List of levels for 148SM

Author: N. Nica | Citation: Nucl. Data Sheets 117, 1 (2014) | Cutoff date: 1-Oct-2013

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
550.255	2+	7.72 ps 32	550.273 9	E2		0.00998	B(E2)(W.u.)=31.2 13, α=0.00998 14, α(K)=0.00825 12, α(L)=0.001360 19, α(M)=0.000296 5, α(N)=6.66E-5 10, α(O)=9.59E-6 14, α(P)=4.78E-7 7, α(N+)=7.67E-5 11
1161.529	3-	0.6 ps +4-2	611.293 8	E1		0.00277	B(E1)(W.u.)=0.0018 +6-12, α=0.00277 4, α(K)=0.00237 4, α(L)=0.000312 5, α(M)=6.63E-5 10, α(N)=1.498E-5 21, α(O)=2.23E-6 4, α(P)=1.358E-7 19, α(N+)=1.735E-5 25
1180.261	4+	2.39 ps 24	629.987 8	E2		0.00710	B(E2)(W.u.)=51 6, α=0.00710 10, α(K)=0.00591 9, α(L)=0.000932 13, α(M)=0.000202 3, α(N)=4.55E-5 7, α(O)=6.61E-6 10, α(P)=3.46E-7 5, α(N+)=5.25E-5 8
1424.46	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 13, α(N)=1.97E-5 3, α(O)=2.91E-6 4, α(P)=1.663E-7 24, α(N+)=2.28E-5 4
1454.115	2+	285 fs 28	903.831 15	M1+E2	+2.32 10	0.00339	B(E2)(W.u.)=30 3, B(M1)(W.u.)=0.0082 11, α=0.00339 6, α(K)=0.00287 5, α(L)=0.000406 7, α(M)=8.72E-5 14, α(N)=1.97E-5 3, α(O)=2.92E-6 5, α(P)=1.72E-7 3, α(N+)=2.28E-5 4
1454.115	2+	285 fs 28	1454.110 20	E2		0.001230	B(E2)(W.u.)=3.3 4, α=0.001230 18, 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 9, α(N+)=6.78E-5
1465.137	1-	92 fs 8	914.916 15	E1		0.001221	B(E1)(W.u.)=0.00117 11, α=0.001221 17, α(K)=0.001050 15, α(L)=0.0001354 19, α(M)=2.88E-5 4, α(N)=6.51E-6 10, α(O)=9.73E-7 14, α(P)=6.07E-8 9, α(N+)=7.54E-6
1465.137	1-	92 fs 8	1465.101 13	E1		0.000704	B(E1)(W.u.)=0.00055 6, α=0.000704 10, α(K)=0.000449 7, 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, α(N+)=0.000186 3
1594.247	5-		414.028 12	E1+M2	-0.013 10	0.00670	α=0.00670 11, α(K)=0.00573 9, α(L)=0.000766 13, α(M)=0.000163 3, α(N)=3.68×10^-5 6, α(O)=5.45E-6 9, α(P)=3.22E-7 6, α(N+)=4.26E-5 7
1594.247	5-		432.745 8	E2		0.0190	α=0.0190, α(K)=0.01544 22, α(L)=0.00281 4, α(M)=0.000617 9, α(N)=0.0001382 20, α(O)=1.96×10^-5 3, α(P)=8.75E-7 13, α(N+)=0.0001587 23
1664.278	2+	0.25 ps 8	1113.92 3	M1+E2	-0.565 21	0.00279	B(E2)(W.u.)=4.5 15, B(M1)(W.u.)=0.032 11, α=0.00279 5, α(K)=0.00239 4, α(L)=0.000319 5, α(M)=6.81E-5 10, α(N)=1.544E-5 23, α(O)=2.32E-6 4, α(P)=1.466E-7 23, α(N+)=1.85E-5 3
1664.278	2+	0.25 ps 8	1664.20 4	E2		0.001042	B(E2)(W.u.)=1.3 5, α=0.001042 15, α(K)=0.000775 11, α(L)=0.0001023 15, α(M)=2.18E-5 3, α(N)=4.94E-6 7, α(O)=7.40E-7 11, α(P)=4.62E-8 7, α(N+)=0.000143
1733.465	4+		279.30 5	E2		0.0703	α=0.0703, 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, α(N+)=0.000715 10
	4+		553.231 14	M1+E2	+1.66 20	0.0117	α=0.0117 4, α(K)=0.0098 4, α(L)=0.00150 4, α(M)=0.000324 8, α(N)=7.31×10^-5 18, α(O)=1.07E-5 3, α(P)=5.83E-7 24, α(N+)=8.43E-5 22
	4+		571.962 7	E1		0.00320	α=0.00320 5, α(K)=0.00274 4, α(L)=0.000361 5, α(M)=7.68×10^-5 11, α(N)=1.735E-5 25, α(O)=2.58E-6 4, α(P)=1.564E-7 22, α(N+)=2.01E-5 3
	4+		1183.208 16	E2		0.001761	α=0.001761 25, α(K)=0.001496 21, α(L)=0.000205 3, α(M)=4.40×10^-5 7, α(N)=9.94E-6 14, α(O)=1.480E-6 21, α(P)=8.91E-8 13, α(N+)=1.555E-5 2
1894.824	4+		300.65 7	[E1]		0.01463	α=0.01463, α(K)=0.01248 18, α(L)=0.001694 24, α(M)=0.000362 5, α(N)=8.14×10^-5 12, α(O)=1.195E-5 17, α(P)=6.86E-7 10, α(N+)=9.40E-5 14
	4+		714.769 13	M1+E2		0.0070	α=0.0070 18, α(K)=0.0060 16, α(L)=0.00084 18, α(M)=0.00018 4, α(N)=4.1×10^-5 9, α(O)=6.1E-6 14, α(P)=3.6E-7 11, α(N+)=4.7E-5 10
	4+		1344.740 23	E2		0.001391	α=0.001391 20, α(K)=0.001162 17, α(L)=0.0001569 22, α(M)=3.35×10^-5 5, α(N)=7.59E-6 11, α(O)=1.133E-6 16, α(P)=6.92E-8 10, α(N+)=3.86E-5
1903.773	3+		1353.509 17	M1+E2	+8.2 12	0.001385	α=0.001385 20, α(K)=0.001155 17, α(L)=0.0001558 22, α(M)=3.33×10^-5 5, α(N)=7.53E-6 11, α(O)=1.125E-6 16, α(P)=6.89E-8 10, α(N+)=4.07E-5
1905.908	6+		311.570 20	E1		0.01337	α=0.01337, α(K)=0.01141 16, α(L)=0.001547 22, α(M)=0.000330 5, α(N)=7.43×10^-5 11, α(O)=1.092E-5 16, α(P)=6.29E-7 9, α(N+)=8.58E-5 12
1905.908	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 20, α(N)=3.13×10^-5 5, α(O)=4.58E-6 7, α(P)=2.50E-7 4, α(N+)=3.61E-5 5
1972.480	2+		1422.216 20	M1+E2	-0.556 24	0.001663	α=0.001663 25, α(K)=0.001379 21, α(L)=0.000182 3, α(M)=3.88×10^-5 6, α(N)=8.80E-6 13, α(O)=1.325E-6 20, α(P)=8.43E-8 13, α(N+)=6.40E-5 9
2031.403	4-		437.18 4	M1		0.0303	α=0.0303, 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, α(N+)=0.000199 3
2031.403	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 11, α(N+)=2.62E-5 11
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2057.960	2-		592.83 3	M1+E2		0.011	α=0.011 3, α(K)=0.009 3, α(L)=0.0014 3, α(M)=0.00029 6, α(N)=6.6×10^-5 13, α(O)=9.8E-6 21, α(P)=5.7E-7 18, α(N+)=7.7E-5 15
2057.960	2-		896.42 3	M1+E2	+1.32 9	0.00386	α=0.00386 9, α(K)=0.00328 8, α(L)=0.000456 10, α(M)=9.77×10^-5 20, α(N)=2.21E-5 5, α(O)=3.29E-6 7, α(P)=1.99E-7 5, α(N+)=2.56E-5 6
2095.595	6+		189.721 16	M1,E2		0.264	α=0.264 16, α(K)=0.21 3, α(L)=0.045 12, α(M)=0.010 3, α(N)=0.0022 6, α(O)=0.00031 7, α(P)=1.2×10^-5 4, α(N+)=0.0025 7
	6+		501.312 11	E1+M2	-0.017 14	0.00431	α=0.00431 8, α(K)=0.00369 7, α(L)=0.000489 9, α(M)=0.0001041 20, α(N)=2.35×10^-5 5, α(O)=3.49E-6 7, α(P)=2.09E-7 4, α(N+)=2.72E-5 5
	6+		915.331 8	E2		0.00300	α=0.00300 5, 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 22, α(N+)=2.04E-5 3
2111.053	4+		216.16 6	M1		0.195	α=0.195, α(K)=0.1657 24, α(L)=0.0232 4, α(M)=0.00497 7, α(N)=0.001127 16, α(O)=0.0001691 24, α(P)=1.052×10^-5 15, α(N+)=0.001307 19
	4+		377.560 20	M1		0.0442	α=0.0442, α(K)=0.0376 6, α(L)=0.00518 8, α(M)=0.001109 16, α(N)=0.000251 4, α(O)=3.78×10^-5 6, α(P)=2.37E-6 4, α(N+)=0.000292 4
	4+		446.52 6	(E2)		0.01744	α=0.01744, 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 12, α(N+)=0.0001437 21
	4+		516.793 14	E1+M2	0.48 8	0.015	α=0.015 3, α(K)=0.013 3, α(L)=0.0019 4, α(M)=0.00041 9, α(N)=9.3×10^-5 20, α(O)=1.4E-5 3, α(P)=8.4E-7 18, α(N+)=0.000108 23
	4+		930.807 19	E2		0.00290	α=0.00290 4, α(K)=0.00245 4, α(L)=0.000350 5, α(M)=7.53×10^-5 11, α(N)=1.701E-5 24, α(O)=2.51E-6 4, α(P)=1.455E-7 21, α(N+)=1.97E-5 3
	4+		1560.786 17	E2		0.001118	α=0.001118 16, α(K)=0.000874 13, α(L)=0.0001161 17, α(M)=2.48×10^-5 4, α(N)=5.61E-6 8, α(O)=8.40E-7 12, α(P)=5.21E-8 8, α(N+)=0.000103
2128.64	7-		222.71 12	E1		0.0318	α=0.0318, α(K)=0.0270 4, α(L)=0.00373 6, α(M)=0.000796 12, α(N)=0.000179 3, α(O)=2.61×10^-5 4, α(P)=1.448E-6 21, α(N+)=0.000206 3
2128.64	7-		534.38 7	E2		0.01077	α=0.01077, α(K)=0.00888 13, α(L)=0.001480 21, α(M)=0.000323 5, α(N)=7.25×10^-5 11, α(O)=1.043E-5 15, α(P)=5.14E-7 8, α(N+)=8.35E-5 12
2146.35	2+	< 64.1 fs	1596.08 3	M1+E2	-0.11 5	0.001447	B(E2)(W.u.)>0.019, B(M1)(W.u.)>0.069, α=0.001447 21, α(K)=0.001137 17, α(L)=0.0001491 22, α(M)=3.18E-5 5, α(N)=7.21E-6 11, α(O)=1.087E-6 16, α(P)=6.98E-8 11, α(N+)=0.000128
2147.499	5+		116.01 4	E1		0.184	α=0.184, α(K)=0.1556 22, α(L)=0.0225 4, α(M)=0.00481 7, α(N)=0.001073 15, α(O)=0.0001528 22, α(P)=7.69×10^-6 11, α(N+)=0.001234 18
	5+		241.653 15	M1+E2	-0.34 11	0.141	α=0.141 3, α(K)=0.119 3, α(L)=0.0176 4, α(M)=0.00379 10, α(N)=0.000857 21, α(O)=0.0001269 23, α(P)=7.41×10^-6 25, α(N+)=0.000991 23
	5+		243.83 4	E2		0.1086	α=0.1086, α(K)=0.0817 12, α(L)=0.0210 3, α(M)=0.00472 7, α(N)=0.001046 15, α(O)=0.0001413 20, α(P)=4.22×10^-6 6, α(N+)=0.001192 17
	5+		252.60 3	M1,E2		0.112	α=0.112 16, α(K)=0.091 18, α(L)=0.0167 17, α(M)=0.0037 5, α(N)=0.00083 9, α(O)=0.000117 7, α(P)=5.4×10^-6 16, α(N+)=0.00095 10
	5+		414.057 16	M1+E2	-1.8 8	0.025	α=0.025 4, α(K)=0.020 4, α(L)=0.00343 23, α(M)=0.00075 5, α(N)=0.000168 11, α(O)=2.42×10^-5 20, α(P)=1.19E-6 24, α(N+)=0.000194 13
	5+		553.260 15	E1		0.00344	α=0.00344 5, α(K)=0.00295 5, α(L)=0.000389 6, α(M)=8.28×10^-5 12, α(N)=1.87E-5 3, α(O)=2.78E-6 4, α(P)=1.680E-7 24, α(N+)=2.16E-5 3
	5+		967.306 17	M1+E2		0.0035	α=0.0035 8, α(K)=0.0030 7, α(L)=0.00040 9, α(M)=8.6×10^-5 18, α(N)=2.0E-5 4, α(O)=2.9E-6 7, α(P)=1.8E-7 5, α(N+)=2.3E-5 5
2194.061	6+		98.530 20	M1+E2	0.18	1.79	α=1.79 3, α(K)=1.486 21, α(L)=0.235 4, α(M)=0.0511 8, α(N)=0.01152 17, α(O)=0.001689 24, α(P)=9.40×10^-5 14, α(N+)=0.01330 19
	6+		288.141 13	M1+E2	+0.088 21	0.0898	α=0.0898, α(K)=0.0763 11, α(L)=0.01061 15, α(M)=0.00228 4, α(N)=0.000516 8, α(O)=7.75×10^-5 11, α(P)=4.82E-6 7, α(N+)=0.000599 9
	6+		599.81 3	E1+M2	-0.021 11	0.00290	α=0.00290 5, α(K)=0.00249 4, α(L)=0.000327 6, α(M)=6.96×10^-5 12, α(N)=1.57E-5 3, α(O)=2.34E-6 4, α(P)=1.423E-7 24, α(N+)=1.82E-5 3
	6+		1013.808 11	E2+M3	-0.025 14	0.00243	α=0.00243 4, α(K)=0.00206 4, α(L)=0.000290 5, α(M)=6.22×10^-5 10, α(N)=1.404E-5 22, α(O)=2.08E-6 4, α(P)=1.224E-7 20, α(N+)=1.62E-5 3
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2214.215	5+		66.72 9	M1		5.43	α=5.43, 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 5, α(N+)=0.0370 6
	5+		182.83 3	E1		0.0537	α=0.0537, α(K)=0.0456 7, α(L)=0.00636 9, α(M)=0.001359 19, α(N)=0.000305 5, α(O)=4.42×10^-5 7, α(P)=2.39E-6 4, α(N+)=0.000351 5
	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 5, α(N)=0.000433 7, α(O)=6.23×10^-5 24, α(P)=3.1E-6 10, α(N+)=0.000498 7
	5+		310.14 10	E2		0.0507	α=0.0507, α(K)=0.0397 6, α(L)=0.00863 13, α(M)=0.00192 3, α(N)=0.000428 6, α(O)=5.90×10^-5 9, α(P)=2.15E-6 3, α(N+)=0.000489 7
	5+		319.270 20	M1,E2		0.057	α=0.057 12, α(K)=0.047 11, α(L)=0.00792 18, α(M)=0.001730 25, α(N)=0.000389 7, α(O)=5.6×10^-5 3, α(P)=2.8E-6 9, α(N+)=0.000448 10
	5+		480.89 8	M1		0.0238	α=0.0238, α(K)=0.0203 3, α(L)=0.00276 4, α(M)=0.000591 9, α(N)=0.0001340 19, α(O)=2.02×10^-5 3, α(P)=1.269E-6 18, α(N+)=0.0001555 22
	5+		620.04 3	E1+M2	+0.13 5	0.0033	α=0.0033 5, α(K)=0.0028 5, α(L)=0.00037 7, α(M)=8.0×10^-5 14, α(N)=1.8E-5 4, α(O)=2.7E-6 5, α(P)=1.6E-7 3, α(N+)=2.1E-5 4
	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 11, α(O)=2.21E-6 17, α(P)=1.33E-7 12, α(N+)=1.71E-5 13
2228.042	4+		495.25 6	M1		0.0221	α=0.0221, α(K)=0.0188 3, α(L)=0.00256 4, α(M)=0.000548 8, α(N)=0.0001243 18, α(O)=1.87×10^-5 3, α(P)=1.177E-6 17, α(N+)=0.0001442 21
	4+		1047.570 20	M1		0.00353	α=0.00353 5, α(K)=0.00302 5, α(L)=0.000401 6, α(M)=8.55×10^-5 12, α(N)=1.94E-5 3, α(O)=2.92E-6 4, α(P)=1.87E-7 3, α(N+)=2.25E-5 4
	4+		1677.85 3	E2		0.001034	α=0.001034 15, α(K)=0.000763 11, α(L)=0.0001007 15, α(M)=2.15×10^-5 3, α(N)=4.86E-6 7, α(O)=7.28E-7 11, α(P)=4.55E-8 7, α(N+)=0.000148
2313.57	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 14, α(P)=4.3E-8 9, α(N+)=1.50E-5 8
2313.57	2+		1763.26 8	M1+E2	+2.2 5	0.00104	α=0.00104 3, α(K)=0.000732 22, α(L)=9.6×10^-5 3, α(M)=2.05E-5 6, α(N)=4.64E-6 14, α(O)=6.97E-7 21, α(P)=4.39E-8 14, α(N+)=0.000189 4
2327.09	4+		432.745 8	M1		0.0311	α=0.0311, 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 24, α(N+)=0.000204 3
2327.09	4+		1146.805 14	M1+E2	-2.0 5	0.00207	α=0.00207 11, α(K)=0.00176 10, 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 7, α(N+)=1.51E-5 7
2339.21	3-		1788.90 9	E1+M2	+0.06 4	0.000804	α=0.000804 15, α(K)=0.000328 12, α(L)=4.15×10^-5 16, α(M)=8.8E-6 4, α(N)=1.99E-6 8, α(O)=2.99E-7 11, α(P)=1.91E-8 7, α(N+)=0.000425 7
2374.447	5+,6+		468.500 12	M1+E2	0.41 GE	0.020	α=0.020 5, α(K)=0.016 4, α(L)=0.0025 4, α(M)=0.00055 7, α(N)=0.000123 16, α(O)=1.8×10^-5 3, α(P)=1.0E-6 3, α(N+)=0.000142 19
2381.67	2+	87 fs 17	1831.40 10	M1+E2	+0.46 8	0.001167	B(E2)(W.u.)>0.79, B(M1)(W.u.)<0.042, α=0.001167 21, α(K)=0.000804 15, α(L)=0.0001051 20, α(M)=2.24E-5 5, α(N)=5.07E-6 10, α(O)=7.65E-7 15, α(P)=4.91E-8 10, α(N+)=0.000235
2390.43	3+		1840.06 8	M1+E2	-1.37 12	0.001047	α=0.001047 18, α(K)=0.000707 13, α(L)=9.25×10^-5 17, α(M)=1.97E-5 4, α(N)=4.47E-6 8, α(O)=6.72E-7 13, α(P)=4.26E-8 8, α(N+)=0.000228 4
2392.32	7+		486.45 6	M1+E2	-0.15 8	0.0229	α=0.0229 5, α(K)=0.0195 4, α(L)=0.00267 5, α(M)=0.000571 9, α(N)=0.0001294 21, α(O)=1.94×10^-5 4, α(P)=1.220E-6 24, α(N+)=0.0001500 24
2490.004	4+		756.581 12	M1,E2		0.0061	α=0.0061 16, α(K)=0.0052 14, α(L)=0.00073 16, α(M)=0.00016 4, α(N)=3.5×10^-5 8, α(O)=5.3E-6 12, α(P)=3.2E-7 9, α(N+)=4.1E-5 9
	4+		1309.778 16	M1+E2		0.0018	α=0.0018 4, α(K)=0.0015 3, α(L)=0.00020 4, α(M)=4.3×10^-5 8, α(N)=9.7E-6 18, α(O)=1.5E-6 3, α(P)=9.2E-8 19, α(N+)=3.4E-5 3
	4+		1328.504 15	E1		0.000708	α=0.000708 10, α(K)=0.000531 8, α(L)=6.76×10^-5 10, α(M)=1.434E-5 20, α(N)=3.25E-6 5, α(O)=4.87E-7 7, α(P)=3.09E-8 5, α(N+)=9.44E-5 1
2524.101	4+		296.21 7	M1		0.0836	α=0.0836, α(K)=0.0711 10, α(L)=0.00985 14, α(M)=0.00211 3, α(N)=0.000479 7, α(O)=7.19×10^-5 10, α(P)=4.49E-6 7, α(N+)=0.000555 8
	4+		310.14 10	M1		0.0740	α=0.0740, α(K)=0.0630 9, α(L)=0.00871 13, α(M)=0.00187 3, α(N)=0.000424 6, α(O)=6.36×10^-5 9, α(P)=3.98E-6 6, α(N+)=0.000491 7
	4+		929.85 3	[E1]		0.001184	α=0.001184 17, α(K)=0.001018 15, α(L)=0.0001312 19, α(M)=2.79×10^-5 4, α(N)=6.30E-6 9, α(O)=9.43E-7 14, α(P)=5.88E-8 9, α(N+)=7.30E-6
	4+		1343.87 3	M1+E2	+0.20	0.00198	α=0.00198 3, α(K)=0.001668 24, α(L)=0.000220 3, α(M)=4.69×10^-5 7, α(N)=1.064E-5 15, α(O)=1.604E-6 23, α(P)=1.026E-7 15, α(N+)=4.41E-5 7
	4+		1362.640 19	E1		0.000702	α=0.000702 10, α(K)=0.000509 8, α(L)=6.46×10^-5 9, α(M)=1.371E-5 20, α(N)=3.10E-6 5, α(O)=4.66E-7 7, α(P)=2.95E-8 5, α(N+)=0.0001155
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2544.67	8+		415.9 1	E1		0.00661	α=0.00661 10, 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 5, α(N+)=4.20E-5 6
	8+		449.0 11	E2		0.0172	α=0.0172 3, α(K)=0.01398 22, α(L)=0.00250 4, α(M)=0.000549 9, α(N)=0.0001230 20, α(O)=1.75×10^-5 3, α(P)=7.96E-7 13, α(N+)=0.0001413 23
	8+		638.5 1	E2		0.00687	α=0.00687 10, α(K)=0.00573 8, α(L)=0.000899 13, α(M)=0.000195 3, α(N)=4.39×10^-5 7, α(O)=6.38E-6 9, α(P)=3.35E-7 5, α(N+)=5.06E-5 7
2567.89	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 5, α(O)=5.8E-7 7, α(P)=3.7E-8 5, α(N+)=0.000319 18
2583.862	4(-)		989.606 10	M1,E2		0.0033	α=0.0033 8, α(K)=0.0028 7, α(L)=0.00038 8, α(M)=8.2×10^-5 17, α(N)=1.9E-5 4, α(O)=2.8E-6 6, α(P)=1.7E-7 5, α(N+)=2.1E-5 5
2633.15	3-		2082.88 9	E1		0.000931	α=0.000931 13, α(K)=0.000253 4, α(L)=3.17×10^-5 5, α(M)=6.73E-6 10, α(N)=1.523E-6 22, α(O)=2.29E-7 4, α(P)=1.471E-8 21, α(N+)=0.000640 9
2641.222	5+		735.00 5	M1+E2	-1.1 6	0.0064	α=0.0064 12, α(K)=0.0055 11, α(L)=0.00077 12, α(M)=0.000165 24, α(N)=3.7×10^-5 6, α(O)=5.6E-6 9, α(P)=3.3E-7 7, α(N+)=4.3E-5 7
2641.222	5+		1460.630 19	M1+E2	+2.1 16	0.0013	α=0.0013 3, α(K)=0.00107 25, α(L)=0.00014 4, α(M)=3.0×10^-5 7, α(N)=6.9E-6 16, α(O)=1.03E-6 24, α(P)=6.4E-8 17, α(N+)=7.1E-5 6
2683.467	4-,5-		1089.154 18	M1		0.00322	α=0.00322 5, α(K)=0.00275 4, α(L)=0.000365 6, 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, α(N+)=2.05E-5 3
2698.539	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)=0.00050 15, α(P)=1.7×10^-5 5, α(N+)=0.0041 15
2698.539	5-,6-		1104.321 16	M1		0.00311	α=0.00311 5, 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, α(N+)=2.02E-5 3
2714.98	8+		586.2 1	E1		0.00303	α=0.00303 5, α(K)=0.00260 4, α(L)=0.000342 5, α(M)=7.27×10^-5 11, α(N)=1.643E-5 23, α(O)=2.44E-6 4, α(P)=1.484E-7 21, α(N+)=1.90E-5 3
2714.98	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)=2.38×10^-5 4, α(O)=3.50E-6 5, α(P)=1.97E-7 3, α(N+)=2.75E-5 4
2723.506	4+		495.25 6	M1		0.0221	α=0.0221, α(K)=0.0188 3, α(L)=0.00256 4, α(M)=0.000548 8, α(N)=0.0001243 18, α(O)=1.87×10^-5 3, α(P)=1.177E-6 17, α(N+)=0.0001442 21
2723.506	4+		1543.289 27	M1+E2		0.00133	α=0.00133 21, α(K)=0.00106 17, α(L)=0.000140 22, α(M)=3.0×10^-5 5, α(N)=6.8E-6 11, α(O)=1.02E-6 16, α(P)=6.4E-8 12, α(N+)=0.000102 6
2753.15	3+		2202.88 6	M1+E2		0.00100	α=0.00100 8, α(K)=0.00051 5, α(L)=6.6×10^-5 7, α(M)=1.41E-5 14, α(N)=3.2E-6 3, α(O)=4.8E-7 5, α(P)=3.1E-8 4, α(N+)=0.000412 24
2801.752	5+		654.220 8	M1+E2	+0.9 3	0.0090	α=0.0090 9, α(K)=0.0076 8, α(L)=0.00108 8, α(M)=0.000231 17, α(N)=5.2×10^-5 4, α(O)=7.8E-6 6, α(P)=4.7E-7 5, α(N+)=6.1E-5 5
	5+		895.847 10	M1+E2	-0.20 11	0.00504	α=0.00504 12, α(K)=0.00431 11, α(L)=0.000576 13, α(M)=0.000123 3, α(N)=2.79×10^-5 7, α(O)=4.20E-6 10, α(P)=2.67E-7 7, α(N+)=3.24E-5 8
	5+		1207.473 14	E1+M2		0.003	α=0.003 3, α(K)=0.0029 23, α(L)=0.0004 4, α(M)=8.E-5 7, α(N)=1.9E-5 16, α(O)=2.9E-6 24, α(P)=1.8E-7 15, α(N+)=3.8E-5 4
	5+		1621.510 20	M1+E2		0.00124	α=0.00124 18, α(K)=0.00096 15, α(L)=0.000126 19, 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, α(N+)=0.000133 8
2807.35	9-		92.2 2	E1		0.343	α=0.343 6, α(K)=0.289 5, α(L)=0.0429 7, α(M)=0.00918 14, α(N)=0.00204 4, α(O)=0.000288 5, α(P)=1.384×10^-5 21, α(N+)=0.00234 4
	9-		262.5	E1		0.0207	α=0.0207, α(K)=0.01764 25, α(L)=0.00241 4, α(M)=0.000514 8, α(N)=0.0001157 17, α(O)=1.694×10^-5 24, α(P)=9.59E-7 14, α(N+)=0.0001336 19
	9-		678.6 1	E2		0.00593	α=0.00593 9, α(K)=0.00496 7, α(L)=0.000764 11, α(M)=0.0001656 24, α(N)=3.73×10^-5 6, α(O)=5.43E-6 8, α(P)=2.91E-7 4, α(N+)=4.30E-5 6
2815.584	4-		1221.37 4	M1		0.00247	α=0.00247 4, α(K)=0.00211 3, α(L)=0.000278 4, α(M)=5.94×10^-5 9, α(N)=1.347E-5 19, α(O)=2.03E-6 3, α(P)=1.299E-7 19, α(N+)=2.44E-5 4
2815.584	4-		1635.31 3	E1+M2		0.0018	α=0.0018 11, α(K)=0.0014 11, α(L)=0.00019 14, α(M)=4.E-5 3, α(N)=9.E-6 7, α(O)=1.4E-6 11, α(P)=9.E-8 7, α(N+)=0.00019 12
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2830.660	5+		683.153 7	M1+E2		0.0079	α=0.0079 21, α(K)=0.0067 18, α(L)=0.00094 20, α(M)=0.00020 4, α(N)=4.6×10^-5 10, α(O)=6.8E-6 15, α(P)=4.1E-7 12, α(N+)=5.3E-5 11
	5+		735.00 5	M1+E2	-1.1 6	0.0064	α=0.0064 12, α(K)=0.0055 11, α(L)=0.00077 12, α(M)=0.000165 24, α(N)=3.7×10^-5 6, α(O)=5.6E-6 9, α(P)=3.3E-7 7, α(N+)=4.3E-5 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 17, α(N)=2.62×10^-5 4, α(O)=3.95E-6 6, α(P)=2.51E-7 4, α(N+)=3.04E-5 5
	5+		1097.18 3	M1		0.00316	α=0.00316 5, α(K)=0.00271 4, α(L)=0.000359 5, α(M)=7.66×10^-5 11, α(N)=1.737E-5 25, α(O)=2.62E-6 4, α(P)=1.672E-7 24, α(N+)=2.02E-5 3
	5+		1236.374 16	E1		0.000743	α=0.000743 11, α(K)=0.000603 9, α(L)=7.69×10^-5 11, α(M)=1.632E-5 23, α(N)=3.69E-6 6, α(O)=5.54E-7 8, α(P)=3.50E-8 5, α(N+)=4.69E-5 7
	5+		1650.436 24	M1+E2		0.00121	α=0.00121 17, α(K)=0.00092 14, α(L)=0.000121 18, α(M)=2.6×10^-5 4, α(N)=5.9E-6 9, α(O)=8.8E-7 13, α(P)=5.6E-8 9, α(N+)=0.000145 8
2861.07	4-,5-		1266.76 5	M1		0.00228	α=0.00228 4, α(K)=0.00194 3, α(L)=0.000255 4, α(M)=5.45×10^-5 8, α(N)=1.236E-5 18, α(O)=1.86E-6 3, α(P)=1.193E-7 17, α(N+)=3.02E-5 5
2976.32	8-		847.4 2	E2(+M1)		0.0047	α=0.0047 12, α(K)=0.0040 10, α(L)=0.00055 12, α(M)=0.000119 25, α(N)=2.7×10^-5 6, α(O)=4.0E-6 9, α(P)=2.4E-7 7, α(N+)=3.1E-5 7
3235.23	10+		690.6 1	E2		0.00569	α=0.00569 8, α(K)=0.00476 7, α(L)=0.000730 11, α(M)=0.0001581 23, α(N)=3.56×10^-5 5, α(O)=5.19E-6 8, α(P)=2.80E-7 4, α(N+)=4.11E-5 6
3253.45	10-		446.1 1	M1+E2	-0.10 5	0.0287	α=0.0287 5, α(K)=0.0244 4, α(L)=0.00334 5, α(M)=0.000716 11, α(N)=0.0001624 24, α(O)=2.44×10^-5 4, α(P)=1.531E-6 24, α(N+)=0.000188 3
3398.13	10+		590.8 1	E1		0.00298	α=0.00298 5, 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)=2.40E-6 4, α(P)=1.460E-7 21, α(N+)=1.87E-5 3
3398.13	10+		683.1 1	E2		0.00584	α=0.00584 9, α(K)=0.00488 7, α(L)=0.000751 11, α(M)=0.0001627 23, α(N)=3.66×10^-5 6, α(O)=5.34E-6 8, α(P)=2.87E-7 4, α(N+)=4.23E-5 6
3421.90	11-		186.7 1	E1		0.0508	α=0.0508, α(K)=0.0432 6, α(L)=0.00601 9, α(M)=0.001284 18, α(N)=0.000288 4, α(O)=4.17×10^-5 6, α(P)=2.27E-6 4, α(N+)=0.000332 5
3421.90	11-		614.5 1	E2		0.00755	α=0.00755 11, α(K)=0.00628 9, α(L)=0.000998 14, α(M)=0.000217 3, α(N)=4.87×10^-5 7, α(O)=7.07E-6 10, α(P)=3.67E-7 6, α(N+)=5.62E-5 8
3614.76	11-		216.6 1	E1		0.0342	α=0.0342, α(K)=0.0291 4, α(L)=0.00402 6, α(M)=0.000858 12, α(N)=0.000193 3, α(O)=2.81×10^-5 4, α(P)=1.553E-6 22, α(N+)=0.000222 4
3614.76	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)=2.39×10^-5 4, α(O)=3.52E-6 5, α(P)=1.97E-7 3, α(N+)=2.76E-5 4
3992.62	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 25, α(O)=2.59E-6 4, α(P)=1.572E-7 22, α(N+)=2.02E-5 3
3992.62	12+		757.3 1	E2		0.00459	α=0.00459 7, α(K)=0.00385 6, α(L)=0.000576 8, α(M)=0.0001245 18, α(N)=2.81×10^-5 4, α(O)=4.11E-6 6, α(P)=2.27E-7 4, α(N+)=3.24E-5 5
4104.39	12+		489.6 1	E1		0.00452	α=0.00452 7, α(K)=0.00387 6, α(L)=0.000514 8, α(M)=0.0001094 16, α(N)=2.47×10^-5 4, α(O)=3.66E-6 6, α(P)=2.20E-7 3, α(N+)=2.86E-5 4
	12+		682.2 2	E1		0.00220	α=0.00220 3, α(K)=0.00188 3, α(L)=0.000246 4, α(M)=5.24×10^-5 8, α(N)=1.183E-5 17, α(O)=1.763E-6 25, α(P)=1.082E-7 16, α(N+)=1.370E-5 20
	12+		706.2 1	E2		0.00540	α=0.00540 8, α(K)=0.00452 7, 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, α(N+)=3.87E-5 6
4397.78	13-		293.3 2	E1		0.01558	α=0.01558, α(K)=0.01329 19, α(L)=0.00181 3, α(M)=0.000385 6, α(N)=8.67×10^-5 13, α(O)=1.273E-5 18, α(P)=7.29E-7 11, α(N+)=0.0001002 15
4397.78	13-		783.0 1	E2		0.00425	α=0.00425 6, α(K)=0.00357 5, α(L)=0.000530 8, α(M)=0.0001145 16, α(N)=2.58×10^-5 4, α(O)=3.79E-6 6, α(P)=2.11E-7 3, α(N+)=2.98E-5 5
4805.18	14+		407.4 2	E1		0.00694	α=0.00694 10, α(K)=0.00593 9, α(L)=0.000794 12, α(M)=0.0001692 24, α(N)=3.82×10^-5 6, α(O)=5.64E-6 8, α(P)=3.33E-7 5, α(N+)=4.41E-5 7
	14+		694.7 2	E1		0.00211	α=0.00211 3, α(K)=0.00181 3, α(L)=0.000237 4, α(M)=5.04×10^-5 7, α(N)=1.138E-5 16, α(O)=1.697E-6 24, α(P)=1.042E-7 15, α(N+)=1.319E-5 19
	14+		700.8 2	E2		0.00549	α=0.00549 8, α(K)=0.00460 7, α(L)=0.000703 10, α(M)=0.0001521 22, α(N)=3.43×10^-5 5, α(O)=5.00E-6 7, α(P)=2.71E-7 4, α(N+)=3.95E-5 6
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
4889.71	14-		373.0 2	E1		0.00858	α=0.00858 12, α(K)=0.00733 11, α(L)=0.000984 14, α(M)=0.000210 3, α(N)=4.73×10^-5 7, α(O)=6.98E-6 10, α(P)=4.09E-7 6, α(N+)=5.47E-5 8
4889.71	14-		781.0 1	E2		0.00427	α=0.00427 6, α(K)=0.00359 5, α(L)=0.000534 8, α(M)=0.0001152 17, α(N)=2.60×10^-5 4, α(O)=3.81E-6 6, α(P)=2.12E-7 3, α(N+)=3.00E-5 5
5136.13	15-		331.0 2	E1		0.01150	α=0.01150, 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 14, α(P)=5.44E-7 8, α(N+)=7.37E-5 11
5136.13	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 5, α(O)=4.38E-6 7, α(P)=2.41E-7 4, α(N+)=3.46E-5 5
5274.93	15+		385.1 2	E1		0.00794	α=0.00794 12, α(K)=0.00678 10, α(L)=0.000910 13, α(M)=0.000194 3, α(N)=4.38×10^-5 7, α(O)=6.46E-6 9, α(P)=3.80E-7 6, α(N+)=5.06E-5 8
5274.93	15+		758.2 1	E2		0.00457	α=0.00457 7, α(K)=0.00384 6, α(L)=0.000575 8, α(M)=0.0001241 18, α(N)=2.80×10^-5 4, α(O)=4.10E-6 6, α(P)=2.27E-7 4, α(N+)=3.23E-5 5
5496.39	16+		360.3 2	E1		0.00933	α=0.00933 14, α(K)=0.00797 12, α(L)=0.001073 15, α(M)=0.000229 4, α(N)=5.15×10^-5 8, α(O)=7.60E-6 11, α(P)=4.44E-7 7, α(N+)=5.96E-5 9
	16+		653.7 2	E1		0.00240	α=0.00240 4, α(K)=0.00206 3, α(L)=0.000270 4, α(M)=5.74×10^-5 8, α(N)=1.296E-5 19, α(O)=1.93E-6 3, α(P)=1.181E-7 17, α(N+)=1.501E-5 21
	16+		691.2 2	E2		0.00568	α=0.00568 8, α(K)=0.00475 7, α(L)=0.000728 11, α(M)=0.0001577 23, α(N)=3.55×10^-5 5, α(O)=5.18E-6 8, α(P)=2.79E-7 4, α(N+)=4.10E-5 6
5946.08	18+		108.7 2	E1		0.220	α=0.220, α(K)=0.185 3, α(L)=0.0270 4, α(M)=0.00577 9, α(N)=0.001288 20, α(O)=0.000183 3, α(P)=9.09×10^-6 14, α(N+)=0.001479 22
	18+		384.9 2	E1		0.00795	α=0.00795 12, α(K)=0.00679 10, α(L)=0.000911 13, α(M)=0.000194 3, α(N)=4.38×10^-5 7, α(O)=6.47E-6 9, α(P)=3.80E-7 6, α(N+)=5.07E-5 8
	18+		449.7 2	E2		0.01710	α=0.01710, α(K)=0.01392 20, α(L)=0.00249 4, α(M)=0.000546 8, α(N)=0.0001224 18, α(O)=1.739×10^-5 25, α(P)=7.93E-7 12, α(N+)=0.0001406 20
6195.29	19-		249	E1		0.0237	α=0.0237, α(K)=0.0202 3, α(L)=0.00277 4, α(M)=0.000591 9, α(N)=0.0001329 19, α(O)=1.94×10^-5 3, α(P)=1.094E-6 16, α(N+)=0.0001535 22
6195.29	19-		358.0 2	E2		0.0329	α=0.0329, α(K)=0.0262 4, α(L)=0.00524 8, α(M)=0.001159 17, α(N)=0.000259 4, α(O)=3.61×10^-5 6, α(P)=1.448E-6 21, α(N+)=0.000296 5
6592.79	20(+)		397.5 2	E1		0.00736	α=0.00736 11, α(K)=0.00629 9, α(L)=0.000842 12, α(M)=0.000180 3, α(N)=4.05×10^-5 6, α(O)=5.98E-6 9, α(P)=3.53E-7 5, α(N+)=4.68E-5 7
6592.79	20(+)		646.6 2	E2		0.00666	α=0.00666 10, α(K)=0.00556 8, α(L)=0.000869 13, α(M)=0.000188 3, α(N)=4.24×10^-5 6, α(O)=6.17E-6 9, α(P)=3.26E-7 5, α(N+)=4.89E-5 7
7329.3	22(+)		416.0 3	E1		0.00660	α=0.00660 10, α(K)=0.00565 8, α(L)=0.000755 11, α(M)=0.0001609 23, α(N)=3.63×10^-5 6, α(O)=5.36E-6 8, α(P)=3.17E-7 5, α(N+)=4.20E-5 6
7329.3	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 5, α(O)=4.41E-6 7, α(P)=2.42E-7 4, α(N+)=3.48E-5 5
7620.4	23(-)		291.2 2	E1		0.01587	α=0.01587, α(K)=0.01353 19, α(L)=0.00184 3, α(M)=0.000393 6, α(N)=8.84×10^-5 13, α(O)=1.297E-5 19, α(P)=7.42E-7 11, α(N+)=0.0001021 15
7620.4	23(-)		707.1 2	E2		0.00538	α=0.00538 8, α(K)=0.00451 7, 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, α(N+)=3.86E-5 6
7977.6	24(+)		357.2 3	E1		0.00953	α=0.00953 14, α(K)=0.00814 12, α(L)=0.001096 16, α(M)=0.000234 4, α(N)=5.27×10^-5 8, α(O)=7.76E-6 11, α(P)=4.53E-7 7, α(N+)=6.09E-5 9
7977.6	24(+)		648.2 2	E2		0.00662	α=0.00662 10, α(K)=0.00553 8, α(L)=0.000863 13, α(M)=0.000187 3, α(N)=4.21×10^-5 6, α(O)=6.13E-6 9, α(P)=3.24E-7 5, α(N+)=4.86E-5 7
8214.5	25(-)		236.9 2	E1		0.0270	α=0.0270, α(K)=0.0230 4, α(L)=0.00316 5, α(M)=0.000675 10, α(N)=0.0001517 22, α(O)=2.21×10^-5 4, α(P)=1.239E-6 18, α(N+)=0.0001751 25
8214.5	25(-)		594.2 2	E2		0.00821	α=0.00821 12, α(K)=0.00682 10, α(L)=0.001095 16, α(M)=0.000238 4, α(N)=5.35×10^-5 8, α(O)=7.75E-6 11, α(P)=3.97E-7 6, α(N+)=6.17E-5 9

Q(β-)=-3037 keV 10	S(n)= 8141.37 keV 28	S(p)= 7583.1 keV 4	Q(α)= 1986.9 keV 10
Reference: 2012WA38

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; GS band
0.0	0+	7×10⁺¹⁵ y 3 % α = 100
550.255 8	2+	7.72 ps 32	550.273 9	100	E2	0.0	0+
1180.261 12	4+	2.39 ps 24	629.987 8	100	E2	550.255	2+
1905.908 13	6+		311.570 20 725.673 9	14.2 3 100 2	E1 E2	1594.247 1180.261	5- 4+
2714.98 16	8+		586.2 1 808.7 1		E1 E2	2128.64 1905.908	7- 6+
3398.13 16	10+		590.8 1 683.1 1 853.4 3 ?		E1 E2	2807.35 2714.98 2544.67	9- 8+ 8+
4104.39 17	12+		489.6 1 682.2 2 706.2 1 869.6 2		E1 E1 E2	3614.76 3421.90 3398.13 3235.23	11- 11- 10+ 10+
4805.18 18	14+		407.4 2 616.0 2 694.7 2 700.8 2 812.6 2		E1 E1 E2	4397.78 4189.28 4110.68 4104.39 3992.62	13- 12+ 13- 12+ 12+
5496.39 19	16+		360.3 2 586.6 2 631.8 2 653.7 2 691.2 2		E1 E1 E2	5136.13 4909.65 4864.69 4842.69 4805.18	15- 14+ 14+ 15- 14+
5946.08 19	18+		108.7 2 296.5 2 384.9 2 421.6 2 449.7 2		E1 E1 E2	5837.32 5649.57 5561.19 5524.48 5496.39	17- 17- 17- 16+ 16+
6592.79 21	20(+)		397.5 2 646.6 2		E1 E2	6195.29 5946.08	19- 18+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
7329.3 3	22(+)		416.0 3 736.5 2		E1 E2	6913.3 6592.79	21(-) 20(+)
7977.6 3	24(+)
8659.5 5	26(+)		445.0 3 681.4 5 ?			8214.5 7977.6	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
1161.529 12	3-	0.6 ps +4-2
1594.247 12	5-		414.028 12 432.745 8	100 3 27.6 15	E1+M2 E2	1180.261 1161.529	4+ 3-
2128.64 7	7-		222.71 12 534.38 7	22.9 21 100 21	E1 E2	1905.908 1594.247	6+ 5-
2807.35 16	9-		92.2 2 262.5 678.6 1	18 100 6	E1 E1 E2	2714.98 2544.67 2128.64	8+ 8+ 7-
3614.76 17	11-		216.6 1 807.4 1		E1 E2	3398.13 2807.35	10+ 9-
4397.78 18	13-		293.3 2 783.0 1		E1 E2	4104.39 3614.76	12+ 11-
5136.13 19	15-		331.0 2 738.3 2		E1 E2	4805.18 4397.78	14+ 13-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - band 3
5837.32 22	17-
6195.29 21	19-		166.1 1 184.0 2 249? 358.0 2		E1 E2	6029.22 6011.15 5946.08 5837.32	18- 18 18+ 17-
6913.3 3	21(-)		718.0 2	100		6195.29	19-
7620.4 3	23(-)		291.2 2 707.1 2		E1 E2	7329.3 6913.3	22(+) 21(-)
8214.5 3	25(-)		236.9 2 594.2 2		E1 E2	7977.6 7620.4	24(+) 23(-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - band 4
2095.595 13	6+
2544.67 15	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	2392.32 2194.061 2128.64 2095.595 1905.908	7+ 6+ 7- 6+ 6+
3235.23 17	10+		690.6 1	100	E2	2544.67	8+
3992.62 17	12+		570.6 2 594.7 2 757.3 1		E1 E2	3421.90 3398.13 3235.23	11- 10+ 10+
4864.69 17	14+		466.9 2 623.3 2 675.3 2 754.0 2 760.3 2 872.0 1			4397.78 4241.52 4189.28 4110.68 4104.39 3992.62	13- 13- 12+ 13- 12+ 12+
5524.48 19	16+		615.0 2 659.6 2 681.7 2 719.4 2			4909.65 4864.69 4842.69 4805.18	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
3421.90 16	11-
4110.68 17	13-		688.8 1	100		3421.90	11-
4842.69 18	15-		732.0 1	100		4110.68	13-
5561.19 20	17-		718.5 1	100		4842.69	15-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - band 6
6694.32 21	21(-)	32 ns 3
7332.92 23	23(-)		638.6 1	100		6694.32	21(-)
8010.61 25	25(-)		677.7 1	100		7332.92	23(-)
8602.2 3	27(-)		591.6 1	100		8010.61	25(-)
9601.2 4	29		999.0 2	100		8602.2	27(-)
10439.0 4	31		837.8 2	100		9601.2	29
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - band 7
3188.31 17	9-
3806.98 18	11-		261.2 2 385.4 2 618.6 1			3545.63 3421.90 3188.31	10- 11- 9-
4512.91 19	13-		316.7 2 402.2 2 705.9 2			4196.25 4110.68 3806.98	12- 13- 11-
5287.77 25	15-		445.0 3 774.9 2			4842.69 4512.91	15- 13-

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	0+	7×10⁺¹⁵ y 3 % α = 100	Rms charge radius <r²>^1/2=5.0009 fm 16 (2004An14). E(level): band 1; GS band.
550.255	2+	7.72 ps 32	μ=+0.508 42 (2005St24,1987Ba65), Q=-0.98 27 (2005St24,1973ClZF) μ, other: +0.61 7 (1987Be08). E(level): band 1; GS band.
1161.529	3-	0.6 ps +4-2	B(E3)\|^=0.37 3 (Coul. ex., 1968Ke04). E(level): band 2; octupole band.
1180.261	4+	2.39 ps 24	E(level): band 1; GS band.
1465.137	1-	92 fs 8	B(E1)\|^=0.013 5 (Coul. ex., 1968Ve01).
1594.247	5-		E(level): band 2; octupole band.
1905.908	6+		E(level): band 1; GS band.
2095.595	6+		E(level): band 4.
2128.64	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.
2146.35	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).
2194.061	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.
2327.09	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).
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).
2339.21	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).
2381.67	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).
2392.32	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.
2467.38	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).
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).
2539.82	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).
2544.67	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.
2567.89	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).
2570.832	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).
2583.862	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
2633.15	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).
2641.222	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).
2697.77	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).
2701.92	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).
2713.334	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).
2714.98	8+		E(level): band 1; GS 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.
2738.79	(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.
2753.15	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).
2806.73	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).
2807.35	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.
2862.06	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).
2942.82	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.
2967.6	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).
2976.32	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.
2980.50	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).
2991.78	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).
3063.25	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).
3089.84	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).
3095.25	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).
3138.46	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).
3164.8	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).
3188.31	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).
E(level)	J^π(level)	T_1/2(level)	Comments
3216.15	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.
3235.23	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.
3253.45	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).
3322.6	(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.
3398.13	10+		E(level): band 1; GS 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.
3421.90	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.
3483.6	(1,2+)		B(E1)\|^=6.0×10^-5 15 (γ,γ’, 1993Zi05).
3526.57	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.
3534.9	(1,2+)		B(E1)\|^=5.8×10^-5 4 (γ,γ’, 1993Zi05).
3545.63	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.
3614.76	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.
3640.4	(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.
3806.98	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.
3843.6	(1,2+)		B(E1)\|^=0.6×10^-5 2 (γ,γ’, 1993Zi05).
3992.62	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.
4104.39	12+		E(level): band 1; GS 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.
4108.70	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.
4110.68	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.
4189.28	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.
4196.25	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.
4241.52	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.
4397.78	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.
4512.91	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.
E(level)	J^π(level)	T_1/2(level)	Comments
4516.75	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.
4805.18	14+		E(level): band 1; GS 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.
4842.69	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.
4864.69	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.
4889.71	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.
4909.65	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.
4917.55	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.
4951.75	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.
5087.55	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.
5136.13	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.
5217.20	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.
5274.93	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.
5287.77	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.
5320.28	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.
5496.39	16+		E(level): band 1; GS 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.
5524.48	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.
5556.54	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.
5561.19	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.
5578.31	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.
5649.57	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.
5777.74	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.
5837.32	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.
5946.08	18+		E(level): band 1; GS 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.
6011.15	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.
6029.22	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.
E(level)	J^π(level)	T_1/2(level)	Comments
6195.29	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.
6392.23	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.
6477.07	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.
6557.5	(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.
6592.79	20(+)		E(level): band 1; GS 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.
6694.32	21(-)	32 ns 3	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.
6913.3	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.
7329.3	22(+)		E(level): band 1; GS 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.
7332.92	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.
7620.4	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.
7942.5	(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.
7977.6	24(+)		E(level): band 1; GS 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.
8010.61	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.
8214.5	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.
8358.8	(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.
8602.2	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.
8659.5	26(+)		E(level): band 1; GS 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.
8931.5	(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.
9045.9	(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.
9601.2	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.
9898.2	(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.
10439.0	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.
10609.1	(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.
11524.7	(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
1161.529	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
2111.053	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.
2214.215	66.72	I(γ): from ce(K) and α(K)
2723.506	332.91	E(γ): 1985Si16 relate this γ to ¹⁵⁰Eu ε decay
3197.4	1743.3	E(γ): multiplet
5287.77	445.0	E(γ): Multiply placed
8659.5	445.0	E(γ): Multiply placed
9898.2	1296.0	E(γ): doublet