List of levels for 161TM

Author: C. W. Reich | Citation: Nucl. Data Sheets 112,2497 (2011) | Cutoff date: 1-Jun-2011

Levels: From measurements following chemical separations by Szilard-Chalmers reactions, 1968GrZX report an `isomer’ of 7 min 2. This has not been confirmed. See, however, the comment below on the half-life of the 7.51 level.

Levels: band(a) 7/2[404] band. α=+1/2 branch.

Q-value: Note: Current evaluation has used the following Q record $ -4056 32 9668 44 3129 37 2506 36 2009AuZZ

Q-value: 2003Au03 report the following: Q(β^-)=-4050 30; S(n)=9670 40; 3130 40; and Q(α)=2510 40.

E(level): From a least-squares fit to the listed γ-ray energies.

J^π(level): For the data from the in-beam studies, the Jπ assignments are based on the expected properties of rotational bands, including level energies, the decrease of γ intensity and the increase of J values with increasing excitation energy. This has been supplemented with the measured γ-ray multipolarities and mixing ratios. These are interpreted as M1⁺E2 and E2, instead of E1⁺M2 M2, in keeping with the interpretation of the associated gammas as being intraband transitions.

E(γ): See ¹⁶¹Yb ε decay and the in-beam study of 1984Fo04 for lists of unplaced γ’s that are not given here.

E(γ): In the two heavy-ion studies (1984Fo04, 1995Sm02) where the data sets overlap, the reported Eγ values are identical in almost all cases, except that 1995Sm02 list no uncertainties. For the Eγ data from these studies, those with listed uncertainties are from 1984Fo04 and those without them are from 1995Sm02.

I(γ): The Iγ data for the γ’s from the heavy-ion studies are mostly from 1995Sm02, whose data are more extensive than those of of 1984Fo04 and for which uncertainties are listed in most cases. 1984Fo04 do not list uncertainties for their Iγ data.

M(γ): Assignments are based on the ce data from ¹⁶¹Yb ε decay and the γγ(θ) (DCO) data (1995Wa21). In the latter case, the the evaluator has made the assignments from reported data.

M(γ): For transitions having listed δ values, the multipolarities are shown as M1⁺E2, rather than E1⁺M2. This is in keeping with their interpretation as intraband transitions and permits the calculation of the relevant reduced transition probabilities where level T_1/2 values are known.

M(γ): For levels having known half-lives, the multipolarities of the crossover quadrupole (ΔJ=2) transitions can be assigned as E2, since RUL eliminates the M2 possibility.

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
18.90	5/2+	< 50 ns	18.90 12	(M1)		67.7	B(M1)(W.u.)>0.00092, α=67.7 16
78.20	7/2-	110 ns 3	78.20 3	E1		0.635	B(E1)(W.u.)=2.66E-6 8, α=0.635
254.80	11/2-		105.6 1	M1+E2	0.23 6
347.89	11/2+		186.1 1	M1+E2	0.64 13
417.50	13/2-		162.7 1	M1+E2	0.26 3
557.34	13/2+		209.5 1	M1+E2	0.67 18
577.40	15/2-	7.5 ps 17	159.9 1	M1+E2	0.162 22	0.810	B(E2)(W.u.)=1.3×10² 5, B(M1)(W.u.)=0.26 6, α=0.810
577.40	15/2-	7.5 ps 17	322.6 1	E2		0.0575	B(E2)(W.u.)=1.3×10² 3, α=0.0575
788.50	15/2+		231.2	M1+E2	0.55 7
815.60	17/2-	3.6 ps 11	238.2 1	M1+E2	0.17 3	0.267	B(E2)(W.u.)=54 25, B(M1)(W.u.)=0.21 7, α=0.267
815.60	17/2-	3.6 ps 11	398.1 1	E2		0.0314	B(E2)(W.u.)=1.1×10² 4, α=0.0314
1008.40	19/2-	2.6 ps 10	192.8 1	M1+E2	0.15 3	0.480	B(E2)(W.u.)=1.1×10² 7, B(M1)(W.u.)=0.35 16, α=0.480
1008.40	19/2-	2.6 ps 10	431.0 1	E2		0.0253	B(E2)(W.u.)=1.5×10² 6, α=0.0253
1036.73	17/2+		248.2 1	M1+E2	0.45 13
1305.03	19/2+		268.3 1	M1+E2	0.48 20
1310.10	21/2-	1.7 ps 4	301.7 1	M1+E2	0.26 3	0.1381	B(E2)(W.u.)=63 21, B(M1)(W.u.)=0.17 4, α=0.1381 22
1310.10	21/2-	1.7 ps 4	494.5 1	E2		0.01762	B(E2)(W.u.)=1.2×10² 3, α=0.01762
1496.1	21/2-	2.7 ps 3	416.0 1	E2		0.0279	B(E2)(W.u.)=3.1×10² 4, α=0.0279
1525.53	23/2-	1.1 ps 3	215.4 1	M1+E2	0.18 4	0.352	B(E2)(W.u.)=1.9×10² 10, B(M1)(W.u.)=0.55 16, α=0.352 6
1525.53	23/2-	1.1 ps 3	517.1 2	E2		0.01572	B(E2)(W.u.)=1.6×10² 5, α=0.01572
1581.65	21/2+		276.7 2	M1+E2	0.46 16
1873.97	25/2-	0.55 ps 7	348.4 2	M1+E2	0.227 19	0.0947	B(E2)(W.u.)=75 16, B(M1)(W.u.)=0.36 5, α=0.0947
1873.97	25/2-	0.55 ps 7	563.9 1	E2		0.01267	B(E2)(W.u.)=1.9×10² 3, α=0.01267
1876.72	23/2+		295	M1+E2	0.42 9
1996.2	25/2-	0.96 ps 5	500.1 2	E2		0.01712	B(E2)(W.u.)=356 19, α=0.01712
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2108.95	27/2-	1.0 ps 3	235.0 1	M1+E2	0.128 23	0.279	B(E2)(W.u.)=5.×10¹ 3, B(M1)(W.u.)=0.37 12, α=0.279
2108.95	27/2-	1.0 ps 3	583.4 1	E2		0.01167	B(E2)(W.u.)=1.1×10² 4, α=0.01167
2480.95	29/2-	0.49 ps 14	372.0	M1+E2	0.15 3	0.0808	B(E2)(W.u.)=22 11, B(M1)(W.u.)=0.27 8, α=0.0808
2480.95	29/2-	0.49 ps 14	607.0 2	E2		0.01061	B(E2)(W.u.)=1.7×10² 5, α=0.01061
2736.57	31/2-		255.6 2	M1+E2	0.125 17
4012.7	41/2-	0.42 ps 10	273.1 1	[M1+E2]	0.3 LT	0.187	B(E2)(W.u.)<8.3×10², B(M1)(W.u.)=1.2 3, α=0.187 4
4012.7	41/2-	0.42 ps 10	536.2	[E2]			B(E2)(W.u.)=2.6×10² 7
4330.4	43/2-	0.42 ps 10	317.7 1	[M1+E2]	0.3 LT	0.122	B(E2)(W.u.)<3.7×10², B(M1)(W.u.)>0.50, α=0.122 4
4330.4	43/2-	0.42 ps 10	590.6 2	E2		0.01133	B(E2)(W.u.)=1.8×10² 5, α=0.01133
4656.0	45/2-	0.28 ps +15-8	325.1	[M1+E2]	0.3 LT	0.114	B(E2)(W.u.)<2.7×10², B(M1)(W.u.)>0.64, α=0.114 3
4656.0	45/2-	0.28 ps +15-8	643.9	[E2]			B(E2)(W.u.)=2.3×10² +7-13
5017.3	47/2-	0.21 ps +21-12	361.5	[M1+E2]	0.3 LT	0.0862	B(E2)(W.u.)<2.2×10², B(M1)(W.u.)>0.64, α=0.0862 23
5017.3	47/2-	0.21 ps +21-12	686.8	E2			B(E2)(W.u.)=2.2×10² +13-22
5394.1	49/2-	0.14 ps 3	376.6	[M1+E2]	0.3 LT	0.0774	B(E2)(W.u.)<3.1×10², B(M1)(W.u.)=0.8 3, α=0.0774 21
5394.1	49/2-	0.14 ps 3	738.1	[E2]			B(E2)(W.u.)=2.5×10² 6
5789.1	51/2-	0.10 ps 3	394.8	[M1+E2]	0.3 LT	0.0683	B(E2)(W.u.)<4.7×10², B(M1)(W.u.)>0.83, α=0.0683 19
5789.1	51/2-	0.10 ps 3	771.9	[E2]			B(E2)(W.u.)=2.4×10² 8
6633.4	(55/2-)	0.11 ps 4	844.3	[E2]			B(E2)(W.u.)=2.3×10² 9
7110.3	(57/2-)	0.08 ps 4	893.7	[E2]			B(E2)(W.u.)=2.4×10² 12
7533.8	(59/2-)	0.07 ps 3	900.4	[E2]			B(E2)(W.u.)=2.6×10² 12
8052.8	(61/2-)	0.07 ps 2	942.5	[E2]			B(E2)(W.u.)=2.1×10² 6
8476.3	(63/2-)	0.07 ps 2	942.5	[E2]			B(E2)(W.u.)=2.1×10² 6
9034.1	(65/2-)	0.11 ps 4	981.3	[E2]			B(E2)(W.u.)=1.1×10² 4
9457.6	(67/2-)	0.11 ps 4	981.3	[E2]			B(E2)(W.u.)=1.1×10² 4

Q(β-)=-4.06×10³ keV 4	S(n)= 9.67×10³ keV 5	S(p)= 3.12×10³ keV 4	Q(α)= 2.51×10³ keV 4
Reference: 2012WA38

References:
A	¹²⁸Te(³⁷Cl,4nγ):SD	B	¹⁵²Sm(¹⁴N,5nγ),¹⁶⁵Ho(⁴He,⁸NG)
C	¹²⁸Te(³⁷Cl,4nγ)	D	¹⁶¹Yb ε decay

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0	B C D	7/2+	30.2 m 8 % ε = 100
7.51 24	B D	1/2+	% IT = ? % ε = ?	7.4S		[M3]	0	7/2+
18.90 9	B C D	5/2+	< 50 ns	18.90 12	100	(M1)	0	7/2+
22.84 17	B C D	3/2+		15.4S	100		7.51	1/2+
78.20 3	B C D	7/2-	110 ns 3	78.20 3	100	E1	0	7/2+
149.20 9	B C	9/2-		71.0 1	100	D	78.20	7/2-
159.11 11	B C D	7/2+		140.25 8	100	D	18.90	5/2+
161.81 8	B C	9/2+		161.8 1	100		0	7/2+
167.28 18	B D	5/2+		144.43 6	100		22.84	3/2+
211.10 17	B C D	7/2+		188.28 5	100		22.84	3/2+
254.80 9	B C	11/2-		105.6 1 176.6 1	100 29 1	M1+E2 E2	149.20 78.20	9/2- 7/2-
326.70 13	B C	9/2+		167.6 1 307.8 2	100 21 21.1 14	D	159.11 18.90	7/2+ 5/2+
337.55 17	D	1/2+,3/2+		314.70 15 318.63 18 330.10 24	97 4 23.3 19 100 6	M1(+E2) M1(+E2)	22.84 18.90 7.51	3/2+ 5/2+ 1/2+
347.89 8	B C	11/2+		186.1 1 347.9 1	53.9 21 100 5	M1+E2	161.81 0	9/2+ 7/2+
367.46 25	B D	1/2-		344.72 28 359.92 17	100 9 77 5		22.84 7.51	3/2+ 1/2+
376.64 18	B C	5/2-		353.7 2 357.7	100 ≤120		22.84 18.90	3/2+ 5/2+
417.50 10	B C	13/2-		162.7 1 268.3 1	100 34.7 5	M1+E2 E2	254.80 149.20	11/2- 9/2-
433.31 20	D	3/2+,5/2,7/2+		222.37 20 266.0 5 410.44 17	19 3 64 21 100 7		211.10 167.28 22.84	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
465.80 21	D			298.46 15 443.02 24	100 6 30 5		167.28 22.84	5/2+ 3/2+
515.75 15	B C	11/2+		189.0 1 356.6	100 ≤127	D	326.70 159.11	9/2+ 7/2+
516.57 17	B C	9/2-		139.9 1 305.5 2	≤172 100 2		376.64 211.10	5/2- 7/2+
531.45 15	B C	11/2+		204.8 1 320.4 2 372.3	32 1 100 2 9.3 5		326.70 211.10 159.11	9/2+ 7/2+ 7/2+
557.34 10	B C	13/2+		209.5 1 395.5 1	70 15 100	M1+E2 E2	347.89 161.81	11/2+ 9/2+
577.40 11	B C	15/2-	7.5 ps 17	159.9 1 322.6 1	100 84 3	M1+E2 E2	417.50 254.80	13/2- 11/2-
625.53 20	D			159.67 19 192.26 14 458.22 16	21 5 20 2 100 4		465.80 433.31 167.28	3/2+,5/2,7/2+ 5/2+
638.74 12	D			560.48 20	100		78.20	7/2-
647.89 13	D			569.73 14	100		78.20	7/2-
678.08 9	D	5/2-		519.12 20 599.88 10 659.10 14	2.4 3 100 5 12.5 5	M1(+E2)	159.11 78.20 18.90	7/2+ 7/2- 5/2+
709.66 9	D	5/2-		70.90 10 550.0 5 631.45 10 690.75 20	3.5 8 1.9 6 100 5 7.8 7	M1(+E2)	638.74 159.11 78.20 18.90	7/2+ 7/2- 5/2+
756.39 15	B C	13/2-		225.0 1 239.8 1 240.6 1	100 2 ≤51 ≤51		531.45 516.57 515.75	11/2+ 9/2- 11/2+
788.50 12	B C	15/2+		231.2 440.6 1	36.5 24 100	M1+E2	557.34 347.89	13/2+ 11/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
815.60 12	B C	17/2-	3.6 ps 11	238.2 1 398.1 1	100 77 4	M1+E2 E2	577.40 417.50	15/2- 13/2-
989.25 18	B	15/2+		457.8 1	100		531.45	11/2+
1008.40 13	B C	19/2-	2.6 ps 10	192.8 1 431.0 1	57 11 100	M1+E2 E2	815.60 577.40	17/2- 15/2-
1036.73 12	B C	17/2+		248.2 1 479.4 1	20 1 100	M1+E2 E2	788.50 557.34	15/2+ 13/2+
1080.1 3	B C	17/2-		323.7 2	100	E2	756.39	13/2-
1180.70 12	D			471.00 10 532.91 23 1022.0 4	100 6 38 6 31 4		709.66 647.89 159.11	5/2- 7/2+
1305.03 14	B C	19/2+		268.3 1 516.6 2	18.9 6 100	M1+E2 E2	1036.73 788.50	17/2+ 15/2+
1310.10 14	B C	21/2-	1.7 ps 4	301.7 1 494.5 1	71.4 20 100	M1+E2 E2	1008.40 815.60	19/2- 17/2-
1496.1 3	B C	21/2-	2.7 ps 3	416.0 1	100	E2	1080.1	17/2-
1525.53 16	B C	23/2-	1.1 ps 3	215.4 1 517.1 2	47 3 100	M1+E2 E2	1310.10 1008.40	21/2- 19/2-
1581.65 15	B C	21/2+		276.7 2 544.9 1	32.8 14 100	M1+E2 E2	1305.03 1036.73	19/2+ 17/2+
1873.97 16	B C	25/2-	0.55 ps 7	348.4 2 563.9 1	71 4 100	M1+E2 E2	1525.53 1310.10	23/2- 21/2-
1876.72 24	B C	23/2+		295 571.7 2	14.1 8 100	M1+E2 E2	1581.65 1305.03	21/2+ 19/2+
1996.2 4	B C	25/2-	0.96 ps 5	500.1 2	100	E2	1496.1	21/2-
2108.95 17	B C	27/2-	1.0 ps 3	235.0 1 583.4 1	31 4 100	M1+E2 E2	1873.97 1525.53	25/2- 23/2-
2172.26 24	B C	25/2+		296 590.6 2	9.3 10 100	E2	1876.72 1581.65	23/2+ 21/2+
2478.0 3	B C	27/2+		306 601.3 2	44.4 25 100		2172.26 1876.72	25/2+ 23/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2480.95 22	B C	29/2-	0.49 ps 14	372.0 607.0 2	49 3 100	M1+E2 E2	2108.95 1873.97	27/2- 25/2-
2570.3 4	B C	29/2-		574.1 2	100		1996.2	25/2-
2736.57 22	B C	31/2-		255.6 2 627.6 2	35.5 25 100	M1+E2 E2	2480.95 2108.95	29/2- 27/2-
2786	C	29/2+		308 614	16.9 25 100		2478.0 2172.26	27/2+ 25/2+
3050.89 23	B C	33/2-		314.4 1 570.0 2	69.4 14 100	D E2	2736.57 2480.95	31/2- 29/2-
3110	C	31/2+		324 632	≤13 100		2786 2478.0	29/2+ 27/2+
3117	C	(33/2-)		381 636	86.5 19 100 6		2736.57 2480.95	31/2- 29/2-
3206.4 5	B C	33/2-		636.1 3	100		2570.3	29/2-
3255.34 24	B C	35/2-		204.5 1 518.4 2	100 65 13	D	3050.89 2736.57	33/2- 31/2-
3381	B C	35/2-		264? 330 644.2			3117 3050.89 2736.57	(33/2-) 33/2- 31/2-
3441	C	33/2+		331 655	11.2 13 100		3110 2786	31/2+ 29/2+
3476.75 31	B C	37/2-		221.4 1 425.9 1	100 66 5	D	3255.34 3050.89	35/2- 33/2-
3723?	C	(37/2-)		342? 606?			3381 3117	35/2- (33/2-)
3739.7 3	B C	39/2-		263.0 2 358 484.3 1	100 5 12.7 5 59 5	E2	3476.75 3381 3255.34	37/2- 35/2- 35/2-
3779	C	35/2+		338 669	12.7 19 100		3441 3110	33/2+ 31/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3886	C	(37/2-)		680	100		3206.4	33/2-
4012.7 3	B C	41/2-	0.42 ps 10	273.1 1 536.2	100 92 3	[M1+E2] [E2]	3739.7 3476.75	39/2- 37/2-
4084?	C	(39/2-)		361? 703?	33 2 100 3		3723 3381	(37/2-) 35/2-
4130	C	37/2+		351? 689	6.9 5 100 5		3779 3441	35/2+ 33/2+
4330.4 3	B C	43/2-	0.42 ps 10	317.7 1 590.6 2	92 8 100	[M1+E2] E2	4012.7 3739.7	41/2- 39/2-
4492	C	(39/2+)		713	100		3779	35/2+
4578	C	(41/2-)		692	100		3886	(37/2-)
4656.0 7	B C	45/2-	0.28 ps +15-8	325.1 643.9	46 3 100	[M1+E2] [E2]	4330.4 4012.7	43/2- 41/2-
4867	C	(41/2+)		737	100		4130	37/2+
5017.3	C	47/2-	0.21 ps +21-12	361.5 686.8	48 5 100	[M1+E2] E2	4656.0 4330.4	45/2- 43/2-
5267	C	(43/2+)		775	100		4492	(39/2+)
5270	C	(45/2-)		692	100		4578	(41/2-)
5394.1	C	49/2-	0.14 ps 3	376.6 738.1	37 11 100	[M1+E2] [E2]	5017.3 4656.0	47/2- 45/2-
5675	C	(45/2+)		808	100		4867	(41/2+)
5789.1	C	51/2-	0.10 ps 3	394.8 771.9	63 8 100	[M1+E2] [E2]	5394.1 5017.3	49/2- 47/2-
5988	C	(49/2-)		718	100		5270	(45/2-)
6113	C	(47/2+)		846	100		5267	(43/2+)
6216.6	C	53/2-	≤ 0.18 ps	426.7? 822.5	100	[E2]	5789.1 5394.1	51/2- 49/2-
6560	C	(49/2+)		885	100		5675	(45/2+)
6633.4	C	(55/2-)	0.11 ps 4	844.3	100	[E2]	5789.1	51/2-
6726?	C	(53/2-)		738?	100		5988	(49/2-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7037?	C	(51/2+)		924?	100		6113	(47/2+)
7110.3	C	(57/2-)	0.08 ps 4	893.7	100	[E2]	6216.6	53/2-
7519?	C	(53/2+)		959?	100		6560	(49/2+)
7533.8	C	(59/2-)	0.07 ps 3	900.4	100	[E2]	6633.4	(55/2-)
8052.8	C	(61/2-)	0.07 ps 2	942.5	100	[E2]	7110.3	(57/2-)
8476.3	C	(63/2-)	0.07 ps 2	942.5	100	[E2]	7533.8	(59/2-)
9034.1	C	(65/2-)	0.11 ps 4	981.3	100	[E2]	8052.8	(61/2-)
9457.6	C	(67/2-)	0.11 ps 4	981.3	100	[E2]	8476.3	(63/2-)
10059.6	C	(69/2-)		1025.5	100		9034.1	(65/2-)
10483.1	C	(71/2-)		1025.5	100		9457.6	(67/2-)
11141?	C	(73/2-)		1081?	100		10059.6	(69/2-)
11582?	C	(75/2-)		1102?	100		10483.1	(71/2-)
X	A	J
881+X	A	J+2		881	100		X	J
1814+X	A	J+4		933	100		881+X	J+2
2795+X	A	J+6		981	100		1814+X	J+4
3825+X	A	J+8		1030	100		2795+X	J+6
4904+X	A	J+10		1079	100		3825+X	J+8
6034+X	A	J+12		1130	100		4904+X	J+10
7215+X	A	J+14		1181	100		6034+X	J+12
8446+X	A	J+16		1231	100		7215+X	J+14
9738+X?	A	J+18		1292?	100		8446+X	J+16

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - 7/2[404] band. α=-1/2 branch.
0	7/2+	30.2 m 8 % ε = 100
347.89 8	11/2+		186.1 1 347.9 1	53.9 21 100 5	M1+E2	161.81 0	9/2+ 7/2+
788.50 12	15/2+		231.2 440.6 1	36.5 24 100	M1+E2	557.34 347.89	13/2+ 11/2+
1305.03 14	19/2+		268.3 1 516.6 2	18.9 6 100	M1+E2 E2	1036.73 788.50	17/2+ 15/2+
1876.72 24	23/2+		295 571.7 2	14.1 8 100	M1+E2 E2	1581.65 1305.03	21/2+ 19/2+
2478.0 3	27/2+		306 601.3 2	44.4 25 100		2172.26 1876.72	25/2+ 23/2+
3110	31/2+		324 632	≤13 100		2786 2478.0	29/2+ 27/2+
3779	35/2+		338 669	12.7 19 100		3441 3110	33/2+ 31/2+
4492	(39/2+)		713	100		3779	35/2+
5267	(43/2+)		775	100		4492	(39/2+)
6113	(47/2+)		846	100		5267	(43/2+)
7037	(51/2+)		924?	100		6113	(47/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - 1/2[411] band.
7.51 24	1/2+	% IT = ? % ε = ?
22.84 17	3/2+		15.4S	100		7.51	1/2+
167.28 18	5/2+		144.43 6	100		22.84	3/2+
211.10 17	7/2+		188.28 5	100		22.84	3/2+
531.45 15	11/2+		204.8 1 320.4 2 372.3	32 1 100 2 9.3 5		326.70 211.10 159.11	9/2+ 7/2+ 7/2+
989.25 18	15/2+		457.8 1	100		531.45	11/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - 5/2[402] band.
18.90 9	5/2+	< 50 ns
159.11 11	7/2+		140.25 8	100	D	18.90	5/2+
326.70 13	9/2+		167.6 1 307.8 2	100 21 21.1 14	D	159.11 18.90	7/2+ 5/2+
515.75 15	11/2+		189.0 1 356.6	100 ≤127	D	326.70 159.11	9/2+ 7/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - 7/2[523] band, α=-1/2 branch.
78.20 3	7/2-	110 ns 3
254.80 9	11/2-		105.6 1 176.6 1	100 29 1	M1+E2 E2	149.20 78.20	9/2- 7/2-
577.40 11	15/2-	7.5 ps 17	159.9 1 322.6 1	100 84 3	M1+E2 E2	417.50 254.80	13/2- 11/2-
1008.40 13	19/2-	2.6 ps 10	192.8 1 431.0 1	57 11 100	M1+E2 E2	815.60 577.40	17/2- 15/2-
1525.53 16	23/2-	1.1 ps 3	215.4 1 517.1 2	47 3 100	M1+E2 E2	1310.10 1008.40	21/2- 19/2-
2108.95 17	27/2-	1.0 ps 3	235.0 1 583.4 1	31 4 100	M1+E2 E2	1873.97 1525.53	25/2- 23/2-
2736.57 22	31/2-		255.6 2 627.6 2	35.5 25 100	M1+E2 E2	2480.95 2108.95	29/2- 27/2-
3255.34 24	35/2-		204.5 1 518.4 2	100 65 13	D	3050.89 2736.57	33/2- 31/2-
3739.7 3	39/2-		263.0 2 358 484.3 1	100 5 12.7 5 59 5	E2	3476.75 3381 3255.34	37/2- 35/2- 35/2-
4330.4 3	43/2-	0.42 ps 10	317.7 1 590.6 2	92 8 100	[M1+E2] E2	4012.7 3739.7	41/2- 39/2-
5017.3	47/2-	0.21 ps +21-12	361.5 686.8	48 5 100	[M1+E2] E2	4656.0 4330.4	45/2- 43/2-
5789.1	51/2-	0.10 ps 3	394.8 771.9	63 8 100	[M1+E2] [E2]	5394.1 5017.3	49/2- 47/2-
6633.4	(55/2-)	0.11 ps 4	844.3	100	[E2]	5789.1	51/2-
7533.8	(59/2-)	0.07 ps 3	900.4	100	[E2]	6633.4	(55/2-)
8476.3	(63/2-)	0.07 ps 2	942.5	100	[E2]	7533.8	(59/2-)
9457.6	(67/2-)	0.11 ps 4	981.3	100	[E2]	8476.3	(63/2-)
10483.1	(71/2-)		1025.5	100		9457.6	(67/2-)
11582	(75/2-)		1102?	100		10483.1	(71/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - 7/2[523] band; α=+1/2 branch.
149.20 9	9/2-
417.50 10	13/2-		162.7 1 268.3 1	100 34.7 5	M1+E2 E2	254.80 149.20	11/2- 9/2-
815.60 12	17/2-	3.6 ps 11	238.2 1 398.1 1	100 77 4	M1+E2 E2	577.40 417.50	15/2- 13/2-
1310.10 14	21/2-	1.7 ps 4	301.7 1 494.5 1	71.4 20 100	M1+E2 E2	1008.40 815.60	19/2- 17/2-
1873.97 16	25/2-	0.55 ps 7	348.4 2 563.9 1	71 4 100	M1+E2 E2	1525.53 1310.10	23/2- 21/2-
2480.95 22	29/2-	0.49 ps 14	372.0 607.0 2	49 3 100	M1+E2 E2	2108.95 1873.97	27/2- 25/2-
3050.89 23	33/2-		314.4 1 570.0 2	69.4 14 100	D E2	2736.57 2480.95	31/2- 29/2-
3476.75 31	37/2-		221.4 1 425.9 1	100 66 5	D	3255.34 3050.89	35/2- 33/2-
4012.7 3	41/2-	0.42 ps 10	273.1 1 536.2	100 92 3	[M1+E2] [E2]	3739.7 3476.75	39/2- 37/2-
4656.0 7	45/2-	0.28 ps +15-8	325.1 643.9	46 3 100	[M1+E2] [E2]	4330.4 4012.7	43/2- 41/2-
5394.1	49/2-	0.14 ps 3	376.6 738.1	37 11 100	[M1+E2] [E2]	5017.3 4656.0	47/2- 45/2-
6216.6	53/2-	≤ 0.18 ps	426.7? 822.5	100	[E2]	5789.1 5394.1	51/2- 49/2-
7110.3	(57/2-)	0.08 ps 4	893.7	100	[E2]	6216.6	53/2-
8052.8	(61/2-)	0.07 ps 2	942.5	100	[E2]	7110.3	(57/2-)
9034.1	(65/2-)	0.11 ps 4	981.3	100	[E2]	8052.8	(61/2-)
10059.6	(69/2-)		1025.5	100		9034.1	(65/2-)
11141	(73/2-)		1081?	100		10059.6	(69/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - 1/2[541] band. α=+1/2 branch.
367.46 25	1/2-
376.64 18	5/2-		353.7 2 357.7	100 ≤120		22.84 18.90	3/2+ 5/2+
516.57 17	9/2-		139.9 1 305.5 2	≤172 100 2		376.64 211.10	5/2- 7/2+
756.39 15	13/2-		225.0 1 239.8 1 240.6 1	100 2 ≤51 ≤51		531.45 516.57 515.75	11/2+ 9/2- 11/2+
1080.1 3	17/2-		323.7 2	100	E2	756.39	13/2-
1496.1 3	21/2-	2.7 ps 3	416.0 1	100	E2	1080.1	17/2-
1996.2 4	25/2-	0.96 ps 5	500.1 2	100	E2	1496.1	21/2-
2570.3 4	29/2-		574.1 2	100		1996.2	25/2-
3206.4 5	33/2-		636.1 3	100		2570.3	29/2-
3886	(37/2-)		680	100		3206.4	33/2-
4578	(41/2-)		692	100		3886	(37/2-)
5270	(45/2-)		692	100		4578	(41/2-)
5988	(49/2-)		718	100		5270	(45/2-)
6726	(53/2-)		738?	100		5988	(49/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - possible 3/2[411] band.
337.55 17	1/2+,3/2+
433.31 20	3/2+,5/2,7/2+		222.37 20 266.0 5 410.44 17	19 3 64 21 100 7		211.10 167.28 22.84	7/2+ 5/2+ 3/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 8 - TRIAXIAL SD band.
X	J
881+X	J+2		881	100		X	J
1814+X	J+4		933	100		881+X	J+2
2795+X	J+6		981	100		1814+X	J+4
3825+X	J+8		1030	100		2795+X	J+6
4904+X	J+10		1079	100		3825+X	J+8
6034+X	J+12		1130	100		4904+X	J+10
7215+X	J+14		1181	100		6034+X	J+12
8446+X	J+16		1231	100		7215+X	J+14
9738+X	J+18		1292?	100		8446+X	J+16

E(level)	J^π(level)	T_1/2(level)	Comments
0	7/2+	30.2 m 8 % ε = 100	Q=+2.90 7, μ=+2.40 2 From an evaluation of data on nuclear rms charge radii, 2004An14 report <r²>^1/2=5.162 fm 5. E(level): From an evaluation of data on nuclear rms charge radii, 2004An14 report <r²>^1/2=5.162 fm 5. 7/2[404] band. α=-1/2 branch.
7.51	1/2+	% IT = ? % ε = ?	Because of its low energy and its sole possible γ-decay mode, namely M3 to the g.s., this level is expected to have a half-life of the order of minutes. In such a case, an ε+β⁺ decay branch would be expected. Neither of these possibilities, however, has yet been reported. E(level): Because of its low energy and its sole possible γ-decay mode, namely M3 to the g.s., this level is expected to have a half-life of the order of minutes. In such a case, an ε+β⁺ decay branch would be expected. Neither of these possibilities, however, has yet been reported. 1/2[411] band. J^π(level): The pattern of transitions populating of these levels from higher-lying levels suggests that they are members of the same rotational band. The spin sequence adopted here is consistent with the pattern of populating γ rays; and the energy spacings within the proposed band are what is expected for the proposed configuration, namely 1/2[411], an orbital that is expected to occur at a low energy in ¹⁶¹Tm.
18.90	5/2+	< 50 ns	E(level): 5/2[402] band.
22.84	3/2+		E(level): 1/2[411] band. J^π(level): The pattern of transitions populating of these levels from higher-lying levels suggests that they are members of the same rotational band. The spin sequence adopted here is consistent with the pattern of populating γ rays; and the energy spacings within the proposed band are what is expected for the proposed configuration, namely 1/2[411], an orbital that is expected to occur at a low energy in ¹⁶¹Tm.
78.20	7/2-	110 ns 3	E(level): 7/2[523] band, α=-1/2 branch.
149.20	9/2-		E(level): 7/2[523] band; α=+1/2 branch.
159.11	7/2+		E(level): 5/2[402] band.
167.28	5/2+		E(level): 1/2[411] band. J^π(level): The pattern of transitions populating of these levels from higher-lying levels suggests that they are members of the same rotational band. The spin sequence adopted here is consistent with the pattern of populating γ rays; and the energy spacings within the proposed band are what is expected for the proposed configuration, namely 1/2[411], an orbital that is expected to occur at a low energy in ¹⁶¹Tm.
211.10	7/2+		E(level): 1/2[411] band. J^π(level): The pattern of transitions populating of these levels from higher-lying levels suggests that they are members of the same rotational band. The spin sequence adopted here is consistent with the pattern of populating γ rays; and the energy spacings within the proposed band are what is expected for the proposed configuration, namely 1/2[411], an orbital that is expected to occur at a low energy in ¹⁶¹Tm.
254.80	11/2-		E(level): 7/2[523] band, α=-1/2 branch.
326.70	9/2+		E(level): 5/2[402] band.
337.55	1/2+,3/2+		E(level): possible 3/2[411] band.
347.89	11/2+		E(level): 7/2[404] band. α=-1/2 branch.
367.46	1/2-		E(level): 1/2[541] band. α=+1/2 branch.
376.64	5/2-		E(level): 1/2[541] band. α=+1/2 branch.
417.50	13/2-		E(level): 7/2[523] band; α=+1/2 branch.
433.31	3/2+,5/2,7/2+		E(level): possible 3/2[411] band.
515.75	11/2+		E(level): 5/2[402] band.
516.57	9/2-		E(level): 1/2[541] band. α=+1/2 branch.
531.45	11/2+		E(level): 1/2[411] band.
577.40	15/2-	7.5 ps 17	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From recoil-distance measurements in ¹²⁸Te(³⁷Cl,4nγ).
756.39	13/2-		E(level): 1/2[541] band. α=+1/2 branch.
788.50	15/2+		E(level): 7/2[404] band. α=-1/2 branch.
815.60	17/2-	3.6 ps 11	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From recoil-distance measurements in ¹²⁸Te(³⁷Cl,4nγ).
989.25	15/2+		E(level): 1/2[411] band.
E(level)	J^π(level)	T_1/2(level)	Comments
1008.40	19/2-	2.6 ps 10	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From recoil-distance measurements in ¹²⁸Te(³⁷Cl,4nγ).
1080.1	17/2-		E(level): 1/2[541] band. α=+1/2 branch.
1305.03	19/2+		E(level): 7/2[404] band. α=-1/2 branch.
1310.10	21/2-	1.7 ps 4	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From recoil-distance measurements in ¹²⁸Te(³⁷Cl,4nγ).
1496.1	21/2-	2.7 ps 3	E(level): 1/2[541] band. α=+1/2 branch. T_1/2(level): From recoil-distance measurements in ¹²⁸Te(³⁷Cl,4nγ).
1525.53	23/2-	1.1 ps 3	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From recoil-distance measurements in ¹²⁸Te(³⁷Cl,4nγ).
1873.97	25/2-	0.55 ps 7	E(level): 7/2[523] band; α=+1/2 branch.
1876.72	23/2+		E(level): 7/2[404] band. α=-1/2 branch.
1996.2	25/2-	0.96 ps 5	E(level): 1/2[541] band. α=+1/2 branch. T_1/2(level): From recoil-distance measurements in ¹²⁸Te(³⁷Cl,4nγ).
2108.95	27/2-	1.0 ps 3	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From recoil-distance measurements in ¹²⁸Te(³⁷Cl,4nγ).
2478.0	27/2+		E(level): 7/2[404] band. α=-1/2 branch.
2480.95	29/2-	0.49 ps 14	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From recoil-distance measurements in ¹²⁸Te(³⁷Cl,4nγ).
2570.3	29/2-		E(level): 1/2[541] band. α=+1/2 branch.
2736.57	31/2-		E(level): 7/2[523] band, α=-1/2 branch.
3050.89	33/2-		E(level): 7/2[523] band; α=+1/2 branch.
3110	31/2+		E(level): 7/2[404] band. α=-1/2 branch.
3206.4	33/2-		E(level): 1/2[541] band. α=+1/2 branch.
3255.34	35/2-		E(level): 7/2[523] band, α=-1/2 branch.
3476.75	37/2-		E(level): 7/2[523] band; α=+1/2 branch.
3739.7	39/2-		E(level): 7/2[523] band, α=-1/2 branch.
3779	35/2+		E(level): 7/2[404] band. α=-1/2 branch.
3886	(37/2-)		E(level): 1/2[541] band. α=+1/2 branch.
4012.7	41/2-	0.42 ps 10	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
4330.4	43/2-	0.42 ps 10	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
4492	(39/2+)		E(level): 7/2[404] band. α=-1/2 branch.
E(level)	J^π(level)	T_1/2(level)	Comments
4578	(41/2-)		E(level): 1/2[541] band. α=+1/2 branch.
4656.0	45/2-	0.28 ps +15-8	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
5017.3	47/2-	0.21 ps +21-12	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
5267	(43/2+)		E(level): 7/2[404] band. α=-1/2 branch.
5270	(45/2-)		E(level): 1/2[541] band. α=+1/2 branch.
5394.1	49/2-	0.14 ps 3	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
5789.1	51/2-	0.10 ps 3	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
5988	(49/2-)		E(level): 1/2[541] band. α=+1/2 branch.
6113	(47/2+)		E(level): 7/2[404] band. α=-1/2 branch.
6216.6	53/2-	≤ 0.18 ps	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
6633.4	(55/2-)	0.11 ps 4	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
6726	(53/2-)		E(level): 1/2[541] band. α=+1/2 branch.
7037	(51/2+)		E(level): 7/2[404] band. α=-1/2 branch.
7110.3	(57/2-)	0.08 ps 4	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
7533.8	(59/2-)	0.07 ps 3	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
8052.8	(61/2-)	0.07 ps 2	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
8476.3	(63/2-)	0.07 ps 2	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
9034.1	(65/2-)	0.11 ps 4	E(level): 7/2[523] band; α=+1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
9457.6	(67/2-)	0.11 ps 4	E(level): 7/2[523] band, α=-1/2 branch. T_1/2(level): From DSAM studies in ¹²⁸Te(³⁷Cl,4nγ). See the comments there regarding the evaluator’s treatment of those data.
10059.6	(69/2-)		E(level): 7/2[523] band; α=+1/2 branch.
10483.1	(71/2-)		E(level): 7/2[523] band, α=-1/2 branch.
11141	(73/2-)		E(level): 7/2[523] band; α=+1/2 branch.
11582	(75/2-)		E(level): 7/2[523] band, α=-1/2 branch.
X	J		E(level): TRIAXIAL SD band.
881+X	J+2		E(level): TRIAXIAL SD band.
E(level)	J^π(level)	T_1/2(level)	Comments
1814+X	J+4		E(level): TRIAXIAL SD band.
2795+X	J+6		E(level): TRIAXIAL SD band.
3825+X	J+8		E(level): TRIAXIAL SD band.
4904+X	J+10		E(level): TRIAXIAL SD band.
6034+X	J+12		E(level): TRIAXIAL SD band.
7215+X	J+14		E(level): TRIAXIAL SD band.
8446+X	J+16		E(level): TRIAXIAL SD band.
9738+X	J+18		E(level): TRIAXIAL SD band.

E(level)	E(gamma)	Comments
18.90	18.90	M(γ): δ\|<0.10 (1981Ad02).
78.20	78.20	M(γ): δ\|<0.045 (1981Ad02).
211.10	188.28	M(γ): γ(θ) suggests γ is dipole, but placement has ΔJ=2. ce data suggest E1 or E2.
417.50	268.3	E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided
515.75	189.0	M(γ): From γ(θ), 1984Fo04.
515.75	356.6	I(γ): From 1995Sm02, where γ is part of a peak containing two γ’s.
516.57	139.9	I(γ): From 1995Sm02, where γ is part of a peak containing two γ’s.
756.39	239.8	I(γ): From 1995Sm02, where γ is part of a peak containing two γ’s.
756.39	240.6	I(γ): From 1995Sm02, where γ is part of a peak containing two γ’s.
1305.03	268.3	E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided
2172.26	590.6	E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided
3110	324	E(γ): 1995Sm02 report Eγ=234 for this transition. The evaluator has assumed that this is a misprint.
4330.4	590.6	E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided
4578	692	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
5270	692	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
8052.8	942.5	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
8476.3	942.5	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
9034.1	981.3	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
9457.6	981.3	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
10059.6	1025.5	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
10483.1	1025.5	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity