List of levels for 139LA

ADOPTED LEVELS, GAMMAS for ¹³⁹La

Authors: P.K. Joshi, B. Singh, S. Singh, A.K. Jain | Citation: Nucl. Data Sheets 138, 1 (2016) | Cutoff date: 15-Oct-2016

Full ENSDF file | Adopted Levels (PDF version)

Q(β-)=-278 keV 7	S(n)= 8778.0 keV 26	S(p)= 6255.7 keV 23	Q(α)= -2071.7 keV 25
Reference: 2012WA38

References:
A	¹³⁹Ba β^- decay (82.93 M)	B	¹³⁹Ce ε decay (137.641 d)
C	¹³⁸Ba(pol p,p),(pol p,p’):IAR	D	¹³⁸Ba(³He,d),(α,t)
E	¹³⁸Ba(⁷Li,⁶He)	F	¹³⁸La(n,γ),(n,n):Resonances
G	¹³⁸La(d,p)	H	¹³⁹La(γ,γ’):E=1.2-4.1 MeV
I	¹³⁹La(γ,γ’):E=6.0-8.6 MeV	J	¹³⁹La(γ,γ’):E=5.4-11.5 MeV
K	¹³⁹La(n,n’γ),(n,n’)	L	¹³⁹La(d,d’),(α,α’)
M	Coulomb Excitation	N	¹⁴⁰Ce(μ^-,nγ)
O	¹⁴⁰Ce(d,³He)	P	²³⁸U(¹²C,Fγ)

Other reactions:

2015Kh02: ¹³⁹La(³He,X)¹³⁸La/¹³⁹La, E=38 MeV; measured Eγ, Iγ; deduced γ-ray strength functions, and nuclear level densities

1997Sa05: ¹³⁹La(pol n,n’), E=0.5-1 eV. Measured parity-violating spin rotation angle near p-wave resonance and deduced parity mixing matrix element.

1996Ha05: ¹³⁹La(π⁺,|K⁺)¹³⁹_|LLa E=1.06 GeV/c. measured hypernuclei mass spectra. Deduced |L hypernuclei spectroscopic properties.

1996Ha47: ¹³⁹La(π⁺,|K⁺)¹³⁹_|LLa E=1.06 GeV/c. measured |L hypernuclei excitation energy spectra. Deduced binding energy mass number dependence.

1995Aj01: ¹³⁹La(π⁺,|K⁺)¹³⁹_|LLa E=1.06 GeV/c. measured σ(θ); superconducting kaon spectrometer. FWHM=2 MeV. Deduced s_|L, p_|L, d_|L, f_|L, and g_|L binding energies.

1994Al35: polarized La(pol n,X), E=0.5-10 eV; measured transmission; deduced J(3 eV res)=11/2 from sign of ε=(N₊-N_-)/(N₊+N_-)

2006MuZX: evaluation of neutron resonances

Q-value: S(2n)=16230.3 28, S(2p)=15260.7 23 (2012Wa38)

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 I J K L M N O P	7/2+	STABLE
165.8577 11	A B D E H I K L M N O P	5/2+	1.50 ns 3	165.8575 11	100	M1	0.0	7/2+
1209.0 3	D E K O	1/2+		1043.1 3	100		165.8577	5/2+
1216 1 ?	H O			1216			0.0	7/2+
1219.047 10	A H I K L M N	9/2+	0.58 ps 9	1053.162 32 1219.044 10	12.8 18 100 1	E2 E2+M1	165.8577 0.0	5/2+ 7/2+
1256.797 10	A I K L M N	(5/2)+		1090.938 10 1256.772 22	100.0 24 39.9 11	M1+E2 M1+E2	165.8577 0.0	5/2+ 7/2+
1381.408 12	A H I K N P	(9/2+)		1215.542 12 1381.560 93	100.0 8 5.2 3		165.8577 0.0	5/2+ 7/2+
1420.3 3	D I O P	(11/2)-		1420.0 5		[M2]	0.0	7/2+
1420.490 7	A E H I K L M N	(7/2)+		1254.631 10 1420.478 10	11.5 1 100	M1+E2	165.8577 0.0	5/2+ 7/2+
1476.489 7	A I K	(9/2+)		1310.617 10 1476.488 10	100 3 11.5 18		165.8577 0.0	5/2+ 7/2+
1536.388 7	A G H I K	7/2+	0.044 ps 7	1370.509 10 1536.391 10	100 4 100.0 10	M1+E2 M1+E2	165.8577 0.0	5/2+ 7/2+
1537.69 10	K L M P	(11/2+)		1537.69 10	100		0.0	7/2+
1558.72 3	A D E K O	3/2+,5/2+		1392.944 75 1558.697 31	47 4 100 5		165.8577 0.0	5/2+ 7/2+
1578.163 14	A H I K L M	5/2+,7/2+		1578.156 14	100	M1+E2	0.0	7/2+
1683.146 10	A H I K L M	7/2+		1517.73 18 1683.133 10	1.62 17 100.0 9	M1+E2	165.8577 0.0	5/2+ 7/2+
1711.66 20	P	(13/2+)		174.0 3 291.3 3 330.3 3	53 9 19 6 100 15		1537.69 1420.3 1381.408	(11/2+) (11/2)- (9/2+)
1716.12 10	H I K L M	5/2+		1716.11 10	100	M1+E2	0.0	7/2+
1740 1	H			1740	100		0.0	7/2+
1761.167 10	A I K			1595.299 10 1761.18 13	100.0 10 2.8 11		165.8577 0.0	5/2+ 7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1766.428 24	A I K L M	(5/2)+		1600.577 26 1766.346 59	100 4 73 3	[E2]	165.8577 0.0	5/2+ 7/2+
1780 15	D E	1/2+
1800.4 4	P	(17/2+)	315 ns 35 % IT = 100	88.7 5	100	[E2]	1711.66	(13/2+)
1810	L
1837 4	E H I
1854 1	H			1854	100		0.0	7/2+
1856.62 4	A D E I K L	(3/2+,5/2+)		1690.750 36	100		165.8577	5/2+
1894.0 5	I K			1894.0 5 ?	100		0.0	7/2+
1920.43 4	A H I K L	(7/2+)		1754.604 82 1920.407 42	68 6 100 5		165.8577 0.0	5/2+ 7/2+
1940.83 12	K L	(7/2+)		174.6 2 363.1 2 403.8 2	100 69 87		1766.428 1578.163 1536.388	(5/2)+ 5/2+,7/2+ 7/2+
1950	O	(3/2+)
1954 4	I
1962.8 3	P	(13/2+)		425.2 3	100		1537.69	(11/2+)
1962.84 11	A D E K L	(5/2)+		1796.97 11	100		165.8577	5/2+
1980 1	H			1980	100		0.0	7/2+
2032.75 25	P	(15/2+)		70.0 3 232.3 4 495.0 3	6.3 26 100 13 37 7	[M1+E2]	1962.8 1800.4 1537.69	(13/2+) (17/2+) (11/2+)
2035	K L
2059.73 10	A H I K			1894.28 13 ? 2059.72 10	35 5 100 7		165.8577 0.0	5/2+ 7/2+
2123 3	I
2136 1	H			2136	100		0.0	7/2+
2152 1	H L			2152	100		0.0	7/2+
2158.1 11	I K			308.3 3 ? 477.0 9 ? 581.3 5 ?	100 14 66 19		1856.62 1683.146 1578.163	(3/2+,5/2+) 7/2+ 5/2+,7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2232 5	E I	(7/2,11/2)
2240 12	D E	3/2+,5/2+
2276 1	H			2276	100		0.0	7/2+
2291 5	I
2310 19	D E L	1/2+
2313 1	H			2313	100		0.0	7/2+
2357 1	H			2357	100		0.0	7/2+
2385 1	H L			2385	100		0.0	7/2+
2390 5	I
2401	E L	(11/2-,9/2-)
2440 1	H L			2440	100		0.0	7/2+
2448 1	H			2448	100		0.0	7/2+
2466	L
2573 1	H L			2573	100		0.0	7/2+
2597	L
2600 1	H			2600	100		0.0	7/2+
2685 1	H L	-		2685	100		0.0	7/2+
2705.0 10	H			2705	100		0.0	7/2+
2712 1 ?	H			2712	100		0.0	7/2+
2724 1	H			2724	100		0.0	7/2+
2747 1	H			2747	100		0.0	7/2+
2774 1	H			2774	100		0.0	7/2+
2780	L	(-)
2800 1	H			2634 2800	100 85 26		165.8577 0.0	5/2+ 7/2+
2811 1	H L	(+)		2811	100		0.0	7/2+
2828 1	H			2828	100		0.0	7/2+
2862 1	H			2696 2862	10 100 19		165.8577 0.0	5/2+ 7/2+
2868 1	H			2868	100		0.0	7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2870	L	+
2877 1 ?	H			2712 2877	100 109 21		165.8577 0.0	5/2+ 7/2+
2885.9 5	P	(19/2+)		853.2 4	100		2032.75	(15/2+)
2890	L	(-)
2918.0 5	P	(17/2+)		1206.3 5	100		1711.66	(13/2+)
2928 1 ?	H			2928	100		0.0	7/2+
2964 1	H			2964	100		0.0	7/2+
2972 1	H			2972	100		0.0	7/2+
2990 1	H			2990	100		0.0	7/2+
3043 1	H			2877 3043	59 100 15		165.8577 0.0	5/2+ 7/2+
3053 1	H			3053	100		0.0	7/2+
3061.2 5	P	(19/2-)		1260.8 5	100		1800.4	(17/2+)
3077 1	H			3077	100		0.0	7/2+
3095 1 ?	H			2928 3095	100 108 15		165.8577 0.0	5/2+ 7/2+
3114 1	H			2948 3114	25 100 18		165.8577 0.0	5/2+ 7/2+
3147 4	G
3150.3 6	P	(19/2+)		232.3 4	100		2918.0	(17/2+)
3175.3 5	P	(21/2+)		1374.9 4	100		1800.4	(17/2+)
3184.3 5	P	(23/2+)		9.0 8 S 298.4 3	0.5 2 100 15	[M1]	3175.3 2885.9	(21/2+) (19/2+)
3196 1 ?	H			3196	100		0.0	7/2+
3221 1	H			3221	100		0.0	7/2+
3247.9 6	P	(21/2-)		97.6 5 186.7 4	100 14 84 13		3150.3 3061.2	(19/2+) (19/2-)
3252 1	H			3252	100		0.0	7/2+
3262 1	H			3095 3262	56 100 20		165.8577 0.0	5/2+ 7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3275 1	H			3275	100		0.0	7/2+
3303 1	H			3303	100		0.0	7/2+
3305.6 6	P	(23/2-)		57.7 8 S 130.3 3	41 6 100 19	[M1]	3247.9 3175.3	(21/2-) (21/2+)
3351 1	H			3351	100		0.0	7/2+
3355 2	G	-
3361 1 ?	H			3196 3361	100 85 11		165.8577 0.0	5/2+ 7/2+
3364.5 6	P	(21/2+)		478.6 4	100		2885.9	(19/2+)
3370 1	H			3370	100		0.0	7/2+
3375 2	G	(15/2)-
3401 1	H			3235 3401	100 138 38		165.8577 0.0	5/2+ 7/2+
3433 2	G
3445 1	H			3445	100		0.0	7/2+
3458 1	H			3292 3458	100 67 13		165.8577 0.0	5/2+ 7/2+
3475 1	H			3475	100		0.0	7/2+
3483 1	H			3317 3483	23 100 19		165.8577 0.0	5/2+ 7/2+
3485 2	G	-
3517 2	G	-
3523 1	H			3523	100		0.0	7/2+
3527 1	H			3361 3527	100 117 30		165.8577 0.0	5/2+ 7/2+
3544 1	H			3378 3544	100 117 22		165.8577 0.0	5/2+ 7/2+
3555 2	G	-
3557 1	H			3391 3557	6 100 32		165.8577 0.0	5/2+ 7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3561 1	H			3395 3561	100 32 6		165.8577 0.0	5/2+ 7/2+
3573 1	H			3407 3573	6 100 20		165.8577 0.0	5/2+ 7/2+
3586 1	H			3586	100		0.0	7/2+
3611 2	G	-
3631 1	H			3631	100		0.0	7/2+
3664 1	H			3664	100		0.0	7/2+
3688 2	G	-
3732 1	H			3732	100		0.0	7/2+
3748 2	G	-
3785 2	G	-
3790 1	H			3790	100		0.0	7/2+
3799 1	H			3799	100		0.0	7/2+
3805 2	G	-
3832 1	H			3832	100		0.0	7/2+
3841 2	G
3854 1	H			3854	100		0.0	7/2+
3868 2	G
3878 1	H			3878	100		0.0	7/2+
3886 1	H			3886	100		0.0	7/2+
3905 2	G	-
3919 1	H			3919	100		0.0	7/2+
3927 2	G	(17/2)-
3931 1	H			3931	100		0.0	7/2+
3941 1	H			3941	100		0.0	7/2+
3952 2	G	-
3963 1	H			3963	100		0.0	7/2+
3980 2	G	-
4014 2	G	-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4095 2	G	-
4116.2 6	P	(25/2+)		940.9 4	100		3175.3	(21/2+)
4148 2	G	-
4230 2	G	-
4252.3 6	P	(23/2+)		887.8 4 1068.0 4	16 3 100 10		3364.5 3184.3	(21/2+) (23/2+)
4336 2	G	(-)
4394 2	G	(-)
4628.0 7	P	(27/2-)		512 1 1322.3 5	11 3 100 10		4116.2 3305.6	(25/2+) (23/2-)
4641.2 7	P	(25/2+)		388.9 3	100		4252.3	(23/2+)
4791.2 8	P			1485.6 6	100		3305.6	(23/2-)
5217.6 8	P	(27/2+)		576.4 4	100		4641.2	(25/2+)
5380.6 6	J			5380.5 6	100		0.0	7/2+
5389.8 12	J			5389.7 12	100		0.0	7/2+
5406.8 13	J			5406.7 13	100		0.0	7/2+
5423.1 7	J			5423.0 7	100		0.0	7/2+
5545.4 7	J			5545.3 7	100		0.0	7/2+
5552.7 9	J			5552.6 9	100		0.0	7/2+
5572.0 11	J			5571.9 11	100		0.0	7/2+
5582.1 10	J			5582.0 10	100		0.0	7/2+
5594.8 7	J			5594.7 7	100		0.0	7/2+
5620.4 8	J			5620.3 8	100		0.0	7/2+
5658.8 7	J			5658.7 7	100		0.0	7/2+
5688.1 5	J			5688.0 5	100		0.0	7/2+
5708.6 7	J			5708.5 7	100		0.0	7/2+
5716.5 6	J			5716.4 6	100		0.0	7/2+
5723.0 3	J			5722.9 3	100		0.0	7/2+
5811.3 8	J			5811.2 8	100		0.0	7/2+
5830.9 9	J			5830.8 9	100		0.0	7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5848.9 6	J			5848.8 6	100		0.0	7/2+
5940.2 8	J			5940.1 8	100		0.0	7/2+
5984.1 20	J			5984 2	100		0.0	7/2+
6015.9 8	I J	7/2-	0.051 eV +14-8	3895 4 4062 4 4334 4 4438 4 4481 4 4538 4 4798 6 5852 4 6015.4 8	1.1 1.1 13.6 27.9 5.8 4.8 14.4 21.5 100	D(+Q) D+Q (E1(+M2)) (E1(+M2))	2123 1954 1683.146 1578.163 1536.388 1476.489 1219.047 165.8577 0.0	7/2+ 5/2+,7/2+ 7/2+ (9/2+) 9/2+ 5/2+ 7/2+
6047.1 14	J			6047.0 14	100		0.0	7/2+
6077.9 11	J			6077.8 11	100		0.0	7/2+
6097.8 12	J			6097.7 12	100		0.0	7/2+
6112.0 15	J			6111.9 15	100		0.0	7/2+
6114.2 4	I	9/2(-)	0.068 eV 34	3956 4055 4221 2 4259 4345 4428 4534 4575 4638 4694? 4734 4858? 4896 5949 6115 2	8 2 4 2 4 1 4 1 21 1 19 1 7 1 5 1 11 1 22 1 9 1 <2 19 1 ≈1 100 1	[M2,E3]	2158.1 2059.73 1894.0 1856.62 1766.428 1683.146 1578.163 1536.388 1476.489 1420.490 1381.408 1256.797 1219.047 165.8577 0.0	(3/2+,5/2+) (5/2)+ 7/2+ 5/2+,7/2+ 7/2+ (9/2+) (7/2)+ (9/2+) (5/2)+ 9/2+ 5/2+ 7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6131.1 9	J			6131.0 9	100		0.0	7/2+
6150.8 10	J			6150.7 10	100		0.0	7/2+
6178 3	J			6178 3	100		0.0	7/2+
6194.1 9	J			6194.0 9	100		0.0	7/2+
6214.2 5	J			6214.1 5	100		0.0	7/2+
6233.3 8	J			6233.1 8	100		0.0	7/2+
6249.2 20	J			6249 2	100		0.0	7/2+
6260.2 20	J			6260 2	100		0.0	7/2+
6269.5 12	J			6269.3 12	100		0.0	7/2+
6301.1 6	J			6300.9 6	100		0.0	7/2+
6326.1 6	J			6325.9 6	100		0.0	7/2+
6354.8 5	J			6354.6 5	100		0.0	7/2+
6366.5 10	J			6366.3 10	100		0.0	7/2+
6383.5 5	J			6383.3 5	100		0.0	7/2+
6402.6 9	J			6402.4 9	100		0.0	7/2+
6417.4 23	I	9/2-	0.081 eV +13-7	4186 4 ? 4356 4 ? 4459 6 ? 4498 4 ? 4580 4 ? 4661 4 ? 4704 4 ? 4838 4 ? 4882 4 4999 4 ? 4999 4 ? 5034 4 6418 4	3.0 1.0 1.0 0.6 0.9 <1 2 4 1 6 1 4 1 4 1 2 1 100 1	D(+Q) D (E1) D(+Q) D(+Q) D(+Q) (E1(+M2))	2232 2059.73 1954 1920.43 1837 1761.167 1716.12 1578.163 1536.388 1420.490 1420.3 1381.408 0.0	(7/2,11/2) (7/2+) 5/2+ 5/2+,7/2+ 7/2+ (7/2)+ (11/2)- (9/2+) 7/2+
6435.2 20	J			6435 2	100		0.0	7/2+
6441.9 11	J			6441.7 11	100		0.0	7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6450.9 4	J			6450.7 4	100		0.0	7/2+
6465.3 7	J			6465.1 7	100		0.0	7/2+
6483.8 16	J			6483.6 16	100		0.0	7/2+
6491.3 8	J			6491.1 8	100		0.0	7/2+
6501.4 6	J			6501.2 6	100		0.0	7/2+
6526.7 6	J			6526.5 6	100		0.0	7/2+
6539.6 5	J			6539.4 5	100		0.0	7/2+
6549.6 8	J			6549.4 8	100		0.0	7/2+
6619.4 6	J			6619.2 6	100		0.0	7/2+
6651.3 7	J			6651.1 7	100		0.0	7/2+
6674.8 8	J			6674.6 8	100		0.0	7/2+
6713.0 6	J			6712.8 6	100		0.0	7/2+
6723.8 15	J			6723.6 15	100		0.0	7/2+
6755.8 7	J			6755.6 7	100		0.0	7/2+
6758.8 16	I	7/2		4704? 5075 4 5180 4 5221 4 5375 4 5502 4 ? 5540 6 6594 4 6760 4	48 9 10 6 20 6 14 6 68 6 60 13 6 100 7 48 7	D D	2059.73 1683.146 1578.163 1536.388 1381.408 1256.797 1219.047 165.8577 0.0	7/2+ 5/2+,7/2+ 7/2+ (9/2+) (5/2)+ 9/2+ 5/2+ 7/2+
6767.6 18	J			6767.4 18	100		0.0	7/2+
6875.4 8	J			6875.2 8	100		0.0	7/2+
6889.9 8	J			6889.7 8	100		0.0	7/2+
6901.1 10	J			6900.9 10	100		0.0	7/2+
6926.3 8	J			6926.1 8	100		0.0	7/2+
6969.0 6	J			6968.8 6	100		0.0	7/2+
6983.4 7	J			6983.2 7	100		0.0	7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7019.7 10	J			7019.5 10	100		0.0	7/2+
7036.1 9	J			7035.9 9	100		0.0	7/2+
7052.4 7	J			7052.2 7	100		0.0	7/2+
7154.0 11	J			7153.8 11	100		0.0	7/2+
7158 3	J			7158 3	100		0.0	7/2+
7272.8 15	J			7272.6 15	100		0.0	7/2+
7278.3 22	I			5150 4 5360 4 5459 4 5699 4 7279 4	100 74 44 48 70		2123 1920.43 1810 1578.163 0.0	(7/2+) 5/2+,7/2+ 7/2+
7320.0 8	J			7319.8 8	100		0.0	7/2+
7327.2 8	J			7327.0 8	100		0.0	7/2+
7370.0 8	J			7369.8 8	100		0.0	7/2+
7400.0 7	J			7399.8 7	100		0.0	7/2+
7414.0 7	J			7413.8 7	100		0.0	7/2+
7444.9 12	J			7444.7 12	100		0.0	7/2+
7451.1 9	J			7450.9 9	100		0.0	7/2+
7462.8 7	J			7462.6 7	100		0.0	7/2+
7472.0 9	J			7471.8 9	100		0.0	7/2+
7506.7 7	J			7506.5 7	100		0.0	7/2+
7552.7 8	J			7552.5 8	100		0.0	7/2+
7562.1 4	J			7561.9 4	100		0.0	7/2+
7570.2 11	J			7570.0 11	100		0.0	7/2+
7579.8 6	J			7579.6 6	100		0.0	7/2+
7591.6 11	J			7591.4 11	100		0.0	7/2+
7599.1 7	J			7598.9 7	100		0.0	7/2+
7636.2 5	I J	7/2-	0.17 eV 4	5867? 7636.0 5	16 2 100 6	E1	1766.428 0.0	(5/2)+ 7/2+
7661.3 18	J			7661.1 18	100		0.0	7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7667 3	J			7667 3	100		0.0	7/2+
7678.6 16	J			7678.4 16	100		0.0	7/2+
7684.7 9	J			7684.5 9	100		0.0	7/2+
7692.4 12	J			7692.2 12	100		0.0	7/2+
7699 3	J			7699 3	100		0.0	7/2+
7765.1 13	J			7764.9 13	100		0.0	7/2+
7789.4 13	J			7789.2 13	100		0.0	7/2+
7905.2 6	J			7905.0 6	100		0.0	7/2+
7912.5 7	J			7912.3 7	100		0.0	7/2+
7922.2 9	J			7922.0 9	100		0.0	7/2+
7961 3	J			7961 3	100		0.0	7/2+
7972.3 7	J			7972.1 7	100		0.0	7/2+
8527.2 10	I			6985 5 7312 5 8527	27 2 15 2 100 5		1536.388 1219.047 0.0	7/2+ 9/2+ 7/2+
8551.5 6	J			8551.2 6	100		0.0	7/2+
8582.3 10	I	(7/2,9/2)		7002? 7363 8582 3	9 6 23 10 100 2		1578.163 1219.047 0.0	5/2+,7/2+ 9/2+ 7/2+
8595.7 5	J			8595.4 5	100		0.0	7/2+
8781.0 1	F
8798.9 1	F
8844.6 3	F
8867.5 4	F
8908.5 7	F
8996.4 1	F
9016.3 2	F
9037.1 2	F
9082.7 3	F
9131.4 3	F
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
16177.8	C	(7/2-)	65.2 keV 5
16808.2	C	(3/2-)	98 keV 1
17263.9	C	(1/2-)	89 keV 1
17482.3	C	(9/2-)	48 keV 4
17612.3	C	(5/2-)	73 keV 1
17752.3	C	(13/2+)	34 keV 9
17818.8	C	(9/2-)	66 keV 11
17869.4	C	(7/2-)	76 keV 3
17888.3	C	(5/2-)	66 keV 2
17957.8	C	(3/2-)	57 keV 6
18019.3	C	(9/2-)	118 keV
18120.6	C	(7/2-)	95 keV 11
18140.4	C	(5/2-)	57 keV 4
18293.3	C	(7/2-)	64 keV 5
18335.0	C	(3/2-)	94 keV 5
18358.9	C	(5/2-)	68 keV 5
18363.8	C	(1/2-)	84 keV 4
18512.7?	C	(5/2-)	76 keV
18624.9?	C	(3/2-)	2 keV

E(level): From least-squares fit to Eγ data, assuming 1 keV uncertainty when not stated. For levels populated in (γ,γ’):E=1.2-4.1 MeV, 1 keV uncertainty is assumed by the evaluators

J^π(level): From angular momentum transfer in inelastic scattering for levels between 2.6 and 3.0 MeV; angular momentum transfer in (d,p) for levels between 3.0 and 4.4 MeV, except as noted; and resonance analysis for unbound states above 16 MeV. For levels populated in (γ,γ’), Jπ is limited to 5/2,7/2,9/2 from expected dipole excitation from 7/2⁺ g.s. of ¹³⁹La

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - γ cascade based on g.s.
0.0	7/2+	STABLE
1537.69 10	(11/2+)		1537.69 10	100		0.0	7/2+
2032.75 25	(15/2+)		70.0 3 232.3 4 495.0 3	6.3 26 100 13 37 7	[M1+E2]	1962.8 1800.4 1537.69	(13/2+) (17/2+) (11/2+)
2885.9 5	(19/2+)		853.2 4	100		2032.75	(15/2+)
3184.3 5	(23/2+)		9.0 8 S 298.4 3	0.5 2 100 15	[M1]	3175.3 2885.9	(21/2+) (19/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - γ cascade based on 5/2⁺
165.8577 11	5/2+	1.50 ns 3
1381.408 12	(9/2+)		1215.542 12 1381.560 93	100.0 8 5.2 3		165.8577 0.0	5/2+ 7/2+
1711.66 20	(13/2+)		174.0 3 291.3 3 330.3 3	53 9 19 6 100 15		1537.69 1420.3 1381.408	(11/2+) (11/2)- (9/2+)
1800.4 4	(17/2+)	315 ns 35 % IT = 100	88.7 5	100	[E2]	1711.66	(13/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - Band based on (23/2⁺)
4252.3 6	(23/2+)
4641.2 7	(25/2+)		388.9 3	100		4252.3	(23/2+)
5217.6 8	(27/2+)		576.4 4	100		4641.2	(25/2+)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
165.8577	5/2+	1.50 ns 3	165.8575 11	M1		0.2516	B(M1)(W.u.)=0.00257 4, α=0.2516 7
1219.047	9/2+	0.58 ps 9	1053.162 32	E2			B(E2)(W.u.)=1.76 24
1219.047	9/2+	0.58 ps 9	1219.044 10	E2+M1	-4.9 4		B(E2)(W.u.)=7.4 11, B(M1)(W.u.)=0.00076 17
1536.388	7/2+	0.044 ps 7	1370.509 10	M1+E2	-0.81 25		B(E2)(W.u.)=13 6, B(M1)(W.u.)=0.06 3
1536.388	7/2+	0.044 ps 7	1536.391 10	M1+E2	-0.89 9		B(E2)(W.u.)=14.0 14, B(M1)(W.u.)=0.070 16
1683.146	7/2+		1683.133 10	M1+E2			B(E2)(W.u.)=11.9 16
1716.12	5/2+		1716.11 10	M1+E2			B(E2)(W.u.)=19.3 22
1766.428	(5/2)+		1766.346 59	[E2]			B(E2)(W.u.)=22 4
1800.4	(17/2+)	315 ns 35 % IT = 100	88.7 5	[E2]		3.05	α=3.05 8
2032.75	(15/2+)		70.0 3	[M1+E2]		5.1	α=5.1 21
3184.3	(23/2+)		9.0 8	[M1]		1.9×10²	α=1.9×10² 7
3305.6	(23/2-)		57.7 8	[M1]		5.29	α=5.29 24
6015.9	7/2-	0.051 eV +14-8	4438 4	D(+Q)	+0.005 15
	7/2-	0.051 eV +14-8	4798 6	D+Q	+0.15 10
	7/2-	0.051 eV +14-8	5852 4	(E1(+M2))	-0.02 6		B(E1)(W.u.)=1.59E-5 +25-44
	7/2-	0.051 eV +14-8	6015.4 8	(E1(+M2))	-0.01 3		B(E1)(W.u.)=6.8E-5 +11-19
6417.4	9/2-	0.081 eV +13-7	4882 4	(E1)			B(E1)(W.u.)=1.8E-5 +4-5
	9/2-	0.081 eV +13-7	4999 4	D(+Q)	-0.1 +3-2
	9/2-	0.081 eV +13-7	4999 4	D(+Q)	-0.03 8
	9/2-	0.081 eV +13-7	6418 4	(E1(+M2))	-0.001 4		B(E1)(W.u.)=0.000134 +13-22
7636.2	7/2-	0.17 eV 4	7636.0 5	E1			B(E1)(W.u.)=0.00018 5

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	7/2+	STABLE	μ=+2.7830455 9 (1977Kr12,2014StZZ), Q=+0.200 6 (2007Ja16,2016St14) Recent hyperfine structure studies: 1994Wa31, 1990Pr03, and 1990Sh13. E(level): Recent hyperfine structure studies: 1994Wa31, 1990Pr03, and 1990Sh13. γ cascade based on g.s.
165.8577	5/2+	1.50 ns 3	T_1/2: weighted av of β^- decay (1.48 ns 3 (1966Be42), 1.50 ns 10 (1956De57), 1.50 ns 10 (1955Ge38)) and ε decay (1.60 ns 4 (1970Ko38), 1.48 ns 3 (1967Ma07), 1.47 ns 6 (1965Ge04), 1.47 ns 5 (1962Be31)). See β^- and ε decay for details. E(level): T_1/2: weighted av of β^- decay (1.48 ns 3 (1966Be42), 1.50 ns 10 (1956De57), 1.50 ns 10 (1955Ge38)) and ε decay (1.60 ns 4 (1970Ko38), 1.48 ns 3 (1967Ma07), 1.47 ns 6 (1965Ge04), 1.47 ns 5 (1962Be31)). See β^- and ε decay for details. γ cascade based on 5/2⁺.
1209.0	1/2+		J^π(level): From angular momentum transfer in (³He,d) or (d,³He).
1219.047	9/2+	0.58 ps 9	T_1/2: from B(E2) in Coulomb excitation and adopted Jπ and γ properties. J^π(level): From γ(θ) and comparison of excitation function to theory in Coulomb excitation.
1381.408	(9/2+)		E(level): γ cascade based on 5/2⁺.
1536.388	7/2+	0.044 ps 7	T_1/2: from B(E2) in Coulomb excitation and adopted Jπ and γ properties. J^π(level): From γ(θ) and comparison of excitation function to theory in Coulomb excitation.
1537.69	(11/2+)		E(level): γ cascade based on g.s.
1558.72	3/2+,5/2+		J^π(level): From angular momentum transfer in (³He,d) or (d,³He).
1578.163	5/2+,7/2+		J^π(level): From γ(θ) and comparison of excitation function to theory in Coulomb excitation.
1711.66	(13/2+)		E(level): γ cascade based on 5/2⁺. J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
1716.12	5/2+		J^π(level): From γ(θ) and comparison of excitation function to theory in Coulomb excitation.
1780	1/2+		J^π(level): From angular momentum transfer in (³He,d) or (d,³He).
1800.4	(17/2+)	315 ns 35 % IT = 100	E(level): γ cascade based on 5/2⁺. J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
1856.62	(3/2+,5/2+)		J^π(level): From angular momentum transfer in (³He,d) or (d,³He).
1962.8	(13/2+)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
2032.75	(15/2+)		E(level): γ cascade based on g.s. J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
2035			XREF: K(?). E(level): From inelastic scattering.
2158.1			XREF: K(?).
2240	3/2+,5/2+		E(level): From inelastic scattering. J^π(level): From angular momentum transfer in (³He,d) or (d,³He).
2310	1/2+		J^π(level): From angular momentum transfer in (³He,d) or (d,³He).
2385			E(level): From inelastic scattering.
2885.9	(19/2+)		E(level): γ cascade based on g.s. J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
2918.0	(17/2+)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
3061.2	(19/2-)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
3150.3	(19/2+)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
E(level)	J^π(level)	T_1/2(level)	Comments
3175.3	(21/2+)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
3184.3	(23/2+)		E(level): γ cascade based on g.s. J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
3247.9	(21/2-)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
3305.6	(23/2-)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
3355	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3364.5	(21/2+)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
3485	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3517	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3555	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3611	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3688	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3748	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3785	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3805	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3905	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3927	(17/2)-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3952	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
3980	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
4014	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
4095	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
4116.2	(25/2+)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
4148	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
4230	-		J^π(level): L(d,p) and/or comparison to theoretical calculations.
4252.3	(23/2+)		E(level): Band based on (23/2⁺). J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
4336	(-)		J^π(level): L(d,p) and/or comparison to theoretical calculations.
E(level)	J^π(level)	T_1/2(level)	Comments
4394	(-)		J^π(level): L(d,p) and/or comparison to theoretical calculations.
4628.0	(27/2-)		J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
4641.2	(25/2+)		E(level): Band based on (23/2⁺). J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
5217.6	(27/2+)		E(level): Band based on (23/2⁺). J^π(level): For high-spin levels from (¹²C,Fγ), tentative assignments are from yrast type of population, band structures and consistency of intensities of cascading and cross over transitions.
6015.9	7/2-	0.051 eV +14-8	Γ from (γ,γ’):E=6.0-8.6 MeV. J^π(level): From γ(θ) and polarization of elastically scattered γ in (γ,γ’) E=6.0-8.6 MeV.
6114.2	9/2(-)	0.068 eV 34	Γ from (γ,γ’):E=6.0-8.6 MeV.
6417.4	9/2-	0.081 eV +13-7	Γ from (γ,γ’):E=6.0-8.6 MeV. J^π(level): From γ(θ) and polarization of elastically scattered γ in (γ,γ’) E=6.0-8.6 MeV.
6758.8	7/2		J^π(level): From γ(θ) in (γ,γ’).
7636.2	7/2-	0.17 eV 4	Γ from (γ,γ’):E=6.0-8.6 MeV. J^π(level): From γ(θ) and polarization of elastically scattered γ in (γ,γ’) E=6.0-8.6 MeV.
8582.3	(7/2,9/2)		J^π(level): From γ-deexcitation pattern.
16177.8	(7/2-)	65.2 keV 5	T_1/2(level): Width from (pol p,p’):IAR.
16808.2	(3/2-)	98 keV 1	T_1/2(level): Width from (pol p,p’):IAR.
17263.9	(1/2-)	89 keV 1	T_1/2(level): Width from (pol p,p’):IAR.
17482.3	(9/2-)	48 keV 4	T_1/2(level): Width from (pol p,p’):IAR.
17612.3	(5/2-)	73 keV 1	T_1/2(level): Width from (pol p,p’):IAR.
17752.3	(13/2+)	34 keV 9	T_1/2(level): Width from (pol p,p’):IAR.
17818.8	(9/2-)	66 keV 11	T_1/2(level): Width from (pol p,p’):IAR.
17869.4	(7/2-)	76 keV 3	T_1/2(level): Width from (pol p,p’):IAR.
17888.3	(5/2-)	66 keV 2	T_1/2(level): Width from (pol p,p’):IAR.
17957.8	(3/2-)	57 keV 6	T_1/2(level): Width from (pol p,p’):IAR.
18019.3	(9/2-)	118 keV	T_1/2(level): Width from (pol p,p’):IAR.
18120.6	(7/2-)	95 keV 11	T_1/2(level): Width from (pol p,p’):IAR.
18140.4	(5/2-)	57 keV 4	T_1/2(level): Width from (pol p,p’):IAR.
18293.3	(7/2-)	64 keV 5	T_1/2(level): Width from (pol p,p’):IAR.
18335.0	(3/2-)	94 keV 5	T_1/2(level): Width from (pol p,p’):IAR.
E(level)	J^π(level)	T_1/2(level)	Comments
18358.9	(5/2-)	68 keV 5	T_1/2(level): Width from (pol p,p’):IAR.
18363.8	(1/2-)	84 keV 4	T_1/2(level): Width from (pol p,p’):IAR.
18512.7	(5/2-)	76 keV	T_1/2(level): Width from (pol p,p’):IAR.
18624.9	(3/2-)	2 keV	T_1/2(level): Width from (pol p,p’):IAR.

E(level)	E(gamma)	Comments
1219.047	1053.162	E(γ): unweighted av of data from Coul. ex., β^- decay, and (n,n’γ).
1219.047	1219.044	E(γ): unweighted av of data from Coul. ex., β^- decay, (n,n’γ), (γ,γ’), and (μ^-,nγ).
1256.797	1256.772	I(γ): from β^- decay. Others: 72.0 17 in Coulomb. ex. and 76 9 in (n,n’γ)
1536.388	1370.509	I(γ): from Coulomb ex. Other: 102 7 in β^- decay is in agreement but somewhat less precise
1558.72	1392.944	I(γ): other: 74 7 in (n,n’γ)
1940.83	403.8	E(γ): somewhat poor fit, level-energy difference=404.4
6015.9	5852	M(γ): from γ(θ) and Iγ/Eγ³ in (γ,γ’).
6114.2	4694	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
6417.4	4882	M(γ): dipole from γ(θ) in (γ,γ’). E1 from decay scheme.
	4999	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity
	4999	E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity