List of levels for 238NP

Authors: E. Browne, J. K. Tuli | Citation: Nucl. Data Sheets 127, 191 (2015) | Cutoff date: 1-Jun-2014

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
26.4266	3+		26.43 2	M1+E2	0.097 6	333	α=333 12, α(L)=248 9, α(M)=62.7 23, α(N)=17.0 6, α(O)=4.13 15, α(P)=0.767 24, α(Q)=0.0469 7, α(N+)=21.9 8
62.330	4+		35.90 2	M1+E2	0.130 3	133.6	α=133.6 24, α(L)=99.8 18, α(M)=25.1 5, α(N)=6.81 13, α(O)=1.65 3, α(P)=0.307 6, α(Q)=0.0188 3, α(N+)=8.78 16
62.330	4+		62.33 3	E2		136.0	α=136.0, α(L)=98.9 14, α(M)=27.5 4, α(N)=7.52 11, α(O)=1.749 25, α(P)=0.285 4, α(Q)=0.000809 12, α(N+)=9.55 14
86.6738	3+		24.37 2	M1(+E2)	0.03 LE	326	α=326 8, α(L)=244 6, α(M)=60.3 15, α(N)=16.3 4, α(O)=4.02 10, α(P)=0.779 17, α(Q)=0.0598 9, α(N+)=21.2 5
	3+		60.243 4	M1+E2	0.089 23	23.5	α=23.5 7, α(L)=17.6 6, α(M)=4.32 15, α(N)=1.17 4, α(O)=0.287 9, α(P)=0.0553 15, α(Q)=0.00410 6, α(N+)=1.52 5
	3+		86.676 2	M1+E2	0.10 3	7.95	α=7.95 18, α(L)=5.98 13, α(M)=1.46 4, α(N)=0.395 10, α(O)=0.0972 23, α(P)=0.0188 4, α(Q)=0.001413 22, α(N+)=0.513 13
106.155	5+		43.84 3	M1+E2	0.111 5	65.3	α=65.3 12, α(L)=48.9 9, α(M)=12.12 24, α(N)=3.29 7, α(O)=0.803 15, α(P)=0.152 3, α(Q)=0.01043 15, α(N+)=4.25 8
106.155	5+		79.74 3	E2		42.0	α=42.0, α(L)=30.6 5, α(M)=8.51 12, α(N)=2.33 4, α(O)=0.542 8, α(P)=0.0888 13, α(Q)=0.000294 5, α(N+)=2.96 5
121.645	4+		34.97 3	M1		110.8	α=110.8, α(L)=83.4 12, α(M)=20.3 3, α(N)=5.50 8, α(O)=1.355 20, α(P)=0.263 4, α(Q)=0.0205 3, α(N+)=7.14 11
	4+		59.31 4	M1		23.4	α=23.4, α(L)=17.64 25, α(M)=4.29 6, α(N)=1.161 17, α(O)=0.286 4, α(P)=0.0556 8, α(Q)=0.00432 7, α(N+)=1.507 22
	4+		95.22 2	(M1)		5.90	α=5.90, α(L)=4.44 7, α(M)=1.078 16, α(N)=0.292 4, α(O)=0.0719 10, α(P)=0.01397 20, α(Q)=0.001084 16, α(N+)=0.379 6
	4+		121.69 4	E2		6.04	α=6.04, α(K)=0.179 3, α(L)=4.26 6, α(M)=1.186 17, α(N)=0.324 5, α(O)=0.0756 11, α(P)=0.01251 18, α(Q)=6.14×10^-5 9, α(N+)=0.412 6
136.0450	3-	6.0 ns	49.372 2	E1		0.820	B(E1)(W.u.)=1.1E-4, α=0.820, α(L)=0.615 9, α(M)=0.1536 22, α(N)=0.0408 6, α(O)=0.00939 14, α(P)=0.001508 22, α(Q)=5.32E-5 8, α(N+)=0.0518 8
	3-	6.0 ns	73.715 4	E1		0.285	B(E1)(W.u.)=2.0E-6, α=0.285, α(L)=0.215 3, α(M)=0.0529 8, α(N)=0.01411 20, α(O)=0.00330 5, α(P)=0.000557 8, α(Q)=2.30E-5 4, α(N+)=0.0180 3
	3-	6.0 ns	109.614 4	E1+M2	0.026 6	0.138	B(E1)(W.u.)=1.0E-6, α=0.138 19
	3-	6.0 ns	136.045 10	E1		0.247	B(E1)(W.u.)=4.3E-7, α=0.247, α(K)=0.190 3, α(L)=0.0436 6, α(M)=0.01064 15, α(N)=0.00285 4, α(O)=0.000679 10, α(P)=0.0001206 17, α(Q)=6.09E-6 9, α(N+)=0.00366 6
165.532	5+		43.98 4	M1+E2	0.13 4	68	α=68 8, α(L)=51 6, α(M)=12.6 16, α(N)=3.4 5, α(O)=0.83 10, α(P)=0.157 17, α(Q)=0.01030 17, α(N+)=4.4 6
165.532	5+		139.05 2	[E2]		3.41	α=3.41, α(K)=0.211 3, α(L)=2.32 4, α(M)=0.647 9, α(N)=0.1767 25, α(O)=0.0413 6, α(P)=0.00685 10, α(Q)=3.96×10^-5 6, α(N+)=0.225 4
179.154	4-		43.11 3	M1+E2	0.08 2	65	α=65 3, α(L)=48.5 21, α(M)=11.9 6, α(N)=3.23 16, α(O)=0.79 4, α(P)=0.152 6, α(Q)=0.01100 16, α(N+)=4.18 20
	4-		92.486 7	E1		0.1574	α=0.1574, α(L)=0.1184 17, α(M)=0.0291 4, α(N)=0.00777 11, α(O)=0.00183 3, α(P)=0.000316 5, α(Q)=1.410×10^-5 20, α(N+)=0.00993 14
	4-		152.69	(E1)		0.189	α=0.189, α(K)=0.1458 21, α(L)=0.0325 5, α(M)=0.00792 11, α(N)=0.00212 3, α(O)=0.000507 7, α(P)=9.07×10^-5 13, α(Q)=4.73E-6 7, α(N+)=0.00272 4
182.8775	2-		46.84 3	M1+E2	0.14 4	56	α=56 6, α(L)=42 5, α(M)=10.5 13, α(N)=2.9 4, α(O)=0.69 8, α(P)=0.131 13, α(Q)=0.00854 14, α(N+)=3.7 5
	2-		156.452 2	E1		0.1784	α=0.1784, α(K)=0.1379 20, α(L)=0.0305 5, α(M)=0.00744 11, α(N)=0.00199 3, α(O)=0.000477 7, α(P)=8.54×10^-5 12, α(Q)=4.49E-6 7, α(N+)=0.00256 4
	2-		182.876 2	E1		0.1239	α=0.1239, α(K)=0.0965 14, α(L)=0.0206 3, α(M)=0.00502 7, α(N)=0.001346 19, α(O)=0.000323 5, α(P)=5.84×10^-5 9, α(Q)=3.20E-6 5, α(N+)=0.001731 25
215.522	3-		32.67 3	M1(+E2)	0.025 LE	136.4	α=136.4 22, α(L)=102.6 17, α(M)=25.0 4, α(N)=6.77 11, α(O)=1.67 3, α(P)=0.324 5, α(Q)=0.0251 4, α(N+)=8.79 15
	3-		79.483 17	E2(+M1)	4 GE	41.7	α=41.7 12, α(L)=30.3 9, α(M)=8.44 24, α(N)=2.31 7, α(O)=0.537 15, α(P)=0.0882 24, α(Q)=0.00034 5, α(N+)=2.93 8
	3-		153.192 12	(E1)		0.187	α=0.187, α(K)=0.1447 21, α(L)=0.0322 5, α(M)=0.00785 11, α(N)=0.00210 3, α(O)=0.000503 7, α(P)=9.00×10^-5 13, α(Q)=4.70E-6 7, α(N+)=0.00270 4
	3-		189.099 6	E1		0.1146	α=0.1146, α(K)=0.0894 13, α(L)=0.0190 3, α(M)=0.00462 7, α(N)=0.001238 18, α(O)=0.000297 5, α(P)=5.38×10^-5 8, α(Q)=2.98E-6 5, α(N+)=0.001592 23
	3-		215.517 5	E1		0.0847	α=0.0847, α(K)=0.0664 10, α(L)=0.01376 20, α(M)=0.00334 5, α(N)=0.000897 13, α(O)=0.000216 3, α(P)=3.94×10^-5 6, α(Q)=2.25E-6 4, α(N+)=0.001154 17
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
217.949	0-		35.07 3	E2		2.21×10³	α=2.21×10³, α(L)=1611 24, α(M)=446 7, α(N)=121.7 18, α(O)=28.3 5, α(P)=4.58 7, α(Q)=0.00987 15, α(N+)=154.5 23
217.949	0-		217.966 20	M2		10.57	α=10.57, α(K)=7.09 10, α(L)=2.56 4, α(M)=0.674 10, α(N)=0.186 3, α(O)=0.0456 7, α(P)=0.00865 13, α(Q)=0.000607 9, α(N+)=0.241 4
218.7	(6+)		52.98	M1+E2	0.17 2	40.1	α=40.1 19, α(L)=29.9 14, α(M)=7.5 4, α(N)=2.03 11, α(O)=0.494 25, α(P)=0.093 4, α(Q)=0.00589 9, α(N+)=2.63 14
232.828	5-		53.70 7	M1+E2	0.271 4	48.3	α=48.3 9, α(L)=35.9 7, α(M)=9.20 17, α(N)=2.50 5, α(O)=0.601 11, α(P)=0.1092 19, α(Q)=0.00549 8, α(N+)=3.22 6
	5-		96.82 5	E2		16.87	α=16.87, α(L)=12.26 18, α(M)=3.42 5, α(N)=0.934 14, α(O)=0.218 3, α(P)=0.0358 5, α(Q)=0.0001386 20, α(N+)=1.187 17
	5-		111.197 15	[E1]		0.0974	α=0.0974, α(L)=0.0733 11, α(M)=0.0179 3, α(N)=0.00480 7, α(O)=0.001138 16, α(P)=0.000199 3, α(Q)=9.45×10^-6 14, α(N+)=0.00615 9
243.959	(1)+		243.959 4	M1+E2	0.10 1	1.93	α=1.93, α(K)=1.528 22, α(L)=0.302 5, α(M)=0.0733 11, α(N)=0.0198 3, α(O)=0.00488 7, α(P)=0.000948 14, α(Q)=7.28×10^-5 11, α(N+)=0.0257 4
250.39	(2)-		223.89 10	(E1)		0.0776	α=0.0776, α(K)=0.0609 9, α(L)=0.01254 18, α(M)=0.00304 5, α(N)=0.000817 12, α(O)=0.000197 3, α(P)=3.60×10^-5 5, α(Q)=2.07E-6 3, α(N+)=0.001052 15
258.853	4-		43.32 3	M1+E2	0.391 20	156	α=156 9, α(L)=115 7, α(M)=30.5 19, α(N)=8.3 5, α(O)=1.97 12, α(P)=0.339 19, α(Q)=0.00996 17, α(N+)=10.6 7
	4-		75.97 7	E2		52.9	α=52.9, α(L)=38.4 6, α(M)=10.71 16, α(N)=2.93 5, α(O)=0.681 10, α(P)=0.1115 17, α(Q)=0.000357 6, α(N+)=3.72 6
	4-		122.76 7	[M1]		13.43	α=13.43, α(K)=10.60 15, α(L)=2.13 3, α(M)=0.517 8, α(N)=0.1401 20, α(O)=0.0345 5, α(P)=0.00670 10, α(Q)=0.000519 8, α(N+)=0.182 3
	4-		232.433 8	E1		0.0712	α=0.0712, α(K)=0.0560 8, α(L)=0.01145 16, α(M)=0.00278 4, α(N)=0.000746 11, α(O)=0.000180 3, α(P)=3.29×10^-5 5, α(Q)=1.92E-6 3, α(N+)=0.000961 14
275.519	5+		153.870 9	M1+E2		4.7	α=4.7 25, α(K)=3 3, α(L)=1.30 19, α(M)=0.34 7, α(N)=0.093 20, α(O)=0.022 4, α(P)=0.0039 5, α(Q)=0.00015 13, α(N+)=0.119 24
277.641	(2)+		251.25 4	E2+(M1)	4.6 GE	0.39	α=0.39 4, α(K)=0.13 3, α(L)=0.184 4, α(M)=0.0504 9, α(N)=0.01375 22, α(O)=0.00324 6, α(P)=0.000554 11, α(Q)=8.9×10^-6 14, α(N+)=0.0176 3
298.368	3+		54.40 4	E2		262	α=262, α(L)=190 3, α(M)=52.9 8, α(N)=14.45 21, α(O)=3.36 5, α(P)=0.548 8, α(Q)=0.001445 21, α(N+)=18.4 3
	3+		236.025 11	M1		2.13	α=2.13, α(K)=1.691 24, α(L)=0.332 5, α(M)=0.0806 12, α(N)=0.0218 3, α(O)=0.00537 8, α(P)=0.001043 15, α(Q)=8.06×10^-5 12, α(N+)=0.0283 4
	3+		271.953 11	M1		1.437	α=1.437, α(K)=1.140 16, α(L)=0.224 4, α(M)=0.0542 8, α(N)=0.01467 21, α(O)=0.00361 5, α(P)=0.000702 10, α(Q)=5.42×10^-5 8, α(N+)=0.0190 3
	3+		298.38 4	M1		1.111	α=1.111, α(K)=0.882 13, α(L)=0.1727 25, α(M)=0.0418 6, α(N)=0.01133 16, α(O)=0.00279 4, α(P)=0.000542 8, α(Q)=4.18×10^-5 6, α(N+)=0.01470 21
312.704	5-		53.88 4	M1+E2	0.22 4	42	α=42 5, α(L)=32 3, α(M)=8.0 9, α(N)=2.17 24, α(O)=0.52 6, α(P)=0.097 9, α(Q)=0.00553 11, α(N+)=2.8 3
	5-		97.22 5	E2		16.54	α=16.54, α(L)=12.03 17, α(M)=3.35 5, α(N)=0.916 13, α(O)=0.213 3, α(P)=0.0351 5, α(Q)=0.0001365 20, α(N+)=1.165 17
	5-		151.07 5			16.7	α=16.7
315.063	4+,5+		82.232 4	E1+M2	0.024 +6-7	0.32	α=0.32 6, α(L)=0.24 5, α(M)=0.061 13, α(N)=0.017 4, α(O)=0.0040 9, α(P)=0.00070 16, α(Q)=3.6×10^-5 10, α(N+)=0.021 5
325.210	1-		107.263 6	M1		4.18	α=4.18, α(L)=3.15 5, α(M)=0.763 11, α(N)=0.207 3, α(O)=0.0509 8, α(P)=0.00990 14, α(Q)=0.000767 11, α(N+)=0.268 4
342.439	5-		66.919 5	E1		0.368	α=0.368, α(L)=0.277 4, α(M)=0.0684 10, α(N)=0.0182 3, α(O)=0.00425 6, α(P)=0.000709 10, α(Q)=2.82×10^-5 4, α(N+)=0.0232 4
342.439	5-		163.26 2	M1+E2	6.26 7	1.86	α=1.86, α(K)=0.310 5, α(L)=1.131 16, α(M)=0.313 5, α(N)=0.0856 12, α(O)=0.0200 3, α(P)=0.00335 5, α(Q)=2.93×10^-5 5, α(N+)=0.1090 16
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
373.684	(1)-		48.50 3	(M1)		42.3	α=42.3, α(L)=31.8 5, α(M)=7.74 11, α(N)=2.10 3, α(O)=0.517 8, α(P)=0.1003 15, α(Q)=0.00781 11, α(N+)=2.72 4
380.60	(3)-		130.215 12	E2(+M1)	7.9 GE	4.56	α=4.56 9, α(K)=0.27 7, α(L)=3.12 5, α(M)=0.867 13, α(N)=0.237 4, α(O)=0.0553 8, α(P)=0.00918 14, α(Q)=5.2×10^-5 4, α(N+)=0.302 5
395.198	(5)+		289.04 8	M1+E2	0.9 3	0.77	α=0.77 19, α(K)=0.57 17, α(L)=0.151 16, α(M)=0.038 4, α(N)=0.0103 9, α(O)=0.00250 23, α(P)=0.00047 6, α(Q)=2.8×10^-5 8, α(N+)=0.0133 12
395.198	(5)+		332.868 16	E2(+M1)	5.9 GE	0.155	α=0.155 10, α(K)=0.071 9, α(L)=0.0617 13, α(M)=0.0166 3, α(N)=0.00454 9, α(O)=0.001073 21, α(P)=0.000187 4, α(Q)=4.2×10^-6 4, α(N+)=0.00580 11
417.641	2+,3+,4+		295.984 15	E2		0.208	α=0.208, α(K)=0.0780 11, α(L)=0.0950 14, α(M)=0.0259 4, α(N)=0.00707 10, α(O)=0.001665 24, α(P)=0.000286 4, α(Q)=5.03×10^-6 7, α(N+)=0.00902 13
417.641	2+,3+,4+		391.27 3	M1+E2	1.34 +26-19	0.25	α=0.25 4, α(K)=0.18 3, α(L)=0.051 4, α(M)=0.0129 9, α(N)=0.00350 23, α(O)=0.00085 6, α(P)=0.000157 12, α(Q)=8.8×10^-6 14, α(N+)=0.0045 3
433.716	3+,4+		174.88 3	E1		0.1375	α=0.1375, α(K)=0.1069 15, α(L)=0.0231 4, α(M)=0.00561 8, α(N)=0.001506 21, α(O)=0.000361 5, α(P)=6.51×10^-5 10, α(Q)=3.52E-6 5, α(N+)=0.00193 3
433.716	3+,4+		297.672 15	E1		0.0410	α=0.0410, α(K)=0.0325 5, α(L)=0.00638 9, α(M)=0.001544 22, α(N)=0.000415 6, α(O)=0.0001003 14, α(P)=1.86×10^-5 3, α(Q)=1.144E-6 16, α(N+)=0.000535 8
497.20	2-,3-,4-		281.79 10	M1+E2	1.0 +5-3	0.77	α=0.77 21, α(K)=0.56 19, α(L)=0.159 17, α(M)=0.040 4, α(N)=0.0109 10, α(O)=0.00265 25, α(P)=0.00049 6, α(Q)=2.7×10^-5 9, α(N+)=0.0141 13
523.83	3+,4+,5+		461.59 9	M1+E2	0.93 +25-20	0.21	α=0.21 4, α(K)=0.16 3, α(L)=0.037 4, α(M)=0.0091 9, α(N)=0.00247 25, α(O)=0.00060 6, α(P)=0.000114 13, α(Q)=7.6×10^-6 13, α(N+)=0.0032 4
529.857	3-		217.26 7	E2		0.589	α=0.589, α(K)=0.1340 19, α(L)=0.332 5, α(M)=0.0915 13, α(N)=0.0250 4, α(O)=0.00586 9, α(P)=0.000991 14, α(Q)=1.090×10^-5 16, α(N+)=0.0319 5
529.857	3-		346.98 1	M1+E2	0.7 4	0.53	α=0.53 15, α(K)=0.41 13, α(L)=0.093 16, α(M)=0.023 4, α(N)=0.0063 9, α(O)=0.00153 23, α(P)=0.00029 5, α(Q)=2.0×10^-5 6, α(N+)=0.0081 12
567.023	3-		334.205 13	E2		0.1441	α=0.1441, α(K)=0.0624 9, α(L)=0.0598 9, α(M)=0.01620 23, α(N)=0.00442 7, α(O)=0.001044 15, α(P)=0.000181 3, α(Q)=3.78×10^-6 6, α(N+)=0.00565 8
	3-		351.37 8	E2		0.1247	α=0.1247, α(K)=0.0569 8, α(L)=0.0497 7, α(M)=0.01342 19, α(N)=0.00366 6, α(O)=0.000865 13, α(P)=0.0001505 22, α(Q)=3.38×10^-6 5, α(N+)=0.00468 7
	3-		384.12 4	M1+E2	0.93 16	0.34	α=0.34 5, α(K)=0.26 4, α(L)=0.063 5, α(M)=0.0156 11, α(N)=0.0042 3, α(O)=0.00103 8, α(P)=0.000195 15, α(Q)=1.24×10^-5 17, α(N+)=0.0055 4
	3-		430.96 3	M1+E2	0.87 22	0.26	α=0.26 5, α(K)=0.20 4, α(L)=0.046 6, α(M)=0.0114 12, α(N)=0.0031 4, α(O)=0.00076 8, α(P)=0.000144 17, α(Q)=9.6×10^-6 18, α(N+)=0.0040 5
646.76	2+,3+,(4)+		620.28 6	M1+E2	0.97 21	0.093	α=0.093 15, α(K)=0.072 12, α(L)=0.0157 19, α(M)=0.0039 5, α(N)=0.00105 12, α(O)=0.00026 3, α(P)=4.9×10^-5 6, α(Q)=3.4E-6 6, α(N+)=0.00136 16
646.76	2+,3+,(4)+		646.75 7	E2(+M1)	1.9 GE	0.040	α=0.040 12, α(K)=0.029 10, α(L)=0.0083 16, α(M)=0.0021 4, α(N)=0.00057 10, α(O)=0.000139 25, α(P)=2.6×10^-5 5, α(Q)=1.4E-6 5, α(N+)=0.00074 13

Nilsson configurations are from 1990Ho02, unless otherwise noted.

For theoretical investigations see:

1987Be51 - Levels, bandhead energies.

1988Fr16 - Newby shift.

1988Qu03 - coupling effects.

1989Pl10 - level density in second potential well.

1992Gr16 - Half-life for SF.

additional list can be found in 1990Ho02.

Cluster decay

²³⁸Np(³⁰Mg): 2012Sa31, 2011Sh13, 2005Bh02.

Theory:

2013Ni03, 2012Ro34, 2011Sa40, 2010Ni02, 2008Do12, 2006Sa35, 2004Sa55, 2002Sc36.

Q(β-)=1291.5 keV 5	S(n)= 5488.3 keV 2	S(p)= 5224.6 keV 6	Q(α)= 4691 keV 4
Reference: 2012WA38

References:
A	²³⁷Np(n,γ) E=TH:PRIMARY γ’S	B	²⁴²Am α decay (141 Y)
C	²³⁷Np(n,γ) E=TH:SECONDARY γ’S	D	²³⁷Np(d,p)
E	²³⁷Np(n,γ) E=resonance	F	²³⁷Np(n,γ) E=RES:AVG

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A B C D	2+	2.099 d 2 % β^- = 100
26.4266 21	B C D E	3+		26.43 2	100	M1+E2	0.0	2+
62.330 4	B C D	4+		35.90 2 62.33 3	83 17 100	M1+E2 E2	26.4266 0.0	3+ 2+
86.6738 18	B C D	3+		24.37 2 60.243 4 86.676 2	0.28 4 29.6 22 100 17	M1(+E2) M1+E2 M1+E2	62.330 26.4266 0.0	4+ 3+ 2+
106.155 15	B C D	5+		43.84 3 79.74 3	100 32 7	M1+E2 E2	62.330 26.4266	4+ 3+
121.645 9	B C D	4+		34.97 3 59.31 4 95.22 2 121.69 4	93 13 9.3 15 52 7 100 15	M1 M1 (M1) E2	86.6738 62.330 26.4266 0.0	3+ 4+ 3+ 2+
136.0450 23	A B C E F	3-	6.0 ns	49.372 2 73.715 4 109.614 4 136.045 10	100.0 16 5.7 18 10 4 7.9 13	E1 E1 E1+M2 E1	86.6738 62.330 26.4266 0.0	3+ 4+ 3+ 2+
161.685 24	B	6+
165.532 15	B C D	5+		43.98 4 139.05 2		M1+E2 [E2]	121.645 26.4266	4+ 3+
179.154 7	B C E F	4-		43.11 3 92.486 7 152.69	23 4 100 21 ≤174	M1+E2 E1 (E1)	136.0450 86.6738 26.4266	3- 3+ 3+
182.8775 18	A B C E F	2-		46.84 3 95.7 6 156.452 2 182.876 2	0.80 12 30.4 16 100 12	M1+E2 E1 E1	136.0450 86.6738 26.4266 0.0	3- 3+ 3+ 2+
215.522 4	A B C E F	3-		32.67 3 79.483 17 153.192 12 189.099 6 215.517 5	3.2 5 21 4 53 6 54 5 100 5	M1(+E2) E2(+M1) (E1) E1 E1	182.8775 136.0450 62.330 26.4266 0.0	2- 3- 4+ 3+ 2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
217.949 10	C	0-		35.07 3 217.966 20	3.6 8 100	E2 M2	182.8775 0.0	2- 2+
218.7 6	B D	(6+)		52.98?		M1+E2	165.532	5+
232.828 8	B C	5-		53.70 7 96.82 5 111.197 15	20 3 17 3 100 21	M1+E2 E2 [E1]	179.154 136.0450 121.645	4- 3- 4+
243.959 4	C	(1)+		243.959 4	100	M1+E2	0.0	2+
246.4 14	A E	1 TO 4
250.33 3	B	(1+)		250.33 3	100		0.0	2+
250.39 4	A C E F	(2)-		223.89 10 250.40 4	100 ≤148	(E1)	26.4266 0.0	3+ 2+
258.853 8	A B C E F	4-		43.32 3 75.97 7 122.76 7 152.69 3 196.46 10 232.433 8	1.59 24 2.2 4 6.6 3 ≤114 17 9 100 17	M1+E2 E2 [M1] E1	215.522 182.8775 136.0450 106.155 62.330 26.4266	3- 2- 3- 5+ 4+ 3+
275.519 9	B C D	5+		153.870 9	100	M1+E2	121.645	4+
277.641 18	C	(2)+		251.25 4 277.633 19	61 15 100	E2+(M1)	26.4266 0.0	3+ 2+
285.8 10 ?	A	1 TO 4
297.03 5	B	(6-)		131.49 8 190.88 5	100 39 22		165.532 106.155	5+ 5+
298.368 8	C	3+		54.40 4 236.025 11 271.953 11 298.38 4	0.66 10 100 8 72 5 9.2 10	E2 M1 M1 M1	243.959 62.330 26.4266 0.0	(1)+ 4+ 3+ 2+
299.23 6	B	(3+)		237.02 10 272.75 7 299.20 14	100 5 81 18 60 30		62.330 26.4266 0.0	4+ 3+ 2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
299.788 20	C F	(1)-		116.90 2	100		182.8775	2-
300.68 7	B	1-,2,3,4-		84.9 2 117.2 6 164.67 7			215.522 182.8775 136.0450	3- 2- 3-
300.743 16	B	(6-)		67.93 3 121.3 6 135.19 2 139.05 2 194.61 2	59 5 100 6 ≤2.1 21.0 7		232.828 179.154 165.532 161.685 106.155	5- 4- 5+ 6+ 5+
305.4 20	F	1- TO 4-
312.704 19	B C	5-		53.88 4 97.22 5 151.07 5 176.62 5 250.36 3	10.0 18 32 4 ≈300 100 18 ≤241	M1+E2 E2	258.853 215.522 161.685 136.0450 62.330	4- 3- 6+ 3- 4+
315.063 8	C	4+,5+		82.232 4 135.918 7 179.00 3	100 14 35 5 33 7	E1+M2	232.828 179.154 136.0450	5- 4- 3-
324.314 8	C F	(4)-		108.792 7	100		215.522	3-
325.210 9	A C E F	1-		107.263 6 142.328 10	100 68 20	M1	217.949 182.8775	0- 2-
328.6 5	B D	6+		163.25 2 ?			165.532	5+
334.0 6	A B E F	1- TO 3-
342.439 8	B C	5-		66.919 5 109.614 4 163.26 2 206.37 2	97 3 ≤120 100 6 10.2 12	E1 M1+E2	275.519 232.828 179.154 136.0450	5+ 5- 4- 3-
348.8 9	A E F	1- TO 3-
352.46 4	C E F	(3)-		52.60 5 93.67 5	1.8 5 100		299.788 258.853	(1)- 4-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
367.26 3	A C E F	(2)-		184.38 3	100		182.8775	2-
373.684 14	A C E F	(1)-		48.50 3 155.731 11	5.0 10 100	(M1)	325.210 217.949	1- 0-
374.7 10	B D	(5+)
376.70 7	B	(6-)		117.8 6 270.55 6			258.853 106.155	4- 5+
380.60 4	C F	(3)-		130.215 12		E2(+M1)	250.39	(2)-
386.3 3	A E	1 TO 4
389.4 5	B D	7+		113.7 6 170.50 1			275.519 218.7	5+ (6+)
395.198 17	C	(5)+		289.04 8 332.868 16	67 15 100	M1+E2 E2(+M1)	106.155 62.330	5+ 4+
397.3 15	B
407.59 6	B	6-		132.6 6 174.76 6			275.519 232.828	5+ 5-
409.5 5	D	(8-)
417.641 12	C	2+,3+,4+		295.984 15 330.966 19 391.27 3 417.60 6	100 8 46 13 59 5 ≤4.9	E2 M1+E2	121.645 86.6738 26.4266 0.0	4+ 3+ 3+ 2+
431.3 6	D	(4+)
433.716 13	C	3+,4+		174.88 3 218.17 3 297.672 15	23 17 42 8 100 12	E1 E1	258.853 215.522 136.0450	4- 3- 3-
442.23 3	A C E F	(4)-		74.975 2			367.26	(2)-
456.3 7	D	(8+)
457.65 19	A E F	1- TO 3-
459.6 6	B	(6+)		117.2 6			342.439	5-
469.1 12	B F	1- TO 4-
473.3 4	F	1- TO 4-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
484 3	B	7-
497.20 3	C F	2-,3-,4-		281.79 10 314.31 3	100 ≤176	M1+E2	215.522 182.8775	3- 2-
505.1 10	F	1- TO 4-
523.83 3	C	3+,4+,5+		358.25 4 417.60 6 461.59 9 497.49 5	79 7 ≤7.2 84 14 100 9	M1+E2	165.532 106.155 62.330 26.4266	5+ 5+ 4+ 3+
524.2 6	D	(6+)
525.3 15	B	(7+)
529.857 10	A C E F	3-		217.26 7 314.31 3 346.98 1	100 10 ≤70 37 10	E2 M1+E2	312.704 215.522 182.8775	5- 3- 2-
543.24 4	C F	3-,4-		310.40 8 364.09 4	9 5 100		232.828 179.154	5- 4-
567.023 13	A C E F	3-		334.205 13 351.37 8 384.12 4 430.96 3	42 12 52 8 29 3 100 12	E2 E2 M1+E2 M1+E2	232.828 215.522 182.8775 136.0450	5- 3- 2- 3-
578 3	B
584.5 3	A F	1- TO 4-
601.2 3	A E F	1- TO 3-
603.7 6	D
619.5 3	E F	1 TO 4
630.6 13	D
635.3 10	E F	1- TO 4-
646.76 4	C	2+,3+,(4)+		584.47 5 620.28 6 646.75 7	63 16 100 13 87 8	M1+E2 E2(+M1)	62.330 26.4266 0.0	4+ 3+ 2+
648.1 9	A D E F	1- TO 3-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
673.6 3	A D E F	1- TO 3-
676.9 18	D F	1- TO 4-
692.1 3	A D E F	1- TO 3-
709.24 25	A
722.4 7	A
764.1 6	A
782.4 6	A
797.4 4	A
800.4 8	A
809.8 3	A
813.9 7	A
834.7 6	A
869.0 5	A
903.3 4	A
916.6 8	A
929.1 6 ?	A
948.9 6 ?	A
970.7 6 ?	A
986.5 4 ?	A
1026.6 6 ?	A
1033.4 7 ?	A
1046.5 6 ?	A
1065.2 5 ?	A
1081.0 6 ?	A
1089.0 6 ?	A
1107.8 7	A
1119.6 7 ?	A
1143.0 6	A
1163.1 4	A
1176.1 6	A
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1256.1 3	A
1260.5 6	A
1276.1 5	A
1291.3 4	A
1313.5 3	A
1330.7 6	A
1364.8 7	A
1369.8 7	A
1375.6 4	A
1384.6 3	A
1392.8 5	A
1408.5 6	A
1445.7 6	A
1484.1 8	A
1492.8 7 ?	A
1509.0 5	A
1546.5 7	A
1711.5 5	A
1822.5 6	A
2104.3 6	A
2109.5 5	A
2300			112 ns 39 % SF ≤ 100
2857.4 6	A

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - K^π=2⁺ 5/2(642)-NU 1/2(631)
0.0	2+	2.099 d 2 % β^- = 100
26.4266 21	3+		26.43 2	100	M1+E2	0.0	2+
62.330 4	4+		35.90 2 62.33 3	83 17 100	M1+E2 E2	26.4266 0.0	3+ 2+
106.155 15	5+		43.84 3 79.74 3	100 32 7	M1+E2 E2	62.330 26.4266	4+ 3+
161.685 24	6+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - K^π=3⁺ 5/2(642)+NU 1/2(631)
86.6738 18	3+
121.645 9	4+		34.97 3 59.31 4 95.22 2 121.69 4	93 13 9.3 15 52 7 100 15	M1 M1 (M1) E2	86.6738 62.330 26.4266 0.0	3+ 4+ 3+ 2+
165.532 15	5+		43.98 4 139.05 2		M1+E2 [E2]	121.645 26.4266	4+ 3+
218.7 6	(6+)		52.98?		M1+E2	165.532	5+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - K^π=3- 5/2(523)+NU 1/2(631)
136.0450 23	3-	6.0 ns
179.154 7	4-		43.11 3 92.486 7 152.69	23 4 100 21 ≤174	M1+E2 E1 (E1)	136.0450 86.6738 26.4266	3- 3+ 3+
232.828 8	5-		53.70 7 96.82 5 111.197 15	20 3 17 3 100 21	M1+E2 E2 [E1]	179.154 136.0450 121.645	4- 3- 4+
297.03 5	(6-)		131.49 8 190.88 5	100 39 22		165.532 106.155	5+ 5+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - K^π=2- 5/2(523)-NU 1/2(631)
182.8775 18	2-
215.522 4	3-		32.67 3 79.483 17 153.192 12 189.099 6 215.517 5	3.2 5 21 4 53 6 54 5 100 5	M1(+E2) E2(+M1) (E1) E1 E1	182.8775 136.0450 62.330 26.4266 0.0	2- 3- 4+ 3+ 2+
258.853 8	4-		43.32 3 75.97 7 122.76 7 152.69 3 196.46 10 232.433 8	1.59 24 2.2 4 6.6 3 ≤114 17 9 100 17	M1+E2 E2 [M1] E1	215.522 182.8775 136.0450 106.155 62.330 26.4266	3- 2- 3- 5+ 4+ 3+
312.704 19	5-		53.88 4 97.22 5 151.07 5 176.62 5 250.36 3	10.0 18 32 4 ≈300 100 18 ≤241	M1+E2 E2	258.853 215.522 161.685 136.0450 62.330	4- 3- 6+ 3- 4+
376.70 7	(6-)		117.8 6 270.55 6			258.853 106.155	4- 5+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - K^π=5⁺ 5/2(642)+NU 5/2(622)
275.519 9	5+
328.6 5	6+		163.25 2 ?			165.532	5+
389.4 5	7+		113.7 6 170.50 1			275.519 218.7	5+ (6+)
456.3 7	(8+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - K^π=0- 1/2(530)-NU 1/2(631)
217.949 10	0-
250.39 4	(2)-		223.89 10 250.40 4	100 ≤148	(E1)	26.4266 0.0	3+ 2+
324.314 8	(4)-		108.792 7	100		215.522	3-
325.210 9	1-		107.263 6 142.328 10	100 68 20	M1	217.949 182.8775	0- 2-
380.60 4	(3)-		130.215 12		E2(+M1)	250.39	(2)-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - K^π=0⁺ 1/2(400)-NU 1/2(631)
243.959 4	(1)+
277.641 18	(2)+		251.25 4 277.633 19	61 15 100	E2+(M1)	26.4266 0.0	3+ 2+
298.368 8	3+		54.40 4 236.025 11 271.953 11 298.38 4	0.66 10 100 8 72 5 9.2 10	E2 M1 M1 M1	243.959 62.330 26.4266 0.0	(1)+ 4+ 3+ 2+
395.198 17	(5)+		289.04 8 332.868 16	67 15 100	M1+E2 E2(+M1)	106.155 62.330	5+ 4+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 8 - K^π=1- 1/2(530)+NU 1/2(631)
373.684 14	(1)-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 9 - K^π=6⁺ 5/2(523)+NU 7/2(743)
459.6 6	(6+)
525.3 15	(7+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 10 - K^π=6- 5/2(642)+NU 7/2(743)
300.743 16	(6-)
409.5 5	(8-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 11 - K^π=0- 5/2(523)-NU 5/2(622)
299.788 20	(1)-
352.46 4	(3)-		52.60 5 93.67 5	1.8 5 100		299.788 258.853	(1)- 4-
367.26 3	(2)-		184.38 3	100		182.8775	2-
442.23 3	(4)-		74.975 2			367.26	(2)-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 12 - K^π=0⁺ 5/2(642)-NU 5/2(622)
250.33 3	(1+)
299.23 6	(3+)		237.02 10 272.75 7 299.20 14	100 5 81 18 60 30		62.330 26.4266 0.0	4+ 3+ 2+
374.7 10	(5+)
431.3 6	(4+)
524.2 6	(6+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 13 - K^π=5- 5/2(523)+NU 5/2(622)
342.439 8	5-
407.59 6	6-		132.6 6 174.76 6			275.519 232.828	5+ 5-
484 3	7-

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	2+	2.099 d 2 % β^- = 100	E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=2⁺ 5/2(642)-NU 1/2(631). From α decay. Not seen in (n,γ).
26.4266	3+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=2⁺ 5/2(642)-NU 1/2(631). From α decay. Not seen in (n,γ).
62.330	4+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=2⁺ 5/2(642)-NU 1/2(631). From α decay. Not seen in (n,γ).
86.6738	3+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=3⁺ 5/2(642)+NU 1/2(631). From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits.
106.155	5+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=2⁺ 5/2(642)-NU 1/2(631). From α decay. Not seen in (n,γ).
121.645	4+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=3⁺ 5/2(642)+NU 1/2(631). From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits.
136.0450	3-	6.0 ns	E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=3- 5/2(523)+NU 1/2(631). From (n,γ) one has Eγ=314.31 3 with mult=M1⁺E2 doubly placed from the 497 and 530 levels. Both placements involve Δπ=no.
161.685	6+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=2⁺ 5/2(642)-NU 1/2(631). From α decay. Not seen in (n,γ).
165.532	5+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=3⁺ 5/2(642)+NU 1/2(631). From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits.
179.154	4-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=3- 5/2(523)+NU 1/2(631). From (n,γ) one has Eγ=314.31 3 with mult=M1⁺E2 doubly placed from the 497 and 530 levels. Both placements involve Δπ=no.
182.8775	2-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=2- 5/2(523)-NU 1/2(631). In (n,γ) one has Eγ=417.60 6 with mult=M1 doubly placed from the 418 and 524 levels. Both placements involve Δπ=no.
215.522	3-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=2- 5/2(523)-NU 1/2(631). In (n,γ) one has Eγ=417.60 6 with mult=M1 doubly placed from the 418 and 524 levels. Both placements involve Δπ=no.
217.949	0-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=0- 1/2(530)-NU 1/2(631).
218.7	(6+)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=3⁺ 5/2(642)+NU 1/2(631). From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits.
232.828	5-		E(level): K^π=3- 5/2(523)+NU 1/2(631). From (n,γ) one has Eγ=314.31 3 with mult=M1⁺E2 doubly placed from the 497 and 530 levels. Both placements involve Δπ=no. 1990Ho02 estimate confidence in the evidence for a level configuration as well established.
243.959	(1)+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=0⁺ 1/2(400)-NU 1/2(631).
250.33	(1+)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=0⁺ 5/2(642)-NU 5/2(622).
250.39	(2)-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=0- 1/2(530)-NU 1/2(631).
258.853	4-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=2- 5/2(523)-NU 1/2(631). In (n,γ) one has Eγ=417.60 6 with mult=M1 doubly placed from the 418 and 524 levels. Both placements involve Δπ=no.
275.519	5+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=5⁺ 5/2(642)+NU 5/2(622). In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no.
277.641	(2)+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=0⁺ 1/2(400)-NU 1/2(631).
297.03	(6-)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=3- 5/2(523)+NU 1/2(631). From (n,γ) one has Eγ=314.31 3 with mult=M1⁺E2 doubly placed from the 497 and 530 levels. Both placements involve Δπ=no.
298.368	3+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=0⁺ 1/2(400)-NU 1/2(631).
299.23	(3+)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=0⁺ 5/2(642)-NU 5/2(622).
299.788	(1)-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=0- 5/2(523)-NU 5/2(622). In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level.
E(level)	J^π(level)	T_1/2(level)	Comments
300.743	(6-)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=6- 5/2(642)+NU 7/2(743).
312.704	5-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=2- 5/2(523)-NU 1/2(631). In (n,γ) one has Eγ=417.60 6 with mult=M1 doubly placed from the 418 and 524 levels. Both placements involve Δπ=no.
324.314	(4)-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=0- 1/2(530)-NU 1/2(631).
325.210	1-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=0- 1/2(530)-NU 1/2(631).
328.6	6+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=5⁺ 5/2(642)+NU 5/2(622). In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no.
342.439	5-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=5- 5/2(523)+NU 5/2(622).
352.46	(3)-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=0- 5/2(523)-NU 5/2(622). In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level.
367.26	(2)-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=0- 5/2(523)-NU 5/2(622). In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level.
373.684	(1)-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=1- 1/2(530)+NU 1/2(631).
374.7	(5+)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=0⁺ 5/2(642)-NU 5/2(622).
376.70	(6-)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=2- 5/2(523)-NU 1/2(631). In (n,γ) one has Eγ=417.60 6 with mult=M1 doubly placed from the 418 and 524 levels. Both placements involve Δπ=no.
380.60	(3)-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=0- 1/2(530)-NU 1/2(631).
389.4	7+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=5⁺ 5/2(642)+NU 5/2(622). In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no.
395.198	(5)+		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as speculative. K^π=0⁺ 1/2(400)-NU 1/2(631).
407.59	6-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=5- 5/2(523)+NU 5/2(622).
409.5	(8-)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as speculative. K^π=6- 5/2(642)+NU 7/2(743).
431.3	(4+)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=0⁺ 5/2(642)-NU 5/2(622).
442.23	(4)-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=0- 5/2(523)-NU 5/2(622). In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level.
456.3	(8+)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=5⁺ 5/2(642)+NU 5/2(622). In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no.
459.6	(6+)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=6⁺ 5/2(523)+NU 7/2(743).
484	7-		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as well established. K^π=5- 5/2(523)+NU 5/2(622).
524.2	(6+)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as probable. K^π=0⁺ 5/2(642)-NU 5/2(622).
525.3	(7+)		E(level): 1990Ho02 estimate confidence in the evidence for a level configuration as plausible. K^π=6⁺ 5/2(523)+NU 7/2(743).
2300		112 ns 39 % SF ≤ 100	γ branch from a shape isomer with T_1/2 between 2 μs and 20 ms was searched for its decay by 1974Bo02 in ²³⁸U(p,n) reaction, and no γ could be assigned definitely. E(level): γ branch from a shape isomer with T_1/2 between 2 μs and 20 ms was searched for its decay by 1974Bo02 in ²³⁸U(p,n) reaction, and no γ could be assigned definitely.

E(level)	E(gamma)	Comments
136.0450	109.614	E(γ): Multiply placed with intensity suitably divided. In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no I(γ): Multiply placed with intensity suitably divided. In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no M(γ): In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no
179.154	152.69	E(γ): Multiply placed with undivided intensity. In (n,γ) one has Eγ=152.69 3 with tentative mult=E1 doubly placed from the 179 and 259 levels. The same transition is also seen in α decay with the same placements. Both placements involve Δπ=yes I(γ): Multiply placed with undivided intensity M(γ): In (n,γ) one has Eγ=152.69 3 with tentative mult=E1 doubly placed from the 179 and 259 levels. The same transition is also seen in α decay with the same placements. Both placements involve Δπ=yes
215.522	189.099	I(γ): Iγ/Iγ(216γ)=0.46 11 in α decay
250.33	250.33	E(γ): From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits I(γ): From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits
250.39	250.40	E(γ): From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits I(γ): From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits
258.853	152.69	E(γ): Multiply placed with undivided intensity. In (n,γ) one has Eγ=152.69 3 with tentative mult=E1 doubly placed from the 179 and 259 levels. The same transition is also seen in α decay with the same placements. Both placements involve Δπ=yes I(γ): Multiply placed with undivided intensity M(γ): In (n,γ) one has Eγ=152.69 3 with tentative mult=E1 doubly placed from the 179 and 259 levels. The same transition is also seen in α decay with the same placements. Both placements involve Δπ=yes
258.853	196.46	E(γ): From α decay. Not seen in (n,γ) I(γ): From α decay. Not seen in (n,γ)
300.68	117.2	E(γ): Multiply placed
312.704	250.36	E(γ): From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits I(γ): From (n,γ) one has Eγ=250.40 4 with mult=E1 or E2, doubly placed from the 250.39 and 313 levels, and from α decay one has Eγ=250.33 3 doubly placed from the 250.32 and 313 levels. All placements involve Δπ=yes, except for the 250.39 level. The evaluators adopt a weighted average of 250.36 3 for placement from the 313 level, and the branchings for all placements are upper limits
328.6	163.25	E(γ): In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level I(γ): In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level M(γ): In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level
342.439	109.614	E(γ): Multiply placed with intensity suitably divided. In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no I(γ): Multiply placed with intensity suitably divided. In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no M(γ): In (n,γ) one has Eγ=109.614 4 with mult mainly E1 doubly placed from the 136 and 342 levels. The transition is also seen in α decay. From a comparison of the branchings in (n,γ) and α decay the intensity can be divided between the two placements. Most of the intensity belongs with the 136 level, and mult=E1 can be assigned to this placement. Placement from the 342 level involves Δπ=no
	163.26	E(γ): In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level I(γ): In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level M(γ): In α decay one has Eγ=163.25 2 doubly placed from the 329 and 342 levels. Eγ=163.29 5 is reported in (n,γ) with mult=M1⁺E2, and placed from the 342 level only. From a comparison of branchings from the two sources, all the intensity of the 163γ in α decay can be accounted for by placement from the 342 level
	206.37	E(γ): From α decay. Not seen in (n,γ) I(γ): From α decay. Not seen in (n,γ)
352.46	52.60	M(γ): 1990Ho02 assign mult=E2 in (n,γ), and the placement requires ΔJ=2, Δπ=no; however, the ce ratios suggest an M1 component. One gets δ=1.44 8, 0.27 3, and 0.93 7 from L1/L2, L3/L2, and M1/M2, respectively. M3/M2 gives δ>0.25
417.641	417.60	E(γ): Multiply placed with undivided intensity. In (n,γ) one has Eγ=417.60 6 with mult=M1 doubly placed from the 418 and 524 levels. Both placements involve Δπ=no I(γ): Multiply placed with undivided intensity M(γ): In (n,γ) one has Eγ=417.60 6 with mult=M1 doubly placed from the 418 and 524 levels. Both placements involve Δπ=no
459.6	117.2	E(γ): Multiply placed
497.20	314.31	E(γ): Multiply placed with undivided intensity. From (n,γ) one has Eγ=314.31 3 with mult=M1⁺E2 doubly placed from the 497 and 530 levels. Both placements involve Δπ=no I(γ): Multiply placed with undivided intensity M(γ): From (n,γ) one has Eγ=314.31 3 with mult=M1⁺E2 doubly placed from the 497 and 530 levels. Both placements involve Δπ=no
523.83	417.60	E(γ): Multiply placed with undivided intensity. In (n,γ) one has Eγ=417.60 6 with mult=M1 doubly placed from the 418 and 524 levels. Both placements involve Δπ=no I(γ): Multiply placed with undivided intensity M(γ): In (n,γ) one has Eγ=417.60 6 with mult=M1 doubly placed from the 418 and 524 levels. Both placements involve Δπ=no
529.857	314.31	E(γ): Multiply placed with undivided intensity. From (n,γ) one has Eγ=314.31 3 with mult=M1⁺E2 doubly placed from the 497 and 530 levels. Both placements involve Δπ=no I(γ): Multiply placed with undivided intensity M(γ): From (n,γ) one has Eγ=314.31 3 with mult=M1⁺E2 doubly placed from the 497 and 530 levels. Both placements involve Δπ=no