17/2+) | 444.8 5 | (E2) | 0.0332 | α=0.0332, α(K)=0.0238 4, α(L)=0.00714 10, α(M)=0.001746 25, α(N)=0.000429 6, α(O)=7.18×10^{-5} 10, α(P)=2.49E-6 4 | ||

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |

955.0 | (21/2+) | 175.4 ps 49 | 455.8 1 | (E2) | 0.0312 | B(E2)(W.u.)=2.47 7, α=0.0312, α(K)=0.0225 4, α(L)=0.00660 10, α(M)=0.001612 23, α(N)=0.000396 6, α(O)=6.65E-5 10, α(P)=2.36E-6 4 | |

983.5 | (19/2+) | 452.2 1 | (E2) | 0.0318 | α=0.0318, α(K)=0.0229 4, α(L)=0.00677 10, α(M)=0.001654 24, α(N)=0.000406 6, α(O)=6.82×10^{-5} 10, α(P)=2.40E-6 4 | ||

1081.1 | (17/2-) | 472.4 1 | (E2) | α(K)=0.0207 3, α(L)=0.00589 9, α(M)=0.001436 21, α(N)=0.000353 5, α(O)=5.94×10^{-5} 9, α(P)=2.18E-6 3 | |||

1160.87 | (3/2+) | 631.2 9 | E1 | 0.00511 | α=0.00511, α(K)=0.00427 6, α(L)=0.000646 10, α(M)=0.0001477 22, α(N)=3.64×10^{-5} 6, α(O)=6.46E-6 10, α(P)=4.12E-7 6 | ||

(3/2+) | 713.24 17 | E1 | 0.00401 | α=0.00401, α(K)=0.00335 5, α(L)=0.000503 7, α(M)=0.0001149 17, α(N)=2.83×10^{-5} 4, α(O)=5.04E-6 7, α(P)=3.25E-7 5 | |||

(3/2+) | 812.8 3 | E1 | 0.00311 | α=0.00311, α(K)=0.00261 4, α(L)=0.000388 6, α(M)=8.86×10^{-5} 13, α(N)=2.18E-5 3, α(O)=3.90E-6 6, α(P)=2.55E-7 4 | |||

(3/2+) | 1071.5 6 | E1 | 0.00187 | α=0.00187, α(K)=0.001572 22, α(L)=0.000230 4, α(M)=5.24×10^{-5} 8, α(N)=1.290E-5 19, α(O)=2.31E-6 4, α(P)=1.546E-7 22 | |||

(3/2+) | 1160.6 3 | E1 | 1.63×10^{-3} | α=1.63×10^{-3}, α(K)=0.001364 20, α(L)=0.000199 3, α(M)=4.52E-5 7, α(N)=1.115E-5 16, α(O)=2.00E-6 3, α(P)=1.344E-7 19 | |||

1185.31 | (19/2+) | 531.5 1 | (E2) | 0.0214 | α=0.0214, α(K)=0.01597 23, α(L)=0.00411 6, α(M)=0.000994 14, α(N)=0.000244 4, α(O)=4.15×10^{-5} 6, α(P)=1.685E-6 24 | ||

1361.5 | (17/2-) | 280.4 3 | (E2) | 0.1207 | α=0.1207, α(K)=0.0723 11, α(L)=0.0366 6, α(M)=0.00919 14, α(N)=0.00225 4, α(O)=0.000365 6, α(P)=7.22×10^{-6} 11 | ||

1444.0 | (21/2+) | 500.0 1 | (E2) | 0.0248 | α=0.0248, α(K)=0.0183 3, α(L)=0.00494 7, α(M)=0.001200 17, α(N)=0.000295 5, α(O)=4.98×10^{-5} 7, α(P)=1.92E-6 3 | ||

1490.4 | (19/2-) | 128.9 1 | (E2) | 1.77 | α=1.77, α(K)=0.473 7, α(L)=0.977 15, α(M)=0.252 4, α(N)=0.0615 9, α(O)=0.00963 14, α(P)=4.68×10^{-5} 7 | ||

(19/2-) | 409.3 1 | (E2) | 0.0412 | α=0.0412, α(K)=0.0288 4, α(L)=0.00938 14, α(M)=0.00231 4, α(N)=0.000566 8, α(O)=9.43×10^{-5} 14, α(P)=3.00E-6 5 | |||

1512.1 | (21/2-) | 150.6 3 | (E2) | 0.985 | α=0.985 16, α(K)=0.338 5, α(L)=0.486 8, α(M)=0.1251 21, α(N)=0.0305 5, α(O)=0.00480 8, α(P)=3.22×10^{-5} 5 | ||

1529.3 | (25/2+) | 574.3 1 | (E2) | 0.01780 | α=0.01780, α(K)=0.01351 19, α(L)=0.00328 5, α(M)=0.000789 11, α(N)=0.000194 3, α(O)=3.31×10^{-5} 5, α(P)=1.428E-6 20 | ||

1555.7 | (23/2+) | 572.2 3 | (E2) | 0.0180 | α=0.0180, α(K)=0.01362 20, α(L)=0.00331 5, α(M)=0.000797 12, α(N)=0.000196 3, α(O)=3.35×10^{-5} 5, α(P)=1.440E-6 21 | ||

1714.3 | (25/2-) | 202.2 1 | (E2) | 0.346 | α=0.346, α(K)=0.1653 24, α(L)=0.1362 20, α(M)=0.0347 5, α(N)=0.00849 12, α(O)=0.001353 20, α(P)=1.581×10^{-5} 23 | ||

2291.4 | (29/2-) | 577.1 1 | (E2) | 0.01760 | α=0.01760, α(K)=0.01337 19, α(L)=0.00323 5, α(M)=0.000778 11, α(N)=0.000191 3, α(O)=3.27×10^{-5} 5, α(P)=1.414E-6 20 | ||

2303.7 | (29/2-) | 589.4 1 | (E2) | 0.01677 | α=0.01677, α(K)=0.01278 18, α(L)=0.00304 5, α(M)=0.000731 11, α(N)=0.000180 3, α(O)=3.08×10^{-5} 5, α(P)=1.352E-6 19 | ||

2620.4 | (31/2-) | 565.2 1 | (E2) | 0.0185 | α=0.0185, α(K)=0.01398 20, α(L)=0.00343 5, α(M)=0.000827 12, α(N)=0.000203 3, α(O)=3.47×10^{-5} 5, α(P)=1.478E-6 21 | ||

2729.4 | (29/2+) | 539.9 3 | (E2) | 0.0206 | α=0.0206, α(K)=0.01543 22, α(L)=0.00392 6, α(M)=0.000948 14, α(N)=0.000233 4, α(O)=3.96×10^{-5} 6, α(P)=1.629E-6 23 | ||

2839.8 | (33/2-) | 536.1 1 | (E2) | 0.0209 | α=0.0209, α(K)=0.01567 22, α(L)=0.00401 6, α(M)=0.000968 14, α(N)=0.000238 4, α(O)=4.04×10^{-5} 6, α(P)=1.654E-6 24 | ||

(33/2-) | 548.4 3 | (E2) | 0.0198 | α=0.0198, α(K)=0.01492 21, α(L)=0.00375 6, α(M)=0.000904 13, α(N)=0.000222 4, α(O)=3.78×10^{-5} 6, α(P)=1.576E-6 23 | |||

2874.2 | (33/2-) | 582.8 1 | (E2) | 0.01721 | α=0.01721, α(K)=0.01309 19, α(L)=0.00314 5, α(M)=0.000756 11, α(N)=0.000186 3, α(O)=3.18×10^{-5} 5, α(P)=1.385E-6 20 | ||

3201.0 | (33/2+) | 565.5 1 | (E2) | 0.0185 | α=0.0185, α(K)=0.01396 20, α(L)=0.00343 5, α(M)=0.000825 12, α(N)=0.000203 3, α(O)=3.46×10^{-5} 5, α(P)=1.476E-6 21 | ||

E(level) (keV) | J^{π}(level) | T_{1/2}(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |

3376.4 | (37/2+) | 511.7 3 | (E2) | 0.0234 | α=0.0234, α(K)=0.01736 25, α(L)=0.00460 7, α(M)=0.001117 16, α(N)=0.000275 4, α(O)=4.65×10^{-5} 7, α(P)=1.83E-6 3 | ||

3455.4 | (35/2+) | 523.8 5 | (E2) | 0.0221 | α=0.0221, α(K)=0.01649 24, α(L)=0.00429 7, α(M)=0.001039 15, α(N)=0.000255 4, α(O)=4.33×10^{-5} 7, α(P)=1.739E-6 25 | ||

3582.3 | (37/2+) | 381.3 1 | (E2) | 0.0498 | α=0.0498, α(K)=0.0341 5, α(L)=0.01192 17, α(M)=0.00295 5, α(N)=0.000723 11, α(O)=0.0001197 17, α(P)=3.52×10^{-6} 5 | ||

3640.7 | (39/2+) | 185.3 1 | (E2) | 0.467 | α=0.467, α(K)=0.206 3, α(L)=0.197 3, α(M)=0.0504 8, α(N)=0.01232 18, α(O)=0.00195 3, α(P)=1.95×10^{-5} 3 | ||

(39/2+) | 220.6 1 | (E2) | 0.259 | α=0.259, α(K)=0.1326 19, α(L)=0.0949 14, α(M)=0.0241 4, α(N)=0.00590 9, α(O)=0.000944 14, α(P)=1.282×10^{-5} 18 | |||

3648.7 | (39/2-) | 356.3 1 | (E2) | 0.0600 | α=0.0600, α(K)=0.0401 6, α(L)=0.01510 22, α(M)=0.00375 6, α(N)=0.000919 13, α(O)=0.0001515 22, α(P)=4.12×10^{-6} 6 | ||

3848.6 | (43/2+) | 207.9 1 | (E2) | 0.315 | α=0.315, α(K)=0.1541 22, α(L)=0.1213 18, α(M)=0.0309 5, α(N)=0.00756 11, α(O)=0.001205 17, α(P)=1.478×10^{-5} 21 | ||

3947.0 | (41/2+) | 570.6 3 | (E2) | 0.0181 | α=0.0181, α(K)=0.01370 20, α(L)=0.00334 5, α(M)=0.000804 12, α(N)=0.000198 3, α(O)=3.37×10^{-5} 5, α(P)=1.448E-6 21 | ||

4367.8 | (47/2+) | 519.2 1 | (E2) | 0.0226 | α=0.0226, α(K)=0.01681 24, α(L)=0.00441 7, α(M)=0.001068 15, α(N)=0.000262 4, α(O)=4.45×10^{-5} 7, α(P)=1.772E-6 25 | ||

4879.3 | (49/2+) | 193.1 1 | (E2) | 0.405 | α=0.405, α(K)=0.185 3, α(L)=0.1654 24, α(M)=0.0423 6, α(N)=0.01033 15, α(O)=0.001641 24, α(P)=1.767×10^{-5} 25 | ||

5042.3 | (49/2-) | 193.6 5 | (E2) | 0.402 | α=0.402 7, α(K)=0.184 3, α(L)=0.164 3, α(M)=0.0418 8, α(N)=0.01021 19, α(O)=0.00162 3, α(P)=1.76×10^{-5} 3 | ||

(49/2-) | 247.0 3 | (E2) | 0.179 | α=0.179, α(K)=0.0996 15, α(L)=0.0601 9, α(M)=0.01520 23, α(N)=0.00372 6, α(O)=0.000598 9, α(P)=9.77×10^{-6} 14 | |||

(49/2-) | 354.2 3 | (E2) | 0.0610 | α=0.0610, α(K)=0.0406 6, α(L)=0.01542 22, α(M)=0.00383 6, α(N)=0.000939 14, α(O)=0.0001547 23, α(P)=4.17×10^{-6} 6 | |||

5353.7 | (53/2+) | 474.4 1 | (E2) | 0.0282 | α=0.0282, α(K)=0.0205 3, α(L)=0.00581 9, α(M)=0.001417 20, α(N)=0.000348 5, α(O)=5.86×10^{-5} 9, α(P)=2.16E-6 3 | ||

5502.1 | (53/2-) | 459.8 1 | (E2) | 0.0305 | α=0.0305, α(K)=0.0220 3, α(L)=0.00642 9, α(M)=0.001567 22, α(N)=0.000385 6, α(O)=6.46×10^{-5} 9, α(P)=2.31E-6 4 |

__Additional Level Data and Comments__:

E(level) | J^{π}(level) | T_{1/2}(level) | Comments |

0.0 | 3/2- | 10.87 h 12 % ε = 100 | μ=-0.422 7 (1989Du01,2000SaZZ,2014StZZ), Q=-0.95 4 (1992Hi07,1989Du01,2016St14) RMS charge radius <r ^{2}>^{1/2}=5.4060 fm 35 (2013An02 evaluation).E(level): The g.s. band. |

6.40 | 5/2- | E(level): Transition unobserved. Energy from energy level differences. The g.s. band. J ^{π}(level): The 6.4 level is populated by an M1^{+}E2 γ from the 88.4 level which is 1/2-,3/2- from L=1 in (p,d). The 172.8 and 493 levels are populated with low log ft (≈5) from ^{189}Au ε decay (4.59 min) indicating Jπ=9/2-,11/2-,13/2-. An E2 γ from 172.6 to 6.2 thus establishes Jπ(6.2)=5/2-, Jπ(88.4)=3/2-, and Jπ(172.6)=9/2-. From γ(θ) on oriented nuclei the 493 level is uniquely determined as 11/2-. | |

88.30 | 3/2- | E(level): Transition unobserved. Energy from energy level differences. J ^{π}(level): The 6.4 level is populated by an M1^{+}E2 γ from the 88.4 level which is 1/2-,3/2- from L=1 in (p,d). The 172.8 and 493 levels are populated with low log ft (≈5) from ^{189}Au ε decay (4.59 min) indicating Jπ=9/2-,11/2-,13/2-. An E2 γ from 172.6 to 6.2 thus establishes Jπ(6.2)=5/2-, Jπ(88.4)=3/2-, and Jπ(172.6)=9/2-. From γ(θ) on oriented nuclei the 493 level is uniquely determined as 11/2-. | |

172.79 | 9/2- | 464 ns 25 % IT = 100 | E(level): Transition unobserved. Energy from energy level differences. J ^{π}(level): The 6.4 level is populated by an M1^{+}E2 γ from the 88.4 level which is 1/2-,3/2- from L=1 in (p,d). The 172.8 and 493 levels are populated with low log ft (≈5) from ^{189}Au ε decay (4.59 min) indicating Jπ=9/2-,11/2-,13/2-. An E2 γ from 172.6 to 6.2 thus establishes Jπ(6.2)=5/2-, Jπ(88.4)=3/2-, and Jπ(172.6)=9/2-. From γ(θ) on oriented nuclei the 493 level is uniquely determined as 11/2-. |

191.4 | (13/2+) | 143 µs 5 % IT = 100 | E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. |

237.4 | (9/2)- | E(level): The g.s. band. | |

348.45 | (5/2,3/2)- | XREF: E(340). | |

493.3 | 11/2- | E(level): Transition unobserved. Energy from energy level differences. J ^{π}(level): The 6.4 level is populated by an M1^{+}E2 γ from the 88.4 level which is 1/2-,3/2- from L=1 in (p,d). The 172.8 and 493 levels are populated with low log ft (≈5) from ^{189}Au ε decay (4.59 min) indicating Jπ=9/2-,11/2-,13/2-. An E2 γ from 172.6 to 6.2 thus establishes Jπ(6.2)=5/2-, Jπ(88.4)=3/2-, and Jπ(172.6)=9/2-. From γ(θ) on oriented nuclei the 493 level is uniquely determined as 11/2-. | |

499.2 | (17/2+) | 211.4 ps 55 | Q(transition)=11.05 29 (2013He25).E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. T _{1/2}(level): From ^{176}Yb(^{18}O,5nγ), using the recoil-distance method (2013He25). |

531.3 | (15/2+) | E(level): 13/2^{+} band, α=-1/2. | |

608.6 | (13/2-) | E(level): The g.s. band. | |

944.0 | (17/2+) | E(level): From ^{189}Au ε decay (4.59 min). Band based on (17/2^{+}). | |

955.0 | (21/2+) | 175.4 ps 49 | Q(transition)=2.49 7 (2013He25).E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. T _{1/2}(level): From ^{176}Yb(^{18}O,5nγ), using the recoil-distance method (2013He25). |

983.5 | (19/2+) | E(level): 13/2^{+} band, α=-1/2. | |

1081.1 | (17/2-) | E(level): The g.s. band. | |

1444.0 | (21/2+) | E(level): From ^{189}Au ε decay (4.59 min). Band based on (17/2^{+}). | |

1490.4 | (19/2-) | E(level): The g.s. band. | |

1529.3 | (25/2+) | E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. | |

1555.7 | (23/2+) | E(level): 13/2^{+} band, α=-1/2. | |

1714.3 | (25/2-) | E(level): ΔJ=2 band based on (25/2-). | |

2009.5 | (25/2+) | E(level): From ^{189}Au ε decay (4.59 min). Band based on (17/2^{+}). | |

2189.5 | (29/2+) | E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. | |

2219.4 | (27/2+) | E(level): 13/2^{+} band, α=-1/2. | |

2291.4 | (29/2-) | E(level): ΔJ=2 band based on (29/2-). | |

2303.7 | (29/2-) | E(level): ΔJ=2 band based on (25/2-). | |

E(level) | J^{π}(level) | T_{1/2}(level) | Comments |

2635.5 | (29/2+) | E(level): From ^{189}Au ε decay (4.59 min). Band based on (17/2^{+}). | |

2839.8 | (33/2-) | E(level): ΔJ=2 band based on (25/2-). | |

2864.7 | (33/2+) | E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. | |

2874.2 | (33/2-) | E(level): ΔJ=2 band based on (29/2-). | |

2931.6 | (31/2+) | E(level): 13/2^{+} band, α=-1/2. | |

3201.0 | (33/2+) | E(level): From ^{189}Au ε decay (4.59 min). Band based on (17/2^{+}). | |

3376.4 | (37/2+) | E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. | |

3452.7 | (37/2-) | E(level): ΔJ=2 band based on (25/2-). | |

3574.1 | (37/2-) | E(level): ΔJ=2 band based on (29/2-). | |

3582.3 | (37/2+) | E(level): From ^{189}Au ε decay (4.59 min). Band based on (17/2^{+}). | |

3640.7 | (39/2+) | E(level): γ cascade based on (39/2^{+}). | |

3848.6 | (43/2+) | E(level): γ cascade based on (39/2^{+}). | |

3947.0 | (41/2+) | E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. | |

3976.0 | E(level): From ^{189}Au ε decay (4.59 min). Band based on (17/2^{+}). | ||

4168.6 | (41/2-) | E(level): ΔJ=2 band based on (25/2-). | |

4367.8 | (47/2+) | E(level): γ cascade based on (39/2^{+}). | |

4647.4 | (45/2+) | E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. | |

4879.3 | (49/2+) | E(level): γ cascade based on (39/2^{+}). | |

5042.3 | (49/2-) | E(level): γ cascade based on (49/2-). | |

5353.7 | (53/2+) | E(level): γ cascade based on (39/2^{+}). | |

5464.5 | (49/2+) | E(level): From ^{189}Au ε decay (28.7 min). 13/2^{+} band, α=+1/2. | |

5502.1 | (53/2-) | E(level): γ cascade based on (49/2-). | |

6474.8 | (57/2-) | E(level): γ cascade based on (49/2-). | |

6476.5 | (55/2+) | E(level): γ cascade based on (39/2^{+}). | |

6761.9 | E(level): γ cascade based on (49/2-). | ||

E(level) | J^{π}(level) | T_{1/2}(level) | Comments |

6841.6 | (57/2+) | E(level): γ cascade based on (39/2^{+}). | |

7272.3 | E(level): γ cascade based on (39/2^{+}). | ||

7358.0 | E(level): γ cascade based on (49/2-). | ||

7764.8 | E(level): γ cascade based on (39/2^{+}). | ||

8135.3 | E(level): γ cascade based on (49/2-). | ||

8843.1 | E(level): γ cascade based on (49/2-). |

E(level) | E(gamma) | Comments |

6.40 | 6.40 | E(γ): Transition unobserved. Energy from energy level differences |

45.78 | 39.47 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). |

45.69 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

88.30 | 42.75 | E(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). |

82.2 | E(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

88.41 | E(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

172.79 | 166.40 | E(γ): Using the higher precision value from 4.59 min ε decay M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). |

191.4 | 18.7 | E(γ): Transition unobserved. Energy from energy level differences |

202.2 | 11.3 | E(γ): Transition unobserved. Energy from energy level differences |

222.30 | 134.26 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). |

176.1 | E(γ): From ^{189}Au ε decay (28.7 min) | |

215.68 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

221.95 | E(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

237.4 | 231.0 | E(γ): Weighted average from (^{18}O,4nγ) and 28.7 min ε decay.M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). |

348.45 | 110.8 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). |

126.31 | I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

259.68 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

302.4 | E(γ): From ^{189}Au ε decay (28.7 min) | |

342.0 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min) | |

348.15 | E(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

447.67 | 225.7 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). |

359.4 | E(γ): From ^{189}Au ε decay (28.7 min) | |

441.04 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

447.77 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

493.3 | 321.1 | E(γ): From ^{189}Au ε decay (4.59 min) |

E(level) | E(gamma) | Comments |

499.2 | 307.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

529.62 | 484.2 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min) |

523.4 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min) | |

529.59 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

531.3 | 329.2 | E(γ): Only in (α,3nγ) |

339.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

608.6 | 371.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

653.8 | 462.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

712.0 | 539.5 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

944.0 | 412.7 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

444.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

955.0 | 455.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

983.5 | 452.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

484.3 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

1081.1 | 472.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

1160.87 | 631.2 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). |

713.24 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

812.8 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

1071.5 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

1160.6 | E(γ): From ^{189}Au ε decay (28.7 min)I(γ): From ^{189}Au ε decay (28.7 min)M(γ): From Ice data in ^{189}Au ε decay (28.7 min) and ^{189}Au ε decay (4.59 min). | |

1185.31 | 531.5 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

686.1 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

1361.5 | 280.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

649.5 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

862.3 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

E(level) | E(gamma) | Comments |

1444.0 | 460.5 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

500.0 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

944.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

1490.4 | 128.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

409.3 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

536 | E(γ): only in (α,3nγ). Uncertainty assumed by evaluators. | |

1512.1 | 150.6 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

326.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

1529.3 | 574.3 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

1555.7 | 572.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

600.7 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

1695.7 | 183.6 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

1714.3 | 18.6 | E(γ): in (α,3nγ) and the previous evaluation, this γ was placed from a 1530 keV level with (23/2-). In (^{18}O,5nγ), coincidence relations found the 740.7 feeding the 945 keV level. This matches the 184 γ feeding the 1512 keV level followed by the 557 γ populating the 954 keV level. The 18.6 keV and and 184 γ’s match and are parallel to the 202 γ feeding the 1512 keV level but with the order of the 18.6 and 184 γ rays now reversed. See 2009Hu12 for further discussion.. Transition unobserved. Energy from energy level differences |

202.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

2009.5 | 565.5 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |

1054.5 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

2055.2 | 340.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

2189.5 | 660.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

2219.4 | 663.7 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

2291.4 | 236.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

577.1 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

2303.7 | 248.5 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

589.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

2539.7 | 1010.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

2620.4 | 316.7 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

329.0 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

565.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

E(level) | E(gamma) | Comments |

2635.5 | 626.0 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

1106.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

2688.4 | 397.0 | E(γ): Observed only in ^{176}Yb(^{18}O,5nγ)M(γ): From directional correlation of oriented nuclei (DCO) ratios from ( ^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

633.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

2729.4 | 539.9 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided M(γ): From directional correlation of oriented nuclei (DCO) ratios from ( ^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

1200.1 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

2839.8 | 536.1 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

548.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

2864.7 | 675.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

2874.2 | 582.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

2931.6 | 712.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

2979.3 | 759.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3066.2 | 876.7 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3201.0 | 565.5 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided M(γ): From directional correlation of oriented nuclei (DCO) ratios from ( ^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3292.4 | 91.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

418.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

452.6 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

604.0 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

672.0 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

3376.4 | 511.7 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3420.1 | 219.1 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

580.3 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

3452.7 | 612.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3455.4 | 254.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

523.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

E(level) | E(gamma) | Comments |

3574.1 | 699.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3582.3 | 381.3 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3640.7 | 185.3 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

188.0 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

220.6 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

3648.7 | 356.3 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3809.3 | 160.6 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3848.6 | 207.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

3947.0 | 570.6 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

4168.6 | 715.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

4367.8 | 519.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

4437.2 | 627.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

788.5 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

4647.4 | 700.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

4686.2 | 837.6 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

4688.1 | 250.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

4708.4 | 859.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

4795.3 | 986.0 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

4848.7 | 1039.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

4879.3 | 170.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

193.1 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

511.5 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

5042.3 | 193.6 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

247.0 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

333.9 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

354.2 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. | |

E(level) | E(gamma) | Comments |

5353.7 | 474.4 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

5464.5 | 817.1 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

5502.1 | 459.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

6474.8 | 972.7 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

6476.5 | 1122.8 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

6841.6 | 365.1 | M(γ): From directional correlation of oriented nuclei (DCO) ratios from (^{18}O,5nγ), assuming quadrupole transitions are E2, stretched dipoles are E1 or M1, and mixed multipolarity are M1^{+}E2. Where Jπ values were already tentatively assigned, level scheme placement based on corroborating transitions, was used to distinguish between M1 or E1. |

^{189}Pt produced and identified by 1955Sm42 in Ir(p,xn),E=50-130 MeV. Measured β, γ and half-life of the activity. Later studies of this decay: 1960Po07, 1960Ma28, 1961Kr02, 1961An02, 1962Kr04, 1962Ha24, 1962Gr27, 1963Th07, 1964Le07, 1964Kr03, 1965Ja12, 1967Na02, 1970Ba10, 1970Ba56, 1971Pl08, 1972Ba21, 1972He05, 1975Ru06, 1980Be27, 2000Mo05, 2000Zi04Q-value: S(2n)=15927

26, S(2p)=982810(2017Wa10)