List of levels for 242AM

Authors: M.J. Martin, C.D. Nesaraja | Citation: Nucl. Data Sheets 186, 261 (2022) | Cutoff date: 31-Dec-2021

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
44.093	0-		44.092 3	M1		68.5	α=68.5 10, α(L)=51.5 7, α(M)=12.58 18, α(N)=3.44 5, α(O)=0.866 12, α(P)=0.1658 23, α(Q)=0.01062 15
48.603	5-	141 y 2 % IT = 99.550 10 % α = 0.450 10 % SF < 4.7E-9	48.63 5	E4		7.01×10⁵	B(E4)(W.u.)=6.00E-6 14, α=7.01E5 11, α(L)=3.31E5 5, α(M)=2.65E5 4, α(N)=8.40E4 13, α(O)=1.908E4 30, α(P)=1891 30, α(Q)=2.86 4
52.714	3-		52.770 36	E2		358	α=358 5, α(L)=259 4, α(M)=72.7 10, α(N)=20.11 29, α(O)=4.79 7, α(P)=0.754 11, α(Q)=0.001783 26
75.820	2-		75.823 4	M1		13.99	α=13.99 20, α(L)=10.51 15, α(M)=2.57 4, α(N)=0.702 10, α(O)=0.1768 25, α(P)=0.0338 5, α(Q)=0.002162 30
99.285	0+,1+,2+		99.269 15	E1		0.1386	α=0.1386 19, α(L)=0.1040 15, α(M)=0.0257 4, α(N)=0.00693 10, α(O)=0.001673 23, α(P)=0.000280 4, α(Q)=1.046×10^-5 15
149.707	4-		73.864 11	E2		71.5	α=71.5 10, α(L)=51.8 7, α(M)=14.55 20, α(N)=4.02 6, α(O)=0.960 13, α(P)=0.1521 21, α(Q)=0.000434 6
149.707	4-		96.994 2	M1		6.84	α=6.84 10, α(L)=5.14 7, α(M)=1.254 18, α(N)=0.343 5, α(O)=0.0864 12, α(P)=0.01652 23, α(Q)=0.001055 15
168.387	1-,2-,3-		69.101 8	(E1)		0.356	α=0.356 5, α(L)=0.267 4, α(M)=0.0664 9, α(N)=0.01790 25, α(O)=0.00427 6, α(P)=0.000682 10, α(Q)=2.257×10^-5 32
168.387	1-,2-,3-		92.568 26	M1+E2		16	α=16 8, α(L)=12 6, α(M)=3.2 18, α(N)=0.9 5, α(O)=0.22 12, α(P)=0.036 17, α(Q)=7.E-4 5
181.4	(5+)		132.8 5	(E1)		0.268	α=0.268 4, α(K)=0.2029 33, α(L)=0.0492 8, α(M)=0.01209 21, α(N)=0.00327 6, α(O)=0.000796 14, α(P)=0.0001366 23, α(Q)=5.59×10^-6 9
200.581	3-,4-		147.870 22	M1+E2	1.26 +16-14	5.6	α=5.6 4, α(K)=3.0 4, α(L)=1.87 4, α(M)=0.503 14, α(N)=0.139 4, α(O)=0.0337 9, α(P)=0.00574 11, α(Q)=0.000141 16
230.527	1+		154.708 2	E1		0.1892	α=0.1892 26, α(K)=0.1447 20, α(L)=0.0334 5, α(M)=0.00820 11, α(N)=0.002220 31, α(O)=0.000542 8, α(P)=9.42×10^-5 13, α(Q)=4.03E-6 6
230.527	1+		186.433 2	E1		0.1230	α=0.1230 17, α(K)=0.0951 13, α(L)=0.02100 29, α(M)=0.00514 7, α(N)=0.001392 19, α(O)=0.000341 5, α(P)=6.01×10^-5 8, α(Q)=2.70E-6 4
244.381	3-		94.671 6	M1+E2	0.71 11	12.3	α=12.3 11, α(L)=9.1 8, α(M)=2.41 23, α(N)=0.66 6, α(O)=0.162 15, α(P)=0.0277 21, α(Q)=0.00081 7
	3-		191.667 5	M1		4.57	α=4.57 6, α(K)=3.60 5, α(L)=0.729 10, α(M)=0.1778 25, α(N)=0.0486 7, α(O)=0.01223 17, α(P)=0.002340 33, α(Q)=0.0001487 21
	3-		195.778 6	E2		0.994	α=0.994 14, α(K)=0.1522 21, α(L)=0.611 9, α(M)=0.1706 24, α(N)=0.0472 7, α(O)=0.01131 16, α(P)=0.001854 26, α(Q)=1.455×10^-5 20
269.854	3+		39.42 6	(E2)		1470	α=1470 23, α(L)=1067 17, α(M)=299 5, α(N)=82.5 13, α(O)=19.65 31, α(P)=3.08 5, α(Q)=0.00631 10
274.330	1-		198.498 12	M1+E2	0.73 6	3.03	α=3.03 13, α(K)=2.18 12, α(L)=0.631 9, α(M)=0.1609 23, α(N)=0.0442 6, α(O)=0.01093 15, α(P)=0.001990 31, α(Q)=9.3×10^-5 5
	1-		230.242 7	M1		2.73	α=2.73 4, α(K)=2.150 30, α(L)=0.435 6, α(M)=0.1059 15, α(N)=0.0289 4, α(O)=0.00729 10, α(P)=0.001394 20, α(Q)=8.85×10^-5 12
	1-		274.331 6	M1		1.674	α=1.674 23, α(K)=1.320 18, α(L)=0.266 4, α(M)=0.0648 9, α(N)=0.01771 25, α(O)=0.00446 6, α(P)=0.000852 12, α(Q)=5.41×10^-5 8
289.028	4-		88.44 5	M1+E2	1.17 +17-12	21.4	α=21.4 14, α(L)=15.6 10, α(M)=4.29 30, α(N)=1.18 8, α(O)=0.285 20, α(P)=0.0469 29, α(Q)=0.00070 8
	4-		213.37 8	E2		0.720	α=0.720 10, α(K)=0.1356 19, α(L)=0.424 6, α(M)=0.1181 17, α(N)=0.0326 5, α(O)=0.00784 11, α(P)=0.001290 18, α(Q)=1.145×10^-5 16
	4-		240.443 32	M1+E2	1.33 13	1.17	α=1.17 10, α(K)=0.76 9, α(L)=0.304 7, α(M)=0.0796 16, α(N)=0.0219 4, α(O)=0.00537 11, α(P)=0.000949 25, α(Q)=3.36×10^-5 34
292.831	2-		217.043 28	M1+E2	1.01 14	1.93	α=1.93 19, α(K)=1.32 18, α(L)=0.453 11, α(M)=0.1174 20, α(N)=0.0323 5, α(O)=0.00794 15, α(P)=0.00142 4, α(Q)=5.7×10^-5 7
292.831	2-		240.115 14	M1+E2	1.03 +11-10	1.42	α=1.42 10, α(K)=0.99 9, α(L)=0.321 8, α(M)=0.0827 16, α(N)=0.0227 4, α(O)=0.00561 12, α(P)=0.001009 27, α(Q)=4.2×10^-5 4
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
296.401	2-		52.05 7	M1(+E2)	0.7 9	1.5×10²	α=1.5×10² 13, α(L)=1.1×10⁺² 10, α(M)=31 27, α(N)=8 8, α(O)=2.0 18, α(P)=0.33 27, α(Q)=0.0050 18
	2-		220.600 24	M1		3.08	α=3.08 4, α(K)=2.424 34, α(L)=0.490 7, α(M)=0.1195 17, α(N)=0.0327 5, α(O)=0.00822 12, α(P)=0.001572 22, α(Q)=9.99×10^-5 14
	2-		243.690 11	M1+E2	0.71 6	1.70	α=1.70 8, α(K)=1.26 7, α(L)=0.328 7, α(M)=0.0827 14, α(N)=0.0227 4, α(O)=0.00564 10, α(P)=0.001040 22, α(Q)=5.28×10^-5 27
	2-		296.412 25	M1+E2	0.89 +10-9	0.86	α=0.86 6, α(K)=0.63 5, α(L)=0.169 6, α(M)=0.0427 13, α(N)=0.01172 35, α(O)=0.00291 9, α(P)=0.000535 20, α(Q)=2.65×10^-5 21
311.832	1+,2+		41.997 34	E2		1081	α=1081 16, α(L)=784 11, α(M)=219.6 32, α(N)=60.7 9, α(O)=14.45 21, α(P)=2.264 33, α(Q)=0.00479 7
	1+,2+		81.312 15	M1+E2	0.78 9	24.2	α=24.2 19, α(L)=17.8 14, α(M)=4.8 4, α(N)=1.32 11, α(O)=0.320 26, α(P)=0.054 4, α(Q)=0.00121 8
	1+,2+		212.536 14	(M1+E2)	2.54 +11-10	1.090	α=1.090 30, α(K)=0.479 25, α(L)=0.446 6, α(M)=0.1218 17, α(N)=0.0336 5, α(O)=0.00813 11, α(P)=0.001370 20, α(Q)=2.49×10^-5 10
327.884	3-		178.11 7	M1+E2	2.7 +4-3	1.94	α=1.94 12, α(K)=0.68 12, α(L)=0.916 13, α(M)=0.252 4, α(N)=0.0697 10, α(O)=0.01680 24, α(P)=0.00279 4, α(Q)=3.9×10^-5 5
327.884	3-		252.049 15	M1+E2	3.73 10	0.513	α=0.513 9, α(K)=0.210 6, α(L)=0.2212 31, α(M)=0.0605 9, α(N)=0.01671 23, α(O)=0.00404 6, α(P)=0.000681 10, α(Q)=1.147×10^-5 27
330.740	3-		41.71 5	M1+E2	0.199 +10-11	120	α=120 4, α(L)=89.1 32, α(M)=22.9 9, α(N)=6.29 25, α(O)=1.55 6, α(P)=0.277 9, α(Q)=0.01223 18
330.837	2-,3-		34.441 13	M1+E2	0.042 29	147	α=147 9, α(L)=110 7, α(M)=27.0 18, α(N)=7.4 5, α(O)=1.86 12, α(P)=0.353 19, α(Q)=0.02203 31
	2-,3-		38.005 5	M1+E2	0.116 +20-24	128	α=128 8, α(L)=96 6, α(M)=24.0 17, α(N)=6.6 5, α(O)=1.64 11, α(P)=0.302 17, α(Q)=0.01635 23
	2-,3-		56.577 38	E2		256	α=256 4, α(L)=185.3 27, α(M)=52.0 7, α(N)=14.38 21, α(O)=3.43 5, α(P)=0.540 8, α(Q)=0.001324 19
341.593	0+		111.100 18	(M1)		4.62	α=4.62 6, α(L)=3.47 5, α(M)=0.847 12, α(N)=0.2315 32, α(O)=0.0583 8, α(P)=0.01115 16, α(Q)=0.000711 10
342.805	2-,3-		46.42 5	M1+E2	0.0606 +34-31
342.805	2-,3-		193.128 31	E2		1.047	α=1.047 15, α(K)=0.1548 22, α(L)=0.648 9, α(M)=0.1809 25, α(N)=0.0500 7, α(O)=0.01199 17, α(P)=0.001964 28, α(Q)=1.512×10^-5 21
355.715	2+		27.82 6	E1+M2	0.0049 +9-8	4.58	α=4.58 31, α(L)=3.36 22, α(M)=0.90 7, α(N)=0.244 19, α(O)=0.057 5, α(P)=0.0080 8, α(Q)=0.00024 4
	2+		62.876 15	(E1+M2)	0.076 +6-7	4.7	α=4.7 7, α(L)=3.4 5, α(M)=0.96 15, α(N)=0.27 4, α(O)=0.067 11, α(P)=0.0120 19, α(Q)=0.00062 10
	2+		111.27 5	E1+M2	0.045 4	0.228	α=0.228 23, α(L)=0.168 17, α(M)=0.044 5, α(N)=0.0122 13, α(O)=0.00302 33, α(P)=0.00053 6, α(Q)=2.61×10^-5 33
363.434	2+,3+		51.619 35	M1+E2	0.455 +31-32	104	α=104 7, α(L)=76 5, α(M)=20.4 15, α(N)=5.6 4, α(O)=1.37 10, α(P)=0.230 15, α(Q)=0.00587 12
364.658	2+		23.12 7	E2		1.25×10⁴	α=1.25×10⁴ 3
	2+		94.804 5	M1+E2	1.25 +17-14	16.3	α=16.3 9, α(L)=11.9 6, α(M)=3.26 19, α(N)=0.90 5, α(O)=0.217 12, α(P)=0.0357 18, α(Q)=0.00054 6
	2+		134.20 7	M1(+E2)	0.13 14	12.4	α=12.4 4, α(K)=9.7 5, α(L)=2.03 7, α(M)=0.498 22, α(N)=0.136 6, α(O)=0.0343 14, α(P)=0.00653 19, α(Q)=0.000406 20
369.207	1-,2-		72.806 30	(E2)		76.5	α=76.5 11, α(L)=55.4 8, α(M)=15.59 22, α(N)=4.31 6, α(O)=1.028 15, α(P)=0.1628 23, α(Q)=0.000461 6
369.207	1-,2-		94.874 22	M1+E2	1.4 +4-3	17.0	α=17.0 17, α(L)=12.4 12, α(M)=3.4 4, α(N)=0.94 10, α(O)=0.227 24, α(P)=0.0372 34, α(Q)=0.00049 11
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
372.490	4-		41.71 5	M1+E2	0.199 +10-11	120	α=120 4, α(L)=89.1 32, α(M)=22.9 9, α(N)=6.29 25, α(O)=1.55 6, α(P)=0.277 9, α(Q)=0.01223 18
	4-		76.092 14	(E2)		62.1	α=62.1 9, α(L)=45.0 6, α(M)=12.64 18, α(N)=3.50 5, α(O)=0.834 12, α(P)=0.1322 19, α(Q)=0.000385 5
	4-		171.951 25	(M1)		6.20	α=6.20 9, α(K)=4.88 7, α(L)=0.992 14, α(M)=0.2420 34, α(N)=0.0661 9, α(O)=0.01665 23, α(P)=0.00319 4, α(Q)=0.0002026 28
	4-		319.75 6	M1+E2	1.14 +26-18	0.58	α=0.58 9, α(K)=0.42 8, α(L)=0.123 9, α(M)=0.0313 19, α(N)=0.0086 5, α(O)=0.00213 14, α(P)=0.000388 29, α(Q)=1.77×10^-5 30
373.686	4-		45.91 6	M1+E2	0.141 +9-10	73.3	α=73.3 20, α(L)=54.7 15, α(M)=13.7 4, α(N)=3.76 11, α(O)=0.937 26, α(P)=0.173 4, α(Q)=0.00931 14
373.686	4-		80.905 19	E2		46.4	α=46.4 7, α(L)=33.6 5, α(M)=9.46 13, α(N)=2.62 4, α(O)=0.624 9, α(P)=0.0991 14, α(Q)=0.000300 4
376.947	3+		84.124 20	(E1+M2)	0.113 6	2.80	α=2.80 28, α(L)=2.02 20, α(M)=0.57 6, α(N)=0.159 16, α(O)=0.040 4, α(P)=0.0071 7, α(Q)=0.00038 4
376.947	3+		132.565 4	E1+M2	0.0104 +24-32	0.277	α=0.277 6, α(K)=0.208 4, α(L)=0.0518 14, α(M)=0.0128 4, α(N)=0.00347 11, α(O)=0.000845 26, α(P)=0.000146 5, α(Q)=6.08×10^-6 26
388.112	3+		95.44 6	E1		0.1534	α=0.1534 22, α(L)=0.1152 16, α(M)=0.0284 4, α(N)=0.00768 11, α(O)=0.001852 26, α(P)=0.000308 4, α(Q)=1.138×10^-5 16
388.112	3+		143.789 28	E1+M2	0.185 +20-30	2.0	α=2.0 5, α(K)=1.20 30, α(L)=0.56 15, α(M)=0.15 4, α(N)=0.042 12, α(O)=0.0106 29, α(P)=0.0019 5, α(Q)=1.08×10^-4 30
397.147	2-,3-,4-		69.253 11	M1+E2	0.41 +9-10	30	α=30 4, α(L)=21.8 32, α(M)=5.7 9, α(N)=1.57 26, α(O)=0.38 6, α(P)=0.067 9, α(Q)=0.00249 13
400.521	1-		69.781 6	(E2)		93.6	α=93.6 13, α(L)=67.8 10, α(M)=19.07 27, α(N)=5.27 7, α(O)=1.258 18, α(P)=0.1990 28, α(Q)=0.000548 8
400.521	1-		324.84 6	M1+E2	1.17 +30-22	0.54	α=0.54 9, α(K)=0.39 8, α(L)=0.116 9, α(M)=0.0295 20, α(N)=0.0081 6, α(O)=0.00201 15, α(P)=0.000365 31, α(Q)=1.65×10^-5 32
405.933	4+		33.443 2	E1		2.375	α=2.375 33, α(L)=1.766 25, α(M)=0.455 6, α(N)=0.1218 17, α(O)=0.0280 4, α(P)=0.00390 5, α(Q)=9.81×10^-5 14
405.933	4+		50.27 4	(E2)		452	α=452 7, α(L)=328 5, α(M)=91.9 13, α(N)=25.4 4, α(O)=6.05 9, α(P)=0.951 14, α(Q)=0.002197 32
417.746	(4)+		147.870 22	M1+E2	1.26 +16-14	5.6	α=5.6 4, α(K)=3.0 4, α(L)=1.87 4, α(M)=0.503 14, α(N)=0.139 4, α(O)=0.0337 9, α(P)=0.00574 11, α(Q)=0.000141 16
418.084	4+		90.178 22	E1+M2	0.175 +25-29	4.7	α=4.7 13, α(L)=3.4 10, α(M)=0.95 27, α(N)=0.27 8, α(O)=0.067 19, α(P)=0.0120 35, α(Q)=6.5×10^-4 19
	4+		129.056 29	E1+M2	1.2 +9-4	46	α=46 17, α(K)=26 10, α(L)=14 5, α(M)=4.0 15, α(N)=1.1 4, α(O)=0.28 11, α(P)=0.051 19, α(Q)=0.0029 11
	4+		173.60 16	E1+M2	0.15 +5-9	0.7	α=0.7 5, α(K)=0.48 31, α(L)=0.19 14, α(M)=0.05 4, α(N)=0.014 10, α(O)=0.0035 26, α(P)=6.E-4 5, α(Q)=3.6E-5 27
419.085	2-		91.229 24	M1+E2	0.43 9	11.0	α=11.0 10, α(L)=8.2 7, α(M)=2.10 22, α(N)=0.58 6, α(O)=0.142 14, α(P)=0.0255 21, α(Q)=0.00109 6
419.085	2-		366.351 33	M1		0.753	α=0.753 11, α(K)=0.595 8, α(L)=0.1192 17, α(M)=0.0290 4, α(N)=0.00793 11, α(O)=0.001996 28, α(P)=0.000382 5, α(Q)=2.420×10^-5 34
420.651	2+,3+,4+		32.526 21	M1+E2	0.33 5	5.2×10²	α=5.2×10² 10, α(L)=3.8E2 7, α(M)=103 21, α(N)=28 6, α(O)=6.8 13, α(P)=1.14 21, α(Q)=0.0250 5
420.651	2+,3+,4+		57.236 28	M1+E2	2.4 +14-6	211	α=211 19, α(L)=153 13, α(M)=43 4, α(N)=11.8 11, α(O)=2.82 25, α(P)=0.45 4, α(Q)=0.00180 32
442.385	5+		36.453 3	M1(+E2)	0.5 7	5×10²	α=5×10² 8, α(L)=4×10⁺² 6, α(M)=1.1E+2 16, α(N)=3.E1 4, α(O)=7 11, α(P)=1.1 16, α(Q)=0.017 4
446.702	3-		90.985 4	E1		0.1738	α=0.1738 24, α(L)=0.1304 18, α(M)=0.0322 5, α(N)=0.00870 12, α(O)=0.002095 29, α(P)=0.000347 5, α(Q)=1.260×10^-5 18
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
457.090	5+		168.125 30	E1		0.1561	α=0.1561 22, α(K)=0.1200 17, α(L)=0.0271 4, α(M)=0.00665 9, α(N)=0.001801 25, α(O)=0.000440 6, α(P)=7.70×10^-5 11, α(Q)=3.37E-6 5
464.362	3-,4-		76.258 13	E1+M2	0.113 +23-29	4.2	α=4.2 18, α(L)=3.1 13, α(M)=0.9 4, α(N)=0.24 10, α(O)=0.061 25, α(P)=0.011 5, α(Q)=5.8×10^-4 25
	3-,4-		175.314 34	M1+E2	1.62 +33-24	2.73	α=2.73 30, α(K)=1.40 31, α(L)=0.972 14, α(M)=0.263 5, α(N)=0.0724 14, α(O)=0.01756 30, α(P)=0.00299 4, α(Q)=6.7×10^-5 12
	3-,4-		194.510 5	E1+M2	0.292 +11-12	1.53	α=1.53 11, α(K)=1.00 7, α(L)=0.390 28, α(M)=0.104 8, α(N)=0.0290 21, α(O)=0.0073 5, α(P)=0.00135 10, α(Q)=7.7×10^-5 6
	3-,4-		314.71 7	M1+E2	2.5 +9-5	0.32	α=0.32 6, α(K)=0.19 5, α(L)=0.102 6, α(M)=0.0271 13, α(N)=0.00746 35, α(O)=0.00182 9, α(P)=0.000316 20, α(Q)=8.8×10^-6 20
483.640	4-		65.557 3	E1+M2	0.028 +3-4	0.89	α=0.89 13, α(L)=0.65 9, α(M)=0.175 26, α(N)=0.049 7, α(O)=0.0119 19, α(P)=0.00203 33, α(Q)=9.2×10^-5 18
495.721	3+		89.799 24	M1+E2	1.5 +9-4	22.3	α=22.3 32, α(L)=16.2 23, α(M)=4.5 7, α(N)=1.24 19, α(O)=0.30 4, α(P)=0.048 6, α(Q)=5.4×10^-4 18
495.721	3+		122.031 7	E1+M2	0.017 +6-12	0.094	α=0.094 11, α(L)=0.070 8, α(M)=0.0175 22, α(N)=0.0047 6, α(O)=0.00116 16, α(P)=0.000199 29, α(Q)=8.5×10^-6 16
501.569	(3)-		45.91 6	M1+E2	0.141 +9-10	73.3	α=73.3 20, α(L)=54.7 15, α(M)=13.7 4, α(N)=3.76 11, α(O)=0.937 26, α(P)=0.173 4, α(Q)=0.00931 14
	(3)-		82.484 17	M1+E2	4.6 15	41.0	α=41.0 16, α(L)=29.7 12, α(M)=8.33 35, α(N)=2.30 10, α(O)=0.550 23, α(P)=0.0876 34, α(Q)=0.00034 7
	(3)-		212.536 14	(M1+E2)	2.54 +11-10	1.090	α=1.090 30, α(K)=0.479 25, α(L)=0.446 6, α(M)=0.1218 17, α(N)=0.0336 5, α(O)=0.00813 11, α(P)=0.001370 20, α(Q)=2.49×10^-5 10
502.04	1+,2+		271.54 4	M1+E2	0.54 19	1.40	α=1.40 17, α(K)=1.07 15, α(L)=0.248 15, α(M)=0.0615 29, α(N)=0.0168 8, α(O)=0.00421 21, α(P)=0.00079 5, α(Q)=4.4×10^-5 6
506.648	2+		87.592 29	E1+M2	0.096 +18-21	1.8	α=1.8 6, α(L)=1.3 5, α(M)=0.36 13, α(N)=0.10 4, α(O)=0.025 9, α(P)=0.0045 17, α(Q)=2.4×10^-4 9
	2+		106.100 25	E1+M2	0.167 +20-22	2.2	α=2.2 5, α(L)=1.6 4, α(M)=0.44 10, α(N)=0.122 29, α(O)=0.031 7, α(P)=0.0055 13, α(Q)=0.00030 7
	2+		236.789 30	M1+E2	0.48 +14-16	2.14	α=2.14 19, α(K)=1.64 18, α(L)=0.378 13, α(M)=0.0938 24, α(N)=0.0257 6, α(O)=0.00642 18, α(P)=0.00120 5, α(Q)=6.8×10^-5 7
506.964	(3)+		89.216 20	M1+E2	0.58 8	13.9	α=13.9 11, α(L)=10.2 8, α(M)=2.70 23, α(N)=0.74 6, α(O)=0.182 15, α(P)=0.0315 22, α(Q)=0.00106 6
506.964	(3)+		142.306 25	M1+E2	1.30 +15-13	6.2	α=6.2 4, α(K)=3.2 4, α(L)=2.19 5, α(M)=0.591 16, α(N)=0.163 5, α(O)=0.0396 10, α(P)=0.00671 14, α(Q)=0.000154 16
528.545	3+		163.93 5	M1+E2	1.2 +5-3	4.1	α=4.1 8, α(K)=2.4 8, α(L)=1.245 33, α(M)=0.332 15, α(N)=0.091 4, α(O)=0.0223 9, α(P)=0.00385 7, α(Q)=1.10×10^-4 32
528.545	3+		165.08 4	M1+E2	1.6 +5-3	3.4	α=3.4 5, α(K)=1.7 5, α(L)=1.234 24, α(M)=0.334 10, α(N)=0.0922 27, α(O)=0.0223 6, α(P)=0.00378 6, α(Q)=8.1×10^-5 20
533.815	2-		69.448 11	M1+E2	0.33 +9-10	26	α=26 4, α(L)=19.1 29, α(M)=4.9 8, α(N)=1.35 23, α(O)=0.33 5, α(P)=0.059 8, α(Q)=0.00257 12
533.815	2-		133.293 28	M1+E2	2.3 +11-5	6.0	α=6.0 6, α(K)=1.7 8, α(L)=3.12 11, α(M)=0.87 4, α(N)=0.239 10, α(O)=0.0575 23, α(P)=0.00943 30, α(Q)=1.07×10^-4 30
544.756	2-,3-		80.400 33	M1		11.80	α=11.80 17, α(L)=8.86 12, α(M)=2.163 30, α(N)=0.592 8, α(O)=0.1490 21, α(P)=0.0285 4, α(Q)=0.001821 26
	2-,3-		89.070 20	M1+E2	0.26 +8-11	10.1	α=10.1 9, α(L)=7.5 6, α(M)=1.89 18, α(N)=0.52 5, α(O)=0.129 12, α(P)=0.0238 18, α(Q)=0.00128 5
	2-,3-		201.98 7	M1+E2	1.9 +8-4	1.55	α=1.55 30, α(K)=0.79 29, α(L)=0.555 12, α(M)=0.1501 21, α(N)=0.0414 6, α(O)=0.01004 15, α(P)=0.00171 4, α(Q)=3.8×10^-5 11
559.790	2-		113.122 34	M1+E2	0.95 +17-15	6.9	α=6.9 5, α(L)=5.07 32, α(M)=1.36 10, α(N)=0.375 28, α(O)=0.091 6, α(P)=0.0155 9, α(Q)=0.00039 5
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
568.215	4-		125.832 4	E1		0.0752	α=0.0752 11
	4-		150.10 5	E1+M2	0.427 15	7.2	α=7.2 4, α(K)=4.34 26, α(L)=2.06 12, α(M)=0.560 34, α(N)=0.157 9, α(O)=0.0393 24, α(P)=0.0072 4, α(Q)=0.000409 25
	4-		191.234 33	E1		0.1161	α=0.1161 16, α(K)=0.0898 13, α(L)=0.01973 28, α(M)=0.00482 7, α(N)=0.001308 18, α(O)=0.000321 4, α(P)=5.65×10^-5 8, α(Q)=2.56E-6 4
574.089	(2,3,4)-		176.97 5	M1+E2	0.46 +19-23	5.0	α=5.0 5, α(K)=3.7 5, α(L)=0.920 13, α(M)=0.230 6, α(N)=0.0631 18, α(O)=0.01572 35, α(P)=0.00292 4, α(Q)=0.000157 21
596.425	2-,3-,4-		94.874 22	M1+E2	1.4 +4-3	17.0	α=17.0 17, α(L)=12.4 12, α(M)=3.4 4, α(N)=0.94 10, α(O)=0.227 24, α(P)=0.0372 34, α(Q)=0.00049 11
	2-,3-,4-		149.713 11	M1+E2	0.20 5	8.94	α=8.94 18, α(K)=6.95 17, α(L)=1.492 23, α(M)=0.367 6, α(N)=0.1003 18, α(O)=0.0252 4, α(P)=0.00478 7, α(Q)=0.000291 7
	2-,3-,4-		199.291 20	M1		4.09	α=4.09 6, α(K)=3.22 5, α(L)=0.653 9, α(M)=0.1592 22, α(N)=0.0435 6, α(O)=0.01095 15, α(P)=0.002095 29, α(Q)=0.0001331 19
603.889	(3,4)+		185.786 25	M1+E2	5.6 +24-11	1.33	α=1.33 6, α(K)=0.28 6, α(L)=0.766 11, α(M)=0.2133 30, α(N)=0.0589 8, α(O)=0.01415 20, α(P)=0.002325 33, α(Q)=2.14×10^-5 24
	(3,4)+		186.127 34	M1+E2	2.44 27	1.75	α=1.75 12, α(K)=0.70 12, α(L)=0.764 11, α(M)=0.2095 30, α(N)=0.0578 8, α(O)=0.01396 20, α(P)=0.002334 34, α(Q)=3.8×10^-5 5
	(3,4)+		334.061 32	M1+E2	0.70 +16-1	0.70	α=0.70 8, α(K)=0.54 7, α(L)=0.127 8, α(M)=0.0315 18, α(N)=0.0086 5, α(O)=0.00215 13, α(P)=0.000403 27, α(Q)=2.22×10^-5 27
612.758	2-		53.00 5	M1+E2	0.06 +3-2	41.0	α=41.0 15, α(L)=30.8 11, α(M)=7.55 30, α(N)=2.07 8, α(O)=0.519 20, α(P)=0.0988 32, α(Q)=0.00616 9
	2-		78.945 19	E2		52.1	α=52.1 7, α(L)=37.8 5, α(M)=10.62 15, α(N)=2.94 4, α(O)=0.701 10, α(P)=0.1112 16, α(Q)=0.000332 5
	2-		106.100 25	E1+M2	0.167 +20-22	2.2	α=2.2 5, α(L)=1.6 4, α(M)=0.44 10, α(N)=0.122 29, α(O)=0.031 7, α(P)=0.0055 13, α(Q)=0.00030 7
	2-		193.677 23	E2		1.036	α=1.036 15, α(K)=0.1542 22, α(L)=0.640 9, α(M)=0.1787 25, α(N)=0.0494 7, α(O)=0.01185 17, α(P)=0.001941 27, α(Q)=1.500×10^-5 21
	2-		316.377 25	M1+E2	4.77 11	0.230	α=0.230 4, α(K)=0.1060 22, α(L)=0.0909 13, α(M)=0.02469 35, α(N)=0.00681 10, α(O)=0.001650 23, α(P)=0.000281 4, α(Q)=5.55×10^-6 10
	2-		319.91 6	M1+E2		0.6	α=0.6 5, α(K)=0.5 4, α(L)=0.13 5, α(M)=0.033 10, α(N)=0.0089 26, α(O)=0.0022 7, α(P)=4.1×10^-4 15, α(Q)=2.0E-5 16
	2-		368.24 6	M1+E2		0.43	α=0.43 31, α(K)=0.32 27, α(L)=0.084 34, α(M)=0.021 8, α(N)=0.0058 21, α(O)=0.0014 5, α(P)=2.6×10^-4 11, α(Q)=1.3E-5 10
	2-		382.234 30	E1+M2	0.05 4	0.030	α=0.030 10, α(K)=0.024 7, α(L)=0.0049 22, α(M)=0.0012 6, α(N)=3.3×10^-4 16, α(O)=8.E-5 4, α(P)=1.5E-5 8, α(Q)=8.E-7 4
621.527	1-,2-		87.726 31	M1+E2	0.34 +8-9	11.5	α=11.5 11, α(L)=8.5 8, α(M)=2.17 22, α(N)=0.60 6, α(O)=0.148 15, α(P)=0.0269 22, α(Q)=0.00129 6
621.527	1-,2-		165.79 6	M1+E2	0.67 +29-27	5.3	α=5.3 9, α(K)=3.8 9, α(L)=1.149 31, α(M)=0.294 15, α(N)=0.081 4, α(O)=0.0200 9, α(P)=0.00361 7, α(Q)=0.000163 35
628.523	3-,4-,5-		144.890 29	M1+E2	0.32 4	9.45	α=9.45 20, α(K)=7.20 20, α(L)=1.680 28, α(M)=0.417 8, α(N)=0.1143 22, α(O)=0.0286 5, α(P)=0.00535 8, α(Q)=0.000303 8
	3-,4-,5-		254.840 16	M1+E2	0.70 +10-9	1.50	α=1.50 10, α(K)=1.12 9, α(L)=0.286 9, α(M)=0.0720 17, α(N)=0.0197 5, α(O)=0.00491 13, α(P)=0.000908 29, α(Q)=4.7×10^-5 4
	3-,4-,5-		256.007 33	M1+E2	1.42 +31-22	0.92	α=0.92 13, α(K)=0.60 12, α(L)=0.241 11, α(M)=0.0631 21, α(N)=0.0173 6, α(O)=0.00425 15, α(P)=0.00075 4, α(Q)=2.6×10^-5 5
630.291	2-,3-,4-		96.433 27	E2		20.36	α=20.36 29, α(L)=14.75 21, α(M)=4.15 6, α(N)=1.147 16, α(O)=0.274 4, α(P)=0.0437 6, α(Q)=0.0001515 21
630.291	2-,3-,4-		183.48 5	M1+E2		3.2	α=3.2 19, α(K)=2.1 20, α(L)=0.816 14, α(M)=0.214 13, α(N)=0.059 4, α(O)=0.0144 6, α(P)=0.00255 11, α(Q)=9.E-5 8
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
672.248	(2,3,4)-		75.823 4	M1		13.99	α=13.99 20, α(L)=10.51 15, α(M)=2.57 4, α(N)=0.702 10, α(O)=0.1768 25, α(P)=0.0338 5, α(Q)=0.002162 30
	(2,3,4)-		98.161 5	M1		6.61	α=6.61 9, α(L)=4.96 7, α(M)=1.211 17, α(N)=0.331 5, α(O)=0.0834 12, α(P)=0.01596 22, α(Q)=0.001019 14
	(2,3,4)-		275.087 16	M1		1.661	α=1.661 23, α(K)=1.310 18, α(L)=0.264 4, α(M)=0.0643 9, α(N)=0.01757 25, α(O)=0.00442 6, α(P)=0.000846 12, α(Q)=5.37×10^-5 8
675.482	(2,3,4)+		71.593 7	M1+E2	0.141 +10-11	17.84	α=17.84 31, α(L)=13.36 23, α(M)=3.30 6, α(N)=0.905 17, α(O)=0.227 4, α(P)=0.0426 7, α(Q)=0.00252 4
	(2,3,4)+		168.519 8	M1+E2		4.2	α=4.2 24, α(K)=2.7 25, α(L)=1.11 6, α(M)=0.29 4, α(N)=0.080 10, α(O)=0.0197 21, α(P)=0.00345 9, α(Q)=1.2×10^-4 10
	(2,3,4)+		254.840 16	M1+E2	0.70 +10-9	1.50	α=1.50 10, α(K)=1.12 9, α(L)=0.286 9, α(M)=0.0720 17, α(N)=0.0197 5, α(O)=0.00491 13, α(P)=0.000908 29, α(Q)=4.7×10^-5 4
	(2,3,4)+		278.319 16	(E1)		0.0499	α=0.0499 7, α(K)=0.0393 5, α(L)=0.00804 11, α(M)=0.001956 27, α(N)=0.000531 7, α(O)=0.0001310 18, α(P)=2.362×10^-5 33, α(Q)=1.170E-6 16
681.894	3-		113.699 11	M1		4.32	α=4.32 6, α(L)=3.25 5, α(M)=0.792 11, α(N)=0.2166 30, α(O)=0.0545 8, α(P)=0.01043 15, α(Q)=0.000665 9
681.894	3-		137.159 27	M1+E2	5.27 14	4.47	α=4.47 6, α(K)=0.491 18, α(L)=2.89 4, α(M)=0.809 11, α(N)=0.2237 31, α(O)=0.0536 8, α(P)=0.00867 12, α(Q)=5.52×10^-5 10
704.030	1-,2-,3-		82.484 17	M1+E2	4.6 15	41.0	α=41.0 16, α(L)=29.7 12, α(M)=8.33 35, α(N)=2.30 10, α(O)=0.550 23, α(P)=0.0876 34, α(Q)=0.00034 7
	1-,2-,3-		202.421 39	E2		0.876	α=0.876 12, α(K)=0.1458 20, α(L)=0.530 7, α(M)=0.1478 21, α(N)=0.0409 6, α(O)=0.00981 14, α(P)=0.001610 23, α(Q)=1.324×10^-5 19
	1-,2-,3-		376.155 32	M1+E2	3.9 +10-6	0.152	α=0.152 13, α(K)=0.084 11, α(L)=0.0498 16, α(M)=0.0133 4, α(N)=0.00367 10, α(O)=0.000894 26, α(P)=0.000155 5, α(Q)=4.0×10^-6 4
710.389	1-,2-,3-		81.864 32	M1		11.19	α=11.19 16, α(L)=8.41 12, α(M)=2.053 29, α(N)=0.561 8, α(O)=0.1414 20, α(P)=0.0270 4, α(Q)=0.001728 24
	1-,2-,3-		88.869 19	M1+E2	0.30 +10-12	10.6	α=10.6 12, α(L)=7.9 8, α(M)=1.99 25, α(N)=0.54 7, α(O)=0.135 16, α(P)=0.0248 24, α(Q)=0.00127 7
	1-,2-,3-		136.299 23	M1(+E2)	0.14 16	11.8	α=11.8 5, α(K)=9.2 6, α(L)=1.95 7, α(M)=0.477 25, α(N)=0.131 7, α(O)=0.0328 16, α(P)=0.00625 20, α(Q)=0.000388 23
712.442	2-,3-,4-		83.926 12	M1+E2	1.3 +4-3	28	α=28 4, α(L)=20.7 26, α(M)=5.7 8, α(N)=1.58 22, α(O)=0.38 5, α(P)=0.062 8, α(Q)=0.00076 17
	2-,3-,4-		138.352 12	M1+E2	1.5 +5-3	6.3	α=6.3 8, α(K)=2.9 10, α(L)=2.51 11, α(M)=0.69 4, α(N)=0.189 11, α(O)=0.0457 24, α(P)=0.00766 29, α(Q)=0.00015 4
	2-,3-,4-		293.34 6	E2		0.2413	α=0.2413 34, α(K)=0.0815 11, α(L)=0.1165 16, α(M)=0.0321 4, α(N)=0.00885 12, α(O)=0.002134 30, α(P)=0.000358 5, α(Q)=5.04×10^-6 7
731.225	3+,4+,5+		102.698 5	E1+M2	0.122 +13-15	1.40	α=1.40 29, α(L)=1.02 21, α(M)=0.28 6, α(N)=0.079 17, α(O)=0.020 4, α(P)=0.0036 8, α(Q)=0.00019 4
731.225	3+,4+,5+		313.20 7	M1+E2	2.2 +8-4	0.36	α=0.36 7, α(K)=0.22 6, α(L)=0.106 7, α(M)=0.0282 15, α(N)=0.0078 4, α(O)=0.00190 11, α(P)=0.000332 23, α(Q)=1.00×10^-5 24
873.996	2-		192.108 6	M1+E2	4.1 +13-7	1.26	α=1.26 8, α(K)=0.35 8, α(L)=0.666 9, α(M)=0.1846 26, α(N)=0.0510 7, α(O)=0.01226 17, α(P)=0.002027 29, α(Q)=2.28×10^-5 31
	2-		243.690 11	M1+E2	0.71 6	1.70	α=1.70 8, α(K)=1.26 7, α(L)=0.328 7, α(M)=0.0827 14, α(N)=0.0227 4, α(O)=0.00564 10, α(P)=0.001040 22, α(Q)=5.28×10^-5 27
	2-		314.33 7	E2		0.1946	α=0.1946 27, α(K)=0.0723 10, α(L)=0.0892 13, α(M)=0.02447 34, α(N)=0.00675 9, α(O)=0.001631 23, α(P)=0.000275 4, α(Q)=4.26×10^-6 6
	2-		599.55 12	M1+E2	2.84 34	0.055	α=0.055 5, α(K)=0.038 4, α(L)=0.0122 6, α(M)=0.00315 14, α(N)=0.00086 4, α(O)=0.000213 10, α(P)=3.86×10^-5 20, α(Q)=1.62E-6 15
902.494	(3)-		192.108 6	M1+E2	4.1 +13-7	1.26	α=1.26 8, α(K)=0.35 8, α(L)=0.666 9, α(M)=0.1846 26, α(N)=0.0510 7, α(O)=0.01226 17, α(P)=0.002027 29, α(Q)=2.28×10^-5 31
	(3)-		230.242 7	M1		2.73	α=2.73 4, α(K)=2.150 30, α(L)=0.435 6, α(M)=0.1059 15, α(N)=0.0289 4, α(O)=0.00729 10, α(P)=0.001394 20, α(Q)=8.85×10^-5 12
	(3)-		328.409 19	M1		1.017	α=1.017 14, α(K)=0.803 11, α(L)=0.1613 23, α(M)=0.0393 5, α(N)=0.01073 15, α(O)=0.00270 4, α(P)=0.000517 7, α(Q)=3.28×10^-5 5
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
906.499	(3)-		32.526 21	M1+E2	0.33 5	5.2×10²	α=5.2×10² 10, α(L)=3.8E2 7, α(M)=103 21, α(N)=28 6, α(O)=6.8 13, α(P)=1.14 21, α(Q)=0.0250 5
	(3)-		202.421 39	E2		0.876	α=0.876 12, α(K)=0.1458 20, α(L)=0.530 7, α(M)=0.1478 21, α(N)=0.0409 6, α(O)=0.00981 14, α(P)=0.001610 23, α(Q)=1.324×10^-5 19
	(3)-		450.69 6	M1+E2	0.86 +35-27	0.28	α=0.28 6, α(K)=0.21 5, α(L)=0.049 7, α(M)=0.0122 17, α(N)=0.0033 5, α(O)=0.00084 12, α(P)=0.000157 24, α(Q)=8.7×10^-6 20
949.660	(4-)		75.664 7	(E2)		63.7	α=63.7 9, α(L)=46.2 6, α(M)=12.98 18, α(N)=3.59 5, α(O)=0.857 12, α(P)=0.1358 19, α(Q)=0.000394 6
1002.618	(5-)		53.00 5	M1+E2	0.06 +3-2	41.0	α=41.0 15, α(L)=30.8 11, α(M)=7.55 30, α(N)=2.07 8, α(O)=0.519 20, α(P)=0.0988 32, α(Q)=0.00616 9
1002.618	(5-)		96.115 16	(E2)		20.67	α=20.67 29, α(L)=14.97 21, α(M)=4.21 6, α(N)=1.165 16, α(O)=0.278 4, α(P)=0.0444 6, α(Q)=0.0001534 21
1161.97	1-,2-,3-,4-		255.467 38	E2		0.380	α=0.380 5, α(K)=0.1028 14, α(L)=0.2016 28, α(M)=0.0558 8, α(N)=0.01542 22, α(O)=0.00371 5, α(P)=0.000618 9, α(Q)=7.11×10^-6 10
	1-,2-,3-,4-		451.60 13	E2		0.07133	α=0.07133 99, α(K)=0.0382 5, α(L)=0.02427 34, α(M)=0.00651 9, α(N)=0.001792 25, α(O)=0.000436 6, α(P)=7.57×10^-5 11, α(Q)=1.875E-6 26
	1-,2-,3-,4-		617.207 40	M1		0.1829	α=0.1829 26, α(K)=0.1448 20, α(L)=0.0287 4, α(M)=0.00697 10, α(N)=0.001905 27, α(O)=0.000479 7, α(P)=9.17×10^-5 13, α(Q)=5.82E-6 8

For references on theory, refer to the NSR file at the Web site given in the abstract.

For neutron resonances see 2014Fr03, 2015No03 and references therein.

Levels: band(b) Kπ=5- (π 5/2[523]+ν 5/2[622]). α=1

Levels: band(c) Kπ=6- (π 5/2[523]+ν 7/2[624]). α=1

Levels: band(d) Kπ=(5⁺) (π 5/2[642]+ν 5/2[622]). α=1 (?)

Levels: band(e) Unspecified sequence

Q-value: S(2n)=12185 14, S(2p)=11426 17 (2021Wa16)

Q(β-)=664.3 keV 4	S(n)= 5537.64 keV 10	S(p)= 4776.07 keV 19	Q(α)= 5588.50 keV 25
Reference: 2021WA16

References:
A	²⁴¹Am(d,p)	B	²⁴³Am(d,t)
C	Coulomb Excitation	D	²⁴¹Am(n,γ) E=TH:PRIMARY γ’S
E	²⁴¹Am(n,γ) E=TH:SECONDARY γ’S	F	²⁴¹Am(n,γ):Resonances 0-320 EV
G	²⁴¹Am(n,γ):Resonances 0-149 EV	H	²⁴²Am IT decay (141 Y)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - Kπ=0- (π 5/2[523]-ν 5/2[622])
0.0	1-	16.01 h 2 % β^- = 83.0 3 % ε = 17.0 3 % α < 10×10^-5
44.093 3	0-		44.092 3	100	M1	0.0	1-
52.714 7	3-		52.770 36	100	E2	0.0	1-
75.820 3	2-		75.823 4	100	M1	0.0	1-
148	5-
149.707 7	4-		73.864 11 96.994 2	0.96 Calc. 100 4	E2 M1	75.820 52.714	2- 3-
263	(6- AND 7-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - Kπ=5- (π 5/2[523]+ν 5/2[622]). α=0
114	6-
276	8-		162.3 5	100		114	6-
479	10-		133 202.9 5			347 276	9- 8-
722	12-		126 242.5 5			596.2 479	11- 10-
1002	14-		144 188 280.5 5			858.0 814 722	13- 13- 12-
1316	16-		314.2 5	100		1002	14-
1652	18-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - Kπ=6- (π 5/2[523]+ν 7/2[624]). α=0
100.1 7	6-
254.3	8-		82 154.2 5			172 100.1	7- 6-
448.9	10-		194.6 5	100		254.3	8-
682.7	12-		233.8 5	100		448.9	10-
954.1	14-		140 271.4 5			814 682.7	13- 12-
1260.9	16-		306.8 5	100		954.1	14-
1599.0	18-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - Kπ=(5⁺) (π 5/2[642]+ν 5/2[622]). α=0 (?)
247+X	(8+)
409+X	(10+)		162.1 5	100		247+X	(8+)
611+X	(12+)		202.2 5	100		409+X	(10+)
852+X	(14+)		241.1 5	100		611+X	(12+)
1132+X	(16+)		280			852+X	(14+)
1453+X	(18+)		321	100		1132+X	(16+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - Unspecified sequence
692+X
1151+X			424 540			727.4+X 611+X	(13+) (12+)
1434+X			445 581?			988.6+X 852+X	(15+) (14+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - Kπ=0⁺ (π 5/2[642]-ν 5/2[622])
230.527 3	1+
269.854 10	3+		39.42 6	100	(E2)	230.527	1+
341.593 14	0+		111.100 18 341.528 22	70 10 100 12	(M1)	230.527 0.0	1+ 1-
364.658 11	2+		23.12 7 94.804 5 134.20 7	0.2 100 11 63 19	E2 M1+E2 M1(+E2)	341.593 269.854 230.527	0+ 3+ 1+
417.746 15	(4)+		147.870 22	100	M1+E2	269.854	3+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - Kπ=3- (π 5/2[523]+ν 1/2[631])
244.381 8	3-
289.028 13	4-		88.44 5 213.37 8 240.443 32	≈2.9 100 36 54 7	M1+E2 E2 M1+E2	200.581 75.820 48.603	3-,4- 2- 5-
342	5-
409	(6-)
486	(7-)
581	(8-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 8 - Kπ=1- (π 5/2[523]-ν 7/2[624])
274.330 5	1-
296.401 8	2-		52.05 7 220.600 24 243.690 11 296.412 25	0.5 Calc. 65 4 ≤70 100 8	M1(+E2) M1 M1+E2 M1+E2	244.381 75.820 52.714 0.0	3- 2- 3- 1-
330.740 8	3-		37.910 5 41.71 5 56.421 18 86.316 30 278.000 18	52 12 ≤12.8 <72 100 7	M1+E2	292.831 289.028 274.330 244.381 52.714	2- 4- 1- 3- 3-
372.490 9	4-		41.71 5 76.092 14 171.951 25 222.75 9 296.732 34 319.75 6	<19.2 54 16 51 8 43 16 100 12 75 16	M1+E2 (E2) (M1) M1+E2	330.740 296.401 200.581 149.707 75.820 52.714	3- 2- 3-,4- 4- 2- 3-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 9 - Kπ=2- (π 5/2[523]-ν 1/2[631])
292.831 8	2-
327.884 9	3-		35.049 11 178.11 7 252.049 15	56 10 100 18	M1+E2 M1+E2	292.831 149.707 75.820	2- 4- 2-
373.686 9	4-		45.91 6 80.905 19	≤23 100 30	M1+E2 E2	327.884 292.831	3- 2-
434	(5-)
500	(6-)
581	(7-)
677	(8-)
796	(9-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 10 - Kπ=3⁺ (π 5/2[642]+ν 1/2[631])
388.112 9	3+
418.084 11	4+		29.94 6 90.178 22 129.056 29 173.60 16	100 28 71 24 41 27	E1+M2 E1+M2 E1+M2	388.112 327.884 289.028 244.381	3+ 3- 4- 3-
457.090 11	5+		38.996 9 68.997 17 83.399 17 168.125 30	≈5.7 48 14 100 20 31 8	E1	418.084 388.112 373.686 289.028	4+ 3+ 4- 4-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 11 - Kπ=2⁺ (π 5/2[642]-ν 1/2[631])
355.715 10	2+
376.947 8	3+		46.128 33 49.03 5 84.124 20 132.565 4	36.3 11 100.0 10	(E1+M2) E1+M2	330.837 327.884 292.831 244.381	2-,3- 3- 2- 3-
405.933 9	4+		33.443 2 50.27 4	100 18 0.07 Calc.	E1 (E2)	372.490 355.715	4- 2+
442.385 8	5+		36.453 3 65.408 28 68.701 3	49 10 14 5 100 7	M1(+E2)	405.933 376.947 373.686	4+ 3+ 4-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 12 - Kπ=1- (π 3/2[521]-ν 5/2[622])+(π 3/2[521]-ν 1/2[631])+
400.521 9	1-
419.085 9	2-		30.973 1 46.598 16 88.322 31 91.229 24 366.351 33	≤290 0.56 Calc. 45 20 57 18 100 19	M1+E2 M1	388.112 372.490 330.740 327.884 52.714	3+ 4- 3- 3- 3-
446.702 10	3-		28.937 25 46.128 33 74.248 23 90.985 4 296.996 25	3.5 Calc. 77 7 100 14	E1	417.746 400.521 372.490 355.715 149.707	(4)+ 1- 4- 2+ 4-
483.640 11	4-		64.54 3 65.557 3 435.038 22	32 4 100 5	E1+M2	419.085 418.084 48.603	2- 4+ 5-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 13 - Kπ=2- (π 5/2[523]-ν 1/2[620])
873.996 12	2-
906.499 19	(3)-		32.526 21 202.421 39 450.69 6	≤1.0 ≤85 100 21	M1+E2 E2 M1+E2	873.996 704.030 455.688	2- 1-,2-,3- 1-,2-,3-
949.660 14	(4-)		43.17 5 75.664 7	≤15 100 18	(E2)	906.499 873.996	(3)- 2-
1002.618 23	(5-)		53.00 5 96.115 16	≤75 100 20	M1+E2 (E2)	949.660 906.499	(4-) (3)-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 14 - Kπ=3- (π 5/2[523]+ν 1/2[620])
902.494 11	(3)-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 15 - Kπ=3⁺ (π 5/2[523]+ν 1/2[501])
974.9 5	(3+)
1011	(4+)
1066	(5+)
1151	(6+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 16 - Kπ=2⁺ (π 5/2[523]-ν 1/2[501])
1011	(2+)
1049	(3+)
1097	(4+)

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1-	16.01 h 2 % β^- = 83.0 3 % ε = 17.0 3 % α < 10×10^-5	Q=-2.44 3, μ=+0.3854 17 E(level): Kπ=0- (π 5/2[523]-ν 5/2[622]).
44.093	0-		E(level): Kπ=0- (π 5/2[523]-ν 5/2[622]).
48.603	5-	141 y 2 % IT = 99.550 10 % α = 0.450 10 % SF < 4.7×10^-9	Q=+6.7 4, μ=+1.00 5 T_1/2(SF)=9.5×10¹¹ y 35 (1967Ca04), >3.0×10¹² y (1986Ze06), 2000Ho27 adopt the limit value. E(level): T_1/2(SF)=9.5×10¹¹ y 35 (1967Ca04), >3.0×10¹² y (1986Ze06), 2000Ho27 adopt the limit value.
52.714	3-		E(level): Kπ=0- (π 5/2[523]-ν 5/2[622]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
75.820	2-		E(level): Kπ=0- (π 5/2[523]-ν 5/2[622]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
100.1	6-		E(level): Kπ=6- (π 5/2[523]+ν 7/2[624]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
114	6-		E(level): Kπ=5- (π 5/2[523]+ν 5/2[622]). α=0. From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
148	5-		XREF: α(149)B(148). E(level): Kπ=0- (π 5/2[523]-ν 5/2[622]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
149.707	4-		XREF: α(149)B(148). E(level): Kπ=0- (π 5/2[523]-ν 5/2[622]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
172	7-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
181.4	(5+)		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
181.4+X	(7+)		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
190.6	7-		E(level): From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
197.5			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
230.527	1+		E(level): Kπ=0⁺ (π 5/2[642]-ν 5/2[622]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
244.381	3-		E(level): Kπ=3- (π 5/2[523]+ν 1/2[631]).
247+X	(8+)		E(level): Kπ=(5⁺) (π 5/2[642]+ν 5/2[622]). α=0 (?). J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
254.3	8-		E(level): Kπ=6- (π 5/2[523]+ν 7/2[624]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
263	(6- AND 7-)		E(level): Kπ=0- (π 5/2[523]-ν 5/2[622]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
269.854	3+		E(level): Kπ=0⁺ (π 5/2[642]-ν 5/2[622]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
274.330	1-		E(level): Kπ=1- (π 5/2[523]-ν 7/2[624]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
276	8-		E(level): Kπ=5- (π 5/2[523]+ν 5/2[622]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
283.3			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
289.028	4-		E(level): Kπ=3- (π 5/2[523]+ν 1/2[631]).
292.831	2-		E(level): Kπ=2- (π 5/2[523]-ν 1/2[631]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
E(level)	J^π(level)	T_1/2(level)	Comments
296.401	2-		E(level): Kπ=1- (π 5/2[523]-ν 7/2[624]).
306.9			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
323.4+X	(9+)		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
327.884	3-		E(level): Kπ=2- (π 5/2[523]-ν 1/2[631]).
330.740	3-		E(level): Kπ=1- (π 5/2[523]-ν 7/2[624]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
341.593	0+		E(level): Kπ=0⁺ (π 5/2[642]-ν 5/2[622]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
342	5-		E(level): Kπ=3- (π 5/2[523]+ν 1/2[631]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
347	9-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
355.715	2+		E(level): Kπ=2⁺ (π 5/2[642]-ν 1/2[631]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
364.658	2+		E(level): Kπ=0⁺ (π 5/2[642]-ν 5/2[622]).
372.490	4-		E(level): Kπ=1- (π 5/2[523]-ν 7/2[624]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
373.3	9-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
373.686	4-		E(level): Kπ=2- (π 5/2[523]-ν 1/2[631]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
376.947	3+		E(level): Kπ=2⁺ (π 5/2[642]-ν 1/2[631]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
388.112	3+		E(level): Kπ=3⁺ (π 5/2[642]+ν 1/2[631]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
400.521	1-		E(level): Kπ=1- (π 3/2[521]-ν 5/2[622])+(π 3/2[521]-ν 1/2[631])+. J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
405.880	2-,3,4		J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
405.933	4+		E(level): Kπ=2⁺ (π 5/2[642]-ν 1/2[631]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
409	(6-)		E(level): Kπ=3- (π 5/2[523]+ν 1/2[631]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
409+X	(10+)		E(level): Kπ=(5⁺) (π 5/2[642]+ν 5/2[622]). α=0 (?). J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
417.746	(4)+		The intense 5119.7-keV primary gamma in ²⁴¹Am(thermal n,γ) reaction is assigned to feed this level, rather than the 418.12-keV level, since the 1⁺, 2⁺ and 3⁺ members of the (π 5/2[642]-ν 5/2[622]) band are populated by strong primary gammas; whereas, the 3⁺ level of the (π 5/2[642]+ν 1/2[631]) rotational band is not populated (the 418.12-keV level is the 4⁺ member). E(level): The intense 5119.7-keV primary gamma in ²⁴¹Am(thermal n,γ) reaction is assigned to feed this level, rather than the 418.12-keV level, since the 1⁺, 2⁺ and 3⁺ members of the (π 5/2[642]-ν 5/2[622]) band are populated by strong primary gammas; whereas, the 3⁺ level of the (π 5/2[642]+ν 1/2[631]) rotational band is not populated (the 418.12-keV level is the 4⁺ member). Kπ=0⁺ (π 5/2[642]-ν 5/2[622]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
418.084	4+		E(level): Kπ=3⁺ (π 5/2[642]+ν 1/2[631]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
419.085	2-		E(level): Kπ=1- (π 3/2[521]-ν 5/2[622])+(π 3/2[521]-ν 1/2[631])+. J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
428.6			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
434	(5-)		E(level): Kπ=2- (π 5/2[523]-ν 1/2[631]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
E(level)	J^π(level)	T_1/2(level)	Comments
442.385	5+		E(level): Kπ=2⁺ (π 5/2[642]-ν 1/2[631]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
446.702	3-		E(level): Kπ=1- (π 3/2[521]-ν 5/2[622])+(π 3/2[521]-ν 1/2[631])+. J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
448.9	10-		E(level): Kπ=6- (π 5/2[523]+ν 7/2[624]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
457.090	5+		E(level): Kπ=3⁺ (π 5/2[642]+ν 1/2[631]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
479	10-		E(level): Kπ=5- (π 5/2[523]+ν 5/2[622]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
483.640	4-		E(level): Kπ=1- (π 3/2[521]-ν 5/2[622])+(π 3/2[521]-ν 1/2[631])+. J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
486	(7-)		E(level): Kπ=3- (π 5/2[523]+ν 1/2[631]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
500	(6-)		E(level): Kπ=2- (π 5/2[523]-ν 1/2[631]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
505.4+X	(11+)		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
561	11-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
581	(7-)		E(level): Kπ=2- (π 5/2[523]-ν 1/2[631]). From Coulomb excitation. J^π(level): 1976KaZL propose that the 581-keV level may be a doublet, and tentatively assign the possible second component as the 8- member of the Kπ=3- band. From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
581	(8-)		E(level): Kπ=3- (π 5/2[523]+ν 1/2[631]). J^π(level): 1976KaZL propose that the 581-keV level may be a doublet, and tentatively assign the possible second component as the 8- member of the Kπ=3- band.
583.4			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
596.2	11-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
611+X	(12+)		E(level): Kπ=(5⁺) (π 5/2[642]+ν 5/2[622]). α=0 (?). J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
640.2			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
644.3			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
651.3			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
660.6			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
664.1			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
670.0			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
677	(8-)		E(level): Kπ=2- (π 5/2[523]-ν 1/2[631]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
682.7	12-		E(level): Kπ=6- (π 5/2[523]+ν 7/2[624]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
689.3			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
692+X			E(level): Unspecified sequence.
E(level)	J^π(level)	T_1/2(level)	Comments
700.2			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
715.3			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
721.3			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
722	12-		E(level): Kπ=5- (π 5/2[523]+ν 5/2[622]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
724.4			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
727.4+X	(13+)		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
734.8			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
744.7			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
759.4			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
766.9			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
779.6			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
795.7			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
796	(9-)		E(level): Kπ=2- (π 5/2[523]-ν 1/2[631]).
802.4			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
814	13-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
818.1			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
823.2			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
851.9			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
852+X	(14+)		E(level): Kπ=(5⁺) (π 5/2[642]+ν 5/2[622]). α=0 (?). J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
858.0	13-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
864.5			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
873.996	2-		E(level): Kπ=2- (π 5/2[523]-ν 1/2[620]). From Coulomb excitation. J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available. From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
883.8			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
896.6			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
902.494	(3)-		E(level): Kπ=3- (π 5/2[523]+ν 1/2[620]). From Coulomb excitation. J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available. From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
E(level)	J^π(level)	T_1/2(level)	Comments
904+X			J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
906.499	(3)-		E(level): Kπ=2- (π 5/2[523]-ν 1/2[620]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
919.5			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
930.4			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
934.6			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
949.660	(4-)		E(level): Kπ=2- (π 5/2[523]-ν 1/2[620]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
954.1	14-		E(level): Kπ=6- (π 5/2[523]+ν 7/2[624]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
968.7			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
974.9	(3+)		E(level): Kπ=3⁺ (π 5/2[523]+ν 1/2[501]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
978.3			J^π(level): Fed by primary transition in (n,γ) from the 2-, 3- capturing state. The probable spins thus lie in the range J=1 to J=4.
988.6+X	(15+)		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1002	14-		E(level): Kπ=5- (π 5/2[523]+ν 5/2[622]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1002.618	(5-)		E(level): Kπ=2- (π 5/2[523]-ν 1/2[620]). J^π(level): Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available. Fit to a band as proposed by 1988Sa18 in (n,γ) based on energy spacings, rotational parameters, and decay patterns. Additional explicit arguments are given where available.
1011	(2+)		XREF: α(1012). E(level): Kπ=2⁺ (π 5/2[523]-ν 1/2[501]). From Coulomb excitation. J^π(level): The peak at 1011 is assigned in (d,t) by 1976Gr19 as a doublet consisting of the 2⁺ member of the Kπ=2⁺ band and the 4⁺ member of the Kπ=3⁺ band. 1976KaZL assign just the 2⁺ member of the Kπ=2⁺ band to this peak. They assign the 4⁺ member of the Kπ=3⁺ band to the 1029 level. From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
1011	(4+)		XREF: α(1012). E(level): Kπ=3⁺ (π 5/2[523]+ν 1/2[501]). From Coulomb excitation. J^π(level): The peak at 1011 is assigned in (d,t) by 1976Gr19 as a doublet consisting of the 2⁺ member of the Kπ=2⁺ band and the 4⁺ member of the Kπ=3⁺ band. 1976KaZL assign just the 2⁺ member of the Kπ=2⁺ band to this peak. They assign the 4⁺ member of the Kπ=3⁺ band to the 1029 level. From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
1029			J^π(level): The peak at 1011 is assigned in (d,t) by 1976Gr19 as a doublet consisting of the 2⁺ member of the Kπ=2⁺ band and the 4⁺ member of the Kπ=3⁺ band. 1976KaZL assign just the 2⁺ member of the Kπ=2⁺ band to this peak. They assign the 4⁺ member of the Kπ=3⁺ band to the 1029 level.
1049	(3+)		E(level): Kπ=2⁺ (π 5/2[523]-ν 1/2[501]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
1066	(5+)		E(level): Kπ=3⁺ (π 5/2[523]+ν 1/2[501]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
1097	(4+)		E(level): Kπ=2⁺ (π 5/2[523]-ν 1/2[501]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
1103	15-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1132+X	(16+)		E(level): Kπ=(5⁺) (π 5/2[642]+ν 5/2[622]). α=0 (?). J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1151	(6+)		E(level): Kπ=3⁺ (π 5/2[523]+ν 1/2[501]). From Coulomb excitation. J^π(level): From (d,p) and/or (d,t) data based on a comparison of observed and theoretical cross section patterns and on rotational band parameters. Additional explicit arguments are given where available.
1151+X			E(level): Unspecified sequence.
1156.1	15-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1260.9	16-		E(level): Kπ=6- (π 5/2[523]+ν 7/2[624]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
E(level)	J^π(level)	T_1/2(level)	Comments
1287+X			J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1316	16-		XREF: B(?). E(level): Kπ=5- (π 5/2[523]+ν 5/2[622]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1426	17-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1434+X			E(level): Unspecified sequence.
1453+X	(18+)		E(level): Kπ=(5⁺) (π 5/2[642]+ν 5/2[622]). α=0 (?). J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1482.8	17-		J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1599.0	18-		E(level): Kπ=6- (π 5/2[523]+ν 7/2[624]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
1652	18-		E(level): Kπ=5- (π 5/2[523]+ν 5/2[622]). α=0. J^π(level): Assigned by 2010Ha24 in Coulomb Excitation to band structures based on observation of cascade transitions in gated spectra, energy spacing, and inertial parameters. For the band built on the ¹⁴¹Y isomer, the authors extend the band established in (d,p), (d,t).
2200	(2+,3-)	13.9 ms 2 % SF ≈ 100 % IT = ? % α < 0.005	μ=-1.14 8, Q=35.5 16 Alpha decay from this isomeric level has not been observed: (I(α)/SF) \|< 0.1 (no α observed; 1965Le22, 1983WeZT); (I(α)/SF) \|< 0.015 (No 8500α observed; 1973Be05); (I(α)/SF) \|< 0.00005 (1985AcZZ). Other measurement: 1963Fl08. E(level): Alpha decay from this isomeric level has not been observed: (I(α)/SF) \|< 0.1 (no α observed; 1965Le22, 1983WeZT); (I(α)/SF) \|< 0.015 (No 8500α observed; 1973Be05); (I(α)/SF) \|< 0.00005 (1985AcZZ). Other measurement: 1963Fl08.

E(level)	E(gamma)	Comments
48.603	48.63	M(γ): From subshell ratios in IT decay
75.820	75.823	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
181.4	132.8	E(γ): From Coulomb excitation
190.6	90	E(γ): From Coulomb excitation
190.6	142.0	E(γ): From Coulomb excitation
200.581	32.195	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<87 14. Multiply placed with undivided intensity
200.581	147.870	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<41 5. Multiply placed with undivided intensity
254.3	82	E(γ): From Coulomb excitation
254.3	154.2	E(γ): From Coulomb excitation
276	162.3	E(γ): From Coulomb excitation
296.401	243.690	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<66 4. Multiply placed with undivided intensity
311.832	212.536	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<206 11. Multiply placed with undivided intensity
323.4+X	142.0	E(γ): From Coulomb excitation
330.740	41.71	E(γ): Multiply placed with undivided intensity I(γ): Iγ<11.6 12. Multiply placed with undivided intensity
330.740	86.316	E(γ): Multiply placed with undivided intensity I(γ): Iγ<53 19. Multiply placed with undivided intensity
342.805	30.973	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<281 39. Multiply placed with undivided intensity
347	92	E(γ): From Coulomb excitation
369.207	94.874	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<7.2⁺10³ 18. Multiply placed with undivided intensity
372.490	41.71	E(γ): Multiply placed with undivided intensity I(γ): Iγ<17.4 18. Multiply placed with undivided intensity
373.3	97	E(γ): From Coulomb excitation
373.3	182.7	E(γ): From Coulomb excitation
373.686	45.91	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<≈23. Multiply placed with undivided intensity
376.947	46.128	E(γ): Multiply placed
405.880	28.937	E(γ): Multiply placed
	32.195	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<136 22. Multiply placed with undivided intensity
	77.988	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<26 11. Multiply placed with undivided intensity
E(level)	E(gamma)	Comments
409+X	162.1	E(γ): From Coulomb excitation
417.746	147.870	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
419.085	30.973	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<255 35. Multiply placed with undivided intensity
420.651	32.526	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<≈1.8. Multiply placed with undivided intensity
446.702	28.937	E(γ): Multiply placed
446.702	46.128	E(γ): Multiply placed
448.9	194.6	E(γ): From Coulomb excitation
455.688	159.283	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<170 8. Multiply placed with undivided intensity
457.090	38.996	I(γ): Calculated value
479	133	E(γ): From Coulomb excitation
479	202.9	E(γ): From Coulomb excitation
501.569	45.91	E(γ): Multiply placed with undivided intensity I(γ): Iγ≈5.2 for this doubly placed transition. Multiply placed with undivided intensity
	82.484	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<37 9. Multiply placed with undivided intensity
	212.536	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<95 5 for this doubly placed transition. Multiply placed with undivided intensity
505.4+X	182.0	E(γ): From Coulomb excitation
506.648	106.100	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<346 52. Multiply placed with undivided intensity
506.964	86.316	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<73 27. Multiply placed with undivided intensity
528.545	86.173	M(γ): Mult=(M1⁺E2) from ce data. Placement in the level scheme requires ΔJ=2, Δπ=no
544.756	43.17	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<≈14. Multiply placed with undivided intensity
544.756	144.254	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<71 9. Multiply placed with undivided intensity
559.790	159.283	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<217 11. Multiply placed with undivided intensity
561	112	E(γ): From Coulomb excitation
561	214.4	E(γ): From Coulomb excitation
596.2	147	E(γ): From Coulomb excitation
596.2	222.9	E(γ): From Coulomb excitation
E(level)	E(gamma)	Comments
596.425	94.874	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<83 21. Multiply placed with undivided intensity
603+X	356	E(γ): From Coulomb excitation
603+X	422	E(γ): From Coulomb excitation
612.758	53.00	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<45 9. Multiply placed with undivided intensity
	106.100	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<182 {28. Multiply placed with undivided intensity
	382.234	M(γ): 1988Sa18 report mult=E1 or E2. Placement in the level scheme requires Δπ=yes.
628.523	254.840	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<109 9. Multiply placed with undivided intensity
672.248	75.823	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
675.482	254.840	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<61 5. Multiply placed with undivided intensity
681.894	77.988	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<21 {9. Multiply placed with undivided intensity
682.7	233.8	E(γ): From Coulomb excitation
692+X	369	E(γ): From Coulomb excitation
692+X	445	E(γ): From Coulomb excitation
704.030	82.484	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<37 9. Multiply placed with undivided intensity
	144.254	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<44 6. Multiply placed with undivided intensity
	202.421	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<38 10. Multiply placed with undivided intensity
722	126	E(γ): From Coulomb excitation
722	242.5	E(γ): From Coulomb excitation
727.4+X	222.0	E(γ): From Coulomb excitation
794+X	385	E(γ): From Coulomb excitation
794+X	471	E(γ): From Coulomb excitation
814	131	E(γ): From Coulomb excitation
814	252.8	E(γ): From Coulomb excitation
852+X	241.1	E(γ): From Coulomb excitation
858.0	136	E(γ): From Coulomb excitation
858.0	261.8	E(γ): From Coulomb excitation
E(level)	E(gamma)	Comments
873.996	192.108	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<60.5 25. Multiply placed with undivided intensity
873.996	243.690	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<30.5 16. Multiply placed with undivided intensity
902.494	192.108	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<65.2 27. Multiply placed with undivided intensity
902.494	230.242	I(γ): Iγ\|<95.3 20
904+X	399	E(γ): From Coulomb excitation
904+X	495	E(γ): From Coulomb excitation
906.499	32.526	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<≈1.0. Multiply placed with undivided intensity
906.499	202.421	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<68 17. Multiply placed with undivided intensity
949.660	43.17	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<≈15. Multiply placed with undivided intensity
954.1	140	E(γ): From Coulomb excitation
954.1	271.4	E(γ): From Coulomb excitation
988.6+X	261.2	E(γ): From Coulomb excitation
1002	144	E(γ): From Coulomb excitation
	188	E(γ): From Coulomb excitation
	280.5	E(γ): From Coulomb excitation
1002.618	53.00	E(γ): Multiply placed with undivided intensity I(γ): Iγ\|<63 12. Multiply placed with undivided intensity
1024+X	413	E(γ): From Coulomb excitation
1024+X	519	E(γ): From Coulomb excitation
1103	149	E(γ): From Coulomb excitation
1103	289.4	E(γ): From Coulomb excitation
1132+X	280	E(γ): From Coulomb excitation
1151+X	424	E(γ): From Coulomb excitation
1151+X	540	E(γ): From Coulomb excitation
1156.1	154	E(γ): From Coulomb excitation
1156.1	298.1	E(γ): From Coulomb excitation
E(level)	E(gamma)	Comments
1260.9	306.8	E(γ): From Coulomb excitation
1287+X	435	E(γ): From Coulomb excitation
1287+X	560	E(γ): From Coulomb excitation
1287.6+X	299	E(γ): From Coulomb excitation
1316	314.2	E(γ): From Coulomb excitation
1426	323.1	E(γ): From Coulomb excitation
1434+X	445	E(γ): From Coulomb excitation
1434+X	581	E(γ): From Coulomb excitation
1453+X	321	E(γ): From Coulomb excitation
1482.8	326.7	E(γ): From Coulomb excitation
1587+X	455	E(γ): From Coulomb excitation
1599.0	338.1	E(γ): From Coulomb excitation
1652	335.2	E(γ): From Coulomb excitation
2200	2200	E(γ): From ²⁴¹Am(n,γ) (1979Va25).

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A B D E H	1-	16.01 h 2 % β^- = 83.0 3 % ε = 17.0 3 % α < 10×10^-5
44.093 3	E	0-		44.092 3	100	M1	0.0	1-
48.603 9	A B C E H	5-	141 y 2 % IT = 99.550 10 % α = 0.450 10 % SF < 4.7×10^-9	48.63 5	100	E4	0.0	1-
52.714 7	A B D E	3-		52.770 36	100	E2	0.0	1-
75.820 3	A B D E	2-		75.823 4	100	M1	0.0	1-
99.285 9	E	0+,1+,2+		99.269 15	100	E1	0.0	1-
100.1 7	B C	6-
114	A B C	6-
148	A B	5-
149.707 7	A B D E	4-		73.864 11 96.994 2	0.96 Calc. 100 4	E2 M1	75.820 52.714	2- 3-
168.387 9	E	1-,2-,3-		69.101 8 92.568 26	30 11 100 32	(E1) M1+E2	99.285 75.820	0+,1+,2+ 2-
172	B C	7-
181.4 10	C	(5+)		132.8 5	100	(E1)	48.603	5-
181.4+X	C	(7+)
190.6 5	A B C	7-		90 142.0 5			100.1 48.603	6- 5-
197.5 7	D
200.581 9	E	3-,4-		32.195 2 124.755 22 147.870 22	≤101 100 16 ≤46	M1+E2	168.387 75.820 52.714	1-,2-,3- 2- 3-
230.527 3	D E	1+		154.708 2 186.433 2	100.0 8 91.2 9	E1 E1	75.820 44.093	2- 0-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
244.381 8	A B D E	3-		94.671 6 191.667 5 195.778 6	18.0 18 96.3 11 100.0 10	M1+E2 M1 E2	149.707 52.714 48.603	4- 3- 5-
247+X	C	(8+)
254.3	C	8-		82 154.2 5			172 100.1	7- 6-
263	B	(6- AND 7-)
269.854 10	D E	3+		39.42 6	100	(E2)	230.527	1+
274.330 5	E	1-		198.498 12 230.242 7 274.331 6	23.9 9 <40 100.0 10	M1+E2 M1 M1	75.820 44.093 0.0	2- 0- 1-
276	C	8-		162.3 5	100		114	6-
283.3 2	D
289.028 13	A B E	4-		88.44 5 213.37 8 240.443 32	≈2.9 100 36 54 7	M1+E2 E2 M1+E2	200.581 75.820 48.603	3-,4- 2- 5-
292.831 8	A B D E	2-		48.514 30 217.043 28 240.115 14	1.8 1 100 9 98 9	M1+E2 M1+E2	244.381 75.820 52.714	3- 2- 3-
296.401 8	E	2-		52.05 7 220.600 24 243.690 11 296.412 25	0.5 Calc. 65 4 ≤70 100 8	M1(+E2) M1 M1+E2 M1+E2	244.381 75.820 52.714 0.0	3- 2- 3- 1-
306.9 4	D
311.832 10	E	1+,2+		41.997 34 81.312 15 212.536 14	6.0 Calc. 100 15 ≤217	E2 M1+E2 (M1+E2)	269.854 230.527 99.285	3+ 1+ 0+,1+,2+
323.4+X	C	(9+)		142.0 5	100		181.4+X	(7+)
327.884 9	A B D E	3-		35.049 11 178.11 7 252.049 15	56 10 100 18	M1+E2 M1+E2	292.831 149.707 75.820	2- 4- 2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
330.740 8	E	3-		37.910 5 41.71 5 56.421 18 86.316 30 278.000 18	52 12 ≤12.8 <72 100 7	M1+E2	292.831 289.028 274.330 244.381 52.714	2- 4- 1- 3- 3-
330.837 9	E	2-,3-		34.441 13 ? 38.005 5 56.577 38	1.5 Calc. 100 24 24 9	M1+E2 M1+E2 E2	296.401 292.831 274.330	2- 2- 1-
341.593 14	E	0+		111.100 18 341.528 22	70 10 100 12	(M1)	230.527 0.0	1+ 1-
342	A B	5-
342.805 10	E	2-,3-		30.973 1 46.42 5 193.128 31	≤320 100 17	M1+E2 E2	311.832 296.401 149.707	1+,2+ 2- 4-
347	C	9-		92 174.4 5			254.3 172	8- 7-
355.715 10	E	2+		27.82 6 62.876 15 111.27 5	40 Calc. 16.2 15 100 9	E1+M2 (E1+M2) E1+M2	327.884 292.831 244.381	3- 2- 3-
363.434 11	D E	2+,3+		51.619 35	100	M1+E2	311.832	1+,2+
364.658 11	E	2+		23.12 7 94.804 5 134.20 7	0.2 100 11 63 19	E2 M1+E2 M1(+E2)	341.593 269.854 230.527	0+ 3+ 1+
369.207 17	D E	1-,2-		72.806 30 94.874 22	100 Calc. ≤9000	(E2) M1+E2	296.401 274.330	2- 1-
372.490 9	E	4-		41.71 5 76.092 14 171.951 25 222.75 9 296.732 34 319.75 6	<19.2 54 16 51 8 43 16 100 12 75 16	M1+E2 (E2) (M1) M1+E2	330.740 296.401 200.581 149.707 75.820 52.714	3- 2- 3-,4- 4- 2- 3-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
373.3 7	C	9-		97 182.7 5			276 190.6	8- 7-
373.686 9	A B E	4-		45.91 6 80.905 19	≤23 100 30	M1+E2 E2	327.884 292.831	3- 2-
376.947 8	D E	3+		46.128 33 49.03 5 84.124 20 132.565 4	36.3 11 100.0 10	(E1+M2) E1+M2	330.837 327.884 292.831 244.381	2-,3- 3- 2- 3-
388.112 9	E	3+		95.44 6 143.789 28	100 Calc. 26 6	E1 E1+M2	292.831 244.381	2- 3-
397.147 10	E	2-,3-,4-		33.713 2 69.253 11	100 14 17 7	M1+E2	363.434 327.884	2+,3+ 3-
400.521 9	D E	1-		31.306 36 35.84 8 69.781 6 324.84 6	31 10 100 20	(E2) M1+E2	369.207 364.658 330.740 75.820	1-,2- 2+ 3- 2-
405.880 9	E	2-,3,4		28.937 25 32.195 2 77.988 23 161.459 18	≤158 ≤37 100 15		376.947 373.686 327.884 244.381	3+ 4- 3- 3-
405.933 9	E	4+		33.443 2 50.27 4	100 18 0.07 Calc.	E1 (E2)	372.490 355.715	4- 2+
409	B	(6-)
409+X	C	(10+)		162.1 5	100		247+X	(8+)
417.746 15	D E	(4)+		147.870 22	100	M1+E2	269.854	3+
418.084 11	E	4+		29.94 6 90.178 22 129.056 29 173.60 16	100 28 71 24 41 27	E1+M2 E1+M2 E1+M2	388.112 327.884 289.028 244.381	3+ 3- 4- 3-
419.085 9	E	2-		30.973 1 46.598 16 88.322 31 91.229 24 366.351 33	≤290 0.56 Calc. 45 20 57 18 100 19	M1+E2 M1	388.112 372.490 330.740 327.884 52.714	3+ 4- 3- 3- 3-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
420.651 13	E	2+,3+,4+		32.526 21 43.728 23 57.236 28	≤1.8 11 Calc. 100 9	M1+E2 M1+E2	388.112 376.947 363.434	3+ 3+ 2+,3+
428.6 4	D
434	A B	(5-)
442.385 8	E	5+		36.453 3 65.408 28 68.701 3	49 10 14 5 100 7	M1(+E2)	405.933 376.947 373.686	4+ 3+ 4-
446.702 10	E	3-		28.937 25 46.128 33 74.248 23 90.985 4 296.996 25	3.5 Calc. 77 7 100 14	E1	417.746 400.521 372.490 355.715 149.707	(4)+ 1- 4- 2+ 4-
448.9	C	10-		194.6 5	100		254.3	8-
455.688 14	E	1-,2-,3-		124.947 21 159.283 24	100 24 ≤178		330.740 296.401	3- 2-
457.090 11	E	5+		38.996 9 68.997 17 83.399 17 168.125 30	≈5.7 48 14 100 20 31 8	E1	418.084 388.112 373.686 289.028	4+ 3+ 4- 4-
464.362 9	D E	3-,4-		76.258 13 133.595 28 175.314 34 194.510 5 295.960 14 314.71 7	5.0 22 8.1 19 6.3 14 100.0 10 23.6 10 9.1 21	E1+M2 M1+E2 E1+M2 M1+E2	388.112 330.740 289.028 269.854 168.387 149.707	3+ 3- 4- 3+ 1-,2-,3- 4-
479	C	10-		133 202.9 5			347 276	9- 8-
483.640 11	E	4-		64.54 3 65.557 3 435.038 22	32 4 100 5	E1+M2	419.085 418.084 48.603	2- 4+ 5-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
486	B	(7-)
495.721 11	E	3+		76.668 22 89.799 24 122.031 7	24 11 60 20 100 12	M1+E2 E1+M2	419.085 405.880 373.686	2- 2-,3,4 4-
500	B	(6-)
501.569 13	E	(3)-		45.91 6 82.484 17 212.536 14	≤5.2 ≤46 ≤100	M1+E2 M1+E2 (M1+E2)	455.688 419.085 289.028	1-,2-,3- 2- 4-
502.04 3	D E	1+,2+		160.34 5 271.54 4	43 15 100 14	M1+E2	341.593 230.527	0+ 1+
505.4+X	C	(11+)		182.0 5	100		323.4+X	(9+)
506.648 16	E	2+		87.592 29 106.100 25 236.789 30	58 37 ≤398 100 10	E1+M2 E1+M2 M1+E2	419.085 400.521 269.854	2- 1- 3+
506.964 13	E	(3)+		86.316 30 89.216 20 142.306 25 151.27 4	≤100 100 16 70 8 82 15	M1+E2 M1+E2	420.651 417.746 364.658 355.715	2+,3+,4+ (4)+ 2+ 2+
528.545 21	D E	3+		26.92 6 86.173 31 163.93 5 165.08 4	100 37 52 17 57 17	M1+E2 M1+E2	501.569 442.385 364.658 363.434	(3)- 5+ 2+ 2+,3+
533.815 12	E	2-		69.448 11 133.293 28	46 15 100 31	M1+E2 M1+E2	464.362 400.521	3-,4- 1-
544.756 12	E	2-,3-		43.17 5 80.400 33 89.070 20 144.254 17 201.98 7	≤14 46 11 100 29 ≤80 47 15	M1 M1+E2 M1+E2	501.569 464.362 455.688 400.521 342.805	(3)- 3-,4- 1-,2-,3- 1- 2-,3-
559.790 13	E	2-		113.122 34 140.714 16 159.283 24	100 13 67 11 ≤228	M1+E2	446.702 419.085 400.521	3- 2- 1-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
561	C	11-		112 214.4 5			448.9 347	10- 9-
568.215 9	E	4-		84.601 20 125.832 4 150.10 5 191.234 33	3.8 12 69.4 7 7.6 13 100 10	E1 E1+M2 E1	483.640 442.385 418.084 376.947	4- 5+ 4+ 3+
574.089 11	E	(2,3,4)-		29.351 19 176.97 5	70 Calc. 100 28	M1+E2	544.756 397.147	2-,3- 2-,3-,4-
581	B	(7-)
581?	B	(8-)
583.4 10	D
596.2 9	C	11-		147 222.9 5			448.9 373.3	10- 9-
596.425 10	E	2-,3-,4-		94.874 22 149.713 11 199.291 20	≤104 96 10 100 15	M1+E2 M1+E2 M1	501.569 446.702 397.147	(3)- 3- 2-,3-,4-
603+X?	C			356? 422?			247+X 181.4+X	(8+) (7+)
603.889 12	E	(3,4)+		185.786 25 186.127 34 334.061 32	55 11 100 40 44 10	M1+E2 M1+E2 M1+E2	418.084 417.746 269.854	4+ (4)+ 3+
608	B
611+X	C	(12+)		202.2 5	100		409+X	(10+)
612.758 12	D E	2-		53.00 5 78.945 19 106.100 25 193.677 23 316.377 25 319.91 6 368.24 6 382.234 30	≤54 30 10 ≤210 90 27 78 8 45 11 54 12 100 10	M1+E2 E2 E1+M2 E2 M1+E2 M1+E2 M1+E2 E1+M2	559.790 533.815 506.648 419.085 296.401 292.831 244.381 230.527	2- 2- 2+ 2- 2- 2- 3- 1+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
621.527 14	D E	1-,2-		25.12 5 87.726 31 165.79 6 390.92 4	0.08 Calc. 43 18 42 10 100 13	M1+E2 M1+E2	596.425 533.815 455.688 230.527	2-,3-,4- 2- 1-,2-,3- 1+
626	B
628.523 12	E	3-,4-,5-		144.890 29 254.840 16 256.007 33	88 15 ≤118 100 19	M1+E2 M1+E2 M1+E2	483.640 373.686 372.490	4- 4- 4-
630.291 15	D E	2-,3-,4-		33.80 5 96.433 27 183.48 5	0.8 Calc. 97 35 100 19	E2 M1+E2	596.425 533.815 446.702	2-,3-,4- 2- 3-
640.2 3	D
644.3 5	D
651.3 5	D
658	B
660.6 4	D
664.1 5	D
670.0 7	D
672.248 10	E	(2,3,4)-		75.823 4 98.161 5 275.087 16	≤349 62 7 100 6	M1 M1 M1	596.425 574.089 397.147	2-,3-,4- (2,3,4)- 2-,3-,4-
675.482 12	E	(2,3,4)+		71.593 7 168.519 8 254.840 16 278.319 16	41 2 77 9 ≤66 100 6	M1+E2 M1+E2 M1+E2 (E1)	603.889 506.964 420.651 397.147	(3,4)+ (3)+ 2+,3+,4+ 2-,3-,4-
677	B	(8-)
681.894 12	D E	3-		77.988 23 113.699 11 137.159 27	≤30 100 7 30 6	M1 M1+E2	603.889 568.215 544.756	(3,4)+ 4- 2-,3-
682.7	C	12-		233.8 5	100		448.9	10-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
689.3 5	D E
692+X?	C			369? 445?			323.4+X 247+X	(9+) (8+)
697	B
700.2 5	D
704.030 14	E	1-,2-,3-		82.484 17 144.254 17 202.421 39 376.155 32	≤46 ≤50 ≤48 100 25	M1+E2 E2 M1+E2	621.527 559.790 501.569 327.884	1-,2- 2- (3)- 3-
710.389 11	E	1-,2-,3-		38.145 10 81.864 32 88.869 19 136.299 23	33 18 100 35 34 13	M1 M1+E2 M1(+E2)	672.248 628.523 621.527 574.089	(2,3,4)- 3-,4-,5- 1-,2- (2,3,4)-
712.442 13	E	2-,3-,4-		83.926 12 138.352 12 293.34 6 384.531 27	56 11 53 6 83 8 100 10	M1+E2 M1+E2 E2	628.523 574.089 419.085 327.884	3-,4-,5- (2,3,4)- 2- 3-
715.3 3	D
721.3 3	D
722	C	12-		126 242.5 5			596.2 479	11- 10-
724.4 3	D
727.4+X	C	(13+)		222.0 5			505.4+X	(11+)
731.225 14	E	3+,4+,5+		102.698 5 134.86 4 313.20 7	53 10 100 22 55 13	E1+M2 M1+E2	628.523 596.425 418.084	3-,4-,5- 2-,3-,4- 4+
734.8 5	D
744.7 5	D
759.4 4	D
766.9 3	D
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
779.6 3	D
790	A
794+X?	C			385? 471?			409+X 323.4+X	(10+) (9+)
795.7 4	D
796	B	(9-)
802.4 4	D
814	C	13-		131 252.8 5			682.7 561	12- 11-
818.1 3	D
821	A B
823.2 3	D
833	B
846	B
851.9 3	D
852+X	C	(14+)		241.1 5	100		611+X	(12+)
858.0 10	C	13-		136 261.8 5			722 596.2	12- 11-
864.5 7	D
873.996 12	A B D E	2-		192.108 6 243.690 11 314.33 7 585.21 16 599.55 12 629.64 8	≤63 ≤32 24 4 46 15 39 14 100 34	M1+E2 M1+E2 E2 M1+E2	681.894 630.291 559.790 289.028 274.330 244.381	3- 2-,3-,4- 2- 4- 1- 3-
883.8 4	D
896.6 3	D
902.494 11	A B E	(3)-		192.108 6 230.242 7 328.409 19 658.11 6	≤68 ≤97 37 3 100 16	M1+E2 M1 M1	710.389 672.248 574.089 244.381	1-,2-,3- (2,3,4)- (2,3,4)- 3-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
904+X	C			399? 495?			505.4+X 409+X	(11+) (10+)
906.499 19	D E	(3)-		32.526 21 202.421 39 450.69 6	≤1.0 ≤85 100 21	M1+E2 E2 M1+E2	873.996 704.030 455.688	2- 1-,2-,3- 1-,2-,3-
916	A B
919.5 4	D
930.4 3	D
934.6 4	D
935	A B
949.660 14	E	(4-)		43.17 5 75.664 7	≤15 100 18	(E2)	906.499 873.996	(3)- 2-
951	A
954.1	C	14-		140 271.4 5			814 682.7	13- 12-
968.7 3	D
974.9 5	A B D	(3+)
978.3 3	D
988.6+X	C	(15+)		261.2 5	100		727.4+X	(13+)
994	A B
1002	C	14-		144 188 280.5 5			858.0 814 722	13- 13- 12-
1002.618 23	E	(5-)		53.00 5 96.115 16	≤75 100 20	M1+E2 (E2)	949.660 906.499	(4-) (3)-
1011	A B	(2+)
1011?	A B	(4+)
1024+X	C			413 519			611+X 505.4+X	(12+) (11+)
1029	B
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1049	B	(3+)
1066	A B	(5+)
1073	B
1088	B
1097	B	(4+)
1103	C	15-		149 289.4 5			954.1 814	14- 13-
1119	A B
1132+X	C	(16+)		280			852+X	(14+)
1142	A B
1151	B	(6+)
1151+X	C			424 540			727.4+X 611+X	(13+) (12+)
1156.1 11	C	15-		154? 298.1 5			1002 858.0	14- 13-
1161.97 3	E	1-,2-,3-,4-		255.467 38 451.60 13 617.207 40	98 22 79 21 100 10	E2 E2 M1	906.499 710.389 544.756	(3)- 1-,2-,3- 2-,3-
1162	B
1170	A B
1187	B
1192	B
1199	B
1210	B
1227	B
1243	B
1260.9	C	16-		306.8 5	100		954.1	14-
1262	B
1287	B
1287+X	C			435 560			852+X 727.4+X	(14+) (13+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1287.6+X?	C	(17+)		299	100		988.6+X	(15+)
1300	B
1316	B C	16-		314.2 5	100		1002	14-
1325	B
1343	B
1362	B
1380	B
1406	B
1417	B
1426	C	17-		323.1 5	100		1103	15-
1434+X	C			445 581?			988.6+X 852+X	(15+) (14+)
1443	B
1453+X?	C	(18+)		321	100		1132+X	(16+)
1455	B
1467	B
1482	B
1482.8 12	C	17-		326.7 5	100		1156.1	15-
1507	B
1519	B
1562	B
1587+X?	C			455?	100		1132+X	(16+)
1599.0	C	18-		338.1 5	100		1260.9	16-
1652	C	18-		335.2 5	100		1316	16-
2200 80		(2+,3-)	13.9 ms 2 % SF ≈ 100 % IT = ? % α < 0.005	2200 80 ?	100		0.0	1-