List of levels for 164HO

ADOPTED LEVELS, GAMMAS for ¹⁶⁴Ho

Authors: Balraj Singh and Jun Chen | Citation: Nucl. Data Sheets 147, 1 (2018) | Cutoff date: 30-Nov-2017

Full ENSDF file | Adopted Levels (PDF version)

Q(β-)=961.4 keV 14	S(n)= 6674.5 keV 14	S(p)= 5889.3 keV 14	Q(α)= 429.8 keV 18
Reference: 2017WA10

References:
A	¹⁶⁴Ho IT decay (36.6 M)	B	¹⁶⁰Gd(¹¹B,α3nγ)
C	¹⁶⁴Dy(p,nγ),(d,2nγ)	D	¹⁶⁵Ho(γ,n)
E	¹⁶⁵Ho(γ,nγ)	F	¹⁶⁵Ho(d,t)

Identification and production of ¹⁶⁴Ho by M.L. Pool and L.L. Quill, Phys. Rev. 53, 437 (1938) from bombardment of Ho and Y by fast neutrons

Hyperfine structure, and isotope-shift measurements for g.s.: 1987AlZU, 1987ArZT

For theoretical nuclear structure calculations, consult NSR database, for about 10 references. These are listed in the ENSDF dataset as document records

Q-value: S(2n)=15083 3, S(2p)=13880 40 (2017Wa10)

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A B C D E F	1+	28.8 m 5 % β^- = 40 5 % ε = 60 5
37.341 20	A B C D E F	2+	≤ 2.8 ns	37.34 2	100	M1+E2	0.0	1+
93.99 4	A B C D E F	3+		56.64 5 94.00 5	100 5 2.10 23	M1+E2 E2	37.341 0.0	2+ 1+
139.78 7	A B C D E F	6-	36.6 m 3 % IT = 100	45.79 6	100	E3	93.99	3+
167.4 4	B C D F	4+		73.7			93.99	3+
188.6 5	C	(3+)	≤ 0.5 ns	94.6		[M1]	93.99	3+
191.0 5	B F	6+		51.2			139.78	6-
193.3 4	B C	(1-)		156.0 193.3			37.341 0.0	2+ 1+
203.7 5	B C D F	7-		63.9			139.78	6-
207.8 3	B	(2-)		113.6 170.6 208.0			93.99 37.341 0.0	3+ 2+ 1+
236.1 4	B C D F	(3-)		198.8			37.341	2+
261.7 4	B C D F	5+		94.5 167.4			167.4 93.99	4+ 3+
273.8 4	B D F	(4-)		37.7 179.8			236.1 93.99	(3-) 3+
293.7 7	B F	(8-)		90.1			203.7	7-
297.4 7	C	(4+)		108.7			188.6	(3+)
317.3 8	B F	7+		126.3			191.0	6+
330.9 7	B	(5-)		163.5			167.4	4+
342.6 5	B C D F	5+	2.6 ns 2	202.8		[E1]	139.78	6-
370.2 6	B F	(6+)		108.5			261.7	5+
394 4	D F
398.2 9	B	(6-)		67.3			330.9	(5-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
406.5 7	B	(9-)		112.7 202.8			293.7 203.7	(8-) 7-
421 1	D F
429.9 7	C	(5+)		132.4 241.4			297.4 188.6	(4+) (3+)
452.4 8	B C F	6+		109.8			342.6	5+
460.9 9	B	(8+)		143.5			317.3	7+
486 2	F	(2+)
488.0 10	B	(7-)		89.8			398.2	(6-)
499 2	F
502.7 6	B	(7+)		132.5 241.0			370.2 261.7	(6+) 5+
540.3 7	B	(10-)		133.7 246.7			406.5 293.7	(9-) (8-)
558 1	F	(3+)
579.6 9	B C F	7+		127.3			452.4	6+
586.9 11	B	(8-)		99.0			488.0	(7-)
620 1	F	2-
621.7 9	B	(9+)		160.7 304.5			460.9 317.3	(8+) 7+
644.2 7	B	(8+)		141.3 274.0			502.7 370.2	(7+) (6+)
650 3	F	(4+)
670 2	F	3-
691 4	F
694.2 8	B	(11-)		153.9 287.6			540.3 406.5	(10-) (9-)
711.9 11	B	(9-)		125.1 223.8			586.9 488.0	(8-) (7-)
723.1 9	B C	(8+)		143.6 270.6			579.6 452.4	7+ 6+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
733 1	F	(5-)
777 2	F	(5+)
799.1 9	B	(10+)		177.5 338.1			621.7 460.9	(9+) (8+)
814.0 7	B	(9+)		169.8 311.5			644.2 502.7	(8+) (7+)
833 1	F	(4-)
843.1 11	B	(10-)		131.1 256.2			711.9 586.9	(9-) (8-)
863 4	F
867.0 8	B	(12-)		172.9 326.7			694.2 540.3	(11-) (10-)
881.5 9	B	(9+)		158.2 302.0			723.1 579.6	(8+) 7+
925 1	F	(3-)
967 5	F
985.1 7	B	(10+)		171.2 340.8			814.0 644.2	(9+) (8+)
992.8 9	B	(11+)		193.6 371.2			799.1 621.7	(10+) (9+)
994 4	F	(4-)
1006.7 11	B	(11-)		163.6 294.8			843.1 711.9	(10-) (9-)
1049.9 9	B	(10+)		168.4 326.9			881.5 723.1	(9+) (8+)
1058.2 8	B	(13-)		191.2 363.9			867.0 694.2	(12-) (11-)
1171.3 12	B	(12-)		164.5 328.1			1006.7 843.1	(11-) (10-)
1192.0 8	B	(11+)		206.7 378.2			985.1 814.0	(10+) (9+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1202.1 9	B	(12+)		209.4 403.1			992.8 799.1	(11+) (10+)
1234.8 10	B	(11+)		185.0 353.3			1049.9 881.5	(10+) (9+)
1265.3 9	B	(14-)		207.1 398.5			1058.2 867.0	(13-) (12-)
1377.2 12	B	(13-)		205.8 370.6			1171.3 1006.7	(12-) (11-)
1387.2 8	B	(12+)		195.1 402.0			1192.0 985.1	(11+) (10+)
1420.2 11	B	(12+)		370.3			1049.9	(10+)
1426.8 10	B	(13+)		224.8 433.7			1202.1 992.8	(12+) (11+)
1492.0 9	B	(15-)		226.8 433.6			1265.3 1058.2	(14-) (13-)
1577.2 12	B	(14-)		200.0 405.9			1377.2 1171.3	(13-) (12-)
1631.0 9	B	(13+)		243.8 439.1			1387.2 1192.0	(12+) (11+)
1666.0 10	B	(14+)		239.2 464.0			1426.8 1202.1	(13+) (12+)
1728.2 9	B	(16-)		236.3 462.9			1492.0 1265.3	(15-) (14-)
1825.7 12	B	(15-)		248.5 448.6			1577.2 1377.2	(14-) (13-)
1865.3 7	B	(14+)		477.4?			1387.2	(12+)
1919.0 10	B	(15+)		253.1 492.2			1666.0 1426.8	(14+) (13+)
1990.1 9	B	(17-)		261.9 498.1			1728.2 1492.0	(16-) (15-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2062.4 12	B	(16-)		236.7 485.2			1825.7 1577.2	(15-) (14-)
2113.5 8	B	(15+)		481.8?			1631.0	(13+)
2183.8 11	B	(16+)		517.8			1666.0	(14+)
2249.6 10	B	(18-)		259.2 521.3			1990.1 1728.2	(17-) (16-)
2350.1 13	B	(17-)		287.6 524.5			2062.4 1825.7	(16-) (15-)
2462.5 12	B	(17+)		543.5			1919.0	(15+)
2548.1 10	B	(19-)		298.5 558.4			2249.6 1990.1	(18-) (17-)
2623.9 13	B	(18-)		273.9 561.4			2350.1 2062.4	(17-) (16-)
2825.8 10	B	(20-)		277.7 575.9			2548.1 2249.6	(19-) (18-)
2941.0 13	B	(19-)		317.0 590.9			2623.9 2350.1	(18-) (17-)
3162.0 11	B	(21-)		336.1 614.1			2825.8 2548.1	(20-) (19-)
3250.4 14	B	(20-)		626.5			2623.9	(18-)
3452.0 11	B	(22-)		626.2			2825.8	(20-)
3826.7 12	B	(23-)		664.7			3162.0	(21-)
4125.5 13	B	(24-)		673.5			3452.0	(22-)
4541.8 9	B	(25-)		714.8?			3826.7	(23-)

E(level): From least-squares fit to Eγ data. ΔEγ=0.5 keV assigned by the evaluators when not stated. See ¹⁶⁴Dy(p,nγ),(d,2nγ) for tentative high-spin levels proposed by 1972WaYR at 281.4; 300.3; 376.4, 377.2 and 495.5 keV, and a floating 90.0-112.8-133.8-151.2 γ cascade with level sequence of J=3 to 7.

J^π(level): From probable band assignments in ¹⁶⁰Gd(¹¹B,α3nγ) and ¹⁶⁵Ho(d,t), unless otherwise stated

E(γ): Values with uncertainties are from ¹⁶⁴Ho IT decay (37.5 min). Others are from ¹⁶⁰Gd(¹¹B,α3nγ).

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_
0.0	1+	28.8 m 5 % β^- = 40 5 % ε = 60 5
37.341 20	2+	≤ 2.8 ns	37.34 2	100	M1+E2	0.0	1+
93.99 4	3+		56.64 5 94.00 5	100 5 2.10 23	M1+E2 E2	37.341 0.0	2+ 1+
167.4 4	4+		73.7			93.99	3+
261.7 4	5+		94.5 167.4			167.4 93.99	4+ 3+
370.2 6	(6+)		108.5			261.7	5+
502.7 6	(7+)		132.5 241.0			370.2 261.7	(6+) 5+
644.2 7	(8+)		141.3 274.0			502.7 370.2	(7+) (6+)
814.0 7	(9+)		169.8 311.5			644.2 502.7	(8+) (7+)
985.1 7	(10+)		171.2 340.8			814.0 644.2	(9+) (8+)
1192.0 8	(11+)		206.7 378.2			985.1 814.0	(10+) (9+)
1387.2 8	(12+)		195.1 402.0			1192.0 985.1	(11+) (10+)
1631.0 9	(13+)		243.8 439.1			1387.2 1192.0	(12+) (11+)
1865.3 7	(14+)		477.4?			1387.2	(12+)
2113.5 8	(15+)		481.8?			1631.0	(13+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_
191.0 5	6+
317.3 8	7+		126.3			191.0	6+
460.9 9	(8+)		143.5			317.3	7+
621.7 9	(9+)		160.7 304.5			460.9 317.3	(8+) 7+
799.1 9	(10+)		177.5 338.1			621.7 460.9	(9+) (8+)
992.8 9	(11+)		193.6 371.2			799.1 621.7	(10+) (9+)
1202.1 9	(12+)		209.4 403.1			992.8 799.1	(11+) (10+)
1426.8 10	(13+)		224.8 433.7			1202.1 992.8	(12+) (11+)
1666.0 10	(14+)		239.2 464.0			1426.8 1202.1	(13+) (12+)
1919.0 10	(15+)		253.1 492.2			1666.0 1426.8	(14+) (13+)
2183.8 11	(16+)		517.8			1666.0	(14+)
2462.5 12	(17+)		543.5			1919.0	(15+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^
139.78 7	6-	36.6 m 3 % IT = 100
203.7 5	7-		63.9			139.78	6-
293.7 7	(8-)		90.1			203.7	7-
406.5 7	(9-)		112.7 202.8			293.7 203.7	(8-) 7-
540.3 7	(10-)		133.7 246.7			406.5 293.7	(9-) (8-)
694.2 8	(11-)		153.9 287.6			540.3 406.5	(10-) (9-)
867.0 8	(12-)		172.9 326.7			694.2 540.3	(11-) (10-)
1058.2 8	(13-)		191.2 363.9			867.0 694.2	(12-) (11-)
1265.3 9	(14-)		207.1 398.5			1058.2 867.0	(13-) (12-)
1492.0 9	(15-)		226.8 433.6			1265.3 1058.2	(14-) (13-)
1728.2 9	(16-)		236.3 462.9			1492.0 1265.3	(15-) (14-)
1990.1 9	(17-)		261.9 498.1			1728.2 1492.0	(16-) (15-)
2249.6 10	(18-)		259.2 521.3			1990.1 1728.2	(17-) (16-)
2548.1 10	(19-)		298.5 558.4			2249.6 1990.1	(18-) (17-)
2825.8 10	(20-)		277.7 575.9			2548.1 2249.6	(19-) (18-)
3162.0 11	(21-)		336.1 614.1			2825.8 2548.1	(20-) (19-)
3452.0 11	(22-)		626.2			2825.8	(20-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
3826.7 12	(23-)		664.7			3162.0	(21-)
4125.5 13	(24-)		673.5			3452.0	(22-)
4541.8 9	(25-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^
193.3 4	(1-)
207.8 3	(2-)		113.6 170.6 208.0			93.99 37.341 0.0	3+ 2+ 1+
236.1 4	(3-)		198.8			37.341	2+
273.8 4	(4-)		37.7 179.8			236.1 93.99	(3-) 3+
330.9 7	(5-)		163.5			167.4	4+
398.2 9	(6-)		67.3			330.9	(5-)
488.0 10	(7-)		89.8			398.2	(6-)
586.9 11	(8-)		99.0			488.0	(7-)
711.9 11	(9-)		125.1 223.8			586.9 488.0	(8-) (7-)
843.1 11	(10-)		131.1 256.2			711.9 586.9	(9-) (8-)
1006.7 11	(11-)		163.6 294.8			843.1 711.9	(10-) (9-)
1171.3 12	(12-)		164.5 328.1			1006.7 843.1	(11-) (10-)
1377.2 12	(13-)		205.8 370.6			1171.3 1006.7	(12-) (11-)
1577.2 12	(14-)		200.0 405.9			1377.2 1171.3	(13-) (12-)
1825.7 12	(15-)		248.5 448.6			1577.2 1377.2	(14-) (13-)
2062.4 12	(16-)		236.7 485.2			1825.7 1577.2	(15-) (14-)
2350.1 13	(17-)		287.6 524.5			2062.4 1825.7	(16-) (15-)
2623.9 13	(18-)		273.9 561.4			2350.1 2062.4	(17-) (16-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
2941.0 13	(19-)		317.0 590.9			2623.9 2350.1	(18-) (17-)
3250.4 14	(20-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - Kπ=5⁺,π7/2[523]\|^+ν3/2[521]\|^
342.6 5	5+	2.6 ns 2
452.4 8	6+		109.8			342.6	5+
579.6 9	7+		127.3			452.4	6+
723.1 9	(8+)		143.6 270.6			579.6 452.4	7+ 6+
881.5 9	(9+)		158.2 302.0			723.1 579.6	(8+) 7+
1049.9 9	(10+)		168.4 326.9			881.5 723.1	(9+) (8+)
1234.8 10	(11+)		185.0 353.3			1049.9 881.5	(10+) (9+)
1420.2 11	(12+)		370.3			1049.9	(10+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - Kπ=2⁺,π7/2[523]\|^-ν3/2[521]\|^
486 2	(2+)
558 1	(3+)
650 3	(4+)
777 2	(5+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - Kπ=2-,π7/2[523]\|^-ν3/2[402]\|_
620 1	2-
670 2	3-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 8 - Kπ=5-,π7/2[523]\|^+ν3/2[402]\|_
733 1	(5-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 9 - Kπ=4-,π7/2[523]\|^+ν1/2[400]\|^
833 1	(4-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 10 - Kπ=3-,π7/2[523]\|^-ν1/2[400]\|^
925 1	(3-)
994 4	(4-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 11 - Kπ=3⁺,π7/2[523]\|^-ν1/2[521]\|_
188.6 5	(3+)	≤ 0.5 ns
297.4 7	(4+)		108.7			188.6	(3+)
429.9 7	(5+)		132.4 241.4			297.4 188.6	(4+) (3+)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
37.341	2+	≤ 2.8 ns	37.34 2	M1+E2	0.045 +12-8	7.8	B(E2)(W.u.)>5.4, B(M1)(W.u.)>0.017, α=7.8 3, α(L)=6.10 20, α(M)=1.35 5, α(N)=0.314 11, α(O)=0.0450 13, α(P)=0.00241 4
93.99	3+		56.64 5	M1+E2	0.052 11	14.2	α=14.2 7, α(L)=1.75 4, α(M)=0.388 8, α(N)=0.090 18, α(O)=0.01299 24, α(P)=0.000707 10
93.99	3+		94.00 5	E2		3.56	α=3.56, α(K)=1.272 18, α(L)=1.76 3, α(M)=0.425 6, α(N)=0.0957 14, α(O)=0.01133 17, α(P)=5.27×10^-5 8
139.78	6-	36.6 m 3 % IT = 100	45.79 6	E3		4.53×10³	B(E3)(W.u.)=0.000181 4, α=4.53E3, α(L)=3.38E3 6, α(M)=914 15, α(N)=208 4, α(O)=23.3 4, α(P)=0.01321 21
188.6	(3+)	≤ 0.5 ns	94.6	[M1]		3.06	B(M1)(W.u.)>0.012, α=3.06, α(K)=2.57 4, α(L)=0.383 6, α(M)=0.0845 12, α(N)=0.0196 3, α(O)=0.00285 4, α(P)=0.0001596 23
342.6	5+	2.6 ns 2	202.8	[E1]		0.0485	B(E1)(W.u.)=9.9E-6 8, α=0.0485, α(K)=0.0409 6, α(L)=0.00598 9, α(M)=0.001315 19, α(N)=0.000302 5, α(O)=4.22E-5 6, α(P)=2.05E-6 3

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1+	28.8 m 5 % β^- = 40 5 % ε = 60 5	E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
37.341	2+	≤ 2.8 ns	E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
93.99	3+		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
139.78	6-	36.6 m 3 % IT = 100	E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
167.4	4+		XREF: C(164.3). E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
188.6	(3+)	≤ 0.5 ns	E(level): Kπ=3⁺,π7/2[523]\|^-ν1/2[521]\|_.
191.0	6+		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
193.3	(1-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
203.7	7-		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
207.8	(2-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
236.1	(3-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
261.7	5+		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
273.8	(4-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
293.7	(8-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
297.4	(4+)		E(level): Kπ=3⁺,π7/2[523]\|^-ν1/2[521]\|_.
317.3	7+		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
330.9	(5-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
342.6	5+	2.6 ns 2	XREF: d(338.3). E(level): Kπ=5⁺,π7/2[523]\|^+ν3/2[521]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
370.2	(6+)		XREF: F(367). E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
394			XREF: d(390.5).
398.2	(6-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
406.5	(9-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
421			1970Jo11 suggest possible J=3 from Kπ=3⁺, π7/2[523]\|^-ν1/2[521]\|_, but the authors note that a state with a similar configuration is proposed at 188.6 in (p,nγ).
429.9	(5+)		E(level): Kπ=3⁺,π7/2[523]\|^-ν1/2[521]\|_.
452.4	6+		E(level): Kπ=5⁺,π7/2[523]\|^+ν3/2[521]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
E(level)	J^π(level)	T_1/2(level)	Comments
460.9	(8+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
486	(2+)		E(level): Kπ=2⁺,π7/2[523]\|^-ν3/2[521]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
488.0	(7-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
499			Possible (K=6,π7/2[523]\|^+ν5/2[642]\|^)+Q₂₂ (1970Jo11).
502.7	(7+)		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
540.3	(10-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
558	(3+)		E(level): Kπ=2⁺,π7/2[523]\|^-ν3/2[521]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
579.6	7+		XREF: F(583). E(level): Kπ=5⁺,π7/2[523]\|^+ν3/2[521]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
586.9	(8-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
620	2-		E(level): Kπ=2-,π7/2[523]\|^-ν3/2[402]\|_. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
621.7	(9+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
644.2	(8+)		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
650	(4+)		E(level): Kπ=2⁺,π7/2[523]\|^-ν3/2[521]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
670	3-		E(level): Kπ=2-,π7/2[523]\|^-ν3/2[402]\|_. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
691			Possible (K=1,π7/2[523]\|^-ν5/2[642]\|^)+Q₂₂ (1970Jo11).
694.2	(11-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
711.9	(9-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
723.1	(8+)		XREF: C(720.6). E(level): Kπ=5⁺,π7/2[523]\|^+ν3/2[521]\|^.
733	(5-)		E(level): Kπ=5-,π7/2[523]\|^+ν3/2[402]\|_. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
777	(5+)		E(level): Kπ=2⁺,π7/2[523]\|^-ν3/2[521]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
799.1	(10+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
814.0	(9+)		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
833	(4-)		E(level): Kπ=4-,π7/2[523]\|^+ν1/2[400]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
843.1	(10-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
867.0	(12-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
E(level)	J^π(level)	T_1/2(level)	Comments
881.5	(9+)		E(level): Kπ=5⁺,π7/2[523]\|^+ν3/2[521]\|^.
925	(3-)		E(level): Kπ=3-,π7/2[523]\|^-ν1/2[400]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
985.1	(10+)		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
992.8	(11+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
994	(4-)		E(level): Kπ=3-,π7/2[523]\|^-ν1/2[400]\|^. J^π(level): From 1970Jo11, based on the ’fingerprint’ method, by requiring relative energies to fit the rotational-model formula and comparison of the relative intensity pattern within a band to the calculated theoretical cross sections.
1006.7	(11-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
1049.9	(10+)		E(level): Kπ=5⁺,π7/2[523]\|^+ν3/2[521]\|^.
1058.2	(13-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
1171.3	(12-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
1192.0	(11+)		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
1202.1	(12+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
1234.8	(11+)		E(level): Kπ=5⁺,π7/2[523]\|^+ν3/2[521]\|^.
1265.3	(14-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
1377.2	(13-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
1387.2	(12+)		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
1420.2	(12+)		E(level): Kπ=5⁺,π7/2[523]\|^+ν3/2[521]\|^.
1426.8	(13+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
1492.0	(15-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
1577.2	(14-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
1631.0	(13+)		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
1666.0	(14+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
1728.2	(16-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
1825.7	(15-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
1865.3	(14+)		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
1919.0	(15+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
E(level)	J^π(level)	T_1/2(level)	Comments
1990.1	(17-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
2062.4	(16-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
2113.5	(15+)		E(level): Kπ=1⁺,π7/2[523]\|^-ν5/2[523]\|_.
2183.8	(16+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
2249.6	(18-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
2350.1	(17-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
2462.5	(17+)		E(level): Kπ=6⁺,π7/2[523]\|^+ν5/2[523]\|_.
2548.1	(19-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
2623.9	(18-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
2825.8	(20-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
2941.0	(19-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
3162.0	(21-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
3250.4	(20-)		E(level): Kπ=1-,π7/2[523]\|^-ν5/2[642]\|^.
3452.0	(22-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
3826.7	(23-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
4125.5	(24-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.
4541.8	(25-)		E(level): Kπ=6-,π7/2[523]\|^+ν5/2[642]\|^.