List of levels for 148SM

Author: N. Nica | Citation: Nucl. Data Sheets 208, 1 (2026) | Cutoff date: 17-Jan-2026

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
550.263	2+	7.71 ps 32	550.273 9	E2		0.00998	B(E2)(W.u.)=30.9 +14-12, α=0.00998 14, α(K)=0.00825 12, α(L)=0.001360 19, α(M)=0.000296 4, α(N)=6.66E-5 9, α(O)=9.59E-6 13, α(P)=4.78E-7 7
1161.547	3-	0.6 ps +4-2	611.293 8	E1		0.00277	B(E1)(W.u.)=0.0018 +9-7, α=0.00277 4, α(K)=0.002374 33, α(L)=0.000312 4, α(M)=6.63E-5 9, α(N)=1.498E-5 21, α(O)=2.230E-6 31, α(P)=1.358E-7 19
1180.252	4+	2.37 ps 22	629.987 8	E2		0.00710	B(E2)(W.u.)=51 +6-5, α=0.00710 10, α(K)=0.00591 8, α(L)=0.000932 13, α(M)=0.0002023 28, α(N)=4.55E-5 6, α(O)=6.61E-6 9, α(P)=3.46E-7 5
1424.445	0+		874.18 3	E2		0.00332	α=0.00332 5, α(K)=0.00280 4, α(L)=0.000406 6, α(M)=8.74×10^-5 12, α(N)=1.972E-5 28, α(O)=2.91E-6 4, α(P)=1.663E-7 23
1454.113	2+	285 fs 28	903.831 15	M1+E2	+2.32 10	0.00339	B(E2)(W.u.)=29.8 +32-27, B(M1)(W.u.)=0.0082 +11-9, α=0.00339 5, α(K)=0.00287 4, α(L)=0.000406 6, α(M)=8.72E-5 13, α(N)=1.970E-5 30, α(O)=2.92E-6 4, α(P)=1.722E-7 28
1454.113	2+	285 fs 28	1454.110 20	E2		1.23×10^-3	B(E2)(W.u.)=3.27 +35-29, α=1.23E-3 2, α(K)=0.001000 14, α(L)=0.0001338 19, α(M)=2.86E-5 4, α(N)=6.46E-6 9, α(O)=9.66E-7 14, α(P)=5.96E-8 8
1465.139	1-	92 fs 8	914.916 15	E1		1.22×10^-3	B(E1)(W.u.)=0.00117 +12-10, α=1.22E-3 2, α(K)=0.001050 15, α(L)=0.0001354 19, α(M)=2.88E-5 4, α(N)=6.51E-6 9, α(O)=9.73E-7 14, α(P)=6.07E-8 8
1465.139	1-	92 fs 8	1465.101 13	E1		7.04×10^-4	B(E1)(W.u.)=5.5E-4 5, α=7.04E-4 10, α(K)=0.000449 6, α(L)=5.70E-5 8, α(M)=1.208E-5 17, α(N)=2.74E-6 4, α(O)=4.11E-7 6, α(P)=2.61E-8 4
1594.291	5-		414.028 12	E1+M2	-0.013 10	0.00670	α=0.00670 10, α(K)=0.00573 9, α(L)=0.000766 12, α(M)=0.0001633 26, α(N)=3.68×10^-5 6, α(O)=5.45E-6 9, α(P)=3.22E-7 5
1594.291	5-		432.745 8	E2		0.01903	α=0.01903 27, α(K)=0.01544 22, α(L)=0.00281 4, α(M)=0.000617 9, α(N)=0.0001382 19, α(O)=1.959×10^-5 27, α(P)=8.75E-7 12
1664.188	2+	0.25 ps 8	1113.92 3	M1+E2	-0.565 21	0.00279	B(E2)(W.u.)=4.5 +22-11, B(M1)(W.u.)=0.032 +15-8, α=0.00279 4, α(K)=0.00239 4, α(L)=0.000319 5, α(M)=6.81E-5 10, α(N)=1.544E-5 23, α(O)=2.322E-6 34, α(P)=1.466E-7 22
1664.188	2+	0.25 ps 8	1664.20 4	E2		1.04×10^-3	B(E2)(W.u.)=1.3 +6-3, α=1.04E-3 2, α(K)=0.000775 11, α(L)=0.0001023 14, α(M)=2.182E-5 31, α(N)=4.94E-6 7, α(O)=7.40E-7 10, α(P)=4.62E-8 6
1733.496	4+		279.30 5	E2		0.0703	α=0.0703 10, α(K)=0.0542 8, α(L)=0.01261 18, α(M)=0.00282 4, α(N)=0.000627 9, α(O)=8.56×10^-5 12, α(P)=2.87E-6 4
	4+		553.231 14	M1+E2	+1.66 20	0.0117	α=0.0117 4, α(K)=0.00976 35, α(L)=0.00150 4, α(M)=0.000324 8, α(N)=7.31×10^-5 18, α(O)=1.069E-5 29, α(P)=5.83E-7 24
	4+		571.962 7	E1		0.00320	α=0.00320 4, α(K)=0.00274 4, α(L)=0.000361 5, α(M)=7.68×10^-5 11, α(N)=1.735E-5 24, α(O)=2.58E-6 4, α(P)=1.564E-7 22
	4+		1183.208 16	E2		1.76×10^-3	α=1.76×10^-3 3, α(K)=0.001496 21, α(L)=0.0002054 29, α(M)=4.40E-5 6, α(N)=9.94E-6 14, α(O)=1.480E-6 21, α(P)=8.91E-8 12
1895.000	4+		300.65 7	[E1]		0.01463	α=0.01463 21, α(K)=0.01248 17, α(L)=0.001694 24, α(M)=0.000362 5, α(N)=8.14×10^-5 11, α(O)=1.195E-5 17, α(P)=6.86E-7 10
	4+		714.769 13	M1+E2		0.0070	α=0.0070 18, α(K)=0.0060 16, α(L)=0.00084 17, α(M)=0.00018 4, α(N)=4.1×10^-5 8, α(O)=6.1E-6 13, α(P)=3.6E-7 11
	4+		1344.740 23	E2		1.39×10^-3	α=1.39×10^-3 2, α(K)=0.001162 16, α(L)=0.0001569 22, α(M)=3.35E-5 5, α(N)=7.59E-6 11, α(O)=1.133E-6 16, α(P)=6.92E-8 10
1903.767	3+		1353.509 17	M1+E2	+8.2 12	1.39×10^-3	α=1.39×10^-3 2, α(K)=0.001155 16, α(L)=0.0001558 22, α(M)=3.33E-5 5, α(N)=7.53E-6 11, α(O)=1.125E-6 16, α(P)=6.89E-8 10
1905.917	6+		311.570 20	E1		0.01337	α=0.01337 19, α(K)=0.01141 16, α(L)=0.001547 22, α(M)=0.000330 5, α(N)=7.43×10^-5 10, α(O)=1.092E-5 15, α(P)=6.29E-7 9
1905.917	6+		725.673 9	E2		0.00506	α=0.00506 7, α(K)=0.00424 6, α(L)=0.000642 9, α(M)=0.0001389 19, α(N)=3.13×10^-5 4, α(O)=4.58E-6 6, α(P)=2.501E-7 35
1972.482	2+		1422.216 20	M1+E2	-0.556 24	1.66×10^-3	α=1.66×10^-3 3, α(K)=0.001379 20, α(L)=0.0001820 27, α(M)=3.88E-5 6, α(N)=8.80E-6 13, α(O)=1.325E-6 20, α(P)=8.43E-8 13
2031.451	4-		437.18 4	M1		0.0303	α=0.0303 4, α(K)=0.0258 4, α(L)=0.00353 5, α(M)=0.000756 11, α(N)=0.0001715 24, α(O)=2.58×10^-5 4, α(P)=1.621E-6 23
2031.451	4-		869.891 8	M1+E2	-1.7 3	0.00391	α=0.00391 18, α(K)=0.00331 16, α(L)=0.000466 19, α(M)=0.000100 4, α(N)=2.26×10^-5 9, α(O)=3.36E-6 14, α(P)=2.00E-7 10
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2057.970	2-		592.83 3	M1+E2		0.0111	α=0.0111 29, α(K)=0.0094 26, α(L)=0.00136 26, α(M)=0.00029 5, α(N)=6.6×10^-5 12, α(O)=9.8E-6 20, α(P)=5.7E-7 17
2057.970	2-		896.42 3	M1+E2	+1.32 9	0.00386	α=0.00386 8, α(K)=0.00328 7, α(L)=0.000456 9, α(M)=9.77×10^-5 20, α(N)=2.21E-5 4, α(O)=3.29E-6 7, α(P)=1.99E-7 5
2095.596	6+		189.721 16	M1,E2		0.264	α=0.264 15, α(K)=0.207 30, α(L)=0.045 12, α(M)=0.0100 28, α(N)=0.0022 6, α(O)=0.00031 7, α(P)=1.19×10^-5 32
	6+		501.312 11	E1+M2	-0.017 14	0.00431	α=0.00431 7, α(K)=0.00369 6, α(L)=0.000489 9, α(M)=0.0001041 19, α(N)=2.35×10^-5 4, α(O)=3.49E-6 6, α(P)=2.09E-7 4
	6+		915.331 8	E2		0.00300	α=0.00300 4, α(K)=0.00254 4, α(L)=0.000364 5, α(M)=7.83×10^-5 11, α(N)=1.769E-5 25, α(O)=2.61E-6 4, α(P)=1.508E-7 21
2111.075	4+		216.16 6	M1		0.1952	α=0.1952 27, α(K)=0.1657 23, α(L)=0.02317 32, α(M)=0.00497 7, α(N)=0.001127 16, α(O)=0.0001691 24, α(P)=1.052×10^-5 15
	4+		377.560 20	M1		0.0442	α=0.0442 6, α(K)=0.0376 5, α(L)=0.00518 7, α(M)=0.001109 16, α(N)=0.0002515 35, α(O)=3.78×10^-5 5, α(P)=2.370E-6 33
	4+		446.52 6	(E2)		0.01744	α=0.01744 24, α(K)=0.01419 20, α(L)=0.00255 4, α(M)=0.000559 8, α(N)=0.0001252 18, α(O)=1.778×10^-5 25, α(P)=8.07E-7 11
	4+		516.793 14	E1+M2	0.48 8	0.0150	α=0.0150 30, α(K)=0.0126 25, α(L)=0.0019 4, α(M)=0.00041 9, α(N)=9.3×10^-5 20, α(O)=1.38E-5 29, α(P)=8.4E-7 18
	4+		930.807 19	E2		0.00290	α=0.00290 4, α(K)=0.002452 34, α(L)=0.000350 5, α(M)=7.53×10^-5 11, α(N)=1.701E-5 24, α(O)=2.513E-6 35, α(P)=1.455E-7 20
	4+		1560.786 17	E2		1.12×10^-3	α=1.12×10^-3 2, α(K)=0.000874 12, α(L)=0.0001161 16, α(M)=2.477E-5 35, α(N)=5.61E-6 8, α(O)=8.40E-7 12, α(P)=5.21E-8 7
2128.59	7-		222.71 12	E1		0.0318	α=0.0318 4, α(K)=0.0270 4, α(L)=0.00373 5, α(M)=0.000796 11, α(N)=0.0001788 25, α(O)=2.61×10^-5 4, α(P)=1.448E-6 20
2128.59	7-		534.38 7	E2		0.01077	α=0.01077 15, α(K)=0.00888 12, α(L)=0.001480 21, α(M)=0.000323 5, α(N)=7.25×10^-5 10, α(O)=1.043E-5 15, α(P)=5.14E-7 7
2146.360	2+	< 64.1 fs	1596.08 3	M1+E2	-0.11 5	1.45×10^-3	α=1.45×10^-3 2, α(K)=0.001137 16, α(L)=0.0001491 21, α(M)=3.18E-5 5, α(N)=7.21E-6 10, α(O)=1.087E-6 16, α(P)=6.98E-8 10
2147.552	5+		116.01 4	E1		0.1841	α=0.1841 26, α(K)=0.1556 22, α(L)=0.02248 32, α(M)=0.00481 7, α(N)=0.001073 15, α(O)=0.0001528 21, α(P)=7.69×10^-6 11
	5+		241.653 15	M1+E2	-0.34 11	0.1409	α=0.1409 29, α(K)=0.1185 30, α(L)=0.0176 4, α(M)=0.00379 10, α(N)=0.000857 20, α(O)=0.0001269 23, α(P)=7.41×10^-6 25
	5+		243.83 4	E2		0.1086	α=0.1086 15, α(K)=0.0817 11, α(L)=0.02098 29, α(M)=0.00472 7, α(N)=0.001046 15, α(O)=0.0001413 20, α(P)=4.22×10^-6 6
	5+		252.60 3	M1,E2		0.112	α=0.112 16, α(K)=0.091 18, α(L)=0.0167 16, α(M)=0.0037 4, α(N)=0.00083 9, α(O)=0.000117 7, α(P)=5.4×10^-6 15
	5+		414.057 16	M1+E2	-1.8 8	0.0247	α=0.0247 35, α(K)=0.0203 32, α(L)=0.00343 22, α(M)=0.00075 4, α(N)=0.000168 10, α(O)=2.42×10^-5 19, α(P)=1.19E-6 23
	5+		553.260 15	E1		0.00344	α=0.00344 5, α(K)=0.00295 4, α(L)=0.000389 5, α(M)=8.28×10^-5 12, α(N)=1.869E-5 26, α(O)=2.78E-6 4, α(P)=1.680E-7 24
	5+		967.306 17	M1+E2		0.0035	α=0.0035 8, α(K)=0.0030 7, α(L)=0.00040 8, α(M)=8.6×10^-5 17, α(N)=2.0E-5 4, α(O)=2.9E-6 6, α(P)=1.8E-7 5
2194.071	6+		98.530 20	M1+E2	0.18	1.786	α=1.786 25, α(K)=1.486 21, α(L)=0.2352 33, α(M)=0.0511 7, α(N)=0.01152 16, α(O)=0.001689 24, α(P)=9.40×10^-5 13
	6+		288.141 13	M1+E2	+0.088 21	0.0898	α=0.0898 13, α(K)=0.0763 11, α(L)=0.01061 15, α(M)=0.002277 32, α(N)=0.000516 7, α(O)=7.75×10^-5 11, α(P)=4.82E-6 7
	6+		599.81 3	E1+M2	-0.021 11	0.00290	α=0.00290 5, α(K)=0.00249 4, α(L)=0.000327 5, α(M)=6.96×10^-5 11, α(N)=1.573E-5 26, α(O)=2.34E-6 4, α(P)=1.423E-7 24
	6+		1013.808 11	E2+M3	-0.025 14	0.00243	α=0.00243 4, α(K)=0.002058 31, α(L)=0.000290 5, α(M)=6.22×10^-5 10, α(N)=1.404E-5 22, α(O)=2.082E-6 33, α(P)=1.224E-7 19
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2214.263	5+		66.72 9	M1		5.43	α=5.43 8, α(K)=4.60 7, α(L)=0.656 10, α(M)=0.1410 21, α(N)=0.0319 5, α(O)=0.00478 7, α(P)=0.000294 4
	5+		182.83 3	E1		0.0537	α=0.0537 8, α(K)=0.0456 6, α(L)=0.00636 9, α(M)=0.001359 19, α(N)=0.000305 4, α(O)=4.42×10^-5 6, α(P)=2.391E-6 33
	5+		308.45 10	E2,M1		0.063	α=0.063 12, α(K)=0.052 12, α(L)=0.00882 13, α(M)=0.00193 4, α(N)=0.000433 7, α(O)=6.23×10^-5 24, α(P)=3.1E-6 9
	5+		310.14 10	E2		0.0507	α=0.0507 7, α(K)=0.0397 6, α(L)=0.00863 12, α(M)=0.001920 27, α(N)=0.000428 6, α(O)=5.90×10^-5 8, α(P)=2.145E-6 30
	5+		319.270 20	M1,E2		0.057	α=0.057 11, α(K)=0.047 11, α(L)=0.00792 18, α(M)=0.001730 24, α(N)=0.000389 6, α(O)=5.61×10^-5 29, α(P)=2.8E-6 9
	5+		480.89 8	M1		0.02376	α=0.02376 33, α(K)=0.02025 28, α(L)=0.00276 4, α(M)=0.000591 8, α(N)=0.0001340 19, α(O)=2.016×10^-5 28, α(P)=1.269E-6 18
	5+		620.04 3	E1+M2	+0.13 5	0.0033	α=0.0033 5, α(K)=0.0028 4, α(L)=0.00037 6, α(M)=8.0×10^-5 14, α(N)=1.81E-5 32, α(O)=2.7E-6 5, α(P)=1.64E-7 29
	5+		1033.986 14	M1+E2	-1.9 6	0.00260	α=0.00260 21, α(K)=0.00222 18, α(L)=0.000306 22, α(M)=6.5×10^-5 5, α(N)=1.48E-5 10, α(O)=2.21E-6 16, α(P)=1.33E-7 12
2228.134	4+		495.25 6	M1		0.02205	α=0.02205 31, α(K)=0.01880 26, α(L)=0.00256 4, α(M)=0.000548 8, α(N)=0.0001243 17, α(O)=1.869×10^-5 26, α(P)=1.177E-6 16
	4+		1047.570 20	M1		0.00353	α=0.00353 5, α(K)=0.00302 4, α(L)=0.000401 6, α(M)=8.55×10^-5 12, α(N)=1.940E-5 27, α(O)=2.92E-6 4, α(P)=1.865E-7 26
	4+		1677.85 3	E2		1.03×10^-3	α=1.03×10^-3 1, α(K)=0.000763 11, α(L)=0.0001007 14, α(M)=2.147E-5 30, α(N)=4.86E-6 7, α(O)=7.28E-7 10, α(P)=4.55E-8 6
2313.63	2+		1152.20 15	E1+M2	-0.10 9	0.00086	α=0.00086 15, α(K)=0.00073 13, α(L)=9.5×10^-5 18, α(M)=2.0E-5 4, α(N)=4.5E-6 9, α(O)=6.8E-7 13, α(P)=4.3E-8 8
2313.63	2+		1763.26 8	M1+E2	+2.2 5	1.04×10^-3	α=1.04×10^-3 3, α(K)=0.000732 21, α(L)=9.62E-5 27, α(M)=2.05E-5 6, α(N)=4.64E-6 13, α(O)=6.97E-7 20, α(P)=4.39E-8 14
2327.743	4+		432.745 8	M1		0.0311	α=0.0311 4, α(K)=0.0265 4, α(L)=0.00363 5, α(M)=0.000776 11, α(N)=0.0001761 25, α(O)=2.65×10^-5 4, α(P)=1.664E-6 23
2327.743	4+		1146.805 14	M1+E2	-2.0 5	0.00207	α=0.00207 11, α(K)=0.00176 9, α(L)=0.000240 12, α(M)=5.14×10^-5 25, α(N)=1.16E-5 6, α(O)=1.74E-6 9, α(P)=1.06E-7 6
2339.22	3-		1788.90 9	E1+M2	+0.06 4	8.04×10^-4	α=8.04×10^-4 15, α(K)=0.000328 11, α(L)=4.15E-5 15, α(M)=8.79E-6 32, α(N)=1.99E-6 7, α(O)=2.99E-7 11, α(P)=1.91E-8 7
2374.426	5+,6+		468.500 12	M1+E2	0.41 GE	0.020	α=0.020 4, α(K)=0.016 4, α(L)=0.00252 33, α(M)=0.00055 7, α(N)=0.000123 15, α(O)=1.80×10^-5 27, α(P)=9.9E-7 28
2381.68	2+	87 fs 17	1831.40 10	M1+E2	+0.46 8	1.17×10^-3	B(E2)(W.u.)=1.18 +47-36, B(M1)(W.u.)=0.034 +8-6, α=1.17E-3 2, α(K)=0.000804 15, α(L)=0.0001051 19, α(M)=2.24E-5 4, α(N)=5.07E-6 9, α(O)=7.65E-7 14, α(P)=4.91E-8 9
2390.43	3+		1840.06 8	M1+E2	-1.37 12	1.05×10^-3	α=1.05×10^-3 2, α(K)=0.000707 13, α(L)=9.25E-5 16, α(M)=1.971E-5 35, α(N)=4.47E-6 8, α(O)=6.72E-7 12, α(P)=4.26E-8 8
2392.38	7+		486.45 6	M1+E2	-0.15 8	0.0229	α=0.0229 4, α(K)=0.0195 4, α(L)=0.00267 4, α(M)=0.000571 9, α(N)=0.0001294 21, α(O)=1.944×10^-5 32, α(P)=1.220E-6 24
2490.056	4+		756.581 12	M1,E2		0.0061	α=0.0061 16, α(K)=0.0052 14, α(L)=0.00073 15, α(M)=0.000157 32, α(N)=3.5×10^-5 7, α(O)=5.3E-6 12, α(P)=3.2E-7 9
	4+		1309.778 16	M1+E2		0.00179	α=0.00179 33, α(K)=0.00151 28, α(L)=0.000201 35, α(M)=4.3×10^-5 7, α(N)=9.7E-6 17, α(O)=1.46E-6 26, α(P)=9.2E-8 19
	4+		1328.504 15	E1		7.08×10^-4	α=7.08×10^-4 10, α(K)=0.000531 7, α(L)=6.76E-5 9, α(M)=1.434E-5 20, α(N)=3.25E-6 5, α(O)=4.87E-7 7, α(P)=3.09E-8 4
2524.30	4+		296.21 7	M1		0.0836	α=0.0836 12, α(K)=0.0711 10, α(L)=0.00985 14, α(M)=0.002112 30, α(N)=0.000479 7, α(O)=7.19×10^-5 10, α(P)=4.49E-6 6
	4+		310.14 10	M1		0.0740	α=0.0740 10, α(K)=0.0630 9, α(L)=0.00871 12, α(M)=0.001868 26, α(N)=0.000424 6, α(O)=6.36×10^-5 9, α(P)=3.98E-6 6
	4+		929.85 3	[E1]		1.18×10^-3	α=1.18×10^-3 2, α(K)=0.001018 14, α(L)=0.0001312 18, α(M)=2.79E-5 4, α(N)=6.30E-6 9, α(O)=9.43E-7 13, α(P)=5.88E-8 8
	4+		1343.87 3	M1+E2	+0.20	1.98×10^-3	α=1.98×10^-3 3, α(K)=0.001668 23, α(L)=0.0002200 31, α(M)=4.69E-5 7, α(N)=1.064E-5 15, α(O)=1.604E-6 22, α(P)=1.026E-7 14
	4+		1362.640 19	E1		7.02×10^-4	α=7.02×10^-4 10, α(K)=0.000509 7, α(L)=6.46E-5 9, α(M)=1.371E-5 19, α(N)=3.10E-6 4, α(O)=4.66E-7 7, α(P)=2.95E-8 4
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2544.46	8+		415.9 1	E1		0.00661	α=0.00661 9, α(K)=0.00565 8, α(L)=0.000755 11, α(M)=0.0001610 23, α(N)=3.63×10^-5 5, α(O)=5.37E-6 8, α(P)=3.18E-7 4
	8+		449.0 11	E2		0.01717	α=0.01717 27, α(K)=0.01398 22, α(L)=0.00250 4, α(M)=0.000549 9, α(N)=0.0001230 20, α(O)=1.748×10^-5 28, α(P)=7.96E-7 12
	8+		638.5 1	E2		0.00687	α=0.00687 10, α(K)=0.00573 8, α(L)=0.000899 13, α(M)=0.0001951 27, α(N)=4.39×10^-5 6, α(O)=6.38E-6 9, α(P)=3.35E-7 5
2567.90	2+		2017.65 19	M1+E2		0.00102	α=0.00102 10, α(K)=0.00061 7, α(L)=7.9×10^-5 9, α(M)=1.69E-5 19, α(N)=3.8E-6 4, α(O)=5.8E-7 7, α(P)=3.7E-8 5
2583.901	4(-)		989.606 10	M1,E2		0.0033	α=0.0033 7, α(K)=0.0028 7, α(L)=0.00038 8, α(M)=8.2×10^-5 16, α(N)=1.9E-5 4, α(O)=2.8E-6 6, α(P)=1.7E-7 4
2633.16	3-		2082.88 9	E1		9.31×10^-4	α=9.31×10^-4 13, α(K)=0.0002527 35, α(L)=3.17E-5 4, α(M)=6.73E-6 9, α(N)=1.523E-6 21, α(O)=2.293E-7 32, α(P)=1.471E-8 21
2640.89	5+		735.00 5	M1+E2	-1.1 6	0.0064	α=0.0064 12, α(K)=0.0055 10, α(L)=0.00077 11, α(M)=0.000165 24, α(N)=3.7×10^-5 5, α(O)=5.6E-6 9, α(P)=3.3E-7 7
2640.89	5+		1460.630 19	M1+E2	+2.1 16	0.00131	α=0.00131 29, α(K)=0.00107 25, α(L)=0.000142 31, α(M)=3.0×10^-5 7, α(N)=6.9E-6 15, α(O)=1.03E-6 23, α(P)=6.4E-8 16
2683.460	4-,5-		1089.154 18	M1		0.00322	α=0.00322 5, α(K)=0.00275 4, α(L)=0.000365 5, α(M)=7.79×10^-5 11, α(N)=1.767E-5 25, α(O)=2.66E-6 4, α(P)=1.701E-7 24
2698.614	5-,6-		166.15 3	M1,E2		0.397	α=0.397 8, α(K)=0.30 4, α(L)=0.073 25, α(M)=0.016 6, α(N)=0.0036 13, α(O)=5.0×10^-4 15, α(P)=1.7E-5 5
2698.614	5-,6-		1104.321 16	M1		0.00311	α=0.00311 4, α(K)=0.00267 4, α(L)=0.000353 5, α(M)=7.54×10^-5 11, α(N)=1.710E-5 24, α(O)=2.58E-6 4, α(P)=1.646E-7 23
2714.76	8+		586.2 1	E1		0.00303	α=0.00303 4, α(K)=0.00260 4, α(L)=0.000342 5, α(M)=7.27×10^-5 10, α(N)=1.643E-5 23, α(O)=2.444E-6 34, α(P)=1.484E-7 21
2714.76	8+		808.7 1	E2		0.00395	α=0.00395 6, α(K)=0.00333 5, α(L)=0.000490 7, α(M)=0.0001056 15, α(N)=2.382×10^-5 33, α(O)=3.50E-6 5, α(P)=1.967E-7 28
2723.527	4+		495.25 6	M1		0.02205	α=0.02205 31, α(K)=0.01880 26, α(L)=0.00256 4, α(M)=0.000548 8, α(N)=0.0001243 17, α(O)=1.869×10^-5 26, α(P)=1.177E-6 16
2723.527	4+		1543.289 27	M1+E2		0.00133	α=0.00133 20, α(K)=0.00106 17, α(L)=0.000140 21, α(M)=3.0×10^-5 5, α(N)=6.8E-6 10, α(O)=1.02E-6 16, α(P)=6.4E-8 11
2753.16	3+		2202.88 6	M1+E2		0.00100	α=0.00100 8, α(K)=0.00051 5, α(L)=6.6×10^-5 6, α(M)=1.41E-5 13, α(N)=3.19E-6 30, α(O)=4.8E-7 5, α(P)=3.08E-8 32
2801.772	5+		654.220 8	M1+E2	+0.9 3	0.0090	α=0.0090 8, α(K)=0.0076 7, α(L)=0.00108 8, α(M)=0.000231 16, α(N)=5.2×10^-5 4, α(O)=7.8E-6 6, α(P)=4.7E-7 5
	5+		895.847 10	M1+E2	-0.20 11	0.00504	α=0.00504 12, α(K)=0.00431 10, α(L)=0.000576 13, α(M)=0.0001231 27, α(N)=2.79×10^-5 6, α(O)=4.20E-6 9, α(P)=2.67E-7 7
	5+		1207.473 14	E1+M2		0.00081	α=0.00081 5, α(K)=0.00067 5, α(L)=8.7×10^-5 6, α(M)=1.84E-5 14, α(N)=4.16E-6 31, α(O)=6.2E-7 5, α(P)=3.94E-8 29
	5+		1621.510 20	M1+E2		0.00124	α=0.00124 17, α(K)=0.00096 14, α(L)=0.000126 18, α(M)=2.7×10^-5 4, α(N)=6.1E-6 9, α(O)=9.2E-7 14, α(P)=5.8E-8 10
2807.13	9-		92.2 2	E1		0.343	α=0.343 5, α(K)=0.289 4, α(L)=0.0429 7, α(M)=0.00918 14, α(N)=0.002043 31, α(O)=0.000288 4, α(P)=1.384×10^-5 21
	9-		262.5	E1		0.02070	α=0.02070 29, α(K)=0.01764 25, α(L)=0.002410 34, α(M)=0.000514 7, α(N)=0.0001157 16, α(O)=1.694×10^-5 24, α(P)=9.59E-7 13
	9-		678.6 1	E2		0.00593	α=0.00593 8, α(K)=0.00496 7, α(L)=0.000764 11, α(M)=0.0001656 23, α(N)=3.73×10^-5 5, α(O)=5.43E-6 8, α(P)=2.91E-7 4
2815.603	4-		1221.37 4	M1		2.47×10^-3	α=2.47×10^-3 4, α(K)=0.002107 29, α(L)=0.000278 4, α(M)=5.94E-5 8, α(N)=1.347E-5 19, α(O)=2.030E-6 28, α(P)=1.299E-7 18
2815.603	4-		1635.31 3	E1+M2		7.64×10^-4	α=7.64×10^-4 24, α(K)=0.000394 21, α(L)=5.00E-5 29, α(M)=1.06E-5 6, α(N)=2.40E-6 14, α(O)=3.61E-7 21, α(P)=2.30E-8 13
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2830.700	5+		683.153 7	M1+E2		0.0079	α=0.0079 20, α(K)=0.0067 18, α(L)=0.00094 19, α(M)=0.00020 4, α(N)=4.6×10^-5 9, α(O)=6.8E-6 15, α(P)=4.1E-7 12
	5+		735.00 5	M1+E2	-1.1 6	0.0064	α=0.0064 12, α(K)=0.0055 10, α(L)=0.00077 11, α(M)=0.000165 24, α(N)=3.7×10^-5 5, α(O)=5.6E-6 9, α(P)=3.3E-7 7
	5+		924.75 3	M1		0.00474	α=0.00474 7, α(K)=0.00406 6, α(L)=0.000541 8, α(M)=0.0001155 16, α(N)=2.62×10^-5 4, α(O)=3.95E-6 6, α(P)=2.513E-7 35
	5+		1097.18 3	M1		0.00316	α=0.00316 4, α(K)=0.00271 4, α(L)=0.000359 5, α(M)=7.66×10^-5 11, α(N)=1.737E-5 24, α(O)=2.62E-6 4, α(P)=1.672E-7 23
	5+		1236.374 16	E1		7.43×10^-4	α=7.43×10^-4 10, α(K)=0.000603 8, α(L)=7.69E-5 11, α(M)=1.632E-5 23, α(N)=3.69E-6 5, α(O)=5.54E-7 8, α(P)=3.50E-8 5
	5+		1650.436 24	M1+E2		0.00121	α=0.00121 16, α(K)=0.00092 14, α(L)=0.000121 17, α(M)=2.6×10^-5 4, α(N)=5.9E-6 8, α(O)=8.8E-7 13, α(P)=5.6E-8 9
2861.123	4-,5-		1266.76 5	M1		2.28×10^-3	α=2.28×10^-3 3, α(K)=0.001936 27, α(L)=0.000255 4, α(M)=5.45E-5 8, α(N)=1.236E-5 17, α(O)=1.863E-6 26, α(P)=1.193E-7 17
2976.11	8-		847.4 2	E2(+M1)		0.0047	α=0.0047 11, α(K)=0.0040 10, α(L)=0.00055 12, α(M)=0.000119 24, α(N)=2.7×10^-5 6, α(O)=4.0E-6 9, α(P)=2.4E-7 7
3235.01	10+		690.6 1	E2		0.00569	α=0.00569 8, α(K)=0.00476 7, α(L)=0.000730 10, α(M)=0.0001581 22, α(N)=3.56×10^-5 5, α(O)=5.19E-6 7, α(P)=2.80E-7 4
3253.22	10-		446.1 1	M1+E2	-0.10 5	0.0287	α=0.0287 4, α(K)=0.0244 4, α(L)=0.00334 5, α(M)=0.000716 10, α(N)=0.0001624 23, α(O)=2.440×10^-5 35, α(P)=1.531E-6 23
3397.91	10+		590.8 1	E1		0.00298	α=0.00298 4, α(K)=0.00255 4, α(L)=0.000336 5, α(M)=7.15×10^-5 10, α(N)=1.615E-5 23, α(O)=2.402E-6 34, α(P)=1.460E-7 20
3397.91	10+		683.1 1	E2		0.00584	α=0.00584 8, α(K)=0.00488 7, α(L)=0.000751 11, α(M)=0.0001627 23, α(N)=3.66×10^-5 5, α(O)=5.34E-6 7, α(P)=2.87E-7 4
3421.68	11-		186.7 1	E1		0.0508	α=0.0508 7, α(K)=0.0432 6, α(L)=0.00601 8, α(M)=0.001284 18, α(N)=0.000288 4, α(O)=4.17×10^-5 6, α(P)=2.266E-6 32
3421.68	11-		614.5 1	E2		0.00755	α=0.00755 11, α(K)=0.00628 9, α(L)=0.000998 14, α(M)=0.0002167 30, α(N)=4.87×10^-5 7, α(O)=7.07E-6 10, α(P)=3.67E-7 5
3614.54	11-		216.6 1	E1		0.0342	α=0.0342 5, α(K)=0.0291 4, α(L)=0.00402 6, α(M)=0.000858 12, α(N)=0.0001927 27, α(O)=2.81×10^-5 4, α(P)=1.553E-6 22
3614.54	11-		807.4 1	E2		0.00396	α=0.00396 6, α(K)=0.00334 5, α(L)=0.000492 7, α(M)=0.0001060 15, α(N)=2.391×10^-5 33, α(O)=3.52E-6 5, α(P)=1.974E-7 28
3992.41	12+		570.6 2	E1		0.00322	α=0.00322 5, α(K)=0.00275 4, α(L)=0.000363 5, α(M)=7.72×10^-5 11, α(N)=1.744E-5 24, α(O)=2.59E-6 4, α(P)=1.572E-7 22
3992.41	12+		757.3 1	E2		0.00459	α=0.00459 6, α(K)=0.00385 5, α(L)=0.000576 8, α(M)=0.0001245 17, α(N)=2.81×10^-5 4, α(O)=4.11E-6 6, α(P)=2.274E-7 32
4104.17	12+		489.6 1	E1		0.00452	α=0.00452 6, α(K)=0.00387 5, α(L)=0.000514 7, α(M)=0.0001094 15, α(N)=2.470×10^-5 35, α(O)=3.66E-6 5, α(P)=2.195E-7 31
	12+		682.2 2	E1		2.20×10^-3	α=2.20×10^-3 3, α(K)=0.001884 26, α(L)=0.0002461 34, α(M)=5.24E-5 7, α(N)=1.183E-5 17, α(O)=1.763E-6 25, α(P)=1.082E-7 15
	12+		706.2 1	E2		0.00540	α=0.00540 8, α(K)=0.00452 6, α(L)=0.000689 10, α(M)=0.0001491 21, α(N)=3.36×10^-5 5, α(O)=4.90E-6 7, α(P)=2.66E-7 4
4397.56	13-		293.3 2	E1		0.01558	α=0.01558 22, α(K)=0.01329 19, α(L)=0.001806 25, α(M)=0.000385 5, α(N)=8.67×10^-5 12, α(O)=1.273E-5 18, α(P)=7.29E-7 10
4397.56	13-		783.0 1	E2		0.00425	α=0.00425 6, α(K)=0.00357 5, α(L)=0.000530 7, α(M)=0.0001145 16, α(N)=2.58×10^-5 4, α(O)=3.79E-6 5, α(P)=2.112E-7 30
4804.96	14+		407.4 2	E1		0.00694	α=0.00694 10, α(K)=0.00593 8, α(L)=0.000794 11, α(M)=0.0001692 24, α(N)=3.82×10^-5 5, α(O)=5.64E-6 8, α(P)=3.33E-7 5
	14+		694.7 2	E1		2.11×10^-3	α=2.11×10^-3 3, α(K)=0.001814 25, α(L)=0.0002368 33, α(M)=5.04E-5 7, α(N)=1.138E-5 16, α(O)=1.697E-6 24, α(P)=1.042E-7 15
	14+		700.8 2	E2		0.00549	α=0.00549 8, α(K)=0.00460 6, α(L)=0.000703 10, α(M)=0.0001521 21, α(N)=3.43×10^-5 5, α(O)=5.00E-6 7, α(P)=2.71E-7 4
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
4889.48	14-		373.0 2	E1		0.00858	α=0.00858 12, α(K)=0.00733 10, α(L)=0.000984 14, α(M)=0.0002099 30, α(N)=4.73×10^-5 7, α(O)=6.98E-6 10, α(P)=4.09E-7 6
4889.48	14-		781.0 1	E2		0.00427	α=0.00427 6, α(K)=0.00359 5, α(L)=0.000534 7, α(M)=0.0001152 16, α(N)=2.60×10^-5 4, α(O)=3.81E-6 5, α(P)=2.124E-7 30
5135.91	15-		331.0 2	E1		0.01150	α=0.01150 16, α(K)=0.00982 14, α(L)=0.001326 19, α(M)=0.000283 4, α(N)=6.37×10^-5 9, α(O)=9.38E-6 13, α(P)=5.44E-7 8
5135.91	15-		738.3 2	E2		0.00486	α=0.00486 7, α(K)=0.00408 6, α(L)=0.000615 9, α(M)=0.0001328 19, α(N)=2.99×10^-5 4, α(O)=4.38E-6 6, α(P)=2.406E-7 34
5274.70	15+		385.1 2	E1		0.00794	α=0.00794 11, α(K)=0.00678 10, α(L)=0.000910 13, α(M)=0.0001941 27, α(N)=4.38×10^-5 6, α(O)=6.46E-6 9, α(P)=3.80E-7 5
5274.70	15+		758.2 1	E2		0.00457	α=0.00457 6, α(K)=0.00384 5, α(L)=0.000575 8, α(M)=0.0001241 17, α(N)=2.80×10^-5 4, α(O)=4.10E-6 6, α(P)=2.268E-7 32
5496.17	16+		360.3 2	E1		0.00933	α=0.00933 13, α(K)=0.00797 11, α(L)=0.001073 15, α(M)=0.0002287 32, α(N)=5.15×10^-5 7, α(O)=7.60E-6 11, α(P)=4.44E-7 6
	16+		653.7 2	E1		2.40×10^-3	α=2.40×10^-3 3, α(K)=0.002060 29, α(L)=0.000270 4, α(M)=5.74E-5 8, α(N)=1.296E-5 18, α(O)=1.930E-6 27, α(P)=1.181E-7 17
	16+		691.2 2	E2		0.00568	α=0.00568 8, α(K)=0.00475 7, α(L)=0.000728 10, α(M)=0.0001577 22, α(N)=3.55×10^-5 5, α(O)=5.18E-6 7, α(P)=2.79E-7 4
5945.86	18+		108.7 2	E1		0.2197	α=0.2197 33, α(K)=0.1855 28, α(L)=0.0270 4, α(M)=0.00577 9, α(N)=0.001288 19, α(O)=0.0001827 27, α(P)=9.09×10^-6 13
	18+		384.9 2	E1		0.00795	α=0.00795 11, α(K)=0.00679 10, α(L)=0.000911 13, α(M)=0.0001943 27, α(N)=4.38×10^-5 6, α(O)=6.47E-6 9, α(P)=3.80E-7 5
	18+		449.7 2	E2		0.01710	α=0.01710 24, α(K)=0.01392 20, α(L)=0.002490 35, α(M)=0.000546 8, α(N)=0.0001224 17, α(O)=1.739×10^-5 24, α(P)=7.93E-7 11
6195.07	19-		249	E1		0.02373	α=0.02373 33, α(K)=0.02021 28, α(L)=0.00277 4, α(M)=0.000591 8, α(N)=0.0001329 19, α(O)=1.943×10^-5 27, α(P)=1.094E-6 15
6195.07	19-		358.0 2	E2		0.0329	α=0.0329 5, α(K)=0.0262 4, α(L)=0.00524 7, α(M)=0.001159 16, α(N)=0.000259 4, α(O)=3.61×10^-5 5, α(P)=1.448E-6 20
6592.57	20(+)		397.5 2	E1		0.00736	α=0.00736 10, α(K)=0.00629 9, α(L)=0.000842 12, α(M)=0.0001796 25, α(N)=4.05×10^-5 6, α(O)=5.98E-6 8, α(P)=3.53E-7 5
6592.57	20(+)		646.6 2	E2		0.00666	α=0.00666 9, α(K)=0.00556 8, α(L)=0.000869 12, α(M)=0.0001885 26, α(N)=4.24×10^-5 6, α(O)=6.17E-6 9, α(P)=3.26E-7 5
7329.07	22(+)		416.0 3	E1		0.00660	α=0.00660 9, α(K)=0.00565 8, α(L)=0.000755 11, α(M)=0.0001609 23, α(N)=3.63×10^-5 5, α(O)=5.36E-6 8, α(P)=3.17E-7 4
7329.07	22(+)		736.5 2	E2		0.00489	α=0.00489 7, α(K)=0.00410 6, α(L)=0.000618 9, α(M)=0.0001337 19, α(N)=3.01×10^-5 4, α(O)=4.41E-6 6, α(P)=2.419E-7 34
7620.18	23(-)		291.2 2	E1		0.01587	α=0.01587 22, α(K)=0.01353 19, α(L)=0.001840 26, α(M)=0.000393 6, α(N)=8.84×10^-5 12, α(O)=1.297E-5 18, α(P)=7.42E-7 10
7620.18	23(-)		707.1 2	E2		0.00538	α=0.00538 8, α(K)=0.00451 6, α(L)=0.000687 10, α(M)=0.0001486 21, α(N)=3.35×10^-5 5, α(O)=4.89E-6 7, α(P)=2.65E-7 4
7977.37	24(+)		357.2 3	E1		0.00953	α=0.00953 13, α(K)=0.00814 12, α(L)=0.001096 16, α(M)=0.0002337 33, α(N)=5.27×10^-5 7, α(O)=7.76E-6 11, α(P)=4.53E-7 6
7977.37	24(+)		648.2 2	E2		0.00662	α=0.00662 9, α(K)=0.00553 8, α(L)=0.000863 12, α(M)=0.0001872 26, α(N)=4.21×10^-5 6, α(O)=6.13E-6 9, α(P)=3.24E-7 5
8214.29	25(-)		236.9 2	E1		0.0270	α=0.0270 4, α(K)=0.02301 33, α(L)=0.00316 4, α(M)=0.000675 10, α(N)=0.0001517 22, α(O)=2.214×10^-5 31, α(P)=1.239E-6 18
8214.29	25(-)		594.2 2	E2		0.00821	α=0.00821 12, α(K)=0.00682 10, α(L)=0.001095 15, α(M)=0.0002380 33, α(N)=5.35×10^-5 8, α(O)=7.75E-6 11, α(P)=3.97E-7 6

Q(β-)=-3039 keV 10	S(n)= 8141.34 keV 27	S(p)= 7583.1 keV 4	Q(α)= 1987.0 keV 4
Reference: 2021WA16

References:
A	¹⁴⁸Nd 2β^- decay	B	¹⁴⁸Pm β^- decay (5.368 d)
C	¹⁴⁸Pm β^- decay (41.29 d)	D	¹⁴⁸Eu ε decay
E	¹⁵²Gd α decay	F	¹⁴⁷Sm(n,γ) E=THERMAL
G	¹⁴⁷Sm(n,γ) E=0.020-1.0 KEV	H	¹⁴⁷Sm(n,γ) E=0.1-10 KEV
I	¹⁴⁷Sm(n,γ) E=3.4 EV	J	¹⁴⁷Sm(n,γ) E=24.5 KEV
K	¹⁴⁷Sm(n,X):Resonances	L	¹⁴⁷Sm(d,p)
M	¹⁴⁸Sm(γ,γ’)	N	¹⁴⁸Sm(E,E’)
O	¹⁴⁸Sm(n,n’γ)	P	¹⁴⁸Sm(p,p’),(pol p,p’)
Q	¹⁴⁸Sm(d,d’)	R	¹⁴⁹Sm(d,t)
S	¹⁵⁰Sm(p,t)	T	¹⁵¹Eu(μ^-,3nγ)
U	Coulomb Excitation	V	(HI,xnγ)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - Band 1; g.s. band
0.0	0+	6.5×10¹⁵ y +12-13 % α = 100
550.263 8	2+	7.71 ps 32	550.273 9	100	E2	0.0	0+
1180.252 9	4+	2.37 ps 22	629.987 8	100	E2	550.263	2+
1905.917 10	6+		311.570 20 725.673 9	14.2 3 100 2	E1 E2	1594.291 1180.252	5- 4+
2714.76 7	8+		586.2 1 808.7 1		E1 E2	2128.59 1905.917	7- 6+
3397.91 8	10+		590.8 1 683.1 1 853.4 3 ?		E1 E2	2807.13 2714.76 2544.46	9- 8+ 8+
4104.17 9	12+		489.6 1 682.2 2 706.2 1 869.6 2		E1 E1 E2	3614.54 3421.68 3397.91 3235.01	11- 11- 10+ 10+
4804.96 11	14+		407.4 2 616.0 2 694.7 2 700.8 2 812.6 2		E1 E1 E2	4397.56 4189.06 4110.46 4104.17 3992.41	13- 12+ 13- 12+ 12+
5496.17 12	16+		360.3 2 586.6 2 631.8 2 653.7 2 691.2 2		E1 E1 E2	5135.91 4909.43 4864.48 4842.48 4804.96	15- 14+ 14+ 15- 14+
5945.86 13	18+		108.7 2 296.5 2 384.9 2 421.6 2 449.7 2		E1 E1 E2	5837.10 5649.34 5560.98 5524.26 5496.17	17- 17- 17- 16+ 16+
6592.57 16	20(+)		397.5 2 646.6 2		E1 E2	6195.07 5945.86	19- 18+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
7329.07 22	22(+)		416.0 3 736.5 2		E1 E2	6913.07 6592.57	21(-) 20(+)
7977.37 26	24(+)
8659.2 4	26(+)		445.0 3 681.4 5 ?			8214.29 7977.37	25(-) 24(+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - Band 2; octupole band
1161.547 9	3-	0.6 ps +4-2
1594.291 10	5-		414.028 12 432.745 8	100 3 27.6 15	E1+M2 E2	1180.252 1161.547	4+ 3-
2128.59 5	7-		222.71 12 534.38 7	22.9 21 100 21	E1 E2	1905.917 1594.291	6+ 5-
2807.13 7	9-		92.2 2 262.5 678.6 1	18 100 6	E1 E1 E2	2714.76 2544.46 2128.59	8+ 8+ 7-
3614.54 9	11-		216.6 1 807.4 1		E1 E2	3397.91 2807.13	10+ 9-
4397.56 11	13-		293.3 2 783.0 1		E1 E2	4104.17 3614.54	12+ 11-
5135.91 13	15-		331.0 2 738.3 2		E1 E2	4804.96 4397.56	14+ 13-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - Band 3
5837.10 16	17-
6195.07 15	19-		166.1 1 184.0 2 249? 358.0 2		E1 E2	6028.99 6010.93 5945.86 5837.10	18- 18 18+ 17-
6913.07 22	21(-)		718.0 2	100		6195.07	19-
7620.18 24	23(-)		291.2 2 707.1 2		E1 E2	7329.07 6913.07	22(+) 21(-)
8214.29 27	25(-)		236.9 2 594.2 2		E1 E2	7977.37 7620.18	24(+) 23(-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - Band 4
2095.596 11	6+
2544.46 6	8+		152.1 2 350.5 2 415.9 1 449.0 11 638.5 1	1.23 100 5 35 4 32	E1 E2 E2	2392.38 2194.071 2128.59 2095.596 1905.917	7+ 6+ 7- 6+ 6+
3235.01 9	10+		690.6 1	100	E2	2544.46	8+
3992.41 9	12+		570.6 2 594.7 2 757.3 1		E1 E2	3421.68 3397.91 3235.01	11- 10+ 10+
4864.48 10	14+		466.9 2 623.3 2 675.3 2 754.0 2 760.3 2 872.0 1			4397.56 4241.30 4189.06 4110.46 4104.17 3992.41	13- 13- 12+ 13- 12+ 12+
5524.26 13	16+		615.0 2 659.6 2 681.7 2 719.4 2			4909.43 4864.48 4842.48 4804.96	14+ 14+ 15- 14+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - Band 5
3421.68 8	11-
4110.46 10	13-		688.8 1	100		3421.68	11-
4842.48 11	15-		732.0 1	100		4110.46	13-
5560.98 14	17-		718.5 1	100		4842.48	15-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - Band 6
6694.10 15	21(-)	32 ns 3
7332.70 18	23(-)		638.6 1	100		6694.10	21(-)
8010.40 21	25(-)		677.7 1	100		7332.70	23(-)
8602.00 23	27(-)		591.6 1	100		8010.40	25(-)
9601.00 30	29		999.0 2	100		8602.00	27(-)
10438.7 4	31		837.8 2	100		9601.00	29
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - Band 7
3188.09 9	9-
3806.76 10	11-		261.2 2 385.4 2 618.6 1			3545.41 3421.68 3188.09	10- 11- 9-
4512.69 13	13-		316.7 2 402.2 2 705.9 2			4196.03 4110.46 3806.76	12- 13- 11-
5287.56 20	15-		445.0 3 774.9 2			4842.48 4512.69	15- 13-

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	0+	6.5×10¹⁵ y +12-13 % α = 100	Rms charge radius <r²>^1/2=5.0042 fm 34 (2013An02). E(level): Band 1; g.s. band.
550.263	2+	7.71 ps 32	μ=+0.54 7 (2020StZV,1987Ba65), Q=-1.0 3 (2021StZZ,1989Ra17) μ, other: +0.61 7 (1987Be08). E(level): Band 1; g.s. band.
1161.547	3-	0.6 ps +4-2	B(E3)\|^=0.37 3 (Coul. ex., 1968Ke04). E(level): Band 2; octupole band.
1180.252	4+	2.37 ps 22	E(level): Band 1; g.s. band.
1465.139	1-	92 fs 8	B(E1)\|^=0.013 5 (Coul. ex., 1968Ve01).
1594.291	5-		E(level): Band 2; octupole band.
1905.917	6+		E(level): Band 1; g.s. band.
2095.596	6+		E(level): Band 4.
2128.59	7-		E(level): Band 2; octupole band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
2146.360	2+	< 64.1 fs	J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2194.071	6+		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
2277	+		E(level): From ¹⁴⁸Sm(d,t) dataset.
2327.62	3+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2327.743	4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2339.22	3-		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2344	3-,4-		E(level): From ¹⁴⁸Sm(d,t) dataset.
2358	0+		E(level): From ¹⁴⁸Sm(p,t) dataset.
2374.426	5+,6+		XREF: Q(2370).
2381.68	2+	87 fs 17	J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2390.43	3+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2392.38	7+		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
2467.39	3(-)		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2472.48	1	37 fs 3	J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2496	+		E(level): From ¹⁴⁸Sm(d,t) dataset. From ¹⁴⁸Sm(d,p) dataset.
2513.50	1	99 fs 5	J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
E(level)	J^π(level)	T_1/2(level)	Comments
2524.30	4+		XREF: O(2524.920)R(2531).
2539.83	3-		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2544.46	8+		Configuration=((ν[(f³_7/2), \h_9/2])_8⁺π(d^-2_5/2)_0⁺)_8⁺. E(level): Band 4. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
2567.90	2+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2570.811	4(-)		XREF: O(2574). J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2583.901	4(-)		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2633.16	3-		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2640.89	5+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2697.79	3+,4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2701.960	4(-),(3-)		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2713.347	3+,4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2714.76	8+		E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
2723.527	4+		XREF: O(2723.72).
2738.64	(8+)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
2753.16	3+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2806.76	3+,4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2807.13	9-		E(level): Band 2; octupole band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
2822	+		E(level): Average value of Eγ values from ¹⁴⁸(d,t) and ¹⁴⁸(d,p).
2862.09	3+,4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2941.1	2+,3-		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2942.61	8-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
2967.83	3+,4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2976.11	8-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
2980.52	3+,4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
2991.88	3+,4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
E(level)	J^π(level)	T_1/2(level)	Comments
3004			E(level): Average value of Eγ values from ¹⁴⁸(d,t) and ¹⁴⁸(d,p).
3022			E(level): From ¹⁴⁸Sm(d,p) dataset.
3045	+		E(level): Average value of Eγ values from ¹⁴⁸(d,t) and ¹⁴⁸(d,p).
3063.22	3-		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
3073			E(level): From ¹⁴⁸Sm(d,t) dataset.
3089.86	2+,3-		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
3095.02	9(+)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3107.8	3+,4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
3112	+		E(level): From ¹⁴⁸Sm(d,p) dataset.
3138.47	3(-),4(-)		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
3164.9	3+,4+		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
3188.09	9-		E(level): Band 7. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3189.8	2+,3-		J^π(level): From γ(θ), primary-capture γ Iγ/E_γ⁵, and linear-polarization data in (n,γ) E=0.020-1.0 keV and (n,n’γ).
3215.94	9-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3235.01	10+		E(level): Band 4. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3245	+		E(level): Average value of Eγ values from ¹⁴⁸(d,t) and ¹⁴⁸(d,p).
3253.22	10-		Configuration=(ν(i_13/2,f³_7/2)_10-(π(d^-2_5/2)_0⁺)) \_10- and (ν[(i_13/2,h_9/2)_10-(f²_7/2)_0⁺]_10- \(π(d^-2_5/2)_0⁺))_10-. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3255.3	(1,2+)		B(E1)\|^=4.4×10^-5 3 (γ,γ’, 1993Zi05).
3291.5	(1,2+)		B(E1)\|^=1.7×10^-5 2 (γ,γ’, 1993Zi05).
3322.44	(10+)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3347	+		E(level): Average value of Eγ values from ¹⁴⁸(d,t) and ¹⁴⁸(d,p).
3397			E(level): From ¹⁴⁸Sm(d,t) dataset.
3397.91	10+		E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3421.68	11-		Configuration=(ν[(i_13/2,h_9/2)_11-(f²_7/2)_0⁺] \_11-(π(d^-2_5/2)₀))_11-. E(level): Band 5. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3428			E(level): From ¹⁴⁸Sm(d,t) dataset.
E(level)	J^π(level)	T_1/2(level)	Comments
3483.6	(1,2+)		B(E1)\|^=6.0×10^-5 15 (γ,γ’, 1993Zi05).
3488	(3-,4-)		E(level): From ¹⁴⁸Sm(d,t) dataset.
3526.36	10-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3530	(3-,4-)		E(level): From ¹⁴⁸Sm(d,t) dataset.
3535.0	(1,2+)		B(E1)\|^=5.8×10^-5 4 (γ,γ’, 1993Zi05).
3545.41	10-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3546	(3-,4-)		E(level): From ¹⁴⁸Sm(d,t) dataset.
3572			E(level): From ¹⁴⁸Sm(d,t) dataset.
3614.54	11-		E(level): Band 2; octupole band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3628	(3-,4-)		E(level): From ¹⁴⁸Sm(d,t) dataset.
3640.24	(11)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3652	(3-,4-)		E(level): From ¹⁴⁸Sm(d,t) dataset.
3668			E(level): From ¹⁴⁸Sm(d,p) dataset.
3674			E(level): From ¹⁴⁸Sm(d,t) dataset.
3714			E(level): From ¹⁴⁸Sm(d,t) dataset.
3734	(3-,4-)		E(level): From ¹⁴⁸Sm(d,t) dataset.
3752			E(level): From ¹⁴⁸Sm(d,t) dataset.
3774	(3-,4-)		E(level): From ¹⁴⁸Sm(d,t) dataset.
3797			E(level): From ¹⁴⁸Sm(d,t) dataset.
3806.76	11-		E(level): Band 7. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
3817	3-,4-		E(level): From ¹⁴⁸Sm(d,t) dataset.
3843.6	(1,2+)		B(E1)\|^=0.6×10^-5 2 (γ,γ’, 1993Zi05).
3902	3-,4-		E(level): From ¹⁴⁸Sm(d,t) dataset.
3951			E(level): From ¹⁴⁸Sm(d,t) dataset.
3990	(3-,4-)		E(level): From ¹⁴⁸Sm(d,t) dataset.
E(level)	J^π(level)	T_1/2(level)	Comments
3992.41	12+		E(level): Band 4. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4005			E(level): From ¹⁴⁸Sm(d,t) dataset.
4011			E(level): From ¹⁴⁸Sm(d,t) dataset.
4026	3-,4-		E(level): From ¹⁴⁸Sm(d,t) dataset.
4041			E(level): From ¹⁴⁸Sm(d,t) dataset.
4085			E(level): From ¹⁴⁸Sm(d,p) dataset.
4104.17	12+		E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4107			E(level): From ¹⁴⁸Sm(d,p) dataset.
4108.48	12-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4110.46	13-		E(level): Band 5. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4189.06	12+		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4196.03	12-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4241.30	13-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4397.56	13-		E(level): Band 2; octupole band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4512.69	13-		E(level): Band 7. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4516.52	13+		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4804.96	14+		E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4842.48	15-		E(level): Band 5. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4864.48	14+		E(level): Band 4. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4889.48	14-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4909.43	14+		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4917.33	14-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
4951.53	14(-)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5087.33	15-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5135.91	15-		E(level): Band 2; octupole band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
E(level)	J^π(level)	T_1/2(level)	Comments
5216.98	15(-)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5274.70	15+		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5287.56	15-		E(level): Band 7. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5320.06	16-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5496.17	16+		E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5524.26	16+		E(level): Band 4. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5556.32	16-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5560.98	17-		E(level): Band 5. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5578.08	16(+)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5649.34	17-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5777.51	17+		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5837.10	17-		E(level): Band 3. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
5945.86	18+		configuration=(ν[(i_13/2²)_12⁺(f_7/2²)_6⁺]₁₈₊,(π(d{ \-5/2^-2))_0⁺)_18⁺. E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
6010.93	18		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
6028.99	18-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
6195.07	19-		E(level): Band 3. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
6392.01	19-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
6476.85	19-		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
6557.31	(19)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
6592.57	20(+)		configuration=(ν[(i_13/2²)_12⁺(h_9/2,f_7/2)_8⁺]₂₀₊π( \d_5/2^-2)_0⁺)_20⁺. E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
6694.10	21(-)	32 ns 3	configuration=(ν[(i_13/2,h_9/2)_11-(f_7/2²)_0⁺]_11-π \(h_11/2²)_10⁺)_21-. E(level): Band 6. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
6913.07	21(-)		E(level): Band 3. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
7329.07	22(+)		E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
7332.70	23(-)		E(level): Band 6. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
7620.18	23(-)		E(level): Band 3. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
E(level)	J^π(level)	T_1/2(level)	Comments
7942.31	(22)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
7977.37	24(+)		E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
8010.40	25(-)		E(level): Band 6. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
8214.29	25(-)		E(level): Band 3. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
8358.54	(24)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
8602.00	27(-)		E(level): Band 6. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
8659.2	26(+)		E(level): Band 1; g.s. band. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
8931.2	(27)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
9045.65	(26)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
9601.00	29		E(level): Band 6. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
9898.0	(28)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
10438.7	31		E(level): Band 6. J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
10609.0	(30)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.
11524.4	(32)		J^π(level): From (HI,xnγ) based on γ-ray excitation functions, γ(θ), DCO ratios, γ-ray linear polarization, Ice spectra, T_1/2, prompt and delayed Ice spectra. π of levels upto J=19 were deduced from linear-polarization data. Jπ assignments of high-spin levels should be considered as tentative pending publication of detailed data.

E(level)	E(gamma)	Comments
1161.547	611.293	M(γ): E1⁺M2 with δ=+0.026 13 from ¹⁴⁸Sm β^- decay, +0.08 4 from (HI,xnγ), and <0.4 from (n,n’γ). However, RUL estimate of δ is \|<0.007 and the evaluator has set the mult=E1
2111.075	446.52	E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=446.887. Poor fit; uncertainty multiplied by a factor in the fitting
2111.075	930.807	M(γ): from Ice data in ¹⁴⁸Eu ε decay. M1⁺E2 from (n,n’γ); however, since this γ is doubly placed in this reaction, the result is suspect.
2214.263	66.72	I(γ): from ce(K) and α(K)
2228.134	495.25	E(γ): uncertainty multiplied by a factor of 3 in the fitting; level-energy difference=494.637. Poor fit; uncertainty multiplied by a factor in the fitting
	1047.570	E(γ): very poor fit and omitted in the fitting; level-energy difference=1047.877. Very poor fit and omitted in the fitting
	1066.75	E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=1066.583. Poor fit; uncertainty multiplied by a factor in the fitting
2327.743	216.16	E(γ): uncertainty multiplied by a factor of 3 in the fitting; level-energy difference=216.668. Poor fit; uncertainty multiplied by a factor in the fitting
	662.79	E(γ): very poor fit and omitted in the fitting; level-energy difference=663.554. Very poor fit and omitted in the fitting
	732.99	E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=733.450. Poor fit; uncertainty multiplied by a factor in the fitting
	1146.805	E(γ): very poor fit and omitted in the fitting; level-energy difference=1147.486. Very poor fit and omitted in the fitting
	1165.54	E(γ): very poor fit and omitted in the fitting; level-energy difference=1166.192. Very poor fit and omitted in the fitting
	1776.87	E(γ): very poor fit and omitted in the fitting; level-energy difference=1777.469. Very poor fit and omitted in the fitting
2490.056	1939.17	E(γ): very poor fit and omitted in the fitting; level-energy difference=1939.780. Very poor fit and omitted in the fitting
2524.30	620.04	E(γ): very poor fit and omitted in the fitting; level-energy difference=618.38. Very poor fit and omitted in the fitting
	929.85	E(γ): very poor fit and omitted in the fitting; level-energy difference=930.00. Very poor fit and omitted in the fitting
	1069.82	E(γ): very poor fit and omitted in the fitting; level-energy difference=1070.18. Very poor fit and omitted in the fitting
	1343.87	E(γ): very poor fit and omitted in the fitting; level-energy difference=1344.04. Very poor fit and omitted in the fitting
	1362.640	E(γ): very poor fit and omitted in the fitting; level-energy difference=1362.74. Very poor fit and omitted in the fitting
	1973.81	E(γ): very poor fit and omitted in the fitting; level-energy difference=1974.02. Very poor fit and omitted in the fitting
2570.811	667.170	E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=667.043. Poor fit; uncertainty multiplied by a factor in the fitting
2570.811	1409.160	E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=1409.257. Poor fit; uncertainty multiplied by a factor in the fitting
2640.89	1047.570	E(γ): very poor fit and omitted in the fitting; level-energy difference=1046.599. Very poor fit and omitted in the fitting
2640.89	1460.630	E(γ): very poor fit and omitted in the fitting; level-energy difference=1460.634. Very poor fit and omitted in the fitting
2683.460	587.52	E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=587.863. Poor fit; uncertainty multiplied by a factor in the fitting
E(level)	E(gamma)	Comments
2698.614	602.62	E(γ): very poor fit and omitted in the fitting; level-energy difference=603.016. Very poor fit and omitted in the fitting
2713.347	485.90	E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=485.212. Poor fit; uncertainty multiplied by a factor in the fitting
2723.527	332.91	E(γ): 1985Si16 relate this γ to ¹⁵⁰Eu ε decay
2727.44	1565.29	E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=1565.88. Poor fit; uncertainty multiplied by a factor in the fitting
2801.772	161.00	E(γ): very poor fit and omitted in the fitting; level-energy difference=160.878. Very poor fit and omitted in the fitting
2861.123	485.90	E(γ): uncertainty multiplied by a factor of 2 in the fitting; level-energy difference=486.696. Poor fit; uncertainty multiplied by a factor in the fitting
3197.4	1743.3	E(γ): multiplet
5287.56	445.0	E(γ): Multiply placed
8659.2	445.0	E(γ): Multiply placed
9898.0	1296.0	E(γ): doublet