List of levels for 162YB

Author: N. Nica | Citation: Nucl. Data Sheets 195, 1 (2024) | Cutoff date: 19-Sep-2023

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
166.72	2+	415 ps 9	166.71 4	E2		0.499	B(E2)(W.u.)=134.7 30, α=0.499 7, α(K)=0.276 4, α(L)=0.1707 24, α(M)=0.0416 6, α(N)=0.00952 13, α(O)=0.001129 16, α(P)=1.235E-5 17
487.34	4+	14.3 ps 6	320.60 4	E2		0.0606	B(E2)(W.u.)=210 9, α=0.0606 8, α(K)=0.0440 6, α(L)=0.01280 18, α(M)=0.00303 4, α(N)=0.000699 10, α(O)=8.85E-5 12, α(P)=2.275E-6 32
798.42	2+		631.67 5	E2		0.01008	α=0.01008 14, α(K)=0.00814 11, α(L)=0.001511 21, α(M)=0.000345 5, α(N)=8.04×10^-5 11, α(O)=1.091E-5 15, α(P)=4.53E-7 6
798.42	2+		798.48 6	E2		0.00595	α=0.00595 8, α(K)=0.00489 7, α(L)=0.000825 12, α(M)=0.0001869 26, α(N)=4.36×10^-5 6, α(O)=6.02E-6 8, α(P)=2.74E-7 4
924.14	6+	3.47 ps 21	436.80 2	E2		0.0254	B(E2)(W.u.)=191 +13-11, α=0.0254 4, α(K)=0.01957 27, α(L)=0.00448 6, α(M)=0.001043 15, α(N)=0.0002419 34, α(O)=3.17E-5 4, α(P)=1.059E-6 15
992.07	3+		825.29 6	M1+E2	1.60 +37-28	0.0072	α=0.0072 5, α(K)=0.0060 4, α(L)=0.00094 6, α(M)=0.000212 12, α(N)=4.96×10^-5 29, α(O)=7.0E-6 4, α(P)=3.46E-7 27
1006.20	0+		839.40 5	E2		0.00534	α=0.00534 7, α(K)=0.00440 6, α(L)=0.000731 10, α(M)=0.0001652 23, α(N)=3.86×10^-5 5, α(O)=5.34E-6 7, α(P)=2.474E-7 35
1129.59	2+		962.89 6	(E0+M1+E2)		0.0059	α=0.0059 19, α(K)=0.0050 17, α(L)=7.4×10^-4 21, α(M)=1.7E-4 5, α(N)=3.9E-5 11, α(O)=5.5E-6 17, α(P)=2.9E-7 10
1129.59	2+		1129.65 19	E2		0.00290	α=0.00290 4, α(K)=0.002424 34, α(L)=0.000371 5, α(M)=8.32×10^-5 12, α(N)=1.946E-5 27, α(O)=2.74E-6 4, α(P)=1.365E-7 19
1150.21	4+		351.8 2	E2		0.0462	α=0.0462 7, α(K)=0.0343 5, α(L)=0.00922 13, α(M)=0.002171 31, α(N)=0.000502 7, α(O)=6.42×10^-5 9, α(P)=1.801E-6 25
	4+		662.88 8	E2,M1		0.014	α=0.014 5, α(K)=0.012 5, α(L)=0.0019 6, α(M)=4.2×10^-4 12, α(N)=9.9E-5 29, α(O)=1.4E-5 4, α(P)=7.0E-7 30
	4+		983.5 4	E2		0.00384	α=0.00384 5, α(K)=0.00319 4, α(L)=0.000505 7, α(M)=0.0001136 16, α(N)=2.65×10^-5 4, α(O)=3.71E-6 5, α(P)=1.794E-7 25
1393.04	5+		400.7 3	E2		0.0321	α=0.0321 5, α(K)=0.02438 34, α(L)=0.00593 8, α(M)=0.001387 20, α(N)=0.000321 5, α(O)=4.16×10^-5 6, α(P)=1.305E-6 18
1393.04	5+		905.9 3	M1(+E2)		0.0068	α=0.0068 23, α(K)=0.0057 20, α(L)=8.6×10^-4 25, α(M)=1.9E-4 6, α(N)=4.5E-5 13, α(O)=6.4E-6 20, α(P)=3.3E-7 12
1445.56	8+	1.1 ps 3	521.42 2	E2		0.01604	B(E2)(W.u.)=2.5E2 +9-5, α=0.01604 22, α(K)=0.01268 18, α(L)=0.00260 4, α(M)=0.000600 8, α(N)=0.0001394 20, α(O)=1.858E-5 26, α(P)=6.98E-7 10
1483.24	5-		995.74 17	E1		1.51×10^-3	α=1.51×10^-3 2, α(K)=0.001284 18, α(L)=0.0001761 25, α(M)=3.89E-5 5, α(N)=9.10E-6 13, α(O)=1.298E-6 18, α(P)=6.92E-8 10
1573.32	6+		423.12 6	E2		0.0276	α=0.0276 4, α(K)=0.02121 30, α(L)=0.00496 7, α(M)=0.001158 16, α(N)=0.000268 4, α(O)=3.50×10^-5 5, α(P)=1.143E-6 16
1573.32	6+		648.7	E2,M1		0.015	α=0.015 6, α(K)=0.013 5, α(L)=0.0020 6, α(M)=4.5×10^-4 13, α(N)=1.05E-4 30, α(O)=1.5E-5 5, α(P)=7.4E-7 31
1609.00	4-		1121.63 12	E1		1.22×10^-3	α=1.22×10^-3 2, α(K)=0.001034 14, α(L)=0.0001410 20, α(M)=3.11E-5 4, α(N)=7.29E-6 10, α(O)=1.040E-6 15, α(P)=5.58E-8 8
1647.19	6+		304.4 3	E2		0.0708	α=0.0708 10, α(K)=0.0507 7, α(L)=0.01545 22, α(M)=0.00367 5, α(N)=0.000846 12, α(O)=0.0001064 15, α(P)=2.60×10^-6 4
1647.19	6+		1160.2 4	E2		0.00275	α=0.00275 4, α(K)=0.002302 32, α(L)=0.000351 5, α(M)=7.85×10^-5 11, α(N)=1.837E-5 26, α(O)=2.59E-6 4, α(P)=1.296E-7 18
1767.70	7-		843.0	E1		2.07×10^-3	α=2.07×10^-3 3, α(K)=0.001756 25, α(L)=0.0002429 34, α(M)=5.37E-5 8, α(N)=1.257E-5 18, α(O)=1.786E-6 25, α(P)=9.43E-8 13
1879.91	7+		486.8 3	E2		0.01910	α=0.01910 27, α(K)=0.01497 21, α(L)=0.00320 5, α(M)=0.000740 10, α(N)=0.0001718 24, α(O)=2.274×10^-5 32, α(P)=8.19E-7 12
1913.37	6-		304.4 3	E2		0.0708	α=0.0708 10, α(K)=0.0507 7, α(L)=0.01545 22, α(M)=0.00367 5, α(N)=0.000846 12, α(O)=0.0001064 15, α(P)=2.60×10^-6 4
	6-		429.8 3	M1		0.0607	α=0.0607 9, α(K)=0.0510 7, α(L)=0.00756 11, α(M)=0.001687 24, α(N)=0.000396 6, α(O)=5.68×10^-5 8, α(P)=3.06E-6 4
	6-		989.8 3	(E1)		1.53×10^-3	α=1.53×10^-3 2, α(K)=0.001298 18, α(L)=0.0001781 25, α(M)=3.94E-5 6, α(N)=9.21E-6 13, α(O)=1.312E-6 18, α(P)=7.00E-8 10
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
1985.29	8+	1.5 ps 2	338.12 7	E2		0.0519	B(E2)(W.u.)=4.0E2 +6-5, α=0.0519 7, α(K)=0.0381 5, α(L)=0.01059 15, α(M)=0.002500 35, α(N)=0.000577 8, α(O)=7.35E-5 10, α(P)=1.989E-6 28
	8+	1.5 ps 2	412.01 19	E2		0.0297	B(E2)(W.u.)=250 +39-30, α=0.0297 4, α(K)=0.02270 32, α(L)=0.00541 8, α(M)=0.001264 18, α(N)=0.000293 4, α(O)=3.81E-5 5, α(P)=1.219E-6 17
	8+	1.5 ps 2	539.66 6	M1		0.0336	B(M1)(W.u.)=0.0158 +26-21, α=0.0336 5, α(K)=0.0283 4, α(L)=0.00417 6, α(M)=0.000929 13, α(N)=0.0002182 31, α(O)=3.13×10^-5 4, α(P)=1.691E-6 24
	8+	1.5 ps 2	1061.3 3	E2		0.00329	B(E2)(W.u.)=0.77 +12-10, α=0.00329 5, α(K)=0.00274 4, α(L)=0.000426 6, α(M)=9.56E-5 13, α(N)=2.234E-5 31, α(O)=3.13E-6 4, α(P)=1.543E-7 22
2024.06	10+	0.9 ps 3	578.50 3	E2		0.01243	B(E2)(W.u.)=1.8E2 +9-5, α=0.01243 17, α(K)=0.00994 14, α(L)=0.001927 27, α(M)=0.000442 6, α(N)=0.0001029 14, α(O)=1.385E-5 19, α(P)=5.51E-7 8
2152.95	9-	0.54 ps 5	385.25 6	E2		0.0357	B(E2)(W.u.)=394 +48-40, α=0.0357 5, α(K)=0.0270 4, α(L)=0.00676 9, α(M)=0.001584 22, α(N)=0.000367 5, α(O)=4.73E-5 7, α(P)=1.437E-6 20
2152.95	9-	0.54 ps 5	707.6 4	E1		0.00292	B(E1)(W.u.)=0.00098 +10-8, α=0.00292 4, α(K)=0.002476 35, α(L)=0.000346 5, α(M)=7.66E-5 11, α(N)=1.790E-5 25, α(O)=2.54E-6 4, α(P)=1.322E-7 19
2280.29	8-	2.3 ps 5	367.2 3	E2		0.0409	α=0.0409 6, α(K)=0.0306 4, α(L)=0.00795 11, α(M)=0.001869 27, α(N)=0.000432 6, α(O)=5.55×10^-5 8, α(P)=1.618E-6 23
	8-	2.3 ps 5	512.10	M1		0.0385	B(M1)(W.u.)=0.028 +12-7, α=0.0385 5, α(K)=0.0324 5, α(L)=0.00477 7, α(M)=0.001065 15, α(N)=0.0002501 35, α(O)=3.59×10^-5 5, α(P)=1.937E-6 27
	8-	2.3 ps 5	835.2	E1		2.10×10^-3	B(E1)(W.u.)=1.01E-4 +29-25, α=2.10E-3 3, α(K)=0.001788 25, α(L)=0.0002474 35, α(M)=5.47E-5 8, α(N)=1.280E-5 18, α(O)=1.819E-6 25, α(P)=9.60E-8 13
2424.52	10+	1.3 ps +3-1	400.51 8	M1		0.0730	B(M1)(W.u.)=0.0401 +42-66, α=0.0730 10, α(K)=0.0613 9, α(L)=0.00911 13, α(M)=0.002035 29, α(N)=0.000478 7, α(O)=6.85×10^-5 10, α(P)=3.68E-6 5
	10+	1.3 ps +3-1	439.23 2	E2		0.02500	B(E2)(W.u.)=415 +35-62, α=0.02500 35, α(K)=0.01930 27, α(L)=0.00440 6, α(M)=0.001025 14, α(N)=0.0002376 33, α(O)=3.11E-5 4, α(P)=1.045E-6 15
	10+	1.3 ps +3-1	978.5 3	E2		0.00388	α=0.00388 5, α(K)=0.00322 5, α(L)=0.000511 7, α(M)=0.0001149 16, α(N)=2.69×10^-5 4, α(O)=3.75E-6 5, α(P)=1.812E-7 25
2428.94	9+		549.0 3	E2		0.01412	α=0.01412 20, α(K)=0.01123 16, α(L)=0.002237 32, α(M)=0.000515 7, α(N)=0.0001197 17, α(O)=1.603×10^-5 23, α(P)=6.20E-7 9
2572.61	10-	9.6 ps 8	292.33 5	E2		0.0800	B(E2)(W.u.)=208 +20-17, α=0.0800 11, α(K)=0.0566 8, α(L)=0.01794 25, α(M)=0.00426 6, α(N)=0.000983 14, α(O)=0.0001231 17, α(P)=2.88E-6 4
	10-	9.6 ps 8	419.48 25	M1		0.0647	B(M1)(W.u.)=0.0113 10, α=0.0647 9, α(K)=0.0543 8, α(L)=0.00806 11, α(M)=0.001799 25, α(N)=0.000423 6, α(O)=6.06×10^-5 9, α(P)=3.26E-6 5
	10-	9.6 ps 8	548.4	(E1)		0.00496	B(E1)(W.u.)=2.73E-5 +32-28, α=0.00496 7, α(K)=0.00420 6, α(L)=0.000595 8, α(M)=0.0001320 18, α(N)=3.08E-5 4, α(O)=4.34E-6 6, α(P)=2.218E-7 31
2594.85	10+		501.0 3	E2		0.01775	α=0.01775 25, α(K)=0.01396 20, α(L)=0.00293 4, α(M)=0.000677 10, α(N)=0.0001573 22, α(O)=2.088×10^-5 29, α(P)=7.66E-7 11
2594.85	10+		1149.4 3	E2		0.00280	α=0.00280 4, α(K)=0.002344 33, α(L)=0.000358 5, α(M)=8.01×10^-5 11, α(N)=1.874E-5 26, α(O)=2.64E-6 4, α(P)=1.320E-7 18
2604.69	11-	0.62 ps 5	451.76 10	E2		0.02320	B(E2)(W.u.)=4.0E2 6, α=0.02320 33, α(K)=0.01799 25, α(L)=0.00403 6, α(M)=0.000936 13, α(N)=0.0002171 30, α(O)=2.85E-5 4, α(P)=9.77E-7 14
2604.69	11-	0.62 ps 5	580.62 5	E1		0.00439	B(E1)(W.u.)=0.00105 +14-12, α=0.00439 6, α(K)=0.00372 5, α(L)=0.000525 7, α(M)=0.0001165 16, α(N)=2.72E-5 4, α(O)=3.84E-6 5, α(P)=1.970E-7 28
2634.29	12+	1.0 ps +5-8	610.23 4	E2		0.01094	B(E2)(W.u.)=1.3E2 +11-5, α=0.01094 15, α(K)=0.00880 12, α(L)=0.001660 23, α(M)=0.000380 5, α(N)=8.85E-5 12, α(O)=1.197E-5 17, α(P)=4.89E-7 7
2806.29	12+	4.4 ps 6	176.2 3	E2		0.412	α=0.412 6, α(K)=0.2361 35, α(L)=0.1349 21, α(M)=0.0328 5, α(N)=0.00751 12, α(O)=0.000895 14, α(P)=1.071×10^-5 16
	12+	4.4 ps 6	211.8 3	E2		0.2221	α=0.2221 33, α(K)=0.1402 20, α(L)=0.0628 10, α(M)=0.01516 23, α(N)=0.00348 5, α(O)=0.000422 6, α(P)=6.64×10^-6 10
	12+	4.4 ps 6	381.76 3	E2		0.0367	B(E2)(W.u.)=221 +35-27, α=0.0367 5, α(K)=0.0276 4, α(L)=0.00697 10, α(M)=0.001634 23, α(N)=0.000378 5, α(O)=4.88E-5 7, α(P)=1.470E-6 21
	12+	4.4 ps 6	782.2	E2		0.00622	B(E2)(W.u.)=2.02 +35-29, α=0.00622 9, α(K)=0.00510 7, α(L)=0.000868 12, α(M)=0.0001968 28, α(N)=4.59E-5 6, α(O)=6.33E-6 9, α(P)=2.86E-7 4
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2929.34	12+		505.0 3	E2		0.01739	α=0.01739 24, α(K)=0.01369 19, α(L)=0.00286 4, α(M)=0.000661 9, α(N)=0.0001536 22, α(O)=2.040×10^-5 29, α(P)=7.52E-7 11
2938.47	12-	8.3 ps 19	365.86 4	E2		0.0413	B(E2)(W.u.)=1.9E2 +6-4, α=0.0413 6, α(K)=0.0309 4, α(L)=0.00805 11, α(M)=0.001893 27, α(N)=0.000438 6, α(O)=5.62E-5 8, α(P)=1.633E-6 23
2994.9	11+		566.0 3	E2		0.01310	α=0.01310 18, α(K)=0.01046 15, α(L)=0.002050 29, α(M)=0.000471 7, α(N)=0.0001096 15, α(O)=1.472×10^-5 21, α(P)=5.79E-7 8
3077.18	13-		472.49 3	E2		0.02063	α=0.02063 29, α(K)=0.01610 23, α(L)=0.00350 5, α(M)=0.000812 11, α(N)=0.0001885 26, α(O)=2.487×10^-5 35, α(P)=8.78E-7 12
3127.01	14+	28 ps 10	320.72 3	E2		0.0606	B(E2)(W.u.)=1.1E2 +6-3, α=0.0606 8, α(K)=0.0439 6, α(L)=0.01279 18, α(M)=0.00303 4, α(N)=0.000698 10, α(O)=8.84E-5 12, α(P)=2.273E-6 32
3257.35	14+		623.06 7	E2		0.01041	α=0.01041, α(K)=0.00839 12, α(L)=0.001568 22, α(M)=0.000359 5, α(N)=8.35×10^-5 12, α(O)=1.132E-5 16, α(P)=4.67E-7 7
3416.97	14-	1.8 ps +4-13	478.49 4	E2		0.01997	B(E2)(W.u.)=2.3E2 +11-5, α=0.01997 28, α(K)=0.01561 22, α(L)=0.00337 5, α(M)=0.000781 11, α(N)=0.0001812 25, α(O)=2.394E-5 34, α(P)=8.53E-7 12
3461.3	14+		532.0 3	E2		0.01526	α=0.01526 21, α(K)=0.01209 17, α(L)=0.002452 35, α(M)=0.000565 8, α(N)=0.0001313 19, α(O)=1.754×10^-5 25, α(P)=6.67E-7 9
3578.77	16+	3.3 ps 2	451.76 10	E2		0.02320	B(E2)(W.u.)=171 10, α=0.02320 33, α(K)=0.01799 25, α(L)=0.00403 6, α(M)=0.000936 13, α(N)=0.0002171 30, α(O)=2.85E-5 4, α(P)=9.77E-7 14
3597.04	15-		519.86 9	E2		0.01616	α=0.01616 23, α(K)=0.01278 18, α(L)=0.00262 4, α(M)=0.000606 8, α(N)=0.0001407 20, α(O)=1.874×10^-5 26, α(P)=7.03E-7 10
3878.64	16+		621.28 10	E2		0.01048	α=0.01048 15, α(K)=0.00845 12, α(L)=0.001580 22, α(M)=0.000362 5, α(N)=8.42×10^-5 12, α(O)=1.140E-5 16, α(P)=4.70E-7 7
3972.40	16-	0.8 ps 3	555.43 6	E2		0.01372	B(E2)(W.u.)=2.5E2 +15-7, α=0.01372 19, α(K)=0.01093 15, α(L)=0.002163 30, α(M)=0.000498 7, α(N)=0.0001157 16, α(O)=1.551E-5 22, α(P)=6.04E-7 8
4149.15	18+	1.9 ps 3	570.38 4	E2		0.01286	B(E2)(W.u.)=93 +18-13, α=0.01286 18, α(K)=0.01027 14, α(L)=0.002005 28, α(M)=0.000461 6, α(N)=0.0001072 15, α(O)=1.440E-5 20, α(P)=5.69E-7 8
4185.44	17-		588.40 9	E2		0.01193	α=0.01193 17, α(K)=0.00956 13, α(L)=0.001837 26, α(M)=0.000421 6, α(N)=9.81×10^-5 14, α(O)=1.322E-5 19, α(P)=5.30E-7 7
4495.29	18+		616.65 8	E2		0.01067	α=0.01067 15, α(K)=0.00859 12, α(L)=0.001613 23, α(M)=0.000369 5, α(N)=8.60×10^-5 12, α(O)=1.163E-5 16, α(P)=4.78E-7 7
4562.30	18-		589.90 8	E2		0.01186	α=0.01186 17, α(K)=0.00950 13, α(L)=0.001824 26, α(M)=0.000418 6, α(N)=9.74×10^-5 14, α(O)=1.312E-5 18, α(P)=5.27E-7 7
4821.33	19-	0.38 ps +16-31	635.89 8	E2		0.00993	B(E2)(W.u.)=2.7E2 +21-9, α=0.00993 14, α(K)=0.00801 11, α(L)=0.001484 21, α(M)=0.000339 5, α(N)=7.90E-5 11, α(O)=1.072E-5 15, α(P)=4.47E-7 6
4822.28	20+		673.13 8	E2		0.00870	α=0.00870 12, α(K)=0.00706 10, α(L)=0.001274 18, α(M)=0.000291 4, α(N)=6.77×10^-5 9, α(O)=9.23E-6 13, α(P)=3.94E-7 6
5146.4	20+		651.1	E2		0.00940	α=0.00940 13, α(K)=0.00760 11, α(L)=0.001392 19, α(M)=0.000318 4, α(N)=7.41×10^-5 10, α(O)=1.007E-5 14, α(P)=4.24E-7 6
5169.7	20-		607.40 9	E2		0.01106	α=0.01106 15, α(K)=0.00889 12, α(L)=0.001682 24, α(M)=0.000385 5, α(N)=8.97×10^-5 13, α(O)=1.212E-5 17, α(P)=4.94E-7 7
5482.2	21-		660.9	E2		0.00908	α=0.00908 13, α(K)=0.00735 10, α(L)=0.001338 19, α(M)=0.000305 4, α(N)=7.11×10^-5 10, α(O)=9.68E-6 14, α(P)=4.10E-7 6
5584.76	22+		762.48 18	E2		0.00658	α=0.00658 9, α(K)=0.00539 8, α(L)=0.000925 13, α(M)=0.0002099 29, α(N)=4.90×10^-5 7, α(O)=6.74E-6 9, α(P)=3.02E-7 4
5816.6	22-		646.85 11	E2		0.00954	α=0.00954 13, α(K)=0.00771 11, α(L)=0.001417 20, α(M)=0.000324 5, α(N)=7.54×10^-5 11, α(O)=1.024E-5 14, α(P)=4.30E-7 6
5862.0	22+		715.6	E2		0.00758	α=0.00758 11, α(K)=0.00618 9, α(L)=0.001087 15, α(M)=0.0002472 35, α(N)=5.76×10^-5 8, α(O)=7.89E-6 11, α(P)=3.46E-7 5
6174.4	23-		692.2	E2		0.00817	α=0.00817 11, α(K)=0.00664 9, α(L)=0.001184 17, α(M)=0.000270 4, α(N)=6.29×10^-5 9, α(O)=8.59E-6 12, α(P)=3.71E-7 5
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
6423.1	24+		838.3	E2		0.00536	α=0.00536 8, α(K)=0.00441 6, α(L)=0.000733 10, α(M)=0.0001658 23, α(N)=3.87×10^-5 5, α(O)=5.36E-6 8, α(P)=2.481E-7 35
6529.1	24-		712.50 15	E2		0.00765	α=0.00765 11, α(K)=0.00623 9, α(L)=0.001099 15, α(M)=0.0002500 35, α(N)=5.83×10^-5 8, α(O)=7.98E-6 11, α(P)=3.49E-7 5
6651.9	24+		789.9	E2		0.00609	α=0.00609 9, α(K)=0.00500 7, α(L)=0.000847 12, α(M)=0.0001920 27, α(N)=4.48×10^-5 6, α(O)=6.18E-6 9, α(P)=2.81E-7 4
6925.8	25-		751.4	E2		0.00680	α=0.00680 10, α(K)=0.00556 8, α(L)=0.000960 13, α(M)=0.0002179 31, α(N)=5.08×10^-5 7, α(O)=6.99E-6 10, α(P)=3.12E-7 4
7313.8	26+		890.7	E2		0.00471	α=0.00471 7, α(K)=0.00390 5, α(L)=0.000635 9, α(M)=0.0001432 20, α(N)=3.34×10^-5 5, α(O)=4.65E-6 7, α(P)=2.191E-7 31
7319.1	26-		790.0	E2		0.00609	α=0.00609 9, α(K)=0.00500 7, α(L)=0.000847 12, α(M)=0.0001920 27, α(N)=4.48×10^-5 6, α(O)=6.18E-6 9, α(P)=2.81E-7 4
7488.0	26+		835.9	E2		0.00539	α=0.00539 8, α(K)=0.00444 6, α(L)=0.000738 10, α(M)=0.0001669 23, α(N)=3.90×10^-5 5, α(O)=5.39E-6 8, α(P)=2.495E-7 35
7755.2	27-		829.4	E2		0.00548	α=0.00548 8, α(K)=0.00451 6, α(L)=0.000752 11, α(M)=0.0001701 24, α(N)=3.97×10^-5 6, α(O)=5.50E-6 8, α(P)=2.54E-7 4
8187.7	28-		868.6	E2		0.00497	α=0.00497 7, α(K)=0.00410 6, α(L)=0.000673 9, α(M)=0.0001521 21, α(N)=3.55×10^-5 5, α(O)=4.93E-6 7, α(P)=2.306E-7 32
8234.7	28+		920.9	E2		0.00439	α=0.00439 6, α(K)=0.00364 5, α(L)=0.000587 8, α(M)=0.0001323 19, α(N)=3.09×10^-5 4, α(O)=4.30E-6 6, α(P)=2.047E-7 29
8323.9	(28+)		835.9	E2		0.00539	α=0.00539 8, α(K)=0.00444 6, α(L)=0.000738 10, α(M)=0.0001669 23, α(N)=3.90×10^-5 5, α(O)=5.39E-6 8, α(P)=2.495E-7 35
8660.8	29-		905.6	E2		0.00455	α=0.00455 6, α(K)=0.00377 5, α(L)=0.000610 9, α(M)=0.0001377 19, α(N)=3.22×10^-5 5, α(O)=4.47E-6 6, α(P)=2.118E-7 30
9124.8	30-		937.1	E2		0.00424	α=0.00424 6, α(K)=0.00351 5, α(L)=0.000564 8, α(M)=0.0001270 18, α(N)=2.97×10^-5 4, α(O)=4.14E-6 6, α(P)=1.977E-7 28
9153.5	(30+)		918.8	(E2)		0.00442	α=0.00442 6, α(K)=0.00366 5, α(L)=0.000590 8, α(M)=0.0001330 19, α(N)=3.11×10^-5 4, α(O)=4.33E-6 6, α(P)=2.057E-7 29
9606.3	31-		945.5	E2		0.00416	α=0.00416 6, α(K)=0.00345 5, α(L)=0.000552 8, α(M)=0.0001244 17, α(N)=2.91×10^-5 4, α(O)=4.05E-6 6, α(P)=1.941E-7 27
10067.0	32-		942.2	E2		0.00419	α=0.00419 6, α(K)=0.00347 5, α(L)=0.000557 8, α(M)=0.0001254 18, α(N)=2.93×10^-5 4, α(O)=4.09E-6 6, α(P)=1.955E-7 27
10502	(33-)		896.1	(E2)		0.00465	α=0.00465 7, α(K)=0.00385 5, α(L)=0.000626 9, α(M)=0.0001412 20, α(N)=3.30×10^-5 5, α(O)=4.58E-6 6, α(P)=2.164E-7 30
10969.4	(34-)		902.4	E2		0.00458	α=0.00458 6, α(K)=0.00379 5, α(L)=0.000615 9, α(M)=0.0001388 19, α(N)=3.24×10^-5 5, α(O)=4.51E-6 6, α(P)=2.133E-7 30
11420	(35-)		917.2	(E2)		0.00443	α=0.00443 6, α(K)=0.00367 5, α(L)=0.000593 8, α(M)=0.0001336 19, α(N)=3.12×10^-5 4, α(O)=4.34E-6 6, α(P)=2.064E-7 29
11917.8	(36-)		948.4	(E2)		0.00413	α=0.00413 6, α(K)=0.00343 5, α(L)=0.000548 8, α(M)=0.0001235 17, α(N)=2.89×10^-5 4, α(O)=4.03E-6 6, α(P)=1.929E-7 27
12392	(37-)		972.3	(E2)		0.00393	α=0.00393 5, α(K)=0.00326 5, α(L)=0.000518 7, α(M)=0.0001166 16, α(N)=2.72×10^-5 4, α(O)=3.81E-6 5, α(P)=1.835E-7 26

Data are from ¹⁶²Lu ε decay (primarily 2004Mc01) and in-beam γ data of studies, namely the level scheme of 2018Md01, as well as those of 1987Mo21 and 1980BeYG.

Levels: For levels with J=20-32, the average g-factor is 0.24 5 from the evaluation of 1989Ra17 and is based on the data of 1984Ma10.

Gammas: In their lifetime measurements, 1992Mc02 report only partial lifetimes (and, in some cases, reduced transition probabilities) for individual transitions, but not level lifetimes. For those levels having more than one deexciting transition, it has been necessary for the evaluator to compute the level half-life values from these reported quantities.

Q-value: S(2n)=17801 16, S(2p)=8335 29 (2021Wa16)

Q(β-)=-6990 keV 80	S(n)= 10058 keV 21	S(p)= 5210 keV 30	Q(α)= 3058 keV 29
Reference: 2021WA16

References:
A	¹⁶²Lu ε decay (1.37 M+1.5 M,	B	(HI,xnγ)
C	¹⁸⁶W(n,4P21N)

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0	A B	0+	18.87 m 19 % ε = 100
166.72 4	A B C	2+	415 ps 9	166.71 4	100	E2	0	0+
487.34 5	A B C	4+	14.3 ps 6	320.60 4	100	E2	166.72	2+
798.42 4	A B	2+		631.67 5 798.48 6	100.0 10 63.7 8	E2 E2	166.72 0	2+ 0+
924.14 5	A B C	6+	3.47 ps 21	436.80 2	100	E2	487.34	4+
992.07 5	A B	3+		193.5 4 504.45 21 825.29 6	3.3 9 17.8 16 100.0 16	M1+E2	798.42 487.34 166.72	2+ 4+ 2+
1006.20 6	A	0+		839.40 5 1006		E2 E0	166.72 0	2+ 0+
1129.59 5	A B	2+		124? 642.31 6 962.89 6 1129.65 19	49.3 25 80 8 100 6	(E0+M1+E2) E2	1006.20 487.34 166.72 0	0+ 4+ 2+ 0+
1150.21 8	A B	4+		351.8 2 662.88 8 983.5 4	17 4 100 9 13 7	E2 E2,M1 E2	798.42 487.34 166.72	2+ 4+ 2+
1198.01 8	A	2+,3,4+		399.59 8 1031.28 11	66 8 100 11		798.42 166.72	2+ 2+
1337.23 5	A	2+,3,4+		849.85 5 1170.55 5	30 3 100 4		487.34 166.72	4+ 2+
1343.08 17	A B	4+		213? 855.6 3 1176.61 23			1129.59 487.34 166.72	2+ 4+ 2+
1379.46 6	A	2+		387.39 6 581.09 20 892.13 9 1212.6 3 1379.42 24	65 5 30 7 50 5 33 7 100 12		992.07 798.42 487.34 166.72 0	3+ 2+ 4+ 2+ 0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1393.04 19	B	5+		400.7 3 905.9 3		E2 M1(+E2)	992.07 487.34	3+ 4+
1398.22 5	A	1,2+		1231.50 4 1398.19 10	100 8 77 3		166.72 0	2+ 0+
1445.56 5	B C	8+	1.1 ps 3	521.42 2	100	E2	924.14	6+
1454.87 5	A			462.76 8 656.43 4 1288.17 4	18.2 11 100.0 25 66.8 20		992.07 798.42 166.72	3+ 2+ 2+
1483.24 15	A B	5-		995.74 17	100 24	E1	487.34	4+
1500.69 16	A			1333.96 15	100 12		166.72	2+
1552.82 8	A	2+,3,4+		560.71 21 1065.49 9 1386.07 11	18 6 63 5 100 9		992.07 487.34 166.72	3+ 4+ 2+
1568.11 5	A			575.95 18 1401.38 4	12.7 24 100 8		992.07 166.72	3+ 2+
1573.32 10	B	6+		423.12 6 648.7	100 6 69 12	E2 E2,M1	1150.21 924.14	4+ 6+
1609.00 12	A B	4-		617.1 3 1121.63 12	100 12	D E1	992.07 487.34	3+ 4+
1636.59 6	A	1,2+		1469.88 5 1636.39 15	100 4 75 7		166.72 0	2+ 0+
1637.90 6	A			1150.56 4	100 10		487.34	4+
1647.19 10	B	6+		304.4 3 1160.2 4	100	E2 E2	1343.08 487.34	4+ 4+
1673.06 7	A			680.87 8 874.76 9 1506.2 3	25.5 20 100 4 61 7		992.07 798.42 166.72	3+ 2+ 2+
1676.52 11	A	2+,3,4+		1189.18 10 1509.8 3	52 4 100 17		487.34 166.72	4+ 2+
1716.79 10	A			587.16 12 918.44 14	21 5 100 26		1129.59 798.42	2+ 2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1741.31 24	A			1253.97 23	100 18		487.34	4+
1767.70 13	B	7-		284.3 3 843.0	100	E1	1483.24 924.14	5- 6+
1853.65 21	A			1686.92 20	100 19		166.72	2+
1860.58 10	A	1,2+		854.34 13 868.48 17 1062.24 18	37 7 100 17 56 17		1006.20 992.07 798.42	0+ 3+ 2+
1879.91 21	B	7+		486.8 3 955.8 3		E2	1393.04 924.14	5+ 6+
1913.37 18	B	6-		304.4 3 429.8 3 989.8 3		E2 M1 (E1)	1609.00 1483.24 924.14	4- 5- 6+
1938.94 16	A	2+,3,4+		1451.60 18 1772.2 3	100 9 97 16		487.34 166.72	4+ 2+
1985.29 7	B	8+	1.5 ps 2	338.12 7 412.01 19 539.66 6 1061.3 3	59 2 100 3 41 3 35 2	E2 E2 M1 E2	1647.19 1573.32 1445.56 924.14	6+ 6+ 8+ 6+
2024.06 6	B C	10+	0.9 ps 3	578.50 3	100	E2	1445.56	8+
2050.39 22	A			1251.97 21	100 15		798.42	2+
2059.49 9	A	2+,3,4+		1261.08 9 1572.07 21	100 23 85 15		798.42 487.34	2+ 4+
2092.36 16	A			1605.01 15	100 13		487.34	4+
2094.09 20	B	8+		447.0 3 1170.1 3			1647.19 924.14	6+ 6+
2099.00 8	A	1,2+		969.58 9 1092.44 14 1932.18 17	12 5 22 3 100 11		1129.59 1006.20 166.72	2+ 0+ 2+
2152.95 12	B	9-	0.54 ps 5	385.25 6 707.6 4	20.3 14 100 3	E2 E1	1767.70 1445.56	7- 8+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2269.50 11	A			1277.34 21 1471.10 12	39 7 100 12		992.07 798.42	3+ 2+
2280.29 21	B	8-	2.3 ps 5	367.2 3 512.10 835.2	66 5 100 33	E2 M1 E1	1913.37 1767.70 1445.56	6- 7- 8+
2399.0 3	A			1600.59 25	100 19		798.42	2+
2424.52 7	B	10+	1.3 ps +3-1	400.51 8 439.23 2 978.5 3	18.6 14 100 3	M1 E2 E2	2024.06 1985.29 1445.56	10+ 8+ 8+
2428.94 24	B	9+		549.0 3 983.4 3		E2	1879.91 1445.56	7+ 8+
2446.52 12	A	1,2+		1317.17 15 1440.00 17	100 21 32 9		1129.59 1006.20	2+ 0+
2549.67 15	A			1558.00 22 1750.94 19	88 17 100 24		992.07 798.42	3+ 2+
2572.61 21	B	10-	9.6 ps 8	292.33 5 419.48 25 548.4	100 3 91 4 48 4	E2 M1 (E1)	2280.29 2152.95 2024.06	8- 9- 10+
2594.85 20	B	10+		501.0 3 1149.4 3		E2 E2	2094.09 1445.56	8+ 8+
2604.69 8	B	11-	0.62 ps 5	451.76 10 580.62 5	77 100 5	E2 E1	2152.95 2024.06	9- 10+
2630.48 22	B	10+		1185.3 3			1445.56	8+
2634.29 7	B	12+	1.0 ps +5-8	610.23 4	100	E2	2024.06	10+
2789.82 15	A			1116.61 18 1991.60 21	55 5 100 18		1673.06 798.42	2+
2806.29 8	B	12+	4.4 ps 6	176.2 3 211.8 3 381.76 3 782.2	100 2 33 3	E2 E2 E2 E2	2630.48 2594.85 2424.52 2024.06	10+ 10+ 10+ 10+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2815.10 20	A			1360.17 24 1823.1 3	100 22 89 25		1454.87 992.07	3+
2825.80 11	A			1370.99 13 1833.65 14	57 9 100 13		1454.87 992.07	3+
2929.34 22	B	12+		505.0 3 905.1 3		E2	2424.52 2024.06	10+ 10+
2938.47 22	B	12-	8.3 ps 19	365.86 4	100	E2	2572.61	10-
2994.9 4	B	11+		566.0 3		E2	2428.94	9+
2996.55 24	A			2198.12 23	100 21		798.42	2+
3077.18 8	B	13-		472.49 3	100	E2	2604.69	11-
3127.01 8	B	14+	28 ps 10	320.72 3	100	E2	2806.29	12+
3128.89 20	B	(12+)		534.04 3			2594.85	10+
3257.35 10	B	14+		623.06 7	100	E2	2634.29	12+
3416.97 22	B	14-	1.8 ps +4-13	478.49 4	100	E2	2938.47	12-
3461.3 4	B	14+		532.0 3		E2	2929.34	12+
3561.8 5	B	(13+)		566.9 3			2994.9	11+
3578.77 13	B	16+	3.3 ps 2	451.76 10	100	E2	3127.01	14+
3597.04 12	B	15-		519.86 9	100	E2	3077.18	13-
3878.64 14	B	16+		621.28 10	100	E2	3257.35	14+
3972.40 23	B	16-	0.8 ps 3	555.43 6	100	E2	3416.97	14-
4137.7 6	B	(15+)		575.9 3			3561.8	(13+)
4149.15 14	B	18+	1.9 ps 3	570.38 4	100	E2	3578.77	16+
4185.44 15	B	17-		588.40 9	100	E2	3597.04	15-
4495.29 17	B	18+		616.65 8	100	E2	3878.64	16+
4562.30 24	B	18-		589.90 8	100	E2	3972.40	16-
4821.33 17	B	19-	0.38 ps +16-31	635.89 8	100	E2	4185.44	17-
4822.28 16	B	20+		673.13 8	100	E2	4149.15	18+
5146.4 11	B	20+		651.1	100	E2	4495.29	18+
5169.7 3	B	20-		607.40 9	100	E2	4562.30	18-
5482.2 11	B	21-		660.9	100	E2	4821.33	19-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5584.76 24	B	22+		762.48 18	100	E2	4822.28	20+
5816.6 3	B	22-		646.85 11	100	E2	5169.7	20-
5862.0 15	B	22+		715.6	100	E2	5146.4	20+
6174.4 15	B	23-		692.2	100	E2	5482.2	21-
6423.1 11	B	24+		838.3	100	E2	5584.76	22+
6529.1 4	B	24-		712.50 15	100	E2	5816.6	22-
6651.9 18	B	24+		789.9	100	E2	5862.0	22+
6925.8 18	B	25-		751.4	100	E2	6174.4	23-
7313.8 15	B	26+		890.7	100	E2	6423.1	24+
7319.1 11	B	26-		790.0	100	E2	6529.1	24-
7488.0	B	26+		835.9?	100	E2	6651.9	24+
7755.2 20	B	27-		829.4	100	E2	6925.8	25-
8187.7 15	B	28-		868.6	100	E2	7319.1	26-
8234.7 18	B	28+		920.9	100	E2	7313.8	26+
8323.9?	B	(28+)		835.9?	100	E2	7488.0	26+
8660.8 23	B	29-		905.6	100	E2	7755.2	27-
9124.8 18	B	30-		937.1	100	E2	8187.7	28-
9153.5 21	B	(30+)		918.8	100	(E2)	8234.7	28+
9606.3 25	B	31-		945.5	100	E2	8660.8	29-
10067.0 21	B	32-		942.2	100	E2	9124.8	30-
10502 3	B	(33-)		896.1	100	(E2)	9606.3	31-
10969.4 23	B	(34-)		902.4	100	E2	10067.0	32-
11420 3	B	(35-)		917.2	100	(E2)	10502	(33-)
11917.8?	B	(36-)		948.4?	100	(E2)	10969.4	(34-)
12392?	B	(37-)		972.3?	100	(E2)	11420	(35-)

E(level)	J^π(level)	T_1/2(level)	Comments
0	0+	18.87 m 19 % ε = 100	For ¹⁶⁰Yb-¹⁶²Yb, Δ<r²>≈0.22 fm². For ¹⁶²Yb-¹⁶⁴Yb, Δ<r²>≈0.21 fm² (1985Ne09, read from plot by the evaluator). Related calculations: 1989Ba43. Other isotope shift data: 1982Bu21. E(level): For ¹⁶⁰Yb-¹⁶²Yb, Δ<r²>≈0.22 fm². For ¹⁶²Yb-¹⁶⁴Yb, Δ<r²>≈0.21 fm² (1985Ne09, read from plot by the evaluator). Related calculations: 1989Ba43. Other isotope shift data: 1982Bu21. K^π=0⁺ ground-state band.
166.72	2+	415 ps 9	E(level): K^π=0⁺ ground-state band.
487.34	4+	14.3 ps 6	E(level): K^π=0⁺ ground-state band.
798.42	2+		E(level): Even γ band.
924.14	6+	3.47 ps 21	E(level): K^π=0⁺ ground-state band.
992.07	3+		E(level): Odd γ band.
1006.20	0+		E(level): Second K^π=0⁺ band.
1129.59	2+		E(level): Second K^π=0⁺ band.
1150.21	4+		E(level): Even γ band.
1343.08	4+		E(level): Second K^π=0⁺ band.
1393.04	5+		E(level): Odd γ band.
1445.56	8+	1.1 ps 3	E(level): K^π=0⁺ ground-state band.
1483.24	5-		E(level): Negative-parity, odd-spin band.
1573.32	6+		E(level): Even γ band.
1609.00	4-		E(level): Negative-parity, even-spin band.
1647.19	6+		E(level): Second K^π=0⁺ band.
1767.70	7-		E(level): Negative-parity, odd-spin band.
1879.91	7+		E(level): Odd γ band.
1913.37	6-		E(level): Negative-parity, even-spin band.
1985.29	8+	1.5 ps 2	E(level): Even γ band.
2024.06	10+	0.9 ps 3	E(level): K^π=0⁺ ground-state band.
2094.09	8+		E(level): Second K^π=0⁺ band.
2152.95	9-	0.54 ps 5	E(level): Negative-parity, odd-spin band.
2280.29	8-	2.3 ps 5	E(level): Negative-parity, even-spin band.
2424.52	10+	1.3 ps +3-1	E(level): Even γ band.
E(level)	J^π(level)	T_1/2(level)	Comments
2428.94	9+		E(level): Odd γ band.
2572.61	10-	9.6 ps 8	E(level): Negative-parity, even-spin band.
2594.85	10+		E(level): Second K^π=0⁺ band.
2604.69	11-	0.62 ps 5	E(level): Negative-parity, odd-spin band.
2630.48	10+		E(level): Positive-parity, even-spin band.
2634.29	12+	1.0 ps +5-8	E(level): K^π=0⁺ ground-state band.
2806.29	12+	4.4 ps 6	E(level): Positive-parity, even-spin band.
2929.34	12+		E(level): Even γ band.
2938.47	12-	8.3 ps 19	E(level): Negative-parity, even-spin band.
2994.9	11+		E(level): Odd γ band.
3077.18	13-		E(level): Negative-parity, odd-spin band.
3127.01	14+	28 ps 10	E(level): Positive-parity, even-spin band.
3128.89	(12+)		E(level): Second K^π=0⁺ band.
3257.35	14+		E(level): K^π=0⁺ ground-state band.
3416.97	14-	1.8 ps +4-13	E(level): Negative-parity, even-spin band.
3461.3	14+		E(level): Even γ band.
3561.8	(13+)		E(level): Odd γ band.
3578.77	16+	3.3 ps 2	E(level): Positive-parity, even-spin band.
3597.04	15-		E(level): Negative-parity, odd-spin band.
3878.64	16+		E(level): K^π=0⁺ ground-state band.
3972.40	16-	0.8 ps 3	E(level): Negative-parity, even-spin band.
4137.7	(15+)		E(level): Odd γ band.
4149.15	18+	1.9 ps 3	E(level): Positive-parity, even-spin band.
4185.44	17-		E(level): Negative-parity, odd-spin band.
4495.29	18+		E(level): K^π=0⁺ ground-state band.
E(level)	J^π(level)	T_1/2(level)	Comments
4562.30	18-		E(level): Negative-parity, even-spin band.
4821.33	19-	0.38 ps +16-31	E(level): Negative-parity, odd-spin band.
4822.28	20+		E(level): Positive-parity, even-spin band.
5146.4	20+		E(level): K^π=0⁺ ground-state band.
5169.7	20-		E(level): Negative-parity, even-spin band.
5482.2	21-		E(level): Negative-parity, odd-spin band.
5584.76	22+		E(level): Positive-parity, even-spin band.
5816.6	22-		E(level): Negative-parity, even-spin band.
5862.0	22+		E(level): K^π=0⁺ ground-state band.
6174.4	23-		E(level): Negative-parity, odd-spin band.
6423.1	24+		E(level): Positive-parity, even-spin band.
6529.1	24-		E(level): Negative-parity, even-spin band.
6651.9	24+		E(level): K^π=0⁺ ground-state band.
6925.8	25-		E(level): Negative-parity, odd-spin band.
7313.8	26+		E(level): Positive-parity, even-spin band.
7319.1	26-		E(level): Negative-parity, even-spin band.
7488.0	26+		E(level): K^π=0⁺ ground-state band.
7755.2	27-		E(level): Negative-parity, odd-spin band.
8187.7	28-		E(level): Negative-parity, even-spin band.
8234.7	28+		E(level): Positive-parity, even-spin band.
8323.9	(28+)		E(level): K^π=0⁺ ground-state band.
8660.8	29-		E(level): Negative-parity, odd-spin band.
9124.8	30-		E(level): Negative-parity, even-spin band.
9153.5	(30+)		E(level): Positive-parity, even-spin band.
9606.3	31-		E(level): Negative-parity, odd-spin band.
E(level)	J^π(level)	T_1/2(level)	Comments
10067.0	32-		E(level): Negative-parity, even-spin band.
10502	(33-)		E(level): Negative-parity, odd-spin band.
10969.4	(34-)		E(level): Negative-parity, even-spin band.
11420	(35-)		E(level): Negative-parity, odd-spin band.
11917.8	(36-)		E(level): Negative-parity, even-spin band.
12392	(37-)		E(level): Negative-parity, odd-spin band.

E(level)	E(gamma)	Comments
487.34	320.60	E(γ): Multiply placed M(γ): from γ(θ) (1980BeYG), R_DCO and A_P (2018Md01) in ¹⁵⁰Sm(¹⁶O,4nγ). See the comment in the (HI,xnγ) data set.
798.42	631.67	M(γ): mult=Q from γγ(θ) in ¹⁶²Lu ε decay (1983Ge08). From the observed γ decay from this level, the evaluator has concluded that the deexciting γ’s are much more reasonably assigned as E2 than M2.
924.14	436.80	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
1006.20	839.40	M(γ): mult=Q, from γγ(θ) in ¹⁶²Lu ε decay (1983Ge08). The evaluator has regarded mult=E2 to be a more reasonable choice than the alternative, mult=M2.
1129.59	962.89	M(γ): (E2⁺M1) assigned from α(K)exp; however value is considerably larger than that predicted for E2⁺M1 transition, which could indicate an E0 contribution.
1445.56	521.42	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
1647.19	304.4	E(γ): Multiply placed
1913.37	304.4	E(γ): Multiply placed
1985.29	539.66	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
2024.06	578.50	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
2152.95	707.6	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
2424.52	400.51	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
2424.52	439.23	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
2604.69	451.76	E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
2604.69	580.62	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
3077.18	472.49	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
3127.01	320.72	E(γ): Multiply placed
3578.77	451.76	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
3972.40	555.43	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
4149.15	570.38	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
4185.44	588.40	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
4562.30	589.90	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
4821.33	635.89	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
4822.28	673.13	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
6529.1	712.50	M(γ): From internal conversion coefficients measured in the in-beam study of the ¹⁵⁰Sm(¹⁶O,4nγ) reaction (1980BeYG). Usually these data are supplemented by DCO ratios, γ(θ) data and polarization asymmetry measurements from the heavy-ion studies, but we mention only the conversion data, since they alone can provide a distinction between E1/M1 and E2/M2 for dipole and quadrupole transitions, respectively.
E(level)	E(gamma)	Comments
7488.0	835.9	E(γ): Multiply placed
8323.9	835.9	E(γ): Multiply placed