List of levels for 169TM

Author: M. Shamsuzzoha Basunia | Citation: Nucl. Data Sheets 209, 1 (2026) | Cutoff date: 1-Oct-2025

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
8.41017	3/2+	4.09 ns 6	8.41017 15	M1+E2	0.0323 10	260	B(E2)(W.u.)=237 16, B(M1)(W.u.)=0.0346 11, α=260 7, α(M)=206 6, α(N)=47.6 12, α(O)=6.29 15, α(P)=0.2375 33
118.18945	5/2+	62.4 ps 28	109.77924 4	M1+E2	-0.153 11	2.368	B(E2)(W.u.)=64 10, B(M1)(W.u.)=0.0714 +35-32, α=2.368 33, α(K)=1.961 28, α(L)=0.317 5, α(M)=0.0711 12, α(N)=0.01661 27, α(O)=0.00235 4, α(P)=0.0001200 17
118.18945	5/2+	62.4 ps 28	118.18940 14	E2		1.642	B(E2)(W.u.)=209 10, α=1.642 23, α(K)=0.701 10, α(L)=0.721 10, α(M)=0.1759 25, α(N)=0.0400 6, α(O)=0.00469 7, α(P)=2.95E-5 4
138.93316	7/2+	302 ps 9	20.7439 3	M1+E2	0.0280 15	54.7	B(E2)(W.u.)=38.4 43, B(M1)(W.u.)=0.0455 14, α=54.7 8, α(L)=42.6 7, α(M)=9.55 15, α(N)=2.227 35, α(O)=0.315 5, α(P)=0.01613 23
138.93316	7/2+	302 ps 9	130.52293 6	E2		1.143	B(E2)(W.u.)=287 9, α=1.143 16, α(K)=0.541 8, α(L)=0.462 6, α(M)=0.1124 16, α(N)=0.0256 4, α(O)=0.00302 4, α(P)=2.309E-5 32
316.14633	7/2+	660 ns 3	177.21307 6	M1+E2	-0.30 13	0.594	B(E2)(W.u.)=0.0017 +15-11, B(M1)(W.u.)=1.25E-6 +7-10, α=0.594 18, α(K)=0.490 22, α(L)=0.0809 35, α(M)=0.0182 9, α(N)=0.00425 21, α(O)=0.000598 19, α(P)=2.97E-5 16
	7/2+	660 ns 3	197.95675 7	M1+E2	-0.326 6	0.433	B(E2)(W.u.)=1.80E-3 6, B(M1)(W.u.)=1.430E-6 11, α=0.433 6, α(K)=0.358 5, α(L)=0.0586 8, α(M)=0.01318 19, α(N)=0.00308 4, α(O)=0.000433 6, α(P)=2.161E-5 31
	7/2+	660 ns 3	307.73586 10	E2		0.0662	B(E2)(W.u.)=5.755E-4 40, α=0.0662 9, α(K)=0.0481 7, α(L)=0.01390 19, α(M)=0.00327 5, α(N)=0.000752 11, α(O)=9.58E-5 13, α(P)=2.479E-6 35
332.111	9/2+	18.8 ps 5	193.11 4	M1+E2	-0.126 21	0.479	B(E2)(W.u.)=16 +6-5, B(M1)(W.u.)=0.0791 23, α=0.479 7, α(K)=0.401 6, α(L)=0.0611 9, α(M)=0.01363 19, α(N)=0.00319 5, α(O)=0.000457 6, α(P)=2.446E-5 35
332.111	9/2+	18.8 ps 5	213.935 17	E2		0.2080	B(E2)(W.u.)=270 9, α=0.2080 29, α(K)=0.1348 19, α(L)=0.0563 8, α(M)=0.01347 19, α(N)=0.00308 4, α(O)=0.000378 5, α(P)=6.42E-6 9
345.028	5/2-		206.04 4	E1		0.0497	α=0.0497 7, α(K)=0.0417 6, α(L)=0.00624 9, α(M)=0.001386 19, α(N)=0.000321 4, α(O)=4.41×10^-5 6, α(P)=2.051E-6 29
345.028	5/2-		336.618 3	E1(+M2)	0.66 LE	0.07	α=0.07 6, α(K)=0.06 5, α(L)=0.011 9, α(M)=0.0025 21, α(N)=6.E-4 5, α(O)=8.E-5 7, α(P)=4.E-6 4
367.66	11/2+	41.6 ps 21	228.71 5	E2		0.1673	B(E2)(W.u.)=336 17, α=0.1673 23, α(K)=0.1113 16, α(L)=0.0430 6, α(M)=0.01027 14, α(N)=0.002353 33, α(O)=0.000291 4, α(P)=5.39E-6 8
379.26679	7/2-	50.5 ns 16	63.12044 4	E1		1.098	B(E1)(W.u.)=8.14E-6 +28-26, α=1.098 15, α(K)=0.892 12, α(L)=0.1611 23, α(M)=0.0360 5, α(N)=0.00820 11, α(O)=0.001047 15, α(P)=3.77E-5 5
	7/2-	50.5 ns 16	240.331 3	E1(+M2)	+0.12 LT	0.042	B(E1)(W.u.)=3.84E-10 40, α=0.042 9, α(K)=0.035 7, α(L)=0.0056 14, α(M)=0.00125 33, α(N)=2.9E-4 8, α(O)=4.1E-5 11, α(P)=2.0E-6 5
	7/2-	50.5 ns 16	261.07712 9	E1+M2	-0.07 3	0.032	B(E1)(W.u.)=4.41E-9 15, B(M2)(W.u.)=0.0015 +15-10, α=0.032 5, α(K)=0.026 4, α(L)=0.0041 7, α(M)=0.00091 17, α(N)=0.00021 4, α(O)=3.0E-5 6, α(P)=1.43E-6 29
	7/2-	50.5 ns 16	370.854 8	[M2]		0.300	B(M2)(W.u.)=2.70×10^-5 29, α=0.300 4, α(K)=0.2427 34, α(L)=0.0446 6, α(M)=0.01020 14, α(N)=0.002393 34, α(O)=0.000340 5, α(P)=1.751E-5 25
	7/2-	50.5 ns 16	379.284 18	[E3]		0.1270	B(E3)(W.u.)=0.040 16, α=0.1270 18, α(K)=0.0756 11, α(L)=0.0393 6, α(M)=0.00959 13, α(N)=0.002205 31, α(O)=0.000273 4, α(P)=4.66E-6 7
430.122	(9/2)-		291.188 11	E1		0.02068	α=0.02068 29, α(K)=0.01742 24, α(L)=0.00255 4, α(M)=0.000564 8, α(N)=0.0001309 18, α(O)=1.824×10^-5 26, α(P)=8.89E-7 12
433.513	(9/2)+		117.369 19	[M1,E2]		1.82	α=1.82 14, α(K)=1.2 5, α(L)=0.50 25, α(M)=0.12 6, α(N)=0.027 14, α(O)=0.0033 15, α(P)=6.5×10^-5 35
433.513	(9/2)+		294.54 11	M1		0.1522	α=0.1522 21, α(K)=0.1279 18, α(L)=0.01899 27, α(M)=0.00423 6, α(N)=0.000989 14, α(O)=0.0001424 20, α(P)=7.77×10^-6 11
472.88128	9/2-	0.14 ns 7	93.61447 8	M1+E2	+0.183 3	3.75	B(E2)(W.u.)=6E1 +6-2, B(M1)(W.u.)=0.036 +32-12, α=3.75 5, α(K)=3.07 4, α(L)=0.529 8, α(M)=0.1193 17, α(N)=0.0278 4, α(O)=0.00389 6, α(P)=0.0001883 26
	9/2-	0.14 ns 7	105.19 10	E1		0.292	B(E1)(W.u.)=2.6E-7 +25-11, α=0.292 4, α(K)=0.2421 34, α(L)=0.0389 6, α(M)=0.00867 12, α(N)=0.001990 28, α(O)=0.000265 4, α(P)=1.087E-5 15
	9/2-	0.14 ns 7	141.7 2	[E1]		0.1326	B(E1)(W.u.)=5.7E-5 30, α=0.1326 19, α(K)=0.1107 16, α(L)=0.01714 25, α(M)=0.00381 6, α(N)=0.000878 13, α(O)=0.0001188 17, α(P)=5.18E-6 7
	9/2-	0.14 ns 7	156.724 11	E1		0.1016	B(E1)(W.u.)=3.0E-7 +27-10, α=0.1016 14, α(K)=0.0850 12, α(L)=0.01302 18, α(M)=0.00289 4, α(N)=0.000668 9, α(O)=9.08E-5 13, α(P)=4.04E-6 6
	9/2-	0.14 ns 7	333.963 13	[E1]		0.01480	B(E1)(W.u.)=5.5E-9 +49-19, α=0.01480 21, α(K)=0.01248 17, α(L)=0.001808 25, α(M)=0.000400 6, α(N)=9.29E-5 13, α(O)=1.301E-5 18, α(P)=6.44E-7 9
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
570.834	3/2+	10 ps 6	452.64 7	M1+E2	1.5 +9-4	0.030	B(E2)(W.u.)=2.6 +28-13, B(M1)(W.u.)=0.0005 +6-3, α=0.030 4, α(K)=0.025 4, α(L)=0.0045 4, α(M)=0.00101 8, α(N)=0.000235 18, α(O)=3.23E-5 30, α(P)=1.42E-6 25
	3/2+	10 ps 6	562.410 12	M1+E2	0.8 +5-4	0.022	B(E2)(W.u.)=3.3 +41-23, B(M1)(W.u.)=0.0035 +39-18, α=0.022 4, α(K)=0.0184 34, α(L)=0.0029 4, α(M)=0.00064 8, α(N)=0.000149 19, α(O)=2.12E-5 29, α(P)=1.08E-6 21
	3/2+	10 ps 6	570.890 27	M1+E2	0.8 +5-4	0.021	B(E2)(W.u.)=2.9 +35-20, B(M1)(W.u.)=0.0032 +36-16, α=0.021 4, α(K)=0.0177 32, α(L)=0.0027 4, α(M)=0.00061 8, α(N)=0.000143 18, α(O)=2.03E-5 28, α(P)=1.04E-6 21
588.20	11/2-		115.32 5	(M1+E2)		1.93	α=1.93 13, α(K)=1.2 5, α(L)=0.53 27, α(M)=0.13 7, α(N)=0.029 16, α(O)=0.0036 16, α(P)=7.E-5 4
603.19	(13/2-)		235.1 2	(E1(+M2))		0.048	α=0.048 13, α(K)=0.040 10, α(L)=0.0065 21, α(M)=0.0015 5, α(N)=3.4×10^-4 12, α(O)=4.8E-5 16, α(P)=2.3E-6 8
633.292	5/2+	0.27 ps +33-12	494.357 8	M1		0.0389	B(M1)(W.u.)=0.09 +8-5, α=0.0389 5, α(K)=0.0328 5, α(L)=0.00479 7, α(M)=0.001064 15, α(N)=0.0002490 35, α(O)=3.59×10^-5 5, α(P)=1.972E-6 28
	5/2+	0.27 ps +33-12	515.101 6	M1		0.0350	B(M1)(W.u.)=0.23 +19-12, α=0.0350 5, α(K)=0.0295 4, α(L)=0.00430 6, α(M)=0.000956 13, α(N)=0.0002237 31, α(O)=3.23×10^-5 5, α(P)=1.773E-6 25
	5/2+	0.27 ps +33-12	624.881 4	M1		0.02140	B(M1)(W.u.)=0.15 +13-8, α=0.02140 30, α(K)=0.01805 25, α(L)=0.00262 4, α(M)=0.000580 8, α(N)=0.0001358 19, α(O)=1.960×10^-5 27, α(P)=1.080E-6 15
	5/2+	0.27 ps +33-12	633.32 10	[E2]		0.00959	B(E2)(W.u.)=0.24 +20-12, α=0.00959 13, α(K)=0.00778 11, α(L)=0.001410 20, α(M)=0.000320 4, α(N)=7.44E-5 10, α(O)=1.018E-5 14, α(P)=4.35E-7 6
637.01	13/2+	5.4 ps 3	269.4 1	M1+E2	-0.149 26	0.1916	B(E2)(W.u.)=12.7 +48-41, B(M1)(W.u.)=0.090 6, α=0.1916 28, α(K)=0.1606 24, α(L)=0.02417 34, α(M)=0.00539 8, α(N)=0.001260 18, α(O)=0.0001809 25, α(P)=9.75E-6 15
637.01	13/2+	5.4 ps 3	304.9 1	E2		0.0680	B(E2)(W.u.)=320 +21-18, α=0.0680 10, α(K)=0.0494 7, α(L)=0.01438 20, α(M)=0.00339 5, α(N)=0.000778 11, α(O)=9.91E-5 14, α(P)=2.54E-6 4
690.97	15/2+	8.1 ps 3	87.7 1	(E1)		0.471	B(E1)(W.u.)=0.00371 14, α=0.471 7, α(K)=0.389 6, α(L)=0.0645 9, α(M)=0.01438 21, α(N)=0.00329 5, α(O)=0.000432 6, α(P)=1.701E-5 24
690.97	15/2+	8.1 ps 3	323.4 2	E2		0.0571	B(E2)(W.u.)=291 11, α=0.0571 8, α(K)=0.0420 6, α(L)=0.01162 16, α(M)=0.00273 4, α(N)=0.000628 9, α(O)=8.04E-5 11, α(P)=2.182E-6 31
718.786	(7/2+)		386.671 13	[M1,E2]		0.054	α=0.054 20, α(K)=0.044 18, α(L)=0.0077 14, α(M)=0.00175 29, α(N)=0.00041 7, α(O)=5.6×10^-5 12, α(P)=2.6E-6 12
	(7/2+)		579.851 5	(M1)		0.0259	α=0.0259 4, α(K)=0.02181 31, α(L)=0.00317 4, α(M)=0.000703 10, α(N)=0.0001646 23, α(O)=2.375×10^-5 33, α(P)=1.308E-6 18
	(7/2+)		600.603 8	(M1)		0.02366	α=0.02366 33, α(K)=0.01995 28, α(L)=0.00289 4, α(M)=0.000642 9, α(N)=0.0001503 21, α(O)=2.170×10^-5 30, α(P)=1.195E-6 17
725.46	13/2-		137.26 5	(M1+E2)		1.11	α=1.11 15, α(K)=0.76 29, α(L)=0.26 11, α(M)=0.063 27, α(N)=0.014 6, α(O)=0.0018 6, α(P)=4.2×10^-5 22
865.74	(17/2-)		174.7 2	(E1)		0.0764	α=0.0764 11, α(K)=0.0640 9, α(L)=0.00971 14, α(M)=0.002156 31, α(N)=0.000498 7, α(O)=6.81×10^-5 10, α(P)=3.08E-6 4
865.74	(17/2-)		262.7 5	(E2)		0.1076	α=0.1076 16, α(K)=0.0750 11, α(L)=0.0251 4, α(M)=0.00595 9, α(N)=0.001365 22, α(O)=0.0001710 27, α(P)=3.74×10^-6 6
883.59	15/2-		158.1 3	(M1(+E2))		0.71	α=0.71 13, α(K)=0.51 19, α(L)=0.15 5, α(M)=0.036 12, α(N)=0.0083 27, α(O)=0.00106 26, α(P)=2.9×10^-5 15
1027.66	17/2+	1.91 ps 17	336.64 8	M1+E2	-0.18 3	0.1047	B(E2)(W.u.)=13.5 +49-42, B(M1)(W.u.)=0.102 +11-9, α=0.1047 16, α(K)=0.0879 14, α(L)=0.01314 19, α(M)=0.00293 4, α(N)=0.000685 10, α(O)=9.84E-5 14, α(P)=5.32E-6 8
1027.66	17/2+	1.91 ps 17	390.7 1	E2		0.0331	B(E2)(W.u.)=349 +35-30, α=0.0331 5, α(K)=0.02530 35, α(L)=0.00605 8, α(M)=0.001407 20, α(N)=0.000325 5, α(O)=4.24E-5 6, α(P)=1.355E-6 19
1103.73	19/2+	1.94 ps 21	237.9 2	[E1]		0.0344	B(E1)(W.u.)=1.62E-4 +38-35, α=0.0344 5, α(K)=0.0289 4, α(L)=0.00428 6, α(M)=0.000949 13, α(N)=0.0002198 31, α(O)=3.04E-5 4, α(P)=1.444E-6 20
1103.73	19/2+	1.94 ps 21	412.8 1	E2		0.0285	B(E2)(W.u.)=4.2E2 +5-4, α=0.0285 4, α(K)=0.02193 31, α(L)=0.00505 7, α(M)=0.001170 16, α(N)=0.000270 4, α(O)=3.55E-5 5, α(P)=1.183E-6 17
1497.96	21/2+	0.87 ps 9	394.0 5	M1+E2		0.051	α=0.051 19, α(K)=0.042 17, α(L)=0.0073 14, α(M)=0.00165 28, α(N)=0.00038 7, α(O)=5.3×10^-5 12, α(P)=2.4E-6 11
1497.96	21/2+	0.87 ps 9	469.6 5	E2		0.02015	B(E2)(W.u.)=324 +38-31, α=0.02015 29, α(K)=0.01582 23, α(L)=0.00335 5, α(M)=0.000772 11, α(N)=0.0001786 26, α(O)=2.379E-5 34, α(P)=8.66E-7 12
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data

For hfs and/or isotope-shift data see, e.g., 1985Pf01, 1986Al32, 1986Pf03, 1987Mi31, 1988Al04, 1993Ji03, 1995Kr23, 1997Kr16.

For muonic isomer shift data, see 1974Ba77.

For discussion of anapole moment of ¹⁶⁹Tm, see 1999KaZU.

Muonic atom: 1970Ba74, 1974Ba77, 1974En08

Q-value: S(2n)=14874.2 10, S(2p)=13573 5 (2021Wa16)

Q(β-)=-899.1 keV 8	S(n)= 8033.6 keV 15	S(p)= 5574.4 keV 8	Q(α)= 1198.4 keV 10
Reference: 2021WA16

References:
A	¹⁶⁹Er β^- decay (9.39 d)	B	¹⁶⁹Yb ε decay (32.016 d)
C	¹⁶⁸Er(p,p) IAR	D	¹⁶⁸Er(³He,d),(α,t)
E	¹⁶⁹Tm(γ,γ):MOSSBAUER EFFECT	F	¹⁶⁹Tm(γ,γ’)
G	¹⁶⁹Tm(E,E’p) IAR	H	¹⁶⁹Tm(n,n’γ),(pol n,n)
I	¹⁶⁹Tm(³He,³He’)	J	¹⁶⁹Tm(³²S,³²S’γ)
K	Coulomb Excitation	L	¹⁷⁰Er(p,2nγ),(d,3nγ)

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 F H J K L	1/2+	STABLE
8.41017 15	A B D E F H J K L	3/2+	4.09 ns 6	8.41017 15	100	M1+E2	0.0	1/2+
118.18945 4	A B D F H J K L	5/2+	62.4 ps 28	109.77924 4 118.18940 14	100.0 4 10.78 4	M1+E2 E2	8.41017 0.0	3/2+ 1/2+
138.93316 5	B D H J K L	7/2+	302 ps 9	20.7439 3 130.52293 6	1.73 2 100.0 3	M1+E2 E2	118.18945 8.41017	5/2+ 3/2+
316.14633 5	B D H J L	7/2+	660 ns 3	177.21307 6 197.95675 7 307.73586 10	62.01 21 100 27.96 9	M1+E2 M1+E2 E2	138.93316 118.18945 8.41017	7/2+ 5/2+ 3/2+
332.111 11	B H J K L	9/2+	18.8 ps 5	193.11 4 213.935 17	100.0 45.1 13	M1+E2 E2	138.93316 118.18945	7/2+ 5/2+
341.94 4	D H L	(1/2-)		333.53 5 341.95 5	100 50 55 28		8.41017 0.0	3/2+ 1/2+
345.028 3	B D H L	5/2-		206.04 4 226.79 5 336.618 3	36 9 2.6 13 100 3	E1 E1(+M2)	138.93316 118.18945 8.41017	7/2+ 5/2+ 3/2+
367.66 5	B H J K L	11/2+	41.6 ps 21	228.71 5	100	E2	138.93316	7/2+
379.26679 6	B J L	7/2-	50.5 ns 16	63.12044 4 240.331 3 261.07712 9 370.854 8 379.284 18	100.0 4 0.261 14 3.850 16 0.00202 21 0.00068 26	E1 E1(+M2) E1+M2 [M2] [E3]	316.14633 138.93316 118.18945 8.41017 0.0	7/2+ 7/2+ 5/2+ 3/2+ 1/2+
430.122 11	B D H J L	(9/2)-		84.9 5 ? 291.188 11	20 11 100 9	E1	345.028 138.93316	5/2- 7/2+
433.513 18	B L	(9/2)+		101.41? 117.369 19 294.54 11	<18 100 6 2.4 6	[M1,E2] M1	332.111 316.14633 138.93316	9/2+ 7/2+ 7/2+
472.88128 10	B J L	9/2-	0.14 ns 7	93.61447 8 105.19 10 141.7 2 156.724 11 333.963 13	100.0 6 0.10 3 41 14 0.383 10 0.0675 24	M1+E2 E1 [E1] E1 [E1]	379.26679 367.66 332.111 316.14633 138.93316	7/2- 11/2+ 9/2+ 7/2+ 7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
474.968 9	B D H L	(3/2)-		356.74 5 466.2 2 474.970 9	72 3 10.0 11 100.0 22		118.18945 8.41017 0.0	5/2+ 3/2+ 1/2+
570.834 11	B D H K L	3/2+	10 ps 6	452.64 7 562.410 12 570.890 27	15 5 100.0 21 94 6	M1+E2 M1+E2 M1+E2	118.18945 8.41017 0.0	5/2+ 3/2+ 1/2+
575.38 4	L	(11/2+)		141.85 5 259.23 5	100 10 96 48		433.513 316.14633	(9/2)+ 7/2+
588.20 5	D J L	11/2-		115.32 5 209.0 2	100 3 16 6	(M1+E2)	472.88128 379.26679	9/2- 7/2-
603.19 8	J L	(13/2-)		173.1 1 235.1 2	16 8 100 10	(E1(+M2))	430.122 367.66	(9/2)- 11/2+
633.292 3	B D H K L	5/2+	0.27 ps +33-12	494.357 8 515.101 6 624.881 4 633.32 10	29.9 5 84.7 12 100.0 29 0.140 9	M1 M1 M1 [E2]	138.93316 118.18945 8.41017 0.0	7/2+ 5/2+ 3/2+ 1/2+
637.01 7	J K L	13/2+	5.4 ps 3	269.4 1 304.9 1	98.4 24 100 4	M1+E2 E2	367.66 332.111	11/2+ 9/2+
646.758 10	B D H L	(7/2-)		171.6 5 216.4 2 301.6 2 314.6 2 507.8 3 528.569 10	10 5 5.0 5.6 22 1.2 7 100.0 24		474.968 430.122 345.028 332.111 138.93316 118.18945	(3/2)- (9/2)- 5/2- 9/2+ 7/2+ 5/2+
690.97 9	J K L	15/2+	8.1 ps 3	87.7 1 323.4 2	11.20 12 100.00 24	(E1) E2	603.19 367.66	(13/2-) 11/2+
718.786 4	B H K L	(7/2+)		72.028? 386.671 13 579.851 5 600.603 8 710.354 15	<186 17.4 4 100.0 15 59.1 9 1.77 9	[M1,E2] (M1) (M1)	646.758 332.111 138.93316 118.18945 8.41017	(7/2-) 9/2+ 7/2+ 5/2+ 3/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
725.46 7	J L	13/2-		137.26 5 252.5 2	100 3 23 6	(M1+E2)	588.20 472.88128	11/2- 9/2-
741.23 5	L	(13/2+)		165.8 2 307.74 5	100 9 <57		575.38 433.513	(11/2+) (9/2)+
781.796 5	B D H L	(5/2)+		210.94 5 465.65 6 642.873 9 663.599 7 773.386 14 781.64 8	53 91.2 10 36.5 9 92.3 26 100.0 15 1.44 12		570.834 316.14633 138.93316 118.18945 8.41017 0.0	3/2+ 7/2+ 7/2+ 5/2+ 3/2+ 1/2+
832.39 7	B H L	(9/2+)		464.7 500.27 11 693.46 8	41 24 100 9 98 5		367.66 332.111 138.93316	11/2+ 9/2+ 7/2+
865.74 16	J L	(17/2-)		174.7 2 262.7 5	28 13 100 3	(E1) (E2)	690.97 603.19	15/2+ (13/2-)
878.35 10	B H	(7/2+)		546.16 22 739.42 11 760.24 24	80 22 100 12 45 12		332.111 138.93316 118.18945	9/2+ 7/2+ 5/2+
883.59 17	J L	15/2-		158.1 3 295.4 2	100 6 67 3	(M1(+E2))	725.46 588.20	13/2- 11/2-
884.62 20	D L	(11/2-)		281.7 2 ? 454.5 2 552.0 2 ?	100 10 <198		603.19 430.122 332.111	(13/2-) (9/2)- 9/2+
≈900?	K			≈900?	100		0.0	1/2+
929.60 15	L	(15/2+)		188.7 5 353.9 2	37 21 100 10		741.23 575.38	(13/2+) (11/2+)
938 2	D
964.0 4	L	(11/2+)		595.9 5 632.3 5	100 72 38		367.66 332.111	11/2+ 9/2+
1027.66 10	J K L	17/2+	1.91 ps 17	336.64 8 390.7 1	58.6 9 100 5	M1+E2 E2	690.97 637.01	15/2+ 13/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1039.95 15	L			565.2 2 694.7 2			474.968 345.028	(3/2)- 5/2-
1058.54 21	L			716.6 2	100		341.94	(1/2-)
1063.45 21	J L	17/2-		179.6 2 338.0 4	90 9 100 10		883.59 725.46	15/2- 13/2-
1103.73 13	J K L	19/2+	1.94 ps 21	237.9 2 412.8 1	2.0 4 100.0 4	[E1] E2	865.74 690.97	(17/2-) 15/2+
1112.6 5 ?	L			682.5 5 ?	100		430.122	(9/2)-
1135.93 20	L			790.9 2	100		345.028	5/2-
1140.56 15	L	(17/2+)		210.94 5 399.6 2	<39 100 10		929.60 741.23	(15/2+) (13/2+)
1152 2	D	(11/2-)
1189.09 22	L	(15/2-)		552.0 2 ? 585.9 2	<189 100 10		637.01 603.19	13/2+ (13/2-)
1190 20	K	+		1190 20	100		0.0	1/2+
1218.01 20	J L	(21/2-)		352.3 2	100		865.74	(17/2-)
1223.04 15	L			877.9 2 881.2 2			345.028 341.94	5/2- (1/2-)
1243 2	D
1261.83 23	J L	19/2-		197.7 3 378.5 2	100.0 12 2.9 6		1063.45 883.59	17/2- 15/2-
1300.6 5	L	(15/2+)		609.6 5	100		690.97	15/2+
1372 2	D	1/2+
1372.3 6	L	(19/2+)		442.7 5	100		929.60	(15/2+)
1400 2	D
1482.7 3	J L	21/2-		220.8 3 419.3 2	100 10 65 12		1261.83 1063.45	19/2- 17/2-
1497.96 24	J K L	21/2+	0.87 ps 9	280.1 2 394.0 5 469.6 5	2.3 5 51.4 5 100.0 9	M1+E2 E2	1218.01 1103.73 1027.66	(21/2-) 19/2+ 17/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1510.6 10	F	(1/2,3/2)+		1510.6	100		0.0	1/2+
1515 2	D
1527.5 10	F	(1/2,3/2)+		1527.5	100		0.0	1/2+
1548.4 7 ?	L	(19/2-)		682.5 5 ?	100		865.74	(17/2-)
1598.12 21	J K L	(23/2+)		380.0 2 494.5 2	67 17 100 17		1218.01 1103.73	(21/2-) 19/2+
1625.0 6	L	(21/2+)		484.4 5	100		1140.56	(17/2+)
1658.0 3	J L	(25/2-)		440.0 2	100		1218.01	(21/2-)
1706.5 4	J L	23/2-		223.8 2 445?	100 25		1482.7 1261.83	21/2- 19/2-
1864.6 7	F	(1/2,3/2)+		1856.2 1864.6	100 26 47		8.41017 0.0	3/2+ 1/2+
1910.5 6	F	(1/2,3/2)+		1792.3 1902.1 1910.5	100 10 46 5 98		118.18945 8.41017 0.0	5/2+ 3/2+ 1/2+
1922.3 7	F	(1/2,3/2)+		1804.1 1922.3	100 46 79		118.18945 0.0	5/2+ 1/2+
1957.4 4	J	(25/2+)		359.0? 459.4 2	100 3		1598.12 1497.96	(23/2+) 21/2+
1963.7 10	F	(1/2,3/2)		1963.7	100		0.0	1/2+
1978.4 10	F	(1/2,3/2)		1978.4	100		0.0	1/2+
1991.7 7	F	(1/2,3/2)+		1983.3 1991.7	79 36 100		8.41017 0.0	3/2+ 1/2+
2024.8 4	J	(29/2-)		366.8 2	100		1658.0	(25/2-)
2035.0 3	J	(27/2+)		436.9 2	100		1598.12	(23/2+)
2075.5 7	F	(1/2,3/2)+		2067.1 2075.5	100 74 89		8.41017 0.0	3/2+ 1/2+
2168.7 7	F	(1/2,3/2)+		2160.3 2168.7	100 38 72		8.41017 0.0	3/2+ 1/2+
2190.6 10	F	(1/2,3/2)		2190.6	100		0.0	1/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2215.3 10	F	(1/2,3/2)		2215.3	100		0.0	1/2+
2236.1 7	F	(1/2,3/2)+		2117.9 2236.1	56 16 100		118.18945 0.0	5/2+ 1/2+
2262.5 7	F	(1/2,3/2)+		2144.3 2262.5	100 31 72		118.18945 0.0	5/2+ 1/2+
2293.8 10	F	(1/2,3/2)		2293.8	100		0.0	1/2+
2306.3 10	F	(1/2,3/2)		2306.3	100		0.0	1/2+
2312.2 7	F	(1/2,3/2)+		2194.0 2312.2	100 37 92		118.18945 0.0	5/2+ 1/2+
2386.6 10	F	(1/2,3/2)		2386.6	100		0.0	1/2+
2421.6 4	J	(29/2+)		464.2 2	100		1957.4	(25/2+)
2455.8 7	F	(1/2,3/2)		2447.4 2455.8	43 27 100		8.41017 0.0	3/2+ 1/2+
2466.0 10	F	(1/2,3/2)		2466.0	100		0.0	1/2+
2466.4 4	J	(31/2+)		431.4 2	100		2035.0	(27/2+)
2492.0 7	F	(1/2,3/2)+		2373.8 2492.0	47 13 100		118.18945 0.0	5/2+ 1/2+
2553.4 7	F	(1/2,3/2)		2435.2 2553.4	100 43 64		118.18945 0.0	5/2+ 1/2+
2571.4 10	F	(1/2,3/2)		2571.4	100		0.0	1/2+
2598.6 10	F	(1/2,3/2)+		2598.6	100		0.0	1/2+
2602.8 10	F	(1/2,3/2)		2602.8	100		0.0	1/2+
2687.0 10	F	(1/2,3/2)		2687.0	100		0.0	1/2+
2749.4 7	F	(1/2,3/2)+		2741.0 2749.4	96 41 100		8.41017 0.0	3/2+ 1/2+
2756.4 10	F	(1/2,3/2)		2756.4	100		0.0	1/2+
2769.1 7	F	(1/2,3/2)+		2760.7 2769.1	41 11 100		8.41017 0.0	3/2+ 1/2+
2786.5 10	F	(1/2,3/2)		2786.5	100		0.0	1/2+
2814.2 7	F	(1/2,3/2)		2805.8 2814.2	89 79 100		8.41017 0.0	3/2+ 1/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2818.6 10	F	(1/2,3/2)		2818.6	100		0.0	1/2+
2843.1 10	F	(1/2,3/2)		2843.1	100		0.0	1/2+
2861.1 10	F	(1/2,3/2)+		2861.1	100		0.0	1/2+
2943.3 6	F	(1/2,3/2)+		2825.1 2934.9 2943.3	63 56 100 70 70		118.18945 8.41017 0.0	5/2+ 3/2+ 1/2+
2996.2 7	F	(1/2,3/2)+		2878.0 2996.2	100 26 89		118.18945 0.0	5/2+ 1/2+
3127.6 10	F	(1/2,3/2)		3127.6	100		0.0	1/2+
3175.6 10	F	(1/2,3/2)		3175.6	100		0.0	1/2+
3185.0 10	F	(1/2,3/2)		3185.0	100		0.0	1/2+
3187.5 10	F	(1/2,3/2)		3187.5	100		0.0	1/2+
3191.3 7	F	(1/2,3/2)+		3182.9 3191.3	82 33 100		8.41017 0.0	3/2+ 1/2+
3199.7 10	F	(1/2,3/2)+		3199.7	100		0.0	1/2+
3204.8 7	F	(1/2,3/2)+		3086.6 3204.8	56 19 100		118.18945 0.0	5/2+ 1/2+
3254.6 7	F	(1/2,3/2)		3246.2 3254.6	100 53 69		8.41017 0.0	3/2+ 1/2+
3274.5 10	F	(1/2,3/2)+		3274.5	100		0.0	1/2+
3286.5 10	F	(1/2,3/2)+		3286.5	100		0.0	1/2+
3299.6 7	F	(1/2,3/2)+		3291.2 3299.6	100 75 96		8.41017 0.0	3/2+ 1/2+
3308.4 10	F	(1/2,3/2)		3308.4	100		0.0	1/2+
3341.2 7	F	(1/2,3/2)+		3332.8 3341.2	47 18 100		8.41017 0.0	3/2+ 1/2+
3376.4 7	F	(1/2,3/2)+		3368.0 3376.4	100 33 96		8.41017 0.0	3/2+ 1/2+
3383.9 10	F	(1/2,3/2)		3383.9	100		0.0	1/2+
3419.2 10	F	(1/2,3/2)		3419.2	100		0.0	1/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3436.3 7	F	(1/2,3/2)		3318.1 3436.3	67 43 100		118.18945 0.0	5/2+ 1/2+
3442.0 10	F	(1/2,3/2)		3442.0	100		0.0	1/2+
3458.6 10	F	(1/2,3/2)		3458.6	100		0.0	1/2+
3475.7 7	F	(1/2,3/2)+		3467.3 3475.7	100 41 47		8.41017 0.0	3/2+ 1/2+
3480.3 10	F	(1/2,3/2)		3480.3	100		0.0	1/2+
3497.0 10	F	(1/2,3/2)		3497.0	100		0.0	1/2+
3527.0 7	F	(1/2,3/2)		3518.6 3527.0	100 72 72		8.41017 0.0	3/2+ 1/2+
3538.7 10	F	(1/2,3/2)		3538.7	100		0.0	1/2+
3541.9 7	F	(1/2,3/2)+		3423.7 3541.9	100 42 100		118.18945 0.0	5/2+ 1/2+
3573.3 10	F	(1/2,3/2)		3573.3	100		0.0	1/2+
3613.0 10	F	(1/2,3/2)		3613.0	100		0.0	1/2+
3624.8 6	F	(1/2,3/2)+		3506.6 3616.4 3624.8	100 26 86 23 100		118.18945 8.41017 0.0	5/2+ 3/2+ 1/2+
3724.7 7	F	(1/2,3/2)+		3606.5 3724.7	100 26 100		118.18945 0.0	5/2+ 1/2+
3736.2 10	F	(1/2,3/2)		3736.2	100		0.0	1/2+
3741.7 10	F	(1/2,3/2)		3741.7	100		0.0	1/2+
3766.3 10	F	(1/2,3/2)		3766.3	100		0.0	1/2+
3795.8 7	F	(1/2,3/2)		3787.3 3795.7	1.0E2 13 61		8.41017 0.0	3/2+ 1/2+
3806.7 10	F	(1/2,3/2)		3806.7	100		0.0	1/2+
3862.5 10	F	(1/2,3/2)		3862.5	100		0.0	1/2+
3875.3 10	F	(1/2,3/2)		3875.3	100		0.0	1/2+
3916.8 10	F	(1/2,3/2)		3916.8	100		0.0	1/2+
3950.2 10	F	(1/2,3/2)		3950.2	100		0.0	1/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4103.6 10	F	(1/2,3/2)		4103.5	100		0.0	1/2+
4190.2 7	F	(1/2,3/2)		4181.7 4190.1	1.0E2 10 56		8.41017 0.0	3/2+ 1/2+
4279.7 10	F	(1/2,3/2)		4279.6	100		0.0	1/2+
4764.5 10	F	(1/2,3/2)		4764.4	100		0.0	1/2+
4789.8 10	F	(1/2,3/2)		4789.7	100		0.0	1/2+
4853.0 10	F	(1/2,3/2)		4852.9	100		0.0	1/2+
4865.5 7	F	(1/2,3/2)		4857.0 4865.4	1.0E2 11 69		8.41017 0.0	3/2+ 1/2+
4954.0 10	F	(1/2,3/2)		4953.9	100		0.0	1/2+
5211.5 10	F	(1/2,3/2)+		5211.4	100		0.0	1/2+
5507.1 10	F	(1/2,3/2)		5507	100		0.0	1/2+
5529.9 10	F	(1/2,3/2)+		5529.8	100		0.0	1/2+
5593.3 7	F	(1/2,3/2)		5584.8 5593.2	69 81 100		8.41017 0.0	3/2+ 1/2+
5598.3 10	F	(1/2,3/2)		5598.2	100		0.0	1/2+
1.20E+4 5	I
1.47E+4 3	I
1.576E+4 13	G
16104	C	1/2-
1.634E+4 14	G	(1/2)-

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78
0.0	1/2+	STABLE
118.18945 4	5/2+	62.4 ps 28	109.77924 4 118.18940 14	100.0 4 10.78 4	M1+E2 E2	8.41017 0.0	3/2+ 1/2+
332.111 11	9/2+	18.8 ps 5	193.11 4 213.935 17	100.0 45.1 13	M1+E2 E2	138.93316 118.18945	7/2+ 5/2+
637.01 7	13/2+	5.4 ps 3	269.4 1 304.9 1	98.4 24 100 4	M1+E2 E2	367.66 332.111	11/2+ 9/2+
1027.66 10	17/2+	1.91 ps 17	336.64 8 390.7 1	58.6 9 100 5	M1+E2 E2	690.97 637.01	15/2+ 13/2+
1497.96 24	21/2+	0.87 ps 9	280.1 2 394.0 5 469.6 5	2.3 5 51.4 5 100.0 9	M1+E2 E2	1218.01 1103.73 1027.66	(21/2-) 19/2+ 17/2+
1957.4 4	(25/2+)		359.0? 459.4 2	100 3		1598.12 1497.96	(23/2+) 21/2+
2421.6 4	(29/2+)		464.2 2	100		1957.4	(25/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - 1/2[411], α=-1/2
8.41017 15	3/2+	4.09 ns 6
138.93316 5	7/2+	302 ps 9	20.7439 3 130.52293 6	1.73 2 100.0 3	M1+E2 E2	118.18945 8.41017	5/2+ 3/2+
367.66 5	11/2+	41.6 ps 21	228.71 5	100	E2	138.93316	7/2+
690.97 9	15/2+	8.1 ps 3	87.7 1 323.4 2	11.20 12 100.00 24	(E1) E2	603.19 367.66	(13/2-) 11/2+
1103.73 13	19/2+	1.94 ps 21	237.9 2 412.8 1	2.0 4 100.0 4	[E1] E2	865.74 690.97	(17/2-) 15/2+
1598.12 21	(23/2+)		380.0 2 494.5 2	67 17 100 17		1218.01 1103.73	(21/2-) 19/2+
2035.0 3	(27/2+)		436.9 2	100		1598.12	(23/2+)
2466.4 4	(31/2+)		431.4 2	100		2035.0	(27/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - 7/2[404]. Band parameters: α=13.3, B=-6.7 (7/2, 9/2, 11/2,
316.14633 5	7/2+	660 ns 3
433.513 18	(9/2)+		101.41? 117.369 19 294.54 11	<18 100 6 2.4 6	[M1,E2] M1	332.111 316.14633 138.93316	9/2+ 7/2+ 7/2+
575.38 4	(11/2+)		141.85 5 259.23 5	100 10 96 48		433.513 316.14633	(9/2)+ 7/2+
741.23 5	(13/2+)		165.8 2 307.74 5	100 9 <57		575.38 433.513	(11/2+) (9/2)+
929.60 15	(15/2+)		188.7 5 353.9 2	37 21 100 10		741.23 575.38	(13/2+) (11/2+)
1140.56 15	(17/2+)		210.94 5 399.6 2	<39 100 10		929.60 741.23	(15/2+) (13/2+)
1372.3 6	(19/2+)		442.7 5	100		929.60	(15/2+)
1625.0 6	(21/2+)		484.4 5	100		1140.56	(17/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - 1/2[541], α=+1/2. Band parameters: α=9.1, B=+0.8, a=+3.8
341.94 4	(1/2-)
345.028 3	5/2-		206.04 4 226.79 5 336.618 3	36 9 2.6 13 100 3	E1 E1(+M2)	138.93316 118.18945 8.41017	7/2+ 5/2+ 3/2+
430.122 11	(9/2)-		84.9 5 ? 291.188 11	20 11 100 9	E1	345.028 138.93316	5/2- 7/2+
603.19 8	(13/2-)		173.1 1 235.1 2	16 8 100 10	(E1(+M2))	430.122 367.66	(9/2)- 11/2+
865.74 16	(17/2-)		174.7 2 262.7 5	28 13 100 3	(E1) (E2)	690.97 603.19	15/2+ (13/2-)
1218.01 20	(21/2-)		352.3 2	100		865.74	(17/2-)
1658.0 3	(25/2-)		440.0 2	100		1218.01	(21/2-)
2024.8 4	(29/2-)		366.8 2	100		1658.0	(25/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - 1/2[541], α=-1/2. See comment on signature partner band.
474.968 9	(3/2)-
646.758 10	(7/2-)		171.6 5 216.4 2 301.6 2 314.6 2 507.8 3 528.569 10	10 5 5.0 5.6 22 1.2 7 100.0 24		474.968 430.122 345.028 332.111 138.93316 118.18945	(3/2)- (9/2)- 5/2- 9/2+ 7/2+ 5/2+
884.62 20	(11/2-)		281.7 2 ? 454.5 2 552.0 2 ?	100 10 <198		603.19 430.122 332.111	(13/2-) (9/2)- 9/2+
1189.09 22	(15/2-)		552.0 2 ? 585.9 2	<189 100 10		637.01 603.19	13/2+ (13/2-)
1548.4 7	(19/2-)		682.5 5 ?	100		865.74	(17/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - 7/2[523], α=-1/2. Band parameters: α=10.3, B=3.7 (7/2, 9/2,
379.26679 6	7/2-	50.5 ns 16
588.20 5	11/2-		115.32 5 209.0 2	100 3 16 6	(M1+E2)	472.88128 379.26679	9/2- 7/2-
883.59 17	15/2-		158.1 3 295.4 2	100 6 67 3	(M1(+E2))	725.46 588.20	13/2- 11/2-
1261.83 23	19/2-		197.7 3 378.5 2	100.0 12 2.9 6		1063.45 883.59	17/2- 15/2-
1706.5 4	23/2-		223.8 2 445?	100 25		1482.7 1261.83	21/2- 19/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - 7/2[523], α=+1/2.
472.88128 10	9/2-	0.14 ns 7
725.46 7	13/2-		137.26 5 252.5 2	100 3 23 6	(M1+E2)	588.20 472.88128	11/2- 9/2-
1063.45 21	17/2-		179.6 2 338.0 4	90 9 100 10		883.59 725.46	15/2- 13/2-
1482.7 3	21/2-		220.8 3 419.3 2	100 10 65 12		1261.83 1063.45	19/2- 17/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 8 - 3/2[411] + 1/2[411] γ vibration. Band parameters: α=12.6,
570.834 11	3/2+	10 ps 6
633.292 3	5/2+	0.27 ps +33-12	494.357 8 515.101 6 624.881 4 633.32 10	29.9 5 84.7 12 100.0 29 0.140 9	M1 M1 M1 [E2]	138.93316 118.18945 8.41017 0.0	7/2+ 5/2+ 3/2+ 1/2+
718.786 4	(7/2+)		72.028? 386.671 13 579.851 5 600.603 8 710.354 15	<186 17.4 4 100.0 15 59.1 9 1.77 9	[M1,E2] (M1) (M1)	646.758 332.111 138.93316 118.18945 8.41017	(7/2-) 9/2+ 7/2+ 5/2+ 3/2+
832.39 7	(9/2+)		464.7 500.27 11 693.46 8	41 24 100 9 98 5		367.66 332.111 138.93316	11/2+ 9/2+ 7/2+
964.0 4	(11/2+)		595.9 5 632.3 5	100 72 38		367.66 332.111	11/2+ 9/2+
1300.6 5	(15/2+)		609.6 5	100		690.97	15/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 9 - 5/2[402]. Band parameter: α=13.8 (5/2, 7/2 levels).
781.796 5	(5/2)+
878.35 10	(7/2+)		546.16 22 739.42 11 760.24 24	80 22 100 12 45 12		332.111 138.93316 118.18945	9/2+ 7/2+ 5/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 10 - 9/2[514].
1152 2	(11/2-)

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1/2+	STABLE	μ=-0.2310 15 No α decay observed (T_1/2(α)>5×10¹⁶ y if 1.5\|<E(α)\|<3.7, 1956Po16). E(level): No α decay observed (T_1/2(α)>5×10¹⁶ y if 1.5\|<E(α)\|<3.7, 1956Po16). From ¹⁷⁰Er(p,2nγ), (d,3nγ). 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78. No α decay observed (T_{1/2(α)>5×10¹⁶ y if 1.5\|<E(α)\|<3.7, 1956Po16). E(level): No α decay observed (T_{1/2(α)>5×10¹⁶ y if 1.5\|<E(α)\|<3.7, 1956Po16). From ¹⁷⁰Er(p,2nγ), (d,3nγ). 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78.}}
8.41017	3/2+	4.09 ns 6	Q=-1.2 1, μ=+0.513 5 <r²>^1/2(charge)=0.019 fm 10 (from r²=(0.36 fm² 12) × 10^-3) (1967Sc42). E(level): <r²>^1/2(charge)=0.019 fm 10 (from r²=(0.36 fm² 12) × 10^-3) (1967Sc42). 1/2[411], α=-1/2.
118.18945	5/2+	62.4 ps 28	μ=+0.74 5 E(level): 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78. J^π(level): Definite Jπ for g.s. band established from intraband M1⁺E2 and E2 transitions.
138.93316	7/2+	302 ps 9	μ=+1.32 7 E(level): 1/2[411], α=-1/2. J^π(level): Definite Jπ for g.s. band established from intraband M1⁺E2 and E2 transitions.
316.14633	7/2+	660 ns 3	μ=+0.156 8 E(level): From (³²S,³²S’). 7/2[404]. Band parameters: α=13.3, B=-6.7 (7/2, 9/2, 11/2,.
332.111	9/2+	18.8 ps 5	μ=1.56 9 (1999Ro03,2020StZV) E(level): 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78. J^π(level): Definite Jπ for g.s. band established from intraband M1⁺E2 and E2 transitions.
341.94	(1/2-)		E(level): From (³²S,³²S’). 1/2[541], α=+1/2. Band parameters: α=9.1, B=+0.8, a=+3.8.
345.028	5/2-		E(level): From (³²S,³²S’). 1/2[541], α=+1/2. Band parameters: α=9.1, B=+0.8, a=+3.8.
367.66	11/2+	41.6 ps 21	μ=2.28 14 (1999Ro03,2020StZV) E(level): 1/2[411], α=-1/2. J^π(level): Definite Jπ for g.s. band established from intraband M1⁺E2 and E2 transitions.
379.26679	7/2-	50.5 ns 16	μ=+3.04 14 (1997De02,2020StZV) E(level): From (³²S,³²S’). 7/2[523], α=-1/2. Band parameters: α=10.3, B=3.7 (7/2, 9/2,.
430.122	(9/2)-		E(level): From (³²S,³²S’). 1/2[541], α=+1/2. Band parameters: α=9.1, B=+0.8, a=+3.8.
433.513	(9/2)+		E(level): From (³²S,³²S’). 7/2[404]. Band parameters: α=13.3, B=-6.7 (7/2, 9/2, 11/2,.
472.88128	9/2-	0.14 ns 7	E(level): 7/2[523], α=+1/2.
474.968	(3/2)-		E(level): 1/2[541], α=-1/2. See comment on signature partner band.
570.834	3/2+	10 ps 6	E(level): 3/2[411] + 1/2[411] γ vibration. Band parameters: α=12.6,.
575.38	(11/2+)		E(level): From (³²S,³²S’). 7/2[404]. Band parameters: α=13.3, B=-6.7 (7/2, 9/2, 11/2,.
588.20	11/2-		E(level): From (³²S,³²S’). 7/2[523], α=-1/2. Band parameters: α=10.3, B=3.7 (7/2, 9/2,.
603.19	(13/2-)		E(level): From (³²S,³²S’). 1/2[541], α=+1/2. Band parameters: α=9.1, B=+0.8, a=+3.8.
633.292	5/2+	0.27 ps +33-12	E(level): 3/2[411] + 1/2[411] γ vibration. Band parameters: α=12.6,.
637.01	13/2+	5.4 ps 3	μ=2.37 14 (1999Ro03,2020StZV) E(level): 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78. From ¹⁷⁰Er(p,2nγ), (d,3nγ). J^π(level): Definite Jπ for g.s. band established from intraband M1⁺E2 and E2 transitions. Based on coincidence data, rotational structure, and γ-ray angular distributions in ¹⁷⁰Er(p,2nγ), (d,3nγ), except where noted. Definite Jπ is assigned to members of bands defined by a cascade of transitions having regularly changing energies provided the Jπ of at least one member and the multipolarity of at least one intraband transition have been independently determined.
646.758	(7/2-)		E(level): 1/2[541], α=-1/2. See comment on signature partner band.
690.97	15/2+	8.1 ps 3	μ=3.2 3 (1999Ro03,2020StZV) E(level): 1/2[411], α=-1/2. J^π(level): Definite Jπ for g.s. band established from intraband M1⁺E2 and E2 transitions.
718.786	(7/2+)		E(level): 3/2[411] + 1/2[411] γ vibration. Band parameters: α=12.6,.
725.46	13/2-		E(level): 7/2[523], α=+1/2.
741.23	(13/2+)		E(level): From (³²S,³²S’). 7/2[404]. Band parameters: α=13.3, B=-6.7 (7/2, 9/2, 11/2,.
E(level)	J^π(level)	T_1/2(level)	Comments
781.796	(5/2)+		XREF: d(785). E(level): 5/2[402]. Band parameter: α=13.8 (5/2, 7/2 levels).
832.39	(9/2+)		E(level): 3/2[411] + 1/2[411] γ vibration. Band parameters: α=12.6,.
865.74	(17/2-)		E(level): From (³²S,³²S’). 1/2[541], α=+1/2. Band parameters: α=9.1, B=+0.8, a=+3.8.
878.35	(7/2+)		E(level): 5/2[402]. Band parameter: α=13.8 (5/2, 7/2 levels).
883.59	15/2-		E(level): From (³²S,³²S’). 7/2[523], α=-1/2. Band parameters: α=10.3, B=3.7 (7/2, 9/2,.
884.62	(11/2-)		E(level): 1/2[541], α=-1/2. See comment on signature partner band.
929.60	(15/2+)		E(level): From (³²S,³²S’). 7/2[404]. Band parameters: α=13.3, B=-6.7 (7/2, 9/2, 11/2,.
964.0	(11/2+)		E(level): 3/2[411] + 1/2[411] γ vibration. Band parameters: α=12.6,.
1027.66	17/2+	1.91 ps 17	μ=3.2 3 (1999Ro03,2020StZV) E(level): 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78. From ¹⁷⁰Er(p,2nγ), (d,3nγ). J^π(level): Definite Jπ for g.s. band established from intraband M1⁺E2 and E2 transitions. Based on coincidence data, rotational structure, and γ-ray angular distributions in ¹⁷⁰Er(p,2nγ), (d,3nγ), except where noted. Definite Jπ is assigned to members of bands defined by a cascade of transitions having regularly changing energies provided the Jπ of at least one member and the multipolarity of at least one intraband transition have been independently determined.
1063.45	17/2-		E(level): 7/2[523], α=+1/2.
1103.73	19/2+	1.94 ps 21	μ=4.2 8 (1999Ro03,2020StZV) E(level): 1/2[411], α=-1/2. J^π(level): Definite Jπ for g.s. band established from intraband M1⁺E2 and E2 transitions.
1140.56	(17/2+)		E(level): From (³²S,³²S’). 7/2[404]. Band parameters: α=13.3, B=-6.7 (7/2, 9/2, 11/2,.
1152	(11/2-)		E(level): From ¹⁷⁰Er(p,2nγ), (d,3nγ). 9/2[514].
1189.09	(15/2-)		E(level): 1/2[541], α=-1/2. See comment on signature partner band.
1190	+		B(E2)=0.040 9 B(E2)\|^ from Coulomb excitation. E(level): B(E2)\|^ from Coulomb excitation.
1218.01	(21/2-)		E(level): From (³²S,³²S’). 1/2[541], α=+1/2. Band parameters: α=9.1, B=+0.8, a=+3.8.
1261.83	19/2-		E(level): From (³²S,³²S’). 7/2[523], α=-1/2. Band parameters: α=10.3, B=3.7 (7/2, 9/2,.
1300.6	(15/2+)		E(level): 3/2[411] + 1/2[411] γ vibration. Band parameters: α=12.6,.
1372.3	(19/2+)		E(level): From (³²S,³²S’). 7/2[404]. Band parameters: α=13.3, B=-6.7 (7/2, 9/2, 11/2,.
1482.7	21/2-		E(level): 7/2[523], α=+1/2.
1497.96	21/2+	0.87 ps 9	E(level): 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78. From ¹⁷⁰Er(p,2nγ), (d,3nγ). J^π(level): Definite Jπ for g.s. band established from intraband M1⁺E2 and E2 transitions. Based on coincidence data, rotational structure, and γ-ray angular distributions in ¹⁷⁰Er(p,2nγ), (d,3nγ), except where noted. Definite Jπ is assigned to members of bands defined by a cascade of transitions having regularly changing energies provided the Jπ of at least one member and the multipolarity of at least one intraband transition have been independently determined.
1510.6	(1/2,3/2)+		B(M1,E1)\|^(W.u.)=0.078 18. E(level): B(M1,E1)\|^(W.u.)=0.078 18. From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
1527.5	(1/2,3/2)+		B(M1,E1)\|^(W.u.)=0.050 17. E(level): B(M1,E1)\|^(W.u.)=0.050 17. From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
1548.4	(19/2-)		E(level): 1/2[541], α=-1/2. See comment on signature partner band.
1598.12	(23/2+)		E(level): 1/2[411], α=-1/2.
E(level)	J^π(level)	T_1/2(level)	Comments
1625.0	(21/2+)		E(level): From (³²S,³²S’). 7/2[404]. Band parameters: α=13.3, B=-6.7 (7/2, 9/2, 11/2,.
1658.0	(25/2-)		E(level): From (³²S,³²S’). 1/2[541], α=+1/2. Band parameters: α=9.1, B=+0.8, a=+3.8.
1706.5	23/2-		E(level): From (³²S,³²S’). 7/2[523], α=-1/2. Band parameters: α=10.3, B=3.7 (7/2, 9/2,.
1864.6	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
1910.5	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
1922.3	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
1957.4	(25/2+)		E(level): From ¹⁷⁰Er(p,2nγ), (d,3nγ). 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78.
1963.7	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
1978.4	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
1991.7	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2024.8	(29/2-)		E(level): From (³²S,³²S’). 1/2[541], α=+1/2. Band parameters: α=9.1, B=+0.8, a=+3.8.
2035.0	(27/2+)		E(level): 1/2[411], α=-1/2.
2075.5	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2168.7	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2190.6	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2215.3	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2236.1	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2262.5	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2293.8	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2306.3	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2312.2	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2386.6	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2421.6	(29/2+)		E(level): From ¹⁷⁰Er(p,2nγ), (d,3nγ). 1/2[411], α=+1/2. Band parameters: α=12.5, B=-4.8, a=-0.78.
2455.8	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2466.0	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
E(level)	J^π(level)	T_1/2(level)	Comments
2466.4	(31/2+)		E(level): 1/2[411], α=-1/2.
2492.0	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2553.4	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2571.4	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2598.6	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2602.8	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2687.0	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2749.4	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2756.4	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2769.1	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2786.5	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2814.2	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2818.6	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2843.1	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2861.1	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2943.3	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
2996.2	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3127.6	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3175.6	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3185.0	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3187.5	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3191.3	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3199.7	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3204.8	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3254.6	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
E(level)	J^π(level)	T_1/2(level)	Comments
3274.5	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3286.5	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3299.6	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3308.4	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3341.2	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3376.4	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3383.9	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3419.2	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3436.3	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3442.0	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3458.6	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3475.7	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3480.3	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3497.0	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3527.0	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3538.7	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3541.9	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3573.3	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3613.0	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3624.8	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3724.7	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3736.2	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3741.7	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3766.3	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3795.8	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
E(level)	J^π(level)	T_1/2(level)	Comments
3806.7	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3862.5	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3875.3	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3916.8	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
3950.2	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
4103.6	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
4190.2	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
4279.7	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
4764.5	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
4789.8	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
4853.0	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
4865.5	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
4954.0	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
5211.5	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
5507.1	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
5529.9	(1/2,3/2)+		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
5593.3	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
5598.3	(1/2,3/2)		E(level): From ¹⁶⁹Tm(γ,γ’). From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL. J^π(level): From ¹⁶⁹Tm(γ,γ’). d excitation from 1/2⁺ is assumed by 1999Hu01 in (γ,γ’) so J=(1/2,3/2) is assigned; further, π=+ is assigned whenever B(E1)(W.u.) significantly exceeds RUL.
1.20E+4			Γ=6.2×10³ keV, dσ/d\|W(25\|’)=2.5 mb/sr 10 (1975Ho05) from (³He,³He’). E(level): Γ=6.2×10³ keV, dσ/d\|W(25\|’)=2.5 mb/sr 10 (1975Ho05) from (³He,³He’).