List of levels for 169TM

ADOPTED LEVELS, GAMMAS for ¹⁶⁹Tm

Author: Coral M. Baglin | Citation: Nucl. Data Sheets 109, 2033 (2008) | Cutoff date: 15-Jun-2008

Full ENSDF file | Adopted Levels (PDF version)

Q(β-)=-898.5 keV 12	S(n)= 8033.6 keV 15	S(p)= 5573.9 keV 12	Q(α)= 1197.7 keV 13
Reference: 2012WA38

References:
A	¹⁶⁹Er β^- decay	B	¹⁶⁹Yb ε decay (32.018 d)
C	¹⁶⁸Er(p,p) IAR	D	¹⁶⁸Er(³He,d), (α,t)
E	¹⁶⁹Tm(γ,γ):MOSSBAUER EFFECT	F	¹⁶⁹Tm(E,E’p) IAR
G	Coulomb Excitation	H	¹⁷⁰Er(p,2nγ), (d,3nγ)
I	¹⁶⁹Tm(γ,γ’)	J	¹⁶⁹Tm(n,n’γ), (pol n,n)
K	¹⁶⁹Tm(³He,³He’)	L	muonic atom

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.

Levels: band(c) 1/2[541], α=-1/2 band. See comment on signature partner band.

Q-value: Note: Current evaluation has used the following Q record -910 48033.6 155572.2 111199.7 13 2003Au03

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 G H J	1/2+	STABLE
8.41017 11	A B D E G H J	3/2+	4.09 ns 5	8.41017 15	100	M1+E2	0.0	1/2+
118.18945 11	A B D G H J	5/2+	62 ps 3	109.77924 3 118.18940 14	100.0 4 10.78 4	M1+E2 E2	8.41017 0.0	3/2+ 1/2+
138.93315 12	B D G H J	7/2+	302 ps 2	20.752 9 130.52293 6	1.73 2 100.0 3	M1+E2 E2	118.18945 8.41017	5/2+ 3/2+
316.14633 11	B D H J	7/2+	659.9 ns 23	177.21307 6 197.95675 7 307.73586 10	62.01 21 100 27.96 9	M1+E2 M1+E2 E2	138.93315 118.18945 8.41017	7/2+ 5/2+ 3/2+
332.116 11	B G H J	9/2+	18.8 ps 5	193.15 5 213.935 17	100.0 45.9 10	M1+E2 E2	138.93315 118.18945	7/2+ 5/2+
341.94 4	D H J	(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 J	5/2-		205.99 6 226.3 7 336.618 3	36 9 2.7 19 100 3	E1 E1(+M2)	138.93315 118.18945 8.41017	7/2+ 5/2+ 3/2+
367.67 5	B G H J	11/2+	41.6 ps 21	228.71 5	100	E2	138.93315	7/2+
379.26678 12	B H	7/2-	52.2 ns 8	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 138.93315 118.18945 8.41017 0.0	7/2+ 7/2+ 5/2+ 3/2+ 1/2+
430.122 11	B D H J	(9/2)-		84.9 5 ? 291.188 11	20 11 100 9	E1	345.028 138.93315	5/2- 7/2+
433.521 18	B H	(9/2)+		101.41? 117.376 19 294.54 11	<18 100 6 2.4 6	[M1,E2] M1	332.116 316.14633 138.93315	9/2+ 7/2+ 7/2+
472.88128 14	B H	9/2-	0.14 ns 7	93.61447 8 105.19 10 156.724 11 333.963 13	100.0 6 0.10 3 0.383 10 0.0675 24	M1+E2 E1 E1 [E1]	379.26678 367.67 316.14633 138.93315	7/2- 11/2+ 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 J	(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+
570.830 11	B D G H J	3/2+	10 ps 7	452.62 8 562.410 12 570.89 3	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	H	(11/2+)		141.85 5 259.23 5	100 10 96 48		433.521 316.14633	(9/2)+ 7/2+
588.20 5	D H	11/2-		115.32 5 208.8 5	100 10 10 5	(M1+E2)	472.88128 379.26678	9/2- 7/2-
602.82 19	H	(13/2-)		172.7 5 235.1 2	16 8 100 10	(E1(+M2))	430.122 367.67	(9/2)- 11/2+
633.292 3	B D G H J	5/2+	0.27 ps	494.357 8 515.101 6 624.881 4 633.32 10	29.8 5 84.5 12 100.0 25 0.140 9	M1 M1 M1 [E2]	138.93315 118.18945 8.41017 0.0	7/2+ 5/2+ 3/2+ 1/2+
637.08 13	G H	13/2+	5.4 ps 4	269.4 2 305.2 2	98.4 24 100	M1+E2 E2	367.67 332.116	11/2+ 9/2+
646.758 10	B D H J	(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		474.968 430.122 345.028 332.116 138.93315 118.18945	(3/2)- (9/2)- 5/2- 9/2+ 7/2+ 5/2+
691.24 16	G H	15/2+	8.1 ps 4	323.4 2	100	E2	367.67	11/2+
718.786 4	B G H J	(7/2+)		72.028? 386.671 13 579.851 5 600.603 8 710.354 15	<186 17.4 4 100.0 17 59.1 9 1.77 9	[M1,E2] (M1) (M1)	646.758 332.116 138.93315 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
725.44 7	H	13/2-		137.26 5 252.5 2	100 10 29 3	(M1+E2)	588.20 472.88128	11/2- 9/2-
741.25 6	H	(13/2+)		165.8 2 307.74 5	100 9 <57		575.38 433.521	(11/2+) (9/2)+
781.796 6	B D H J	(5/2)+		210.94 5 465.65 642.873 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		570.830 316.14633 138.93315 118.18945 8.41017 0.0	3/2+ 7/2+ 7/2+ 5/2+ 3/2+ 1/2+
832.42 7	B H J	(9/2+)		464.7 500.35 10 693.46 8	41 24 100 9 98 5		367.67 332.116 138.93315	11/2+ 9/2+ 7/2+
865.9 4	H	(17/2-)		175.0 5 262.7 5	41 22 100 16		691.24 602.82	15/2+ (13/2-)
878.35 10	B J	(7/2+)		546.16 22 739.42 11 760.24 24	80 22 100 12 45 12		332.116 138.93315 118.18945	9/2+ 7/2+ 5/2+
883.75 14	H	15/2-		158.3 2 295.4 2	100 10 <78	(M1(+E2))	725.44 588.20	13/2- 11/2-
884.62 20	D H	(11/2-)		281.7 2 ? 454.5 2 552.0 2 ?	36 21 100		602.82 430.122 332.116	(13/2-) (9/2)- 9/2+
≈900?	G			≈900?	100		0.0	1/2+
929.37 19	H	(15/2+)		188.7 5 353.9 2	37 21 100 10		741.25 575.38	(13/2+) (11/2+)
938 2	D
964.0 4	H	(11/2+)		595.9 5 632.3 5	100 72 38		367.67 332.116	11/2+ 9/2+
1027.85 16	G H	17/2+	1.91 ps 18	336.60 5 391.0 2	58.7 7 100	M1+E2 E2	691.24 637.08	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	H			565.2 2 694.7 2	37 100		474.968 345.028	(3/2)- 5/2-
1058.54 21	H			716.6 2	100		341.94	(1/2-)
1063.57 16	H	17/2-		179.6 2 338.3 2	90 9 100 10		883.75 725.44	15/2- 13/2-
1104.18 25	G H	19/2+	1.94 ps 21	413.0 2	100	E2	691.24	15/2+
1112.6 5 ?	H			682.5 5 ?	100		430.122	(9/2)-
1135.93 20	H			790.9 2	100		345.028	5/2-
1140.85 21	H	(17/2+)		210.94 5 399.6 2	<39 100		929.37 741.25	(15/2+) (13/2+)
1152 2	D	(11/2-)
1188.7 3	H	(15/2-)		552.0 2 ? 585.9 2	<189 100 10		637.08 602.82	13/2+ (13/2-)
1190 20	G	+		1190 20	100		0.0	1/2+
1218.1 5	H	(21/2-)		352.2 2	100		865.9	(17/2-)
1223.04 15	H			877.9 2 881.2 2	100 75		345.028 341.94	5/2- (1/2-)
1243 2	D
1262.40 21	H	19/2-		198.3 5 378.7 2	<185 100		1063.57 883.75	17/2- 15/2-
1300.8 6	H	(15/2+)		609.6 5	100		691.24	15/2+
1372 2	D	1/2+
1372.1 6	H	(19/2+)		442.7 5	100		929.37	(15/2+)
1400 2	D
1482.94 22	H	21/2-		220.5 2 419.4 2	100 10 77 8		1262.40 1063.57	19/2- 17/2-
1497.8 4	G H	21/2+	0.87 ps 9	394.0 5 469.6 5	34 13 100 50	E2	1104.18 1027.85	19/2+ 17/2+
1510.6 10	I	(1/2,3/2)+		1510.6	100		0.0	1/2+
1515 2	D
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1527.5 10	I	(1/2,3/2)+		1527.5	100		0.0	1/2+
1548.4 7 ?	H	(19/2-)		682.5 5 ?	100		865.9	(17/2-)
1598.4 4 ?	G H	(23/2+)		494.2 2 ?	100		1104.18	19/2+
1625.3 6	H	(21/2+)		484.4 5	100		1140.85	(17/2+)
1658.1 5	H	(25/2-)		440.0 2	100		1218.1	(21/2-)
1716.9 3	H	23/2-		233? 454.5 2			1482.94 1262.40	21/2- 19/2-
1864.6 7	I	(1/2,3/2)+		1856.2 1864.6	100 26 47		8.41017 0.0	3/2+ 1/2+
1910.5 6	I	(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	I	(1/2,3/2)+		1804.1 1922.3	100 46 79		118.18945 0.0	5/2+ 1/2+
1963.7 10	I	(1/2,3/2)		1963.7	100		0.0	1/2+
1978.4 10	I	(1/2,3/2)		1978.4	100		0.0	1/2+
1991.7 7	I	(1/2,3/2)+		1983.3 1991.7	79 36 100		8.41017 0.0	3/2+ 1/2+
2075.5 7	I	(1/2,3/2)+		2067.1 2075.5	100 74 89		8.41017 0.0	3/2+ 1/2+
2168.7 7	I	(1/2,3/2)+		2160.3 2168.7	100 38 72		8.41017 0.0	3/2+ 1/2+
2190.6 10	I	(1/2,3/2)		2190.6	100		0.0	1/2+
2215.3 10	I	(1/2,3/2)		2215.3	100		0.0	1/2+
2236.1 7	I	(1/2,3/2)+		2117.9 2236.1	56 16 100		118.18945 0.0	5/2+ 1/2+
2262.5 7	I	(1/2,3/2)+		2144.3 2262.5	100 31 72		118.18945 0.0	5/2+ 1/2+
2293.8 10	I	(1/2,3/2)		2293.8	100		0.0	1/2+
2306.3 10	I	(1/2,3/2)		2306.3	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
2312.2 7	I	(1/2,3/2)+		2194.0 2312.2	100 37 92		118.18945 0.0	5/2+ 1/2+
2386.6 10	I	(1/2,3/2)		2386.6	100		0.0	1/2+
2455.8 7	I	(1/2,3/2)		2447.4 2455.8	43 27 100		8.41017 0.0	3/2+ 1/2+
2466.0 10	I	(1/2,3/2)		2466.0	100		0.0	1/2+
2492.0 7	I	(1/2,3/2)+		2373.8 2492.0	47 13 100		118.18945 0.0	5/2+ 1/2+
2553.4 7	I	(1/2,3/2)		2435.2 2553.4	100 43 64		118.18945 0.0	5/2+ 1/2+
2571.4 10	I	(1/2,3/2)		2571.4	100		0.0	1/2+
2598.6 10	I	(1/2,3/2)+		2598.6	100		0.0	1/2+
2602.8 10	I	(1/2,3/2)		2602.8	100		0.0	1/2+
2687.0 10	I	(1/2,3/2)		2687.0	100		0.0	1/2+
2749.4 7	I	(1/2,3/2)+		2741.0 2749.4	96 41 100		8.41017 0.0	3/2+ 1/2+
2756.4 10	I	(1/2,3/2)		2756.4	100		0.0	1/2+
2769.1 7	I	(1/2,3/2)+		2760.7 2769.1	41 11 100		8.41017 0.0	3/2+ 1/2+
2786.5 10	I	(1/2,3/2)		2786.5	100		0.0	1/2+
2814.2 7	I	(1/2,3/2)		2805.8 2814.2	89 79 100		8.41017 0.0	3/2+ 1/2+
2818.6 10	I	(1/2,3/2)		2818.6	100		0.0	1/2+
2843.1 10	I	(1/2,3/2)		2843.1	100		0.0	1/2+
2861.1 10	I	(1/2,3/2)+		2861.1	100		0.0	1/2+
2943.3 6	I	(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	I	(1/2,3/2)+		2878.0 2996.2	100 26 89		118.18945 0.0	5/2+ 1/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3127.6 10	I	(1/2,3/2)		3127.6	100		0.0	1/2+
3175.6 10	I	(1/2,3/2)		3175.6	100		0.0	1/2+
3185.0 10	I	(1/2,3/2)		3185.0	100		0.0	1/2+
3187.5 10	I	(1/2,3/2)		3187.5	100		0.0	1/2+
3191.3 7	I	(1/2,3/2)+		3182.9 3191.3	82 33 100		8.41017 0.0	3/2+ 1/2+
3199.7 10	I	(1/2,3/2)+		3199.7	100		0.0	1/2+
3204.8 7	I	(1/2,3/2)+		3086.6 3204.8	56 19 100		118.18945 0.0	5/2+ 1/2+
3254.6 7	I	(1/2,3/2)		3246.2 3254.6	100 53 69		8.41017 0.0	3/2+ 1/2+
3274.5 10	I	(1/2,3/2)+		3274.5	100		0.0	1/2+
3286.5 10	I	(1/2,3/2)+		3286.5	100		0.0	1/2+
3299.6 7	I	(1/2,3/2)+		3291.2 3299.6	100 75 96		8.41017 0.0	3/2+ 1/2+
3308.4 10	I	(1/2,3/2)		3308.4	100		0.0	1/2+
3341.2 7	I	(1/2,3/2)+		3332.8 3341.2	47 18 100		8.41017 0.0	3/2+ 1/2+
3376.4 7	I	(1/2,3/2)+		3368.0 3376.4	100 33 96		8.41017 0.0	3/2+ 1/2+
3383.9 10	I	(1/2,3/2)		3383.9	100		0.0	1/2+
3419.2 10	I	(1/2,3/2)		3419.2	100		0.0	1/2+
3436.3 7	I	(1/2,3/2)		3318.1 3436.3	67 43 100		118.18945 0.0	5/2+ 1/2+
3442.0 10	I	(1/2,3/2)		3442.0	100		0.0	1/2+
3458.6 10	I	(1/2,3/2)		3458.6	100		0.0	1/2+
3475.7 7	I	(1/2,3/2)+		3467.3 3475.7	100 41 47		8.41017 0.0	3/2+ 1/2+
3480.3 10	I	(1/2,3/2)		3480.3	100		0.0	1/2+
3497.0 10	I	(1/2,3/2)		3497.0	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
3527.0 7	I	(1/2,3/2)		3518.6 3527.0	100 72 72		8.41017 0.0	3/2+ 1/2+
3538.7 10	I	(1/2,3/2)		3538.7	100		0.0	1/2+
3541.9 7	I	(1/2,3/2)+		3423.7 3541.9	100 42 100		118.18945 0.0	5/2+ 1/2+
3573.3 10	I	(1/2,3/2)		3573.3	100		0.0	1/2+
3613.0 10	I	(1/2,3/2)		3613.0	100		0.0	1/2+
3624.8 6	I	(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	I	(1/2,3/2)+		3606.5 3724.7	100 26 100		118.18945 0.0	5/2+ 1/2+
3736.2 10	I	(1/2,3/2)		3736.2	100		0.0	1/2+
3741.7 10	I	(1/2,3/2)		3741.7	100		0.0	1/2+
3766.3 10	I	(1/2,3/2)		3766.3	100		0.0	1/2+
3795.8 7	I	(1/2,3/2)		3787.3 3795.7	1.0E2 13 61		8.41017 0.0	3/2+ 1/2+
3806.7 10	I	(1/2,3/2)		3806.7	100		0.0	1/2+
3862.5 10	I	(1/2,3/2)		3862.5	100		0.0	1/2+
3875.3 10	I	(1/2,3/2)		3875.3	100		0.0	1/2+
3916.8 10	I	(1/2,3/2)		3916.8	100		0.0	1/2+
3950.2 10	I	(1/2,3/2)		3950.2	100		0.0	1/2+
4103.6 10	I	(1/2,3/2)		4103.5	100		0.0	1/2+
4190.2 7	I	(1/2,3/2)		4181.7 4190.1	1.0E2 10 56		8.41017 0.0	3/2+ 1/2+
4279.7 10	I	(1/2,3/2)		4279.6	100		0.0	1/2+
4764.5 10	I	(1/2,3/2)		4764.4	100		0.0	1/2+
4789.8 10	I	(1/2,3/2)		4789.7	100		0.0	1/2+
4853.0 10	I	(1/2,3/2)		4852.9	100		0.0	1/2+
4865.5 7	I	(1/2,3/2)		4857.0 4865.4	1.0E2 11 69		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
4954.0 10	I	(1/2,3/2)		4953.9	100		0.0	1/2+
5211.5 10	I	(1/2,3/2)+		5211.4	100		0.0	1/2+
5507.1 10	I	(1/2,3/2)		5507	100		0.0	1/2+
5529.9 10	I	(1/2,3/2)+		5529.8	100		0.0	1/2+
5593.3 7	I	(1/2,3/2)		5584.8 5593.2	69 81 100		8.41017 0.0	3/2+ 1/2+
5598.3 10	I	(1/2,3/2)		5598.2	100		0.0	1/2+
1.47E+4 3	K
1.576E+4 13	F
16102	C	1/2-
1.634E+4 14	F	(1/2)-

E(level): Least-squares adjusted values based on adopted Eγ, with E(8.4 level) held fixed at 8.41017 15, the difference between E(118γ) and E(110γ), except where noted or where cross references clearly indicate a different source.

J^π(level): 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.

I(γ): Relative photon branching from each level; values are from ¹⁶⁹Yb ε decay (32.018 d), except where noted; upper limits are given for photon branchings affected by multiple placement or by presence of contaminant.

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - 1/2[411] band.
0.0	1/2+	STABLE
8.41017 11	3/2+	4.09 ns 5	8.41017 15	100	M1+E2	0.0	1/2+
118.18945 11	5/2+	62 ps 3	109.77924 3 118.18940 14	100.0 4 10.78 4	M1+E2 E2	8.41017 0.0	3/2+ 1/2+
138.93315 12	7/2+	302 ps 2	20.752 9 130.52293 6	1.73 2 100.0 3	M1+E2 E2	118.18945 8.41017	5/2+ 3/2+
332.116 11	9/2+	18.8 ps 5	193.15 5 213.935 17	100.0 45.9 10	M1+E2 E2	138.93315 118.18945	7/2+ 5/2+
367.67 5	11/2+	41.6 ps 21	228.71 5	100	E2	138.93315	7/2+
637.08 13	13/2+	5.4 ps 4	269.4 2 305.2 2	98.4 24 100	M1+E2 E2	367.67 332.116	11/2+ 9/2+
691.24 16	15/2+	8.1 ps 4	323.4 2	100	E2	367.67	11/2+
1027.85 16	17/2+	1.91 ps 18	336.60 5 391.0 2	58.7 7 100	M1+E2 E2	691.24 637.08	15/2+ 13/2+
1104.18 25	19/2+	1.94 ps 21	413.0 2	100	E2	691.24	15/2+
1497.8 4	21/2+	0.87 ps 9	394.0 5 469.6 5	34 13 100 50	E2	1104.18 1027.85	19/2+ 17/2+
1598.4 4	(23/2+)		494.2 2 ?	100		1104.18	19/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - 7/2[404] band.
316.14633 11	7/2+	659.9 ns 23
433.521 18	(9/2)+		101.41? 117.376 19 294.54 11	<18 100 6 2.4 6	[M1,E2] M1	332.116 316.14633 138.93315	9/2+ 7/2+ 7/2+
575.38 4	(11/2+)		141.85 5 259.23 5	100 10 96 48		433.521 316.14633	(9/2)+ 7/2+
741.25 6	(13/2+)		165.8 2 307.74 5	100 9 <57		575.38 433.521	(11/2+) (9/2)+
929.37 19	(15/2+)		188.7 5 353.9 2	37 21 100 10		741.25 575.38	(13/2+) (11/2+)
1140.85 21	(17/2+)		210.94 5 399.6 2	<39 100		929.37 741.25	(15/2+) (13/2+)
1372.1 6	(19/2+)		442.7 5	100		929.37	(15/2+)
1625.3 6	(21/2+)		484.4 5	100		1140.85	(17/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - 1/2[541], α=+1/2 band.
341.94 4	(1/2-)
345.028 3	5/2-		205.99 6 226.3 7 336.618 3	36 9 2.7 19 100 3	E1 E1(+M2)	138.93315 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	345.028 138.93315	5/2- 7/2+
602.82 19	(13/2-)		172.7 5 235.1 2	16 8 100 10	(E1(+M2))	430.122 367.67	(9/2)- 11/2+
865.9 4	(17/2-)		175.0 5 262.7 5	41 22 100 16		691.24 602.82	15/2+ (13/2-)
1218.1 5	(21/2-)		352.2 2	100		865.9	(17/2-)
1658.1 5	(25/2-)		440.0 2	100		1218.1	(21/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - 7/2[523] band.
379.26678 12	7/2-	52.2 ns 8
472.88128 14	9/2-	0.14 ns 7	93.61447 8 105.19 10 156.724 11 333.963 13	100.0 6 0.10 3 0.383 10 0.0675 24	M1+E2 E1 E1 [E1]	379.26678 367.67 316.14633 138.93315	7/2- 11/2+ 7/2+ 7/2+
588.20 5	11/2-		115.32 5 208.8 5	100 10 10 5	(M1+E2)	472.88128 379.26678	9/2- 7/2-
725.44 7	13/2-		137.26 5 252.5 2	100 10 29 3	(M1+E2)	588.20 472.88128	11/2- 9/2-
883.75 14	15/2-		158.3 2 295.4 2	100 10 <78	(M1(+E2))	725.44 588.20	13/2- 11/2-
1063.57 16	17/2-		179.6 2 338.3 2	90 9 100 10		883.75 725.44	15/2- 13/2-
1262.40 21	19/2-		198.3 5 378.7 2	<185 100		1063.57 883.75	17/2- 15/2-
1482.94 22	21/2-		220.5 2 419.4 2	100 10 77 8		1262.40 1063.57	19/2- 17/2-
1716.9 3	23/2-		233? 454.5 2			1482.94 1262.40	21/2- 19/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - 3/2[411] band + 1/2[411] γ vibration.
570.830 11	3/2+	10 ps 7
633.292 3	5/2+	0.27 ps	494.357 8 515.101 6 624.881 4 633.32 10	29.8 5 84.5 12 100.0 25 0.140 9	M1 M1 M1 [E2]	138.93315 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 17 59.1 9 1.77 9	[M1,E2] (M1) (M1)	646.758 332.116 138.93315 118.18945 8.41017	(7/2-) 9/2+ 7/2+ 5/2+ 3/2+
832.42 7	(9/2+)		464.7 500.35 10 693.46 8	41 24 100 9 98 5		367.67 332.116 138.93315	11/2+ 9/2+ 7/2+
964.0 4	(11/2+)		595.9 5 632.3 5	100 72 38		367.67 332.116	11/2+ 9/2+
1300.8 6	(15/2+)		609.6 5	100		691.24	15/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - 5/2[402] band.
781.796 6	(5/2)+
878.35 10	(7/2+)		546.16 22 739.42 11 760.24 24	80 22 100 12 45 12		332.116 138.93315 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 7 - 9/2[514] band
1152 2	(11/2-)

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 5	8.41017 15	M1+E2	0.0328 5	263	B(E2)(W.u.)=241 10, B(M1)(W.u.)=0.0342 8, α=263 5
118.18945	5/2+	62 ps 3	109.77924 3	M1+E2	-0.139 10	2.37	B(E2)(W.u.)=53 8, B(M1)(W.u.)=0.072 4, α=2.37
118.18945	5/2+	62 ps 3	118.18940 14	E2		1.642	B(E2)(W.u.)=210 11, α=1.642
138.93315	7/2+	302 ps 2	20.752 9	M1+E2	0.0292 16	54.9	B(E2)(W.u.)=42 5, B(M1)(W.u.)=0.0454 13, α=54.9 9
138.93315	7/2+	302 ps 2	130.52293 6	E2		1.143	B(E2)(W.u.)=287 5, α=1.143
316.14633	7/2+	659.9 ns 23	177.21307 6	M1+E2	-0.30 13	0.594	B(E2)(W.u.)=0.0017 14, B(M1)(W.u.)=1.25E-6 10, α=0.594 19
	7/2+	659.9 ns 23	197.95675 7	M1+E2	-0.326 6	0.433	B(E2)(W.u.)=0.00180 7, B(M1)(W.u.)=1.430E-6 14, α=0.433
	7/2+	659.9 ns 23	307.73586 10	E2		0.0662	B(E2)(W.u.)=0.000576 4, α=0.0662
332.116	9/2+	18.8 ps 5	193.15 5	M1+E2	-0.126 21	0.479	B(E2)(W.u.)=16 6, B(M1)(W.u.)=0.0787 22, α=0.479 1
332.116	9/2+	18.8 ps 5	213.935 17	E2		0.208	B(E2)(W.u.)=273 10, α=0.208
345.028	5/2-		205.99 6	E1		0.0497	α=0.0497
345.028	5/2-		336.618 3	E1(+M2)	0.66 LE	0.07	α=0.07 6
367.67	11/2+	41.6 ps 21	228.71 5	E2		0.1673	B(E2)(W.u.)=336 17, α=0.1673
379.26678	7/2-	52.2 ns 8	63.12044 4	E1		1.098	B(E1)(W.u.)=7.88E-6 17, α=1.098
	7/2-	52.2 ns 8	240.331 3	E1(+M2)	+0.12 LT	0.042	B(E1)(W.u.)>3.5E-10, B(M2)(W.u.)<0.00044, α=0.042 9
	7/2-	52.2 ns 8	261.07712 9	E1+M2	-0.07 3	0.032	B(E1)(W.u.)=4.26E-9 9, B(M2)(W.u.)=0.0014 12, α=0.032 5
	7/2-	52.2 ns 8	370.854 8	[M2]		0.300	B(M2)(W.u.)=2.6×10^-5 3, α=0.300
	7/2-	52.2 ns 8	379.284 18	[E3]		0.1270	B(E3)(W.u.)=0.039 15, α=0.1270
430.122	(9/2)-		291.188 11	E1		0.0207	α=0.0207
433.521	(9/2)+		117.376 19	[M1,E2]		1.82	α=1.82 14
433.521	(9/2)+		294.54 11	M1		0.1522	α=0.1522
472.88128	9/2-	0.14 ns 7	93.61447 8	M1+E2	+0.183 3	3.75	B(E2)(W.u.)=70 40, B(M1)(W.u.)=0.039 20, α=3.75
	9/2-	0.14 ns 7	105.19 10	E1		0.292	B(E1)(W.u.)=2.9E-7 17, α=0.292
	9/2-	0.14 ns 7	156.724 11	E1		0.1016	B(E1)(W.u.)=3.3E-7 17, α=0.1016
	9/2-	0.14 ns 7	333.963 13	[E1]		0.01480	B(E1)(W.u.)=6E-9 3, α=0.01480
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
570.830	3/2+	10 ps 7	452.62 8	M1+E2	1.5 +9-4	0.030	B(E2)(W.u.)=2.6 23, B(M1)(W.u.)=0.0005 5, α=0.030 5
	3/2+	10 ps 7	562.410 12	M1+E2	0.8 +5-4	0.022	B(E2)(W.u.)=3 +4-3, B(M1)(W.u.)=0.004 3, α=0.022 4
	3/2+	10 ps 7	570.89 3	M1+E2	0.8 +5-4	0.021	B(E2)(W.u.)=3 3, B(M1)(W.u.)=0.003 3, α=0.021 4
588.20	11/2-		115.32 5	(M1+E2)		1.93	α=1.93 14
602.82	(13/2-)		235.1 2	(E1(+M2))		0.7	α=0.7 7
633.292	5/2+	0.27 ps	494.357 8	M1		0.0389	B(M1)(W.u.)=0.091, α=0.0389
	5/2+	0.27 ps	515.101 6	M1		0.0350	B(M1)(W.u.)=0.23, α=0.0350
	5/2+	0.27 ps	624.881 4	M1		0.0214	B(M1)(W.u.)=0.15, α=0.0214
	5/2+	0.27 ps	633.32 10	[E2]		0.00959	B(E2)(W.u.)=0.24, α=0.00959
637.08	13/2+	5.4 ps 4	269.4 2	M1+E2	-0.149 26	0.192	B(E2)(W.u.)=13 5, B(M1)(W.u.)=0.090 8, α=0.192
637.08	13/2+	5.4 ps 4	305.2 2	E2		0.0678	B(E2)(W.u.)=318 24, α=0.0678
691.24	15/2+	8.1 ps 4	323.4 2	E2		0.0571	B(E2)(W.u.)=337 17, α=0.0571
718.786	(7/2+)		386.671 13	[M1,E2]		0.054	α=0.054 20
	(7/2+)		579.851 5	(M1)		0.0259	α=0.0259
	(7/2+)		600.603 8	(M1)		0.0237	α=0.0237
725.44	13/2-		137.26 5	(M1+E2)		1.11	α=1.11 16
883.75	15/2-		158.3 2	(M1(+E2))		0.71	α=0.71 14
1027.85	17/2+	1.91 ps 18	336.60 5	M1+E2	-0.18 3	0.1048	B(E2)(W.u.)=14 5, B(M1)(W.u.)=0.102 10, α=0.1048 16
1027.85	17/2+	1.91 ps 18	391.0 2	E2		0.0331	B(E2)(W.u.)=350 40, α=0.0331
1104.18	19/2+	1.94 ps 21	413.0 2	E2		0.0284	B(E2)(W.u.)=430 50, α=0.0284
1497.8	21/2+	0.87 ps 9	469.6 5	E2		0.0201	B(E2)(W.u.)=340 220, α=0.0201

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1/2+	STABLE	μ=-0.2316 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] band.
8.41017	3/2+	4.09 ns 5	Q=-1.2 1, μ=+0.5148 48 E(level): From ¹⁷⁰Er(p,2nγ), (d,3nγ). 1/2[411] band.
118.18945	5/2+	62 ps 3	μ=+0.761 45 E(level): 1/2[411] band. J^π(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2⁺, and intraband M1⁺E2 110γ and E2 118γ from 118 level.
138.93315	7/2+	302 ps 2	μ=+1.39 5 E(level): 1/2[411] band. J^π(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2⁺, and intraband M1⁺E2 110γ and E2 118γ from 118 level.
316.14633	7/2+	659.9 ns 23	μ=+0.156 8 E(level): 7/2[404] band.
332.116	9/2+	18.8 ps 5	μ=1.56 9 (1999Ro03) E(level): 1/2[411] band. J^π(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2⁺, and intraband M1⁺E2 110γ and E2 118γ from 118 level.
341.94	(1/2-)		E(level): 1/2[541], α=+1/2 band.
345.028	5/2-		E(level): 1/2[541], α=+1/2 band.
367.67	11/2+	41.6 ps 21	μ=2.28 14 (1999Ro03) E(level): 1/2[411] band. J^π(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2⁺, and intraband M1⁺E2 110γ and E2 118γ from 118 level.
379.26678	7/2-	52.2 ns 8	μ=+3.04 14 (1997De02) E(level): 7/2[523] band.
430.122	(9/2)-		E(level): 1/2[541], α=+1/2 band.
433.521	(9/2)+		E(level): 7/2[404] band.
472.88128	9/2-	0.14 ns 7	E(level): 7/2[523] band.
570.830	3/2+	10 ps 7	E(level): 3/2[411] band + 1/2[411] γ vibration.
575.38	(11/2+)		E(level): 7/2[404] band.
588.20	11/2-		E(level): 7/2[523] band.
602.82	(13/2-)		E(level): 1/2[541], α=+1/2 band.
633.292	5/2+	0.27 ps	E(level): 3/2[411] band + 1/2[411] γ vibration.
637.08	13/2+	5.4 ps 4	μ=2.37 14 (1999Ro03) E(level): 1/2[411] band. J^π(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2⁺, and intraband M1⁺E2 110γ and E2 118γ from 118 level.
691.24	15/2+	8.1 ps 4	μ=3.2 3 (1999Ro03) E(level): 1/2[411] band. J^π(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2⁺, and intraband M1⁺E2 110γ and E2 118γ from 118 level.
718.786	(7/2+)		E(level): 3/2[411] band + 1/2[411] γ vibration.
725.44	13/2-		E(level): 7/2[523] band.
741.25	(13/2+)		E(level): 7/2[404] band.
781.796	(5/2)+		XREF: d(785). E(level): From ¹⁷⁰Er(p,2nγ), (d,3nγ). 5/2[402] band.
832.42	(9/2+)		E(level): 3/2[411] band + 1/2[411] γ vibration.
E(level)	J^π(level)	T_1/2(level)	Comments
865.9	(17/2-)		E(level): 1/2[541], α=+1/2 band.
878.35	(7/2+)		E(level): From ¹⁷⁰Er(p,2nγ), (d,3nγ). 5/2[402] band.
883.75	15/2-		E(level): 7/2[523] band.
929.37	(15/2+)		E(level): 7/2[404] band.
964.0	(11/2+)		E(level): 3/2[411] band + 1/2[411] γ vibration.
1027.85	17/2+	1.91 ps 18	μ=3.1 3 (1999Ro03) E(level): 1/2[411] band. J^π(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2⁺, and intraband M1⁺E2 110γ and E2 118γ from 118 level.
1063.57	17/2-		E(level): 7/2[523] band.
1104.18	19/2+	1.94 ps 21	μ=4.2 8 (1999Ro03) E(level): 1/2[411] band. J^π(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2⁺, and intraband M1⁺E2 110γ and E2 118γ from 118 level.
1140.85	(17/2+)		E(level): 7/2[404] band.
1152	(11/2-)		E(level): From ¹⁷⁰Er(p,2nγ), (d,3nγ). 9/2[514] band.
1190	+		B(E2)=0.040 9 B(E2)\|^ from Coulomb excitation. E(level): B(E2)\|^ from Coulomb excitation.
1218.1	(21/2-)		E(level): 1/2[541], α=+1/2 band.
1262.40	19/2-		E(level): 7/2[523] band.
1300.8	(15/2+)		E(level): 3/2[411] band + 1/2[411] γ vibration.
1372.1	(19/2+)		E(level): 7/2[404] band.
1482.94	21/2-		E(level): 7/2[523] band.
1497.8	21/2+	0.87 ps 9	E(level): 1/2[411] band. J^π(level): Definite Jπ for g.s. band established through J=21/2 based on band structure and independently established Jπ(8-keV level)=3/2⁺, and intraband M1⁺E2 110γ and E2 118γ from 118 level.
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.
1598.4	(23/2+)		E(level): From ¹⁷⁰Er(p,2nγ), (d,3nγ). 1/2[411] band.
1625.3	(21/2+)		E(level): 7/2[404] band.
1658.1	(25/2-)		E(level): 1/2[541], α=+1/2 band.
1716.9	23/2-		E(level): 7/2[523] band.
1864.6	(1/2,3/2)+		B(M1,E1)\|^(W.u.)=0.19 3. E(level): B(M1,E1)\|^(W.u.)=0.19 3. 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)+		B(M1,E1)\|^(W.u.)=0.61 4. E(level): B(M1,E1)\|^(W.u.)=0.61 4. 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
1922.3	(1/2,3/2)+		B(M1,E1)\|^(W.u.)=0.037 11. E(level): B(M1,E1)\|^(W.u.)=0.037 11. 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.
1963.7	(1/2,3/2)		B(M1,E1)\|^(W.u.)=0.019 6. E(level): B(M1,E1)\|^(W.u.)=0.019 6. 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)		B(M1,E1)\|^(W.u.)=0.020 6. E(level): B(M1,E1)\|^(W.u.)=0.020 6. 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)+		B(M1,E1)\|^(W.u.)=0.061 13. E(level): B(M1,E1)\|^(W.u.)=0.061 13. 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.
2075.5	(1/2,3/2)+		B(M1,E1)\|^(W.u.)=0.039 17. E(level): B(M1,E1)\|^(W.u.)=0.039 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.
2168.7	(1/2,3/2)+		B(M1,E1)\|^(W.u.)=0.035 11. E(level): B(M1,E1)\|^(W.u.)=0.035 11. 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)		B(M1,E1)\|^(W.u.)=0.022 4. E(level): B(M1,E1)\|^(W.u.)=0.022 4. 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)		B(M1,E1)\|^(W.u.)=0.018 12. E(level): B(M1,E1)\|^(W.u.)=0.018 12. 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)+		B(M1,E1)\|^(W.u.)=0.050 6. E(level): B(M1,E1)\|^(W.u.)=0.050 6. 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)+		B(M1,E1)\|^(W.u.)=0.043 11. E(level): B(M1,E1)\|^(W.u.)=0.043 11. 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)		B(M1,E1)\|^(W.u.)=0.018 4. E(level): B(M1,E1)\|^(W.u.)=0.018 4. 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)		B(M1,E1)\|^(W.u.)=0.013 4. E(level): B(M1,E1)\|^(W.u.)=0.013 4. 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)+		B(M1,E1)\|^(W.u.)=0.032 9. E(level): B(M1,E1)\|^(W.u.)=0.032 9. 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)		B(M1,E1)\|^(W.u.)=0.020 8. E(level): B(M1,E1)\|^(W.u.)=0.020 8. 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.
2455.8	(1/2,3/2)		B(M1,E1)\|^(W.u.)=0.022 7. E(level): B(M1,E1)\|^(W.u.)=0.022 7. 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)		B(M1,E1)\|^(W.u.)=0.010 3. E(level): B(M1,E1)\|^(W.u.)=0.010 3. 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.
2492.0	(1/2,3/2)+		B(M1,E1)\|^(W.u.)=0.051 5. E(level): B(M1,E1)\|^(W.u.)=0.051 5. 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)		B(M1,E1)\|^(W.u.)=0.025 8. E(level): B(M1,E1)\|^(W.u.)=0.025 8. 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)		B(M1,E1)\|^(W.u.)=0.010 3. E(level): B(M1,E1)\|^(W.u.)=0.010 3. 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)+		B(M1,E1)\|^(W.u.)=0.035 10. E(level): B(M1,E1)\|^(W.u.)=0.035 10. 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)		B(M1,E1)\|^(W.u.)=0.017 3. E(level): B(M1,E1)\|^(W.u.)=0.017 3. 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)		B(M1,E1)\|^(W.u.)=0.011 3. E(level): B(M1,E1)\|^(W.u.)=0.011 3. 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)+		B(M1,E1)\|^(W.u.)=0.031 7. E(level): B(M1,E1)\|^(W.u.)=0.031 7. 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)		B(M1,E1)\|^(W.u.)=0.017 3. E(level): B(M1,E1)\|^(W.u.)=0.017 3. 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)+		B(M1,E1)\|^(W.u.)=0.043 6. E(level): B(M1,E1)\|^(W.u.)=0.043 6. 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
2786.5	(1/2,3/2)		B(M1,E1)\|^(W.u.)=0.021 4. E(level): B(M1,E1)\|^(W.u.)=0.021 4. 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)		B(M1,E1)\|^(W.u.)=0.032 21. E(level): B(M1,E1)\|^(W.u.)=0.032 21. 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)		B(M1,E1)\|^(W.u.)=0.015 6. E(level): B(M1,E1)\|^(W.u.)=0.015 6. 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)		B(M1,E1)\|^(W.u.)=0.011 3. E(level): B(M1,E1)\|^(W.u.)=0.011 3. 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)+		B(M1,E1)\|^(W.u.)=0.033 12. E(level): B(M1,E1)\|^(W.u.)=0.033 12. 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)+		B(M1,E1)\|^(W.u.)=0.043 16. E(level): B(M1,E1)\|^(W.u.)=0.043 16. 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)+		B(M1,E1)\|^(W.u.)=0.033 6. E(level): B(M1,E1)\|^(W.u.)=0.033 6. 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)		B(M1,E1)\|^(W.u.)=0.020 3. E(level): B(M1,E1)\|^(W.u.)=0.020 3. 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)		B(M1,E1)\|^(W.u.)=0.010 3. E(level): B(M1,E1)\|^(W.u.)=0.010 3. 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)		B(M1,E1)\|^(W.u.)=0.030 12. E(level): B(M1,E1)\|^(W.u.)=0.030 12. 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)		B(M1,E1)\|^(W.u.)=0.009 5. E(level): B(M1,E1)\|^(W.u.)=0.009 5. 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)+		B(M1,E1)\|^(W.u.)=0.030 7. E(level): B(M1,E1)\|^(W.u.)=0.030 7. 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)+		B(M1,E1)\|^(W.u.)=0.033 9. E(level): B(M1,E1)\|^(W.u.)=0.033 9. 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)+		B(M1,E1)\|^(W.u.)=0.046 12. E(level): B(M1,E1)\|^(W.u.)=0.046 12. 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)		B(M1,E1)\|^(W.u.)=0.025 7. E(level): B(M1,E1)\|^(W.u.)=0.025 7. 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.
3274.5	(1/2,3/2)+		B(M1,E1)\|^(W.u.)=0.029 7. E(level): B(M1,E1)\|^(W.u.)=0.029 7. 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)+		B(M1,E1)\|^(W.u.)=0.028 4. E(level): B(M1,E1)\|^(W.u.)=0.028 4. 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)+		B(M1,E1)\|^(W.u.)=0.037 15. E(level): B(M1,E1)\|^(W.u.)=0.037 15. 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)		B(M1,E1)\|^(W.u.)=0.012 4. E(level): B(M1,E1)\|^(W.u.)=0.012 4. 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)+		B(M1,E1)\|^(W.u.)=0.037 9. E(level): B(M1,E1)\|^(W.u.)=0.037 9. 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)+		B(M1,E1)\|^(W.u.)=0.030 6. E(level): B(M1,E1)\|^(W.u.)=0.030 6. 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)		B(M1,E1)\|^(W.u.)=0.020 3. E(level): B(M1,E1)\|^(W.u.)=0.020 3. 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)		B(M1,E1)\|^(W.u.)=0.020 4. E(level): B(M1,E1)\|^(W.u.)=0.020 4. 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)		B(M1,E1)\|^(W.u.)=0.027 12. E(level): B(M1,E1)\|^(W.u.)=0.027 12. 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)		B(M1,E1)\|^(W.u.)=0.012 7. E(level): B(M1,E1)\|^(W.u.)=0.012 7. 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
3458.6	(1/2,3/2)		B(M1,E1)\|^(W.u.)=0.013 7. E(level): B(M1,E1)\|^(W.u.)=0.013 7. 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)+		B(M1,E1)\|^(W.u.)=0.055 13. E(level): B(M1,E1)\|^(W.u.)=0.055 13. 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)		B(M1,E1)\|^(W.u.)=0.020 3. E(level): B(M1,E1)\|^(W.u.)=0.020 3. 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)		B(M1,E1)\|^(W.u.)=0.008 3. E(level): B(M1,E1)\|^(W.u.)=0.008 3. 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)		B(M1,E1)\|^(W.u.)=0.017 7. E(level): B(M1,E1)\|^(W.u.)=0.017 7. 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)		B(M1,E1)\|^(W.u.)=0.011 3. E(level): B(M1,E1)\|^(W.u.)=0.011 3. 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)+		B(M1,E1)\|^(W.u.)=0.026 7. E(level): B(M1,E1)\|^(W.u.)=0.026 7. 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)		B(M1,E1)\|^(W.u.)=0.015 9. E(level): B(M1,E1)\|^(W.u.)=0.015 9. 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)		B(M1,E1)\|^(W.u.)=0.013 4. E(level): B(M1,E1)\|^(W.u.)=0.013 4. 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)+		B(M1,E1)\|^(W.u.)=0.057 9. E(level): B(M1,E1)\|^(W.u.)=0.057 9. 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)+		B(M1,E1)\|^(W.u.)=0.034 6. E(level): B(M1,E1)\|^(W.u.)=0.034 6. 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)		B(M1,E1)\|^(W.u.)=0.010 4. E(level): B(M1,E1)\|^(W.u.)=0.010 4. 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)		B(M1,E1)\|^(W.u.)=0.014 4. E(level): B(M1,E1)\|^(W.u.)=0.014 4. 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)		B(M1,E1)\|^(W.u.)=0.012 3. E(level): B(M1,E1)\|^(W.u.)=0.012 3. 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)		B(M1,E1)\|^(W.u.)=0.014 11. E(level): B(M1,E1)\|^(W.u.)=0.014 11. 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.
3806.7	(1/2,3/2)		B(M1,E1)\|^(W.u.)=0.008 3. E(level): B(M1,E1)\|^(W.u.)=0.008 3. 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)		B(M1,E1)\|^(W.u.)=0.012 4. E(level): B(M1,E1)\|^(W.u.)=0.012 4. 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)		B(M1,E1)\|^(W.u.)=0.016 4. E(level): B(M1,E1)\|^(W.u.)=0.016 4. 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)		B(M1,E1)\|^(W.u.)=0.014 4. E(level): B(M1,E1)\|^(W.u.)=0.014 4. 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)		B(M1,E1)\|^(W.u.)=0.015 3. E(level): B(M1,E1)\|^(W.u.)=0.015 3. 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)		B(M1,E1)\|^(W.u.)=0.0056 22. E(level): B(M1,E1)\|^(W.u.)=0.0056 22. 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)		B(M1,E1)\|^(W.u.)=0.021 13. E(level): B(M1,E1)\|^(W.u.)=0.021 13. 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)		B(M1,E1)\|^(W.u.)=0.008 3. E(level): B(M1,E1)\|^(W.u.)=0.008 3. 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)		B(M1,E1)\|^(W.u.)=0.006 3. E(level): B(M1,E1)\|^(W.u.)=0.006 3. 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)		B(M1,E1)\|^(W.u.)=0.008 4. E(level): B(M1,E1)\|^(W.u.)=0.008 4. 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
4853.0	(1/2,3/2)		B(M1,E1)\|^(W.u.)=0.007 4. E(level): B(M1,E1)\|^(W.u.)=0.007 4. 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)		B(M1,E1)\|^(W.u.)=0.015 9. E(level): B(M1,E1)\|^(W.u.)=0.015 9. 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)		B(M1,E1)\|^(W.u.)=0.023 6. E(level): B(M1,E1)\|^(W.u.)=0.023 6. 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)+		B(M1,E1)\|^(W.u.)=0.030 6. E(level): B(M1,E1)\|^(W.u.)=0.030 6. 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)		B(M1,E1)\|^(W.u.)=0.023 26. E(level): B(M1,E1)\|^(W.u.)=0.023 26. 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)+		B(M1,E1)\|^(W.u.)=0.059 21. E(level): B(M1,E1)\|^(W.u.)=0.059 21. 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)		B(M1,E1)\|^(W.u.)=0.05 4. E(level): B(M1,E1)\|^(W.u.)=0.05 4. 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)		B(M1,E1)\|^(W.u.)=0.031 17. E(level): B(M1,E1)\|^(W.u.)=0.031 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.

E(level)	E(gamma)	Comments
8.41017	8.41017	E(γ): from recoil-corrected level-energy difference.
118.18945	109.77924	E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2⁺ to g.s. transition in ¹⁹⁸Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See ¹⁶⁹Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
118.18945	118.18940	E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2⁺ to g.s. transition in ¹⁹⁸Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See ¹⁶⁹Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included. I(γ): from ε decay. However, Iγ=10.21 5 (1999Ro03) in Coulomb excitation is not consistent with this. Other I(118γ)/I(110γ): 11 2 (1967Se09) and 11.0 10 (1977Ta10) in Coulomb excitation; 11 3 in β^- decay.
138.93315	130.52293	E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2⁺ to g.s. transition in ¹⁹⁸Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See ¹⁶⁹Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
316.14633	177.21307	E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2⁺ to g.s. transition in ¹⁹⁸Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See ¹⁶⁹Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
	197.95675	E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2⁺ to g.s. transition in ¹⁹⁸Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See ¹⁶⁹Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
	307.73586	E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2⁺ to g.s. transition in ¹⁹⁸Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See ¹⁶⁹Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
332.116	193.15	I(γ): From Coulomb excitation. M(γ): From Coulomb excitation.
332.116	213.935	I(γ): weighted average of 39 6 in ε decay, 43 9 in (p,2nγ), 45.2 5 (1999Ro03), 49.1 11 (1977Ta10), 56 5 (1967Se09) in Coulomb excitation. M(γ): from Coulomb excitation.
341.94	333.53	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
341.94	341.95	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
367.67	228.71	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). M(γ): from γ(θ) and RUL in Coulomb excitation.. From Coulomb excitation.
379.26678	63.12044	E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2⁺ to g.s. transition in ¹⁹⁸Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See ¹⁶⁹Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
379.26678	261.07712	E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2⁺ to g.s. transition in ¹⁹⁸Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See ¹⁶⁹Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
430.122	84.9	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
430.122	291.188	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
472.88128	93.61447	E(γ): From the evaluation by 2000He14 (with energy scale based on Eγ=411.80205 keV 17 for the "Gold standard " (2⁺ to g.s. transition in ¹⁹⁸Hg)). ΔE quoted here includes the 0.3 ppm uncertainty arising from the energy-wavelength conversion. See ¹⁶⁹Yb ε decay (32.018 d) for uncertainties that do not have that systematic uncertainty included.
474.968	466.2	E(γ): from (p,2nγ).
570.830	452.62	M(γ): From Coulomb excitation.
	562.410	M(γ): From Coulomb excitation.
	570.89	M(γ): From Coulomb excitation.
575.38	141.85	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
575.38	259.23	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
588.20	115.32	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). M(γ): D+Q from (p,2nγ), Δπ=no from level scheme.
588.20	208.8	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
E(level)	E(gamma)	Comments
602.82	172.7	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
602.82	235.1	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). M(γ): d(+Q) from (p,2nγ), Δπ=yes from level scheme.
637.08	269.4	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): weighted average of 99.6 12 (1999Ro03) and 93.7 24 (1977Ta10) in Coulomb excitation. Other Iγ: 101 14 in (p,2nγ); 79 8 (1967Se09) in Coulomb excitation.. From Coulomb excitation. M(γ): From Coulomb excitation.
637.08	305.2	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From Coulomb excitation. M(γ): From Coulomb excitation.
646.758	171.6	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
	216.4	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
	301.6	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
	314.6	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
	528.569	I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
691.24	323.4	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). M(γ): From Coulomb excitation.
725.44	137.26	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). M(γ): D+Q from (p,2nγ), Δπ=no from level scheme.
725.44	252.5	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
741.25	165.8	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
741.25	307.74	E(γ): for multiplet in (p,2nγ).. From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
781.796	210.94	E(γ): Multiply placed. From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
865.9	175.0	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
865.9	262.7	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
883.75	158.3	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). M(γ): d(+Q) from (p,2nγ), Δπ=no from level scheme.
883.75	295.4	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
884.62	281.7	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
	454.5	E(γ): Multiply placed. From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
	552.0	E(γ): Multiply placed. From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
900	900	E(γ): From Coulomb excitation.
929.37	188.7	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
929.37	353.9	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
E(level)	E(gamma)	Comments
964.0	595.9	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
964.0	632.3	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1027.85	336.60	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): from 1999Ro03 in Coulomb excitation. Other Iγ: 52 5 (1977Ta10) in Coulomb excitation; 336 in (p,2nγ); 114 (1974Ba66) in (d,3nγ).. From Coulomb excitation. M(γ): From Coulomb excitation.
1027.85	391.0	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From Coulomb excitation. M(γ): From Coulomb excitation.
1039.95	565.2	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1039.95	694.7	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1058.54	716.6	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1063.57	179.6	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1063.57	338.3	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1104.18	413.0	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). M(γ): From Coulomb excitation.
1112.6	682.5	E(γ): Multiply placed. From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1135.93	790.9	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1140.85	210.94	E(γ): Multiply placed. From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1140.85	399.6	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1188.7	552.0	E(γ): Multiply placed. From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1188.7	585.9	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1190	1190	E(γ): From Coulomb excitation.
1218.1	352.2	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1223.04	877.9	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1223.04	881.2	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1262.40	198.3	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1262.40	378.7	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1300.8	609.6	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1372.1	442.7	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1482.94	220.5	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1482.94	419.4	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
E(level)	E(gamma)	Comments
1497.8	394.0	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): weighted average of 29 15 from Coulomb excitation and 50 26 from (p,2nγ).. From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1497.8	469.6	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). I(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ). M(γ): From Coulomb excitation.
1510.6	1510.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1527.5	1527.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1548.4	682.5	E(γ): Multiply placed. From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1598.4	494.2	E(γ): Multiply placed. From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1625.3	484.4	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1658.1	440.0	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1716.9	233	E(γ): From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1716.9	454.5	E(γ): Multiply placed. From ¹⁷⁰Er(p,2nγ), (d,3nγ).
1864.6	1856.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1864.6	1864.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1910.5	1792.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
	1902.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
	1910.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1922.3	1804.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1922.3	1922.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1963.7	1963.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1978.4	1978.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1991.7	1983.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
1991.7	1991.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2075.5	2067.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2075.5	2075.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2168.7	2160.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2168.7	2168.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
E(level)	E(gamma)	Comments
2190.6	2190.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2215.3	2215.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2236.1	2117.9	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2236.1	2236.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2262.5	2144.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2262.5	2262.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2293.8	2293.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2306.3	2306.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2312.2	2194.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2312.2	2312.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2386.6	2386.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2455.8	2447.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2455.8	2455.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2466.0	2466.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2492.0	2373.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2492.0	2492.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2553.4	2435.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2553.4	2553.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2571.4	2571.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2598.6	2598.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2602.8	2602.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2687.0	2687.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2749.4	2741.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2749.4	2749.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2756.4	2756.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
E(level)	E(gamma)	Comments
2769.1	2760.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2769.1	2769.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2786.5	2786.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2814.2	2805.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2814.2	2814.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2818.6	2818.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2843.1	2843.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2861.1	2861.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2943.3	2825.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
	2934.9	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
	2943.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2996.2	2878.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
2996.2	2996.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3127.6	3127.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3175.6	3175.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3185.0	3185.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3187.5	3187.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3191.3	3182.9	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3191.3	3191.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3199.7	3199.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3204.8	3086.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3204.8	3204.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3254.6	3246.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3254.6	3254.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3274.5	3274.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
E(level)	E(gamma)	Comments
3286.5	3286.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3299.6	3291.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3299.6	3299.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3308.4	3308.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3341.2	3332.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3341.2	3341.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3376.4	3376.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3383.9	3383.9	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3419.2	3419.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3436.3	3318.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3436.3	3436.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3442.0	3442.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3458.6	3458.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3475.7	3467.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3475.7	3475.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3480.3	3480.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3497.0	3497.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3527.0	3518.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3527.0	3527.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3538.7	3538.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3541.9	3423.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3541.9	3541.9	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3573.3	3573.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3613.0	3613.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3624.8	3506.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
	3616.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
	3624.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
E(level)	E(gamma)	Comments
3724.7	3606.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3724.7	3724.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3736.2	3736.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3741.7	3741.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3766.3	3766.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3795.8	3787.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3795.8	3795.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3806.7	3806.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3862.5	3862.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3875.3	3875.3	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3916.8	3916.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
3950.2	3950.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4103.6	4103.5	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4190.2	4181.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4190.2	4190.1	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4279.7	4279.6	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4764.5	4764.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4789.8	4789.7	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4853.0	4852.9	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4865.5	4857.0	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4865.5	4865.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
4954.0	4953.9	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
5211.5	5211.4	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
5507.1	5507	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
5529.9	5529.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
E(level)	E(gamma)	Comments
5593.3	5584.8	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
5593.3	5593.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).
5598.3	5598.2	E(γ): 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. I(γ): From ¹⁶⁹Tm(γ,γ’).