List of levels for 50TI

ADOPTED LEVELS, GAMMAS for ⁵⁰Ti

Authors: Jun Chen and Balraj Singh | Citation: Nucl. Data Sheets 157, 1 (2019) | Cutoff date: 15-Apr-2019

Full ENSDF file | Adopted Levels (PDF version)

Q(β-)=-2207.6 keV 4	S(n)= 10939.19 keV 4	S(p)= 12159.4 keV 27	Q(α)= -10717.2 keV 22
Reference: 2017WA10

References:
A	⁵⁰Sc β^- decay (102.5 S)	B	⁵⁰Sc β^- decay (0.35 S):?
C	⁵⁰V ε decay (2.65×10¹⁷ Y)	D	⁹Be(⁴⁶Ar,5nγ)
E	C(⁴⁶Ca,⁵⁰TiG)	F	⁴⁸Ca(³He,n)
G	⁴⁸Ca(α,2nγ),(⁶Li,3npγ)	H	⁴⁸Ca(⁹Be,3NAG)
I	⁴⁸Ca(¹⁶O,¹⁴C),(¹⁸O,¹⁶C)	J	⁴⁸Ti(t,p),(t,pγ)
K	⁴⁹Ti(n,γ),(pol n,γ) E=THERMAL	L	⁴⁹Ti(n,γ),(n,n):Resonances
M	⁴⁹Ti(d,p)	N	⁴⁹Ti(d,pγ)
O	⁵⁰Ti(γ,γ’)	P	⁵⁰Ti(E,E’)
Q	⁵⁰Ti(π^-,π^-’),(π⁺,π⁺’)	R	⁵⁰Ti(p,p’)
S	⁵⁰Ti(³He,³He’),(α,α’)	T	Coulomb Excitation
U	⁵⁰V(d,²He)	V	⁵¹V(E,E’p)
W	⁵¹V(n,d)	X	⁵¹V(p,2p)
Y	⁵¹V(d,³He),(pol d,³He)	Z	⁵¹V(α,α’p)
a	⁵²Cr(¹⁴C,¹⁶O)

Other measurements:

Mass measurements: 2017Ka53 (using LEBIT at NSCL-MSU), 1972De39

Hyperfine structure measurements:

2004Ga34, 2002Ca47, 2000Ga58: measured hyperfine structure for g.s. using collinear laser spectroscopy; deduced isotope shift, charge radius.

1996Fu23: measured optical isotope shift for g.s., deduced mean square nuclear charge radius.

1996Lu12, 1994Lu18, 1992Az03: measured hyperfine structure, deduced isotope shift for g.s., and mass shifts.

1995Ga44, 1994An35: measured hyperfine structure, deduced isotopes shifts, mass shifts

1983Ku10, 1980Po01: measured pionic x-rays, strong interaction shifts, and widths; deduced rms radius.

1981Wo02: measured muonic x-rays; deduced charge radius, and isotone shifts.

Other reactions:

1990We05: ⁵⁰Ti(π⁺,π^-),E=35 MeV. Measured σ(θ) for double isobaric analog transitions using a clamshell spectrometer.

1975We11: ⁵¹V(γ,p),E=17.62 MeV. Measured σ and correlated the results to L(d,³He)=3 spectroscopic factors for the first 0⁺ and 4⁺ states.

Theory references: consult the NSR database (www.nndc.bnl.gov/nsr/) for 200 primary references dealing with various aspects of nuclear structure

Levels: States at 3771 observed by 1964Bj01 in (d,p) and at 4226, 5282, 5510, and 5919 keV observed by 1989Og01 in (¹⁶O,¹⁴C) have not been adopted by the evaluators

Q-value: S(2n)=19081.59 5, S(2p)=21784.97 9 (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 G H I J K M N O P Q R S T V W X Y Z a	0+	STABLE
1553.794 8	A B C D E F G H I J K M N O P Q R S T V W Y a	2+	1.047 ps 35	1553.768 8	100	E2	0.0	0+
2674.932 10	A D E G H I J K M N P Q R S V W Y a	4+	5.3 ps 11	1121.124 5	100	E2	1553.794	2+
3198.730 21	A D G H I K M N P R V W Y a	6+	418 ps 20	523.792 18	100	E2	2674.932	4+
3862.81 4	K M R W	(2,3)+		2308.98 4	100		1553.794	2+
3868.3 20	J M Q W	0+	0.50 ps 23	2314.4 20	100	(E2)	1553.794	2+
3974.9 10 ?	G			1300.0 10 ?	100		2674.932	4+
4147 7 ?	Y	3-,4-
4147.210 13	A G I J K M N R S	4+	33 fs +7-5	1472.255 8	100	D,E2	2674.932	4+
4172.003 19	A I K M N R Y	3+	> 0.83 ps	1497.054 25 2618.33 7	48 3 100 6		2674.932 1553.794	4+ 2+
4172.8 3	I J M N Q R Y	(2+)	< 11 fs	2618.6 4	100	D,E2	1553.794	2+
4309.86 11	I J K M N O P Q R Y a	2+	6.1 fs 12	2755.89 13 4309.74 20	100 10 19.6 21	M1+E2 [E2]	1553.794 0.0	2+ 0+
4410.02 3	J K M N P Q R S V Y	3-	< 2.8 ns	1735.00 5 2856.13 4	25.5 17 100 7		2674.932 1553.794	4+ 2+
4486.74 6	F K	(2+)		2933.27 12 4486.0 4	100 10 17 3		1553.794 0.0	2+ 0+
4536 20	M
4576 20	M
4789.97 6	I J K M N R S Y	2+	< 14 fs	3236.09 7 4789.3 4	100 7 11.3 19	D,E2 (E2)	1553.794 0.0	2+ 0+
4880.705 15	A K M N P	5+	215 fs +45-35	733.69 9 1681.69 15 2205.722 13	2.12 20 8.3 24 100 6	D,E2 D,E2 D,E2	4147.210 3198.730 2674.932	4+ 6+ 4+
4928 8	J Y	(1:6)-
4940 20	J R	(2)+
5110 8	J M
5186.103 18	J K M N	(3,4)+	< 6.9 fs	1039 1 ? 2511.110 22 3632.10 5	<6 100 7 40.4 24	D,E2 D,E2 D,E2	4147.210 2674.932 1553.794	4+ 4+ 2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5191 8	J R Y	3-,4-
5282?	I
5334 5	M R V Y	(4,5,6)-
5379.942 19	A J K M N R S	4+	33 fs +9-7	1207.930 12 2704.92 4 3826.08 11	54.8 31 100 7 12.8 10	D,E2 D,E2 (E2)	4172.003 2674.932 1553.794	3+ 4+ 2+
5407 8	J S Y	3-,4-
5440.74 20	A I J M R	4+,5+		2765.73 20	100		2674.932	4+
5528 8	I Y	3-,4-
5547.81 4	I K	(4+)		2348.3 3 ? 2872.72 10 3993.87 5	27 6 100 8 82 5		3198.730 2674.932 1553.794	6+ 4+ 2+
5560 20	R	(3)-
5561 6	M	(2:5)+
5600 6	M	(2:5)+
5633 15	J	0+
5694.87 8	J K R	2+,3+		3019.86 11	100		2674.932	4+
5717 6	J M
5771 9	Y	3-,4-
5787 5	R	(4)+
5795 9	S V Y	(1:6)-
5806.54 16	A K M R S	4+,5+		3131.71 19	100		2674.932	4+
5837.2 6	I M N S	(2:5)(+)	26 fs +19-14	1690.0 7 3162 1	100 82	D,E2 D,E2	4147.210 2674.932	4+ 4+
5880 9	I M Y	(0:7)+
5945 5	I R X Y	(3)-
5946.479 22	I K M N Z	3+,4+	19 fs 5	760.31 8 1156.65 16 1799 1 ? 3271.41 3	8.9 9 5.2 8 ≈14 100 6	(M1) D,E2 D,E2 D,E2	5186.103 4789.97 4147.210 2674.932	(3,4)+ 2+ 4+ 4+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6044 5	R V X Y Z	3-,4-
6045 15	J	0+
6072 15	J M	(2)+
6123.15 4	K N R	(4+)	38 fs +12-9	1242.38 4 1636.45 5 1975.8 6 ? 2924.9 5 3448.4 5	100 7 85 6 <15 31 7 20 5	D,E2 (E2) (E2) D,E2	4880.705 4486.74 4147.210 3198.730 2674.932	5+ (2+) 4+ 6+ 4+
6136.3 6	D G H M Y	(7)+		2937.5 6	100	M1+E2	3198.730	6+
6156.47 22	K	(2,3,4+)		4602.50 25	100		1553.794	2+
6172 7	M R Y	(2:5)+
6212 5	J M R	(1:6)(-)
6249 6	M Y	(0:7)+
6301.81 4	K M Y	(1,2,3)-		2128.4 5 4747.73 7	15 5 100 6		4172.8 1553.794	(2+) 2+
6379.88 14	K N R V Y	(5)-	< 19 fs	1498.8 4 ? 2232.3 7 ? 3181.9 6	117 117 100 32		4880.705 4147.210 3198.730	5+ 4+ 6+
6392 6	M R	(2:5)+
6399.81 15	K V Y	(3)-		3724.1 5 4845.6 3	65 15 100 11		2674.932 1553.794	4+ 2+
6.4E3 5	U
6461 9	Y	(1:6)-
6481.2 4	J M N R	3+	< 17 fs	2309.1 4	100	D,E2	4172.003	3+
6521.41 4	K M N R Y	3+,4+	7.6 fs +35-28	1730.8 3 2348.5 7 2373.3 6 ? 2658.75 20 3846.18 11	22 6 21 21 47 7 100 9	D,E2 D,E2 D,E2 D,E2 D,E2	4789.97 4172.8 4147.210 3862.81 2674.932	2+ (2+) 4+ (2,3)+ 4+
6540.7 8	D G H	(8)+		404.4 4	100	M1+E2	6136.3	(7)+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6548 15	J
6583 10	M S V Y	(1:6)-
6608 5	J M R S Y	(3)-
6636 6	J M	(0:7)+
6665 10	M Y	(1:6)-
6710.570 24	J K M N R Y	4+	11 fs 5	1524.53 4 2300.43 5 2538.37 10 5156.46 7	64 5 62 5 100 10 78 5	D,E2 (E1) D,E2 (E2)	5186.103 4410.02 4172.003 1553.794	(3,4)+ 3- 3+ 2+
6729.86 6	J K M S	3-		2867.39 21 4054.75 11	85 11 100 8		3862.81 2674.932	(2,3)+ 4+
6766 10	J Y	(0:7)+
6770.5 9	D G H	(9)+		229.8 4	100	M1+E2	6540.7	(8)+
6837.64 7	K	(2+,3,4+)		1457.6 3 5283.39 14	33 7 100 6		5379.942 1553.794	4+ 2+
6849.05 8	K Y	(5)-		2700.6 6 3649.9 5	100 32 69 20		4147.210 3198.730	4+ 6+
6864 5	M R	(5)+
6933 15	J M
6975 5	J M R V Y	3-,4-
7029.39 25	J K M Y	2+,3+,4+		2719.1 3	100		4309.86	2+
7047 10	R V	(3)-
7049 20	J M Y	(2:5)+
7078.72 23	J K M R Y	(3)-		4402.1 5 5525.5 5	100 23 90 19		2674.932 1553.794	4+ 2+
7094 20	J M Y	(1:6)-
7115 10	R	(1)+
7132 20	M S	3-
7.19E3 6	F I	0+
7210 10	J R	(3)-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7232.19 23	J K M R	(2)+		1852.9 4 5677.8 3	100 32 30 5		5379.942 1553.794	4+ 2+
7249 6	M	(2:5)+
7280 20	M	(1:7)+
7293 10	P
7335 10	R	(2)+
7382 9	J M R	(3)-
7407 20	J M	(2:5)+
7441 15	J M
7471 20	J M R	(2:5)+
7482.96 7	J K M R	(2)+		5929.14 15	100		1553.794	2+
7536 10	M R	(3)-
7539.5 22 ?	G M			770.2 10 ?	100		6770.5	(9)+
7572.6 11	D G H	(10)+		802.1 7	100	M1+E2	6770.5	(9)+
7577 10	J M R	0+,1+
7605 11	V Y	(3-,4-)
7631 20	M R	(5)+
7667 15	J M	(2)+
7699 10	J R S Y	(3)-
7734 15	J S
7808 15	J	(0+)
7867 10	J R	0+,1+
7924 10	J R	(5)-
7941 15	J
8034 10	J R	(4)+
8079 10	J R	(1)+
8150 10	J R
8.15E3 25	U
8203 10	J R	(3)-
8241 10	J R	0+,1+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
8257.7 24 ?	G			1718.0 15 ?	100		6540.7	(8)+
8290 10	J R	(3)-
8407 12	P
8444 10	R	0+,1+
8.56E+3 2	P	1+
8578 10	R	(3)-
8606 10	R	(1)+
8.64E+3 2	P	2-
8.65E3 25	U
8725 10	P R	(2-)
8755 7	P
8793.7 17	D G H	(11+)		1221.1 13	100	(M1+E2)	7572.6	(10)+
8.81E+3 2	P R	1+
8815 10	R	(3)-
8.87E+3 2	P	(2+)
8883 10	P R	(2,3)-
8973 10	P R	(3)-
9.03E+3 2	R	(1)+
9.05E+3 2	P	2-
9061 12	P
9127 10	R
9188 15	P
9.21E+3 2	P R	1+
9232 10	R	(4+,5-)
9240 20	P	(1+,2)
9.28E+3 2	P	(1,2-)
9282 10	R	(5-,6+)
9.3E3 4	U
9339 10	R	(3)-
9368 10	P R	(1+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
9391 10	R	(4)+
9442 10	P
9504 10	R
9508 10	R	(5-,6+)
9550 10	R
9614 10	R	(1)+
9752 10	R	(3)-
9790	R	0+,1+
9809 10	R
9842 10	R	(4-,5+)
9909 10	R	(3)-
9957 14	P R	1+
9999 10	R	(3)-
10.00E+3 2	P	(2-,1+)
10045 10	P R	(1)+
10.05E3 35	U
10.14E+3 2	P	(1+,2-)
10162 10	P R	1+
10206 10	F P R	(1)+
10240 10	F P R	(1+,2-,3-)
10357 14	P R	1+
10.38E+3 2	P	(2-,1+)
10472 11	P R	1+
10495 10	R	(3)-
10.54E+3 2	P	(1+,2-)
10.58E+3 2	P R	1+
10.66E+3 2	P	1+
10.80E+3 2	P R	1+
10.87E+3 2	P	(1,2-)
10.90E+3 2	P	2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
10.91E+3 2	R	(1)+
10939.184 15 S	K	3-,4-		3456.17 7 3707.4 6 3860.1 3 3909.0 4 4089.93 8 4101.32 7 4209.17 6 4228.43 3 4417.55 4 4539.01 18 4559.13 14 4637.13 4 4782.6 4 4815.79 6 4992.420 25 5132.72 25 5244.04 10 5391.07 5 5558.937 24 5752.692 24 6058.105 20 6148.85 14 6451.6 5 6528.72 10 6766.73 5 6791.41 7 8263.51 3 9384.41 6	5.79 22 3.4 23 1.12 17 0.79 13 4.44 17 4.72 17 5.62 17 22.5 4 10.34 22 1.67 12 3.03 17 10.28 22 0.79 12 6.01 17 25.2 4 1.13 11 3.07 12 11.01 22 34.5 5 26.5 3 56.4 6 2.98 17 1.40 22 5.17 17 100.0 17 42.6 11 48.2 6 28.5 4	D D	7482.96 7232.19 7078.72 7029.39 6849.05 6837.64 6729.86 6710.570 6521.41 6399.81 6379.88 6301.81 6156.47 6123.15 5946.479 5806.54 5694.87 5547.81 5379.942 5186.103 4880.705 4789.97 4486.74 4410.02 4172.003 4147.210 2674.932 1553.794	(2)+ (2)+ (3)- 2+,3+,4+ (5)- (2+,3,4+) 3- 4+ 3+,4+ (3)- (5)- (1,2,3)- (2,3,4+) (4+) 3+,4+ 4+,5+ 2+,3+ (4+) 4+ (3,4)+ 5+ 2+ (2+) 3- 3+ 4+ 4+ 2+
10942.94 4	L	3-	0.26 keV 3
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
10943.89 4	L	(2:5)+
10946.67 4	L	(2:5)+
10947.45 5	L	4-	0.28 keV 3
10.95E+3 2	P	1
10952.09 4	L	(2:5)+
10952.89 4	L	(2:5)+
10953.67 5	L	(2:5)+
10955.91 5	L	(2:5)+
10957.41 5	L	(2:5)+
10957.86 5	L	3-	126 eV 23
10960.63 5	L	3-	149 eV 17
10961.65 5	L	(2:5)+
10961.73 5	L	3-	0.65 keV 12
10964.51 6	L	(2:5)+
10965.94 6	L	4-	0.37 keV 6
10966.93 6	L	(2:5)+
10967.25 6	L	(2:5)+
10968.22 6	L	(2:5)+
10968.39 6	L	(2:5)+
10.97E+3 2 ?	P	(2-,3+)
10970.13 6	L		32 eV 16
10970.94 6	L	4-	1.4 keV 4
10972.61 4	L	(2:5)+
10973.80 6	L	(2:5)+
10974.64 6	L	(2:5)+
10975.15 6	L		0.0026 eV 7
10975.41 6	L	(2:5)+	0.39 keV 10
10976.81 6	L	4-	1.51 keV 18
10980.84 6	L	(3)+
10981.05 6	L
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
10981.76 6	L	(4)+
10982.31 7	L	(3)+
10984.21 7	L	(3)+
10987.91 7	L	(3)+
10988.38 7	L
10988.63 7	L	(5)+
10989.60 7	L	(3)	0.23 keV 6
10990.11 8	L
10991.32 8	L
10994.86 8	L	4-	0.53 keV 9
10996.41 8	L
10996.72 8	L
10997.39 8	L
10998.05 9	L	3-	0.45 keV 11
10998.31 9	L	(2:5)+
11000.04 10	L	(2:5)+
11001.13 10	L	(3)	0.23 keV 12
11001.34 10	L	(2:5)+
11005.43 10	L	3-
11005.91 10	L	(2:5)+
11009.74 10	L	(2:5)+
11009.93 10	L	(2:5)+
11010.47 10	L	(2:5)+
11014.34 11	L	4-	0.89 keV 20
11015.54 11	L
11015.96 11	L	(2:5)+
11.03E+3 2	P	(1,2-)
11033.8 3	L	3-
11043.4 3	L	3-
11.07E+3 2	P	1
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
11075.2 4	L	4-
11082.0 4	L	3-
11087.3 5	L	3-
11088.3 5	L	4-
11106.3 5	L	4-
11108.0 5	L	4-
11111.8 5	L	4-
11120.2 5	L	3-
11121.2 6	L	4-
11123.1 6	L	3-
11.13E+3 2	P	(2,1+)
11132.2 6	L	4-
11143.5 6	L	3-
11150.8 6	L	4-
11159.2 7	L	3-
11173.4 7	L	4-
11.19E+3 2	P	(1-,2-)
11.22E+3 2	P	(2-,1+)
11.29E+3 2	P	3
11.3E3 9	U
11.31E+3 2	P	(2-,1+)
11.35E+3 2	P	(2-,1+)
11.42E+3 2	P	2-
11.61E+3 2	P	1
11.83E+3 2	P	2-
13.83E+3 6	F	(2+)
14.1E3 7	U
15.39E3 2	R	(1)+
16.01E+3 6	F	(0+)
16.58E+3 6	F	0+

E(level): From least-squares fit to Eγ data including primary γ rays from (n,γ), keeping the capture-state energy fixed. For levels not populated in γ-ray studies, values are the weighted averages of all the available data. In addition there are high-lying excitations at 6, 11 and 16 MeV in ⁵¹V(α,α’p) reaction

J^π(level): In ⁴⁸Ca(³He,n) and ⁴⁸Ti(t,p) reactions, where Jπ(target g.s.)=0⁺, implied Jπ=0⁺ for L=0, 2⁺ for L=2, 3- for L=3, 4⁺ for L=4, assuming that for strong groups, the two neutrons or two protons are identical particles in S=0 state, whereas for weaker groups, S=1 state is also possible leading to unnatural-parity states with J=L-1 and L+1. In ⁴⁹Ti(d,p); ⁵¹V(e,e’p) and ⁵¹V(d,³He) where Jπ(target g.s.)=7/2-, implied Jπ=3-,4- for L=0,0⁺2; 2 to 5, π=+ for L=1,1⁺3; 1 to 6, π=- for L=2,2⁺4; 0 to 7, π=+ for L=3; and 0 to 8, π=- for L=4. In ⁵⁰V(d,²He) with Jπ(target g.s.=6⁺), implied Jπ=5⁺,6⁺,7⁺ for L=0; and 4 to 8, π=- for L=1.

T_1/2(level): T_1/2 from DSAM in (d,pγ), except as noted

M(γ): The assignment of Mult=d,E2 where given are from measured T_1/2 and γ branchings compared with RUL.

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - Yrast sequence
0.0	0+	STABLE
1553.794 8	2+	1.047 ps 35	1553.768 8	100	E2	0.0	0+
2674.932 10	4+	5.3 ps 11	1121.124 5	100	E2	1553.794	2+
3198.730 21	6+	418 ps 20	523.792 18	100	E2	2674.932	4+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - γ cascade based on (7⁺)
6136.3 6	(7)+
6540.7 8	(8)+		404.4 4	100	M1+E2	6136.3	(7)+
6770.5 9	(9)+		229.8 4	100	M1+E2	6540.7	(8)+
7572.6 11	(10)+		802.1 7	100	M1+E2	6770.5	(9)+
8793.7 17	(11+)		1221.1 13	100	(M1+E2)	7572.6	(10)+

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
1553.794	2+	1.047 ps 35	1553.768 8	E2			B(E2)(W.u.)=5.46 19
2674.932	4+	5.3 ps 11	1121.124 5	E2			B(E2)(W.u.)=5.5 +15-10
3198.730	6+	418 ps 20	523.792 18	E2			B(E2)(W.u.)=3.14 13
3868.3	0+	0.50 ps 23	2314.4 20	(E2)			B(E2)(W.u.)=1.6 +14-5
4309.86	2+	6.1 fs 12	2755.89 13	M1+E2	-0.26 17		B(E2)(W.u.)=2.8 +61-25, B(M1)(W.u.)=0.135 +49-37
4309.86	2+	6.1 fs 12	4309.74 20	[E2]		1.29×10^-3	B(E2)(W.u.)=0.93 +45-28, α=1.29E-3, α(K)=7.37E-6 11, α(L)=6.55E-7 10, α(M)=8.38E-8 12, α(N)=4.57E-9 7
4789.97	2+	< 14 fs	4789.3 4	(E2)		1.43×10^-3	α=1.43×10^-3, α(K)=6.34E-6 9, α(L)=5.63E-7 8, α(M)=7.20E-8 10, α(N)=3.93E-9 6
5379.942	4+	33 fs +9-7	3826.08 11	(E2)		1.12×10^-3	B(E2)(W.u.)=0.15 +7-5, α=1.12E-3, α(K)=8.78E-6 13, α(L)=7.80E-7 11, α(M)=9.98E-8 14, α(N)=5.45E-9 8
5946.479	3+,4+	19 fs 5	760.31 8	(M1)			B(M1)(W.u.)=0.18 +12-7
6136.3	(7)+		2937.5 6	M1+E2	-0.141 25
6540.7	(8)+		404.4 4	M1+E2	-0.017 9
6710.570	4+	11 fs 5	2300.43 5	(E1)			B(E1)(W.u.)=0.0008 +8-3
6710.570	4+	11 fs 5	5156.46 7	(E2)		1.54×10^-3	B(E2)(W.u.)=0.33 +35-13, α=1.54E-3, α(K)=5.72E-6 8, α(L)=5.08E-7 8, α(M)=6.50E-8 9, α(N)=3.55E-9 5
6770.5	(9)+		229.8 4	M1+E2	-0.035 15	0.00233	α=0.00233, α(K)=0.00211 4, α(L)=0.000192 3, α(M)=2.45×10^-5 4, α(N)=1.317E-6 21
7572.6	(10)+		802.1 7	M1+E2	-0.044 18
8793.7	(11+)		1221.1 13	(M1+E2)	-0.17 10

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	0+	STABLE	XREF: B(?). E(level): From ⁵⁰Sc β^- decay. Other precise Eγ=1553.785 6, 1121.130 6, and Eγ=523.759 10 (plus 2.6 ppm systematic uncertainty) from (n,γ).
1553.794	2+	1.047 ps 35	μ=+2.89 15 (2000Sp08,2014StZZ), Q=+0.08 16 (1975To06,2016St14) XREF: B(?)S(1520). E(level): From ⁵⁰Sc β^- decay. Other precise Eγ=1553.785 6, 1121.130 6, and Eγ=523.759 10 (plus 2.6 ppm systematic uncertainty) from (n,γ). T_1/2(level): Mean lifetime \|t=1.51 ps 7 from weighted average of the following experimental results for mean lifetime \|t=1.62 ps 7 (2000Sp08, DSAM in Coul. ex.), 1.73 ps 20 in 2003Sp04, DSAM in C(⁴⁶Ca,⁵⁰Ti), same group as 2000Sp08); 1.30 ps 40 (1976Ra03, from width in (γ,γ’)); 1.44 ps 14 (from B(E2)\|^=0.0315 30 in Coul. ex. 1975To06); 1.10 ps 15 (1972WaYZ, DSAM in Coul. ex.); 1.469 ps 48 (from B(E2)\|^=0.0307 10 in (e,e’) 1971He08, uncertainty increased to 5% in averaging); 1.38 ps 13 (from B(E2)\|^=0.033030 in Coul. ex. 1970Ha24); 1.74 ps 13 (from B(E2)\|^=0.026 2 in Coul. ex. 1965Si02, 0.024 2 in 1965Si02 reanalyzed by 1970Ha24); 1.17 ps 23 (from B(E2)\|^=0.040 8 in Coul. ex. 1962Va22). Other: 2.7 ps 5 (from B(E2)\|^=0.0173 35 in Coul. ex. 1967Af03) seems discrepant thus not used in the averaging procedure. 2016Pr01 evaluation gives \|t=1.64 ps +10-9 from model-independent analyses, and 1.59 ps 8, which includes methods involving some model dependency.
2674.932	4+	5.3 ps 11	XREF: M(2688)S(2640). E(level): From ⁵⁰Sc β^- decay. Other precise Eγ=1553.785 6, 1121.130 6, and Eγ=523.759 10 (plus 2.6 ppm systematic uncertainty) from (n,γ).
3198.730	6+	418 ps 20	μ=+9.4 10 (1976Bo25) E(level): From ⁵⁰Sc β^- decay. Other precise Eγ=1553.785 6, 1121.130 6, and Eγ=523.759 10 (plus 2.6 ppm systematic uncertainty) from (n,γ).
3862.81	(2,3)+		XREF: R(3870).
3868.3	0+	0.50 ps 23	XREF: Q(3870).
4147.210	4+	33 fs +7-5	XREF: I(4180).
4309.86	2+	6.1 fs 12	XREF: n(4322).
4410.02	3-	< 2.8 ns	XREF: J(4424)p(4420)S(4380).
4486.74	(2+)		XREF: F(4440).
4789.97	2+	< 14 fs	XREF: M(4805).
4880.705	5+	215 fs +45-35	XREF: M(4896).
5186.103	(3,4)+	< 6.9 fs	XREF: M(5202).
5191	3-,4-		XREF: R(5203).
5440.74	4+,5+		XREF: I(5420).
5694.87	2+,3+		XREF: R(5679).
5806.54	4+,5+		XREF: M(5821)R(5817).
6172	(2:5)+		XREF: M(6176)R(6166)Y(6191).
6.4E3			L(d,²H)=0 from 6⁺ target for a wide bin.
6665	(1:6)-		XREF: M(6697).
6710.570	4+	11 fs 5	XREF: M(6726).
6729.86	3-		XREF: M(6744)S(6720).
7115	(1)+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
7382	(3)-		XREF: M(7367)R(7407).
7482.96	(2)+		XREF: M(7504).
E(level)	J^π(level)	T_1/2(level)	Comments
7631	(5)+		XREF: R(7650).
8079	(1)+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
8.15E3			L(d,²H)=0 from 6⁺ target for a wide bin.
8606	(1)+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
8.65E3			L(d,²H)=0 from 6⁺ target for a wide bin.
8.81E+3	1+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
9.03E+3	(1)+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
9.21E+3	1+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
9.3E3			L(d,²H)=0(+1) from 6⁺ target for a wide bin.
9614	(1)+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
9957	1+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
10045	(1)+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
10.05E3			L(d,²H)=0(+1) from 6⁺ target for a wide bin.
10.91E+3	(1)+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.
10942.94	3-	0.26 keV 3	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10943.89	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10946.67	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10947.45	4-	0.28 keV 3	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10952.09	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10952.89	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10953.67	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10955.91	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10957.41	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10957.86	3-	126 eV 23	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10960.63	3-	149 eV 17	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
E(level)	J^π(level)	T_1/2(level)	Comments
10961.65	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10961.73	3-	0.65 keV 12	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10964.51	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10965.94	4-	0.37 keV 6	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10966.93	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10967.25	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10968.22	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10968.39	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10970.13		32 eV 16	T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10970.94	4-	1.4 keV 4	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10972.61	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10973.80	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10974.64	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10975.15		0.0026 eV 7	T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10975.41	(2:5)+	0.39 keV 10	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10976.81	4-	1.51 keV 18	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10980.84	(3)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10981.76	(4)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10982.31	(3)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10984.21	(3)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10987.91	(3)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10988.38			J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10988.63	(5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10989.60	(3)	0.23 keV 6	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10994.86	4-	0.53 keV 9	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
E(level)	J^π(level)	T_1/2(level)	Comments
10998.05	3-	0.45 keV 11	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
10998.31	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11000.04	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11001.13	(3)	0.23 keV 12	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11001.34	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11005.43	3-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11005.91	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11009.74	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11009.93	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11010.47	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11014.34	4-	0.89 keV 20	J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances. T_1/2(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11015.96	(2:5)+		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11033.8	3-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11043.4	3-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11075.2	4-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11082.0	3-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11087.3	3-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11088.3	4-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11106.3	4-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11108.0	4-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11111.8	4-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11120.2	3-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11121.2	4-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11123.1	3-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11132.2	4-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
E(level)	J^π(level)	T_1/2(level)	Comments
11143.5	3-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11150.8	4-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11159.2	3-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11173.4	4-		J^π(level): From ⁴⁹Ti(n,γ),(n,n):resonances.
11.3E3			L(d,²H)=0⁺1 from 6⁺ target for a wide bin.
14.1E3			L(d,²H)=1(+0) from 6⁺ target for a wide bin.
15.39E3	(1)+		J^π(level): From L(p,p’)=0 in E_p=201 MeV and theory, V_σ\|t part of the nucleon-nucleon interaction is strongly enhanced compared to the V₀₀ part through which 0⁺ states may be excited and also with respect to the V_σ0 and V_0\|t parts.

E(level)	E(gamma)	Comments
1553.794	1553.768	E(γ): From ⁵⁰Sc β^- decay. Other precise Eγ=1553.785 6, 1121.130 6, and Eγ=523.759 10 (plus 2.6 ppm systematic uncertainty) from (n,γ) M(γ): ΔJ=2, Q from DCO in (⁹Be,3nαγ); M2 ruled out by RUL
2674.932	1121.124	E(γ): From ⁵⁰Sc β^- decay. Other precise Eγ=1553.785 6, 1121.130 6, and Eγ=523.759 10 (plus 2.6 ppm systematic uncertainty) from (n,γ) M(γ): Q from γ(DCO) in (⁹Be,3nαγ); M2 ruled out by RUL
3198.730	523.792	E(γ): From ⁵⁰Sc β^- decay. Other precise Eγ=1553.785 6, 1121.130 6, and Eγ=523.759 10 (plus 2.6 ppm systematic uncertainty) from (n,γ) M(γ): stretched Q from γ(θ) in (α,2nγ) and γ(DCO) in (⁹Be,3nαγ), M2 ruled out by RUL
3868.3	2314.4	E(γ): from (t,pγ) M(γ): d,E2 from comparison to RUL; ΔJ=2 from level scheme
3974.9	1300.0	E(γ): From (α,2nγ)
4172.8	2618.6	E(γ): From (d,pγ)
4789.97	4789.3	M(γ): d,E2 from comparison to RUL; ΔJ=2 from level scheme
4880.705	1681.69	I(γ): 4881 state: Iγ(1682)/Iγ(2206)=0.220 24 in ⁵⁰Sc β^- decay, 0.083 23 in (n,γ), and 0.13 in (d,pγ) are discrepant. 5380 state: Iγ(3826)/Iγ(2705)=0.42 12 in ⁵⁰Sc β^- decay is discrepant with 0.128 9 in (n,γ); 3826γ not observed in (d,pγ)
4880.705	2205.722	I(γ): 4881 state: Iγ(1682)/Iγ(2206)=0.220 24 in ⁵⁰Sc β^- decay, 0.083 23 in (n,γ), and 0.13 in (d,pγ) are discrepant. 5380 state: Iγ(3826)/Iγ(2705)=0.42 12 in ⁵⁰Sc β^- decay is discrepant with 0.128 9 in (n,γ); 3826γ not observed in (d,pγ)
5186.103	1039	E(γ): From (d,pγ) I(γ): From (d,pγ)
5379.942	2704.92	I(γ): 4881 state: Iγ(1682)/Iγ(2206)=0.220 24 in ⁵⁰Sc β^- decay, 0.083 23 in (n,γ), and 0.13 in (d,pγ) are discrepant. 5380 state: Iγ(3826)/Iγ(2705)=0.42 12 in ⁵⁰Sc β^- decay is discrepant with 0.128 9 in (n,γ); 3826γ not observed in (d,pγ)
5379.942	3826.08	I(γ): 4881 state: Iγ(1682)/Iγ(2206)=0.220 24 in ⁵⁰Sc β^- decay, 0.083 23 in (n,γ), and 0.13 in (d,pγ) are discrepant. 5380 state: Iγ(3826)/Iγ(2705)=0.42 12 in ⁵⁰Sc β^- decay is discrepant with 0.128 9 in (n,γ); 3826γ not observed in (d,pγ) M(γ): d,E2 from comparison to RUL; ΔJ=2 from level scheme
5440.74	2765.73	E(γ): From ⁵⁰Sc β^- decay. Other precise Eγ=1553.785 6, 1121.130 6, and Eγ=523.759 10 (plus 2.6 ppm systematic uncertainty) from (n,γ)
5837.2	1690.0	E(γ): From (d,pγ) I(γ): From (d,pγ)
5837.2	3162	E(γ): From (d,pγ) I(γ): From (d,pγ)
5946.479	760.31	M(γ): dipole from comparison to RUL. Δπ=no from level scheme
5946.479	1799	E(γ): From (d,pγ) I(γ): From (d,pγ)
6123.15	1636.45	M(γ): d,E2 from comparison to RUL; ΔJ=2 from level scheme
	1975.8	E(γ): From (d,pγ) I(γ): From (d,pγ)
	2924.9	M(γ): d,E2 from comparison to RUL; ΔJ=2 from level scheme
6136.3	2937.5	E(γ): weighted average of 2938.0 7 from (⁴⁶Ar,5nγ), 2936.4 16 from (α,2nγ), and 2935.5 20 from (⁹Be,3nαγ) M(γ): From γ(θ), γγ(θ)(DCO), and γγ linear polarization in (α,2nγ)
6379.88	1498.8	E(γ): From (d,pγ) I(γ): From (d,pγ)
6379.88	2232.3	E(γ): From (d,pγ) I(γ): From (d,pγ)
6481.2	2309.1	E(γ): From (d,pγ)
6521.41	2348.5	E(γ): From (d,pγ) I(γ): From (d,pγ)
6521.41	2373.3	E(γ): From (d,pγ) I(γ): From (d,pγ)
E(level)	E(gamma)	Comments
6540.7	404.4	E(γ): weighted average of 404.4 4 from (⁴⁶Ar,5nγ) and 404.5 7 from (α,2nγ), M(γ): From γ(θ), γγ(θ)(DCO), and γγ linear polarization in (α,2nγ)
6710.570	2300.43	M(γ): dipole from comparison to RUL. Δπ=no from level scheme
6710.570	5156.46	M(γ): d,E2 from comparison to RUL; ΔJ=2 from level scheme
6770.5	229.8	E(γ): weighted average of 230.39 30 from (⁴⁶Ar,5nγ), 229.6 7 from (α,2nγ), and 229.3 3 from (⁹Be,3nαγ) M(γ): From γ(θ), γγ(θ)(DCO), and γγ linear polarization in (α,2nγ)
7539.5	770.2	E(γ): From (α,2nγ) I(γ): From (α,2nγ)
7572.6	802.1	E(γ): unweighted average of 803.4 4 from (⁴⁶Ar,5nγ), 801.3 6 from (α,2nγ), and 801.5 6 from (⁹Be,3nαγ) M(γ): From γ(θ), γγ(θ)(DCO), and γγ linear polarization in (α,2nγ)
8257.7	1718.0	E(γ): From (α,2nγ)
8793.7	1221.1	E(γ): unweighted average of 1223.7 11 from (⁴⁶Ar,5nγ), 1219.8 10 from (α,2nγ), and 1219.9 10 from (⁹Be,3nαγ) M(γ): From γ(θ), γγ(θ)(DCO), and γγ linear polarization in (α,2nγ)
10939.184	3456.17	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	3707.4	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	3860.1	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	3909.0	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4089.93	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4101.32	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4209.17	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4228.43	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4417.55	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4539.01	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4559.13	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4637.13	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4782.6	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4815.79	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	4992.420	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	5132.72	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	5244.04	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	5391.07	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	5558.937	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	5752.692	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	6058.105	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	6148.85	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	6451.6	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	6528.72	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	6766.73	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	6791.41	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	8263.51	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal
	9384.41	E(γ): Primary γ from (n,γ) E=thermal I(γ): Primary γ from (n,γ) E=thermal