List of levels for 149SM

Authors: Balraj Singh and Jun Chen | Citation: Nucl. Data Sheets 185, 2 (2022) | Cutoff date: 23-Aug-2022

Mass measurements: 1975Ka25, 1972Ba08, 1970Ma05, 1968De17, 1966Ma05

Hyperfine structure studies of the ground state: 2003Pa30, 1999Ku26, 1997Ko33, 1994Ji08, 1990Wa25, 1990En01 (also 1984Ea02), 1987Yo05, 1985Al06 (also 1984Al35,1986Al33) (laser spectroscopy), 1975St15 (NMR technique), 1972Ch55, 1972Ch27, 1968Ro16

Isotope shifts: 1990Wa25, 1990En01, 1987Bo58, 1985Al06, 1980Br15, 1976ClZY, 1973Le16, 1971Le12

Isomer shifts: 1976Co14, 1972Ei05, 1983St17 (compilation)

2017Wi01: measured isotopic abundances of natural Sm samples using inductively coupled plasma mass spectrometry (ICP-ms) technique

Other reactions:

2015Ba20: ²⁰⁸Pb(¹³⁶Xe,Xγ),E=85 MeV; measured Eγ, Iγ, γγ-coin using Gammasphere at ATLAS-ANL facility. Levels and γ rays in ¹⁴⁹Sm populated; deduced cross section.

1993Ge07: measured energies and widths of 22 neutron resonances from 94.9-2955 eV. See ¹⁴⁸Sm(n,γ),(n,n):Resonances dataset for details.

2014Fi17: ¹⁵⁰Sm(γ,n),E=6-17 MeV; measured E(n), I(n), monochromatic and nonmonochromatic σ(E).

2003Ka23: analyzed neutron resonances

¹⁴⁸Sm(n,γ): 1982Ba15, 1986Wi02

¹⁴⁸Sm(n,n): 1990Ly01 (E=0.01-0.5 eV), 1971KaZS (E<0.5 keV)

¹⁴⁹Sm(⁵⁸Ni,⁵⁸Ni),E=245 MeV: 1987Va22, measured σ(θ)

2017No07: theory: calculated single-particle energies, occupation probabilities of the single-particle orbitals, levels, Jπ, B(E2), B(M1), electric quadrupole and magnetic dipole moments using Interacting boson-fermion model (IBFM)

2013Zh28: calculated energies of ground-state band members using several collective rotor and vibrator models.

1983Ma71: calculated levels, rotational characteristics using quasiparticle-rotor model, and variable moments of inertia

Other theoretical studies: consult the NSR database at www.nndc.bnl.gov/nsr/ for 29 references for structure and six for radioactive decay listed under ’document records’ which can be accessed through web retrieval of the ENSDF database at www.nndc.bnl.gov/ensdf/

The statement "in-beam γ-ray " includes the datasets: (α,nγ); and (α,3nγ),(³He,4nγ)

Levels: The band assignments are from 1977Kl04, 1979Ha19, 1990UrZR and 1994Ba01 in ¹⁴⁸Nd(α,3nγ),¹⁵⁰Nd(³He,4nγ) dataset. It should, however, be noted that Nilsson-model assignments proposed by 1994Ba01 may not be valid for n=87 nuclide, and the levels are expected to be strongly (Coriolis) mixed.

Q-value: S(2n)=14012.5 9, S(2p)=13567.0 10 (2021Wa16)

E(level): From least-squares fit to Eγ data for levels populated in γ-ray studies. In cases, where ΔEγ is not stated, 0.3 keV is assumed when Eγ is stated to nearest tenth of a keV, and 1 keV when Eγ is stated to nearest keV. Energy uncertainties of 11 γ rays were doubled to obtain an acceptable reduced χ²=1.9 as compared to critical χ²=1.4. Without this adjustment reduced χ² was 3.7. For levels populated in particle transfer reactions only, weighted averages have been taken of all the available values. In case of unresolved doublets in particle transfer reactions, quoted energy value not included in obtaining average level energy.

J^π(level): When assigned from L(p,d), the following shell-model orbitals are assumed (by 1983Ga07) for the transferred nucleon: p_3/2 for L(n)=1; d_3/2 (below≈1.5 MeV excitation) and d_5/2 (above≈1.5 MeV excitation) for L(n)=2; f_5/2 for L(n)=3; g_7/2 for L(n)=4; h_11/2 for L(n)=5. In in-beam γ-ray study when no γ(θ) and/or ce data are available, it is assumed that in such reactions, levels of ascending Jπ are populated with increasing excitation energy. Absence of transitions to levels of low Jπ values also supports such a conclusion. Unless otherwise stated, L transfers are from 0⁺ targets

T_1/2(level): Unless stated otherwise, values are derived from B(E2) values in Coul. ex., adopted branchings and mixing ratios.

E(γ): As indicated, values for γ rays from low-spin (J|<9/2) are from ¹⁴⁹Eu and ¹⁴⁹Pm decay data, and for higher-spins, values are from (α,nγ) when given with uncertainties, and from ¹⁴⁸Nd(α,3nγ),¹⁵⁰Nd(³He,4nγ), when given without uncertainties, unless otherwise noted.

I(γ): Below 953 excitation energy, Iγ data are mainly from ¹⁴⁹Pm β^- decay or ¹⁴⁹Eu ε decay or weighted average when values from these two datasets have comparable uncertainties; above this energy, values available from (α,nγ) and ¹⁴⁸Nd(α,3nγ), ¹⁵⁰Nd(³He,4nγ) are considered, unless otherwise noted.

M(γ): From ce studies in ¹⁴⁹Pm β^-, ¹⁴⁹Eu ε and in-beam γ-ray. Above 636 keV level, the assignment is from ce and/or γ(θ) and γ(lin pol) data in in-beam γ-ray studies

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
22.5002	5/2-	7.33 ns 9	22.5002 8	M1+E2	0.0784 9	30.0	B(E2)(W.u.)=56.2 17, B(M1)(W.u.)=0.00846 17, α=30.0 5
277.071	5/2-	≤ 0.2 ns	254.566 23	M1+E2	+0.20 +8-6	0.1242	B(E2)(W.u.)>0.15, B(M1)(W.u.)>0.00083, α=0.1242 20
277.071	5/2-	≤ 0.2 ns	277.089 10	M1+E2	-0.08 +1-2	0.0997	B(E2)(W.u.)>0.14, B(M1)(W.u.)>0.0039, α=0.0997 14
285.946	9/2-	0.22 ns 4	263.23 4	[E2]		0.0849	B(E2)(W.u.)=0.123 +27-19, α=0.0849 12
285.946	9/2-	0.22 ns 4	285.95 1	M1(+E2)	+0.06 6	0.0917	B(E2)(W.u.)<0.46, B(M1)(W.u.)=0.0039 +9-6, α=0.0917 13
350.035	3/2-	9.5 ps 3	72.983 10	M1+E2	0.23 4	4.36	B(E2)(W.u.)=91 +32-28, B(M1)(W.u.)=0.0167 10, α=4.36 9
	3/2-	9.5 ps 3	327.526 10	M1+E2	+0.14 3	0.0637	B(E2)(W.u.)=5.5 +26-21, B(M1)(W.u.)=0.0551 18, α=0.0637 9
	3/2-	9.5 ps 3	350.016 10	E2		0.0352	B(E2)(W.u.)=18.4 7, α=0.0352 5
399.08	(1/2-,3/2-)		122.0 2	[M1,E2]		1.05	α=1.05 10
528.593	3/2-	24 ps 3	129.50 7	[M1,E2]		0.87	α=0.87 6
	3/2-	24 ps 3	178.580 16	M1+E2	+0.5 2	0.325	B(E2)(W.u.)=11 7, B(M1)(W.u.)=0.0025 5, α=0.325 6
	3/2-	24 ps 3	251.510 37	[M1,E2]		0.114	α=0.114 16
	3/2-	24 ps 3	506.093 10	E2+M1	+4.9 +31-15	0.0128	B(E2)(W.u.)=7.1 +10-9, B(M1)(W.u.)=0.00014 +15-8, α=0.0128 4
	3/2-	24 ps 3	528.587 10	E2		0.01108	B(E2)(W.u.)=5.6 +8-6, α=0.01108 16
558.373	5/2-	24 ps 8	208.283 21	M1+E2	-0.45 15	0.210	B(E2)(W.u.)=8 +7-4, B(M1)(W.u.)=0.0033 +16-9, α=0.210 4
	5/2-	24 ps 8	272.21 14	[E2]		0.0763	B(E2)(W.u.)=0.32 +33-18, α=0.0763 11
	5/2-	24 ps 8	281.295 16	M1+E2	+0.14 9	0.0954	B(E2)(W.u.)=1.0 +20-9, B(M1)(W.u.)=0.0075 +36-20, α=0.0954 16
	5/2-	24 ps 8	535.897 12	M1+E2	-0.65 +23-43	0.0159	B(E2)(W.u.)=1.1 +12-6, B(M1)(W.u.)=0.0014 +7-6, α=0.0159 18
	5/2-	24 ps 8	558.372 10	M1+E2	+1.2 +7-4	0.0124	B(E2)(W.u.)=2.2 +13-9, B(M1)(W.u.)=0.0009 +6-4, α=0.0124 13
590.883	9/2-	3.0 ps 7	305.22 8	M1(+E2)	+0.15 15	0.0767	B(E2)(W.u.)<5.1, B(M1)(W.u.)=0.0072 +33-22, α=0.0767 18
	9/2-	3.0 ps 7	568.36 7	E2		0.00919	B(E2)(W.u.)=13.4 +41-26, α=0.00919 13
	9/2-	3.0 ps 7	590.88 1	E2+M1	-1.5 +9-4	0.0101	B(E2)(W.u.)=30 +9-13, B(M1)(W.u.)=0.008 +9-3, α=0.0101 25
636.459	7/2-	< 1.5 ps	350.71 7	M1+E2	-0.30 10	0.0521	B(E2)(W.u.)>2.9, B(M1)(W.u.)>0.015, α=0.0521 13
	7/2-	< 1.5 ps	359.57 7	M1+E2	+0.9 5	0.042	B(E2)(W.u.)>9.0, B(M1)(W.u.)>0.0052, α=0.042 6
	7/2-	< 1.5 ps	636.50 5	M1+E2	-0.30 +16-18	0.0114	B(E2)(W.u.)>0.45, B(M1)(W.u.)>0.014, α=0.0114 5
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
664.09	11/2-	2.7 ps 3	73.3	[M1]		4.13	B(M1)(W.u.)=0.83 +14-12, α=4.13 6
	11/2-	2.7 ps 3	378.3 1	M1(+E2)	0.00 3	0.0440	B(E2)(W.u.)<0.037, B(M1)(W.u.)=0.0054 8, α=0.0440 6
	11/2-	2.7 ps 3	664.1 1	E2		0.00625	B(E2)(W.u.)=26.1 +34-27, α=0.00625 9
747.39	13/2-		461.9 1	E2		0.01589	α=0.01589 22
789.51	11/2+		125.4 1	(E1)		0.1490	α=0.1490 21
789.51	11/2+		198.6 1	E1		0.0431	α=0.0431 6
878.80	13/2+		214.8 1	E1		0.0350	α=0.0350 5
1192.80	13/2+		314.0 1	M1(+E2)	+0.4 5	0.069	α=0.069 7
1192.80	13/2+		403.4 1	M1+E2	-1.1 8	0.030	α=0.030 7
1240.13	(15/2)+		492.6 1	E1		0.00446	α=0.00446 6
1308.47	11/2-		1022.4 1	M1+E2	-2.8 4	0.00253	α=0.00253 6
1360.96	17/2-		613.7 1	E2		0.00758	α=0.00758 11
1362.60	17/2+		483.8 1	E2		0.01401	α=0.01401 20
1398.70	15/2-		734.7 1	E2		0.00492	α=0.00492 7
1574.57	(13/2)-		266.1 1	M1+E2	-0.50 5	0.1054	α=0.1054 18
1670.25	(19/2)+		309.4 1	E1		0.01361	α=0.01361 19
1670.25	(19/2)+		430.0 1	E2		0.01937	α=0.01937 27
1695.7	(17/2+)		503.0	(E2)		0.01262	α=0.01262 18
1846.87	(15/2)-		272.3 1	M1+E2	-0.7 2	0.095	α=0.095 4
1925.99	(21/2)+		563.4 1	E2		0.00939	α=0.00939 13
2130.6	(17/2)-		283.8	M1		0.0937	α=0.0937 13
2142.30	(21/2-)		781.4	(E2)		0.00427	α=0.00427 6
2192.2	(23/2)+		521.9	E2		0.01145	α=0.01145 16
2537.2	(25/2)+		611.2	E2		0.00765	α=0.00765 11
2834.3	(27/2)+		642.0	E2		0.00678	α=0.00678 9
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
3181.3	(29/2+)		644.0	(E2)		0.00673	α=0.00673 9
3361.2	(29/2-)		526.9	E1		0.00383	α=0.00383 5
3651.8	(31/2+)		817.0 7	E2		0.00386	α=0.00386 5
3859.6	(33/2+)		678.0	(E2)		0.00594	α=0.00594 8
4686.4	(37/2-)		718.0	(E2)		0.00519	α=0.00519 7

Q(β-)=-695 keV 4	S(n)= 5871.1 keV 9	S(p)= 7559 keV 6	Q(α)= 1871.3 keV 10
Reference: 2021WA16

References:
A	¹⁴⁹Pm β^- decay (53.08 H)	B	¹⁴⁹Eu ε decay (93.1 d)
C	muonic atom	D	¹⁴⁶Nd(α,nγ)
E	¹⁴⁸Nd(α,3nγ),¹⁵⁰Nd(³He,4nγ)	F	¹⁴⁸Sm(n,γ) E=THERMAL
G	¹⁴⁸Sm(n,γ),(n,n):Resonances	H	¹⁴⁸Sm(d,p)
I	¹⁴⁸Sm(α,³He)	J	¹⁴⁸Sm(¹⁶O,¹⁵O),(¹³C,¹²C)
K	¹⁴⁹Sm(γ,γ):MOSSBAUER	L	¹⁴⁹Sm(d,d’)
M	Coulomb Excitation	N	¹⁵⁰Sm(n,2nγ)
O	¹⁵⁰Sm(p,d)	P	¹⁵⁰Sm(d,t)
Q	¹⁵⁰Sm(³He,α)	R	¹⁵¹Sm(p,t)
S	¹⁵¹Eu(μ^-,2nγ)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - ν7/2[633] band.
789.51 6	11/2+
1240.13 11	(15/2)+		450.8 492.6 1	17 3 100 3	E1	789.51 747.39	11/2+ 13/2-
1670.25 12	(19/2)+		309.4 1 430.0 1	100 3 51 3	E1 E2	1360.96 1240.13	17/2- (15/2)+
2192.2 3	(23/2)+		521.9	100	E2	1670.25	(19/2)+
2834.3 4	(27/2)+		642.0	100	E2	2192.2	(23/2)+
3651.8 5	(31/2+)		291 817.0 7	<29 100 8	E2	3361.2 2834.3	(29/2-) (27/2)+
4575.1 9	(35/2+)		607 923			3968.4 3651.8	(33/2-) (31/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - ν9/2[624] band.
878.80 8	13/2+
1362.60 13	17/2+		483.8 1	100	E2	878.80	13/2+
1925.99 16	(21/2)+		563.4 1	100	E2	1362.60	17/2+
2537.2 3	(25/2)+		611.2	100	E2	1925.99	(21/2)+
3181.3 4	(29/2+)		644.0	100	(E2)	2537.2	(25/2)+
3859.6 5	(33/2+)		678.0	100	(E2)	3181.3	(29/2+)
4597.3 6	(37/2+)		737.7	100		3859.6	(33/2+)
5361.3 12	(41/2+)		764			4597.3	(37/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - ν7/2[514] band.
0.0	7/2-	STABLE
664.09 6	11/2-	2.7 ps 3	73.3 378.3 1 664.1 1	5.3 7 4.74 30 100.0 17	[M1] M1(+E2) E2	590.883 285.946 0.0	9/2- 9/2- 7/2-
1398.70 9	15/2-		520.7 1 651.1 1 734.7 1	21.4 14 11 2 100 5	D E2	878.80 747.39 664.09	13/2+ 13/2- 11/2-
2041.0 3	(19/2-)		641 678 680.2			1398.70 1362.60 1360.96	15/2- 17/2+ 17/2-
2701.7 5	(23/2-)		661 776			2041.0 1925.99	(19/2-) (21/2)+
3328.0 8	(27/2-)		626 791			2701.7 2537.2	(23/2-) (25/2)+
3953.3 11	(31/2-)		772			3181.3	(29/2+)
4543.8 6	(35/2-)		489.4 684.0			4054.7 3859.6	(33/2+) (33/2+)
5140.6 9	(39/2-)		543 597			4597.3 4543.8	(37/2+) (35/2-)
5801.6 14	(43/2-)		661			5140.6	(39/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - ν9/2[505] band.
285.946 10	9/2-	0.22 ns 4
747.39 7	13/2-		84 1 ? 461.9 1	100	E2	664.09 285.946	11/2- 9/2-
1360.96 11	17/2-		121.0 8 613.7 1	11.4 3 100	E2	1240.13 747.39	(15/2)+ 13/2-
2142.30 24	(21/2-)		472.0 781.4	≈14 100 27	(E2)	1670.25 1360.96	(19/2)+ 17/2-
2842.2 5	(25/2-)		141 650 700			2701.7 2192.2 2142.30	(23/2-) (23/2)+ (21/2-)
3361.2 4	(29/2-)		519.0 526.9		E1	2842.2 2834.3	(25/2-) (27/2)+
3968.4 6	(33/2-)		316.6 607			3651.8 3361.2	(31/2+) (29/2-)
4686.4 7	(37/2-)		718.0		(E2)	3968.4	(33/2-)
5477.4 12	(41/2-)		791			4686.4	(37/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - ν11/2[505] band.
1308.47 9	11/2-
1574.57 14	(13/2)-		266.1 1	100	M1+E2	1308.47	11/2-
1846.87 17	(15/2)-		272.3 1 538	100	M1+E2	1574.57 1308.47	(13/2)- 11/2-
2130.6 3	(17/2)-		283.8 555.9?	100 43	M1	1846.87 1574.57	(15/2)- (13/2)-
2427.1 3	(19/2-)		296.4 580.2	100 10 ≈16	D	2130.6 1846.87	(17/2)- (15/2)-
2734.9 4	(21/2-)		307.5 606	100		2427.1 2130.6	(19/2-) (17/2)-
3055.1 5	(23/2-)		320.1 629			2734.9 2427.1	(21/2-) (19/2-)
3384.0 9	(25/2-)		329 649			3055.1 2734.9	(23/2-) (21/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - Band based on 13/2⁺
1192.80 8	13/2+
1695.7 3	(17/2+)		283 296 333 455 503.0	<52 100.0 23	(E2)	1413.28 1398.70 1362.60 1240.13 1192.80	(13/2+,15/2+) 15/2- 17/2+ (15/2)+ 13/2+
2344.5 4	(21/2+)		304 419 493 649 674 1			2041.0 1925.99 1851.2 1695.7 1670.25	(19/2-) (21/2)+ (17/2+) (17/2+) (19/2)+
2875.5 4	(25/2+)		174 339 531.0 683			2701.7 2537.2 2344.5 2192.2	(23/2-) (25/2)+ (21/2+) (23/2)+
3364.8 5	(29/2+)		489.4 530 828			2875.5 2834.3 2537.2	(25/2+) (27/2)+ (25/2)+
4054.7 6	(33/2+)		691 875			3364.8 3181.3	(29/2+) (29/2+)
4799.0 10	(37/2+)		744			4054.7	(33/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - Band based on 5/2-
22.5002 8	5/2-	7.33 ns 9
590.883 10	9/2-	3.0 ps 7	305.22 8 568.36 7 590.88 1	3.72 23 25.9 17 100.0 22	M1(+E2) E2 E2+M1	285.946 22.5002 0.0	9/2- 5/2- 7/2-
1343.33 7	(13/2-)		553.6 1 596.1 1 752.5 1	75 13 100 3 73 10		789.51 747.39 590.883	11/2+ 13/2- 9/2-

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	7/2-	STABLE	μ=-0.6677 11 (1990En01,2019StZV), Q=+0.075 8 (1972Ch55,1992Le09,2021StZZ) δ<r²>(¹⁴⁸Sm,¹⁴⁹Sm)=0.080 fm² 8 (1971Le12,1973Le16), 0.084 fm² 28 (1979Po04), 0.092 fm² 5 (1980Br15), 0.092 fm² (1985Al06), 0.080 fm² 8 (1986Al33), 0.093 fm² 5 (1987Bo58), 0.092 fm² 4 (1990Wa25), 0.089 fm² (1990En01). E(level): ν7/2[514] band.
22.5002	5/2-	7.33 ns 9	μ=-0.6200 11 (1970EiZY,2020StZV), Q=+1.01 9 (1981Ba28,2021StZZ) B(E2)=0.229 17 from muonic atom (1981Ba28). E(level): Band based on 5/2-.
285.946	9/2-	0.22 ns 4	Configuration=νh_9/2. E(level): ν9/2[505] band.
399.08	(1/2-,3/2-)		XREF: Q(422).
528.593	3/2-	24 ps 3	XREF: H(535).
558.373	5/2-	24 ps 8	XREF: H(566).
590.883	9/2-	3.0 ps 7	XREF: O(583)R(606). E(level): Band based on 5/2-.
664.09	11/2-	2.7 ps 3	XREF: H(675). E(level): ν7/2[514] band.
709.85	(3/2,5/2+)		XREF: M(?).
747.39	13/2-		E(level): ν9/2[505] band.
789.51	11/2+		E(level): ν7/2[633] band.
878.80	13/2+		XREF: I(910). E(level): ν9/2[624] band.
925.47	(3/2+,5/2+)		XREF: L(914)p(922).
994.65	(9/2,11/2,13/2-)		XREF: p(988).
1083	(LE 7/2)		XREF: L(1072).
1192.80	13/2+		E(level): Band based on 13/2⁺.
1240.13	(15/2)+		E(level): ν7/2[633] band.
1308.47	11/2-		XREF: O(1285)p(1311). E(level): ν11/2[505] band.
1325			XREF: H(1316).
1343.33	(13/2-)		E(level): Band based on 5/2-.
1360.96	17/2-		E(level): ν9/2[505] band.
1362.60	17/2+		E(level): ν9/2[624] band.
1393	(5/2)-		XREF: O(1408).
1398.70	15/2-		E(level): ν7/2[514] band.
1470	(3/2,5/2)+		XREF: O(1456)Q(1474).
E(level)	J^π(level)	T_1/2(level)	Comments
1483	(LE 5/2)		XREF: O(1480)Q(1474).
1574.57	(13/2)-		E(level): ν11/2[505] band.
1670.25	(19/2)+		E(level): ν7/2[633] band.
1685			XREF: H(1678).
1695.7	(17/2+)		E(level): Band based on 13/2⁺.
1699	5/2-		XREF: H(1705).
1776	(7/2+)&(5/2+)		XREF: H(1782).
1846.87	(15/2)-		E(level): ν11/2[505] band.
1851.2	(17/2+)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
1925.99	(21/2)+		E(level): ν9/2[624] band.
2026	(5/2+)&(11/2-)		XREF: Q(2043).
2041.0	(19/2-)		E(level): ν7/2[514] band.
2117	5/2-		XREF: H(2137).
2130.6	(17/2)-		E(level): ν11/2[505] band.
2142.30	(21/2-)		E(level): ν9/2[505] band.
2192.2	(23/2)+		E(level): ν7/2[633] band.
2344.5	(21/2+)		E(level): Band based on 13/2⁺.
2404.4	(21/2+)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
2427.1	(19/2-)		E(level): ν11/2[505] band.
2442	(5/2+) AND (11/2-)		XREF: O(2459).
2537.2	(25/2)+		E(level): ν9/2[624] band.
2701.7	(23/2-)		E(level): ν7/2[514] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
2734.9	(21/2-)		E(level): ν11/2[505] band.
2828.2	(25/2-)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
2834.3	(27/2)+		E(level): ν7/2[633] band.
E(level)	J^π(level)	T_1/2(level)	Comments
2842.2	(25/2-)		E(level): ν9/2[505] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
2875.5	(25/2+)		E(level): Band based on 13/2⁺. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
2987.2	(25/2)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3008.4	(25/2+)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3055.1	(23/2-)		E(level): ν11/2[505] band.
3159.3	(25/2)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3181.3	(29/2+)		E(level): ν9/2[624] band.
3220.3	(25/2)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3328.0	(27/2-)		E(level): ν7/2[514] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3361.2	(29/2-)		E(level): ν9/2[505] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3364.8	(29/2+)		E(level): Band based on 13/2⁺. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3384.0	(25/2-)		E(level): ν11/2[505] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3564.1	(29/2-)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3651.8	(31/2+)		E(level): ν7/2[633] band.
3777.3	(29/2)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3859.6	(33/2+)		E(level): ν9/2[624] band.
3880.3	(31/2-)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3953.3	(31/2-)		E(level): ν7/2[514] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
3968.4	(33/2-)		E(level): ν9/2[505] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
4005.9	(33/2-)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
4054.7	(33/2+)		E(level): Band based on 13/2⁺. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
4486.8	(33/2)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
4543.8	(35/2-)		E(level): ν7/2[514] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
4575.1	(35/2+)		E(level): ν7/2[633] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
4597.3	(37/2+)		E(level): ν9/2[624] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
E(level)	J^π(level)	T_1/2(level)	Comments
4606.6	(37/2-)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
4686.4	(37/2-)		E(level): ν9/2[505] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
4799.0	(37/2+)		E(level): Band based on 13/2⁺. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
5140.6	(39/2-)		E(level): ν7/2[514] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
5173.4	(39/2+)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
5325.4	(39/2)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
5361.3	(41/2+)		E(level): ν9/2[624] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
5372.5	(41/2-)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
5477.4	(41/2-)		E(level): ν9/2[505] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
5791.5	(43/2)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
5801.6	(43/2-)		E(level): ν7/2[514] band. J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.
6189.5	(45/2)		J^π(level): Assignments taken from 1990UrZR and 1990UrZX which are probably based on authors’ γ(θ), γ(lin pol) data. But no details of these data are available. Assignment is considered tentative by evaluators.

E(level)	E(gamma)	Comments
22.5002	22.5002	E(γ): from ¹⁴⁹Eu ε decay, value is from 2011In01. Others: 22.519 8 (1982Me10) and 22.494 11 (1970An17)
277.071	254.566	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases. I(γ): weighted average of 18.3 11 from ¹⁴⁹Pm β^- decay, 17.93 23 from ¹⁴⁹Eu ε decay, and 16.9 6 from (α,nγ). Others: 97 5 from (α,3nγ) and 46 12 from (μ^-,2nγ) are discrepant
277.071	277.089	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
285.946	263.23	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From ¹⁴⁹Pm β^- decay
285.946	285.95	E(γ): From ¹⁴⁹Pm β^- decay
350.035	72.983	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases. I(γ): other: 26 8 from (α,3nγ) is discrepant
	327.526	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	350.016	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases. I(γ): others: 9.6 17 from Coulomb excitation; 16.5 23 from (α,nγ) and 19 8 from (α,3nγ) are discrepant
399.08	122.0	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
399.08	376.5	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
528.593	129.50	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	178.580	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	251.510	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	506.093	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	528.587	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases. I(γ): from ¹⁴⁹Eu ε decay. Others: 100 25 from ¹⁴⁹Pm β^- decay
558.373	208.283	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases. I(γ): weighted average of 9.6 6 from ¹⁴⁹Pm β^- decay, 23.1 19 from ¹⁴⁹Eu ε decay, 8.3 17 from (α,nγ), and 8.1 17 from (α,3nγ). weighted average of 9.6 6 from ¹⁴⁹Pm β^- decay, 8.3 17 from (α,nγ), and 8.1 17 from (α,3nγ). Other: 23 2 from ¹⁴⁹Eu ε decay seems discrepant
	272.21	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	281.295	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	535.897	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases. I(γ): weighted average of 76 4 from ¹⁴⁹Pm β^- decay, 85.5 27 from ¹⁴⁹Eu ε decay, 88 4 from (α,nγ), and 96 27 from Coulomb excitation. Other: 13.9 17 from (α,3nγ) is discrepant
	558.372	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
590.883	305.22	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From ¹⁴⁹Pm β^- decay I(γ): from ¹⁴⁹Pm β^- decay. Others: 3.5 8 from Coulomb excitation and 4.5 18 from (α,3nγ); 2.27 22 from (α,nγ) is discrepant M(γ): ce data in in-beam γ-ray
	568.36	E(γ): From ¹⁴⁹Pm β^- decay I(γ): weighted average of 26.9 18 from ¹⁴⁹Pm β^- decay, 25 9 from ¹⁴⁹Eu ε decay, 24.0 22 from (α,nγ), 31.3 18 from (α,3nγ), and 22.7 14 from Coulomb excitation M(γ): γ(θ,pol) in in-beam γ-ray
	590.88	E(γ): From ¹⁴⁹Pm β^- decay I(γ): from (α,3nγ). Others: 100 4 from ¹⁴⁹Pm β^- decay, 100 9 from ¹⁴⁹Eu ε decay, 100 5 from (α,nγ), 100.0 26 from Coulomb excitation M(γ): ce data in in-beam γ-ray
636.459	350.71	E(γ): From ¹⁴⁹Pm β^- decay M(γ): from RUL; E1⁺M2 not allowed
	359.57	E(γ): From ¹⁴⁹Pm β^- decay M(γ): from RUL; E1⁺M2 not allowed
	613.92	E(γ): From ¹⁴⁹Pm β^- decay
	636.50	E(γ): From ¹⁴⁹Pm β^- decay
E(level)	E(gamma)	Comments
658.66	130.10	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	308.0	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	381.7	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
	636.05	E(γ): From ¹⁴⁹Eu ε decay. Available value from ¹⁴⁹Pm β^- decay is nearly the same but slightly less precise in most cases.
664.09	378.3	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): weighted average of 4.92 25 from (α,nγ), 4.6 7 from (α,3nγ), and 3.5 7 from Coulomb excitation. From (α,nγ) or (α,3nγ),(³He,4nγ)
664.09	664.1	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) M(γ): ce and γ(θ,pol) in in-beam γ-ray
709.85	359.8	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
709.85	432.8	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
747.39	461.9	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
785.23	785.23	E(γ): From ¹⁴⁹Pm β^- decay
789.51	125.4	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) M(γ): γ(θ) data consistent with ΔJ=0, dipole; ΔJπ requires E1
	198.6	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
	504	E(γ): γ from (n,2n) only
830.46	544.27	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From ¹⁴⁹Pm β^- decay
	552.92	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From ¹⁴⁹Pm β^- decay
	808.11	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From ¹⁴⁹Pm β^- decay
	830.53	E(γ): From ¹⁴⁹Pm β^- decay
833.23	242.10	E(γ): From ¹⁴⁹Pm β^- decay
	547.17	E(γ): From ¹⁴⁹Pm β^- decay
	833.40	E(γ): From ¹⁴⁹Pm β^- decay
835.59	550.01	E(γ): From ¹⁴⁹Pm β^- decay
	812.92	E(γ): From ¹⁴⁹Pm β^- decay
	835.55	E(γ): From ¹⁴⁹Pm β^- decay
878.80	89.3	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
878.80	214.8	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
E(level)	E(gamma)	Comments
881.97	323.95	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From ¹⁴⁹Pm β^- decay
	353.46	E(γ): From ¹⁴⁹Pm β^- decay
	531.61	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From ¹⁴⁹Pm β^- decay
	859.46	E(γ): From ¹⁴⁹Pm β^- decay
	881.98	E(γ): From ¹⁴⁹Pm β^- decay
925.47	648.4	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
952.78	930.2	E(γ): From ¹⁴⁹Pm β^- decay
952.78	952.8	E(γ): From ¹⁴⁹Pm β^- decay
994.65	708.7	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1038.97	761.9	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1132.37	385.2	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1132.37	846.2	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1173.21	383.7	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1192.80	314.0	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) M(γ): from γ(θ) and pol data in (α,3nγ),(³He,4nγ)
	403.4	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
	528.6	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): doublet with undivided intensity, where part of its intensity is from 528.6 level. From (α,nγ) or (α,3nγ),(³He,4nγ)
1237.95	952.0	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1240.13	492.6	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1308.47	644.9	E(γ): Uncertainty doubled for fitting purpose, as the Eγ value fits poorly. From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1308.47	1022.4	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1343.33	553.6	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
	596.1	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
	752.5	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1360.96	613.7	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1362.60	483.8	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
E(level)	E(gamma)	Comments
1398.70	520.7	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
	651.1	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
	734.7	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1413.28	623.8	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1413.28	665.7	E(γ): other: 664.1 1 from (α,nγ) is for a doublet
1574.57	266.1	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1670.25	309.4	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1670.25	430.0	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1684.60	285.9	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1846.87	272.3	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)
1925.99	563.4	E(γ): From (α,nγ) or (α,3nγ),(³He,4nγ) I(γ): From (α,nγ) or (α,3nγ),(³He,4nγ)

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 H I J K L M N O P Q R S	7/2-	STABLE
22.5002 8	A B C D E H K M N P Q R S	5/2-	7.33 ns 9	22.5002 8	100	M1+E2	0.0	7/2-
277.071 7	A B D E H M N O P R S	5/2-	≤ 0.2 ns	254.566 23 277.089 10	17.82 25 100.0 5	M1+E2 M1+E2	22.5002 0.0	5/2- 7/2-
285.946 10	A B D E H I J M N O P Q S	9/2-	0.22 ns 4	263.23 4 285.95 1	0.31 1 100	[E2] M1(+E2)	22.5002 0.0	5/2- 7/2-
350.035 6	A B D E H L M N O P Q R S	3/2-	9.5 ps 3	72.983 10 327.526 10 350.016 10	0.347 17 100.0 5 8.95 14	M1+E2 M1+E2 E2	277.071 22.5002 0.0	5/2- 5/2- 7/2-
399.08 7	B D H O P Q	(1/2-,3/2-)		122.0 2 376.5 2 ?	100 72 10 7	[M1,E2]	277.071 22.5002	5/2- 5/2-
528.593 7	A B D E H J L M O P Q R	3/2-	24 ps 3	129.50 7 178.580 16 251.510 37 506.093 10 528.587 10	0.07 4 4.0 2 2.0 2 100.0 8 93.7 13	[M1,E2] M1+E2 [M1,E2] E2+M1 E2	399.08 350.035 277.071 22.5002 0.0	(1/2-,3/2-) 3/2- 5/2- 5/2- 7/2-
558.373 7	A B D E H M N P Q R	5/2-	24 ps 8	208.283 21 272.21 14 ? 281.295 16 535.897 12 558.372 10	9.6 6 0.24 17 46 4 84 3 100 6	M1+E2 [E2] M1+E2 M1+E2 M1+E2	350.035 285.946 277.071 22.5002 0.0	3/2- 9/2- 5/2- 5/2- 7/2-
590.883 10	A B D E H L M N O P Q R	9/2-	3.0 ps 7	305.22 8 568.36 7 590.88 1	3.72 23 25.9 17 100.0 22	M1(+E2) E2 E2+M1	285.946 22.5002 0.0	9/2- 5/2- 7/2-
636.459 18	A B D E H L M N O P Q R	7/2-	< 1.5 ps	287 1 ? 350.71 7 359.57 7 613.92 2 636.50 5	10.0 6 10.0 8 100 4 60 4	M1+E2 M1+E2 M1+E2	350.035 285.946 277.071 22.5002 0.0	3/2- 9/2- 5/2- 5/2- 7/2-
658.66 4	B O	(LE 7/2)		130.10 4 ? 308.0 1 ? 381.7 2 636.05 10 ?	90 23 3 3 100 23 9		528.593 350.035 277.071 22.5002	3/2- 3/2- 5/2- 5/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
664.09 6	A D E H L M N O P Q R	11/2-	2.7 ps 3	73.3 378.3 1 664.1 1	5.3 7 4.74 30 100.0 17	[M1] M1(+E2) E2	590.883 285.946 0.0	9/2- 9/2- 7/2-
697 2	H L O P	(3/2)-
709.85 7	D H L M P Q	(3/2,5/2+)		359.8 1 432.8 1	34 2 100 5		350.035 277.071	3/2- 5/2-
747.39 7	D E M N	13/2-		84 1 ? 461.9 1	100	E2	664.09 285.946	11/2- 9/2-
785.23 12	A L O R	5/2-		785.23 12	100		0.0	7/2-
789.51 6	D E L M N O	11/2+		125.4 1 198.6 1 504	14.9 6 100.0 34	(E1) E1	664.09 590.883 285.946	11/2- 9/2- 9/2-
830.46 5	A L R	(5/2-,7/2,9/2-)		544.27 6 552.92 9 808.11 830.53 7	7.6 4 1.8 1 51 4 100 8		285.946 277.071 22.5002 0.0	9/2- 5/2- 5/2- 7/2-
833.23 5	A H L M R	(5/2-:11/2-)		242.10 14 547.17 7 833.40 7	0.6 1 4.9 4 100 8		590.883 285.946 0.0	9/2- 9/2- 7/2-
835.59 7	A H L R	(5/2-,7/2,9/2-)		550.01 15 812.92 835.55 11	17 3 29 3 100 9		285.946 22.5002 0.0	9/2- 5/2- 7/2-
878.80 8	D E H I J L M N O P Q	13/2+		89.3 1 131 214.8 1	8.5 4 100 3	E1	789.51 747.39 664.09	11/2+ 13/2- 11/2-
881.97 4	A O	(5/2,7/2-)		323.95 9 353.46 11 531.61 6 859.46 6 881.98 5	1.40 14 0.29 3 1.37 12 100 3 22 1		558.373 528.593 350.035 22.5002 0.0	5/2- 3/2- 3/2- 5/2- 7/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
925.47 10	D H L O P Q	(3/2+,5/2+)		648.4 1	100		277.071	5/2-
952.78 9	A H L	(5/2,7/2,9/2-)		930.2 2 952.8 1	68 11 100 11		22.5002 0.0	5/2- 7/2-
967 2	O P	(1/2+)
994.65 10	D E L P Q R	(9/2,11/2,13/2-)		708.7 1	100		285.946	9/2-
1012 3	H O P	(1/2-,3/2-)
1038.97 10	D L	(5/2-)		761.9 1	100	D+Q	277.071	5/2-
1048 2	L O P Q	(3/2)+
1083 2	H L P	(LE 7/2)
1113 5	L P Q
1123 2	H L P R	(LE 7/2)
1132.37 8	D E	(9/2-,11/2,13/2-)		385.2 1 846.2 1	10.8 25 100 5		747.39 285.946	13/2- 9/2-
1154 2	H P Q	(3/2+,5/2,7/2-)
1173.21 12	D	(7/2+,9/2,11/2)		383.7 1	100		789.51	11/2+
1181 10	O	(3/2,5/2)+
1187 3	H L R	5/2-
1192.80 8	D E	13/2+		314.0 1 403.4 1 528.6 1	100 5 75 6 <248	M1(+E2) M1+E2	878.80 789.51 664.09	13/2+ 11/2+ 11/2-
1195 2	L O P Q	1/2+
1207?	R	(5/2-)
1226 10	O
1237.95 10	D L P Q	(9/2-,11/2-)		952.0 1	100		285.946	9/2-
1240.13 11	D E N	(15/2)+		450.8 492.6 1	17 3 100 3	E1	789.51 747.39	11/2+ 13/2-
1282 10	H L
1304 10	P
1308.47 9	D E H L O P Q	11/2-		561.0 644.9 1 1022.4 1 1309	33 5 100 8	M1+E2	747.39 664.09 285.946 0.0	13/2- 11/2- 9/2- 7/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1325 3	H L R
1339 3	L R	5/2-
1343.33 7	D E	(13/2-)		553.6 1 596.1 1 752.5 1	75 13 100 3 73 10		789.51 747.39 590.883	11/2+ 13/2- 9/2-
1353 2	H O P R	(5/2-,7/2-)
1360.96 11	D E	17/2-		121.0 8 613.7 1	11.4 3 100	E2	1240.13 747.39	(15/2)+ 13/2-
1362.60 13	D E N	17/2+		483.8 1	100	E2	878.80	13/2+
1378 2	H L O P Q	(5/2-,7/2,9/2+)
1393 2	L O P	(5/2)-
1398.70 9	D E	15/2-		520.7 1 651.1 1 734.7 1	21.4 14 11 2 100 5	D E2	878.80 747.39 664.09	13/2+ 13/2- 11/2-
1413.28 11	D E	(13/2+,15/2+)		623.8 1 665.7	13 3 100		789.51 747.39	11/2+ 13/2-
1428 4	I P Q	-
1442 2	I P Q	(LE 5/2)
1470 2	H L O P Q R	(3/2,5/2)+
1483 2	H L O P Q R	(LE 5/2)
1505 10	L
1535 10	L O	(1/2+)
1549 2	L P R	5/2-
1558 3	H R
1571 2	H L P Q	(7/2+,9/2,11/2-)
1574.57 14	D E	(13/2)-		266.1 1	100	M1+E2	1308.47	11/2-
1584 2	O P R	(3/2,5/2)+
1617 2	H L O P	(5/2)-
1641 2	L P
1656 2	H L P
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1670.25 12	D E	(19/2)+		309.4 1 430.0 1	100 3 51 3	E1 E2	1360.96 1240.13	17/2- (15/2)+
1672 3	H L O P R	5/2-
1684.60 13	D	(15/2,17/2,19/2-)		285.9 1	100		1398.70	15/2-
1685 10	H L Q
1695.7 3	E	(17/2+)		283 296 333 455 503.0	<52 100.0 23	(E2)	1413.28 1398.70 1362.60 1240.13 1192.80	(13/2+,15/2+) 15/2- 17/2+ (15/2)+ 13/2+
1699 3	H L P Q R	5/2-
1731 10	L
1757 3	H L P R	5/2-
1776 10	H O P Q	(7/2+)&(5/2+)
1782 3	R	5/2-
1817 3	H L R	5/2-
1837 10	L
1846.87 17	D E	(15/2)-		272.3 1 538	100	M1+E2	1574.57 1308.47	(13/2)- 11/2-
1851.2 6	E	(17/2+)		452 611			1398.70 1240.13	15/2- (15/2)+
1857 10	L
1880 10	H O	(7/2)+
1891 3	I L R	5/2-
1917 4	H I L R	5/2-
1924 10	L O	(7/2+)&(5/2+)
1925.99 16	D E	(21/2)+		563.4 1	100	E2	1362.60	17/2+
1950 10	H L O	(7/2+)&(5/2+)
1979 10	H L P
1993 3	H R
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2005 3	R
2026 10	H O P Q	(5/2+)&(11/2-)
2041.0 3	E	(19/2-)		641 678 680.2			1398.70 1362.60 1360.96	15/2- 17/2+ 17/2-
2059 4	H L P R	5/2-
2098 3	H L R	5/2-
2117 4	H L R	5/2-
2130.6 3	E	(17/2)-		283.8 555.9?	100 43	M1	1846.87 1574.57	(15/2)- (13/2)-
2139 10	H L O	(5/2+)&(11/2-)
2142.30 24	E	(21/2-)		472.0 781.4	≈14 100 27	(E2)	1670.25 1360.96	(19/2)+ 17/2-
2145.5 4 ?	E	(15/2,17/2,19/2-)		746.8?	100		1398.70	15/2-
2159 15	H
2183 10	H L O Q	(5/2+)&(11/2-)
2192.2 3	E	(23/2)+		521.9	100	E2	1670.25	(19/2)+
2210 10	H O	(5/2+)&(11/2-)
2242 10	H O	(5/2+)&(11/2-)
2272 10	H L O	(5/2+)&(7/2+)
2280 15	H O	(5/2+)&(7/2+)
2299 10	H L Q
2332 15	H
2344.5 4	E	(21/2+)		304 419 493 649 674 1			2041.0 1925.99 1851.2 1695.7 1670.25	(19/2-) (21/2)+ (17/2+) (17/2+) (19/2)+
2358 13	H
2377 15	H
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2387 10	H
2404.4 7	E	(21/2+)		553 709 734			1851.2 1695.7 1670.25	(17/2+) (17/2+) (19/2)+
2415 10	H O Q	(5/2+)&(11/2-)
2427.1 3	E	(19/2-)		296.4 580.2	100 10 ≈16	D	2130.6 1846.87	(17/2)- (15/2)-
2442 10	H O Q	(5/2+) AND (11/2-)
2487 10	H Q	(11/2-)
2508 11	H
2534 11	H
2537.2 3	E	(25/2)+		611.2	100	E2	1925.99	(21/2)+
2568 11	H
2590 10	H O Q	(5/2)+
2622 11	H
2640 11	H
2671 11	H
2701.7 5	E	(23/2-)		661 776			2041.0 1925.99	(19/2-) (21/2)+
2711 11	H O	(5/2+)&(11/2-)
2723 15	H O	(5/2+)&(11/2-)
2734.9 4	E	(21/2-)		307.5 606	100		2427.1 2130.6	(19/2-) (17/2)-
2737 12	H
2762 12	H
2797 12	H
2828.2 9	E	(25/2-)		636			2192.2	(23/2)+
2830 12	H
2834.3 4	E	(27/2)+		642.0	100	E2	2192.2	(23/2)+
2842.2 5	E	(25/2-)		141 650 700			2701.7 2192.2 2142.30	(23/2-) (23/2)+ (21/2-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2858 12	H
2875.5 4	E	(25/2+)		174 339 531.0 683			2701.7 2537.2 2344.5 2192.2	(23/2-) (25/2)+ (21/2+) (23/2)+
2891 12	H
2923 12	H
2932.9 4	E	(21/2,23/2,25/2-)		790.6	100		2142.30	(21/2-)
2949 12	H
2968 12	H
2987.2 9	E	(25/2)		159 795			2828.2 2192.2	(25/2-) (23/2)+
2995 12	H
3008.4 12	E	(25/2+)		604			2404.4	(21/2+)
3015 12	H
3055.1 5	E	(23/2-)		320.1 629			2734.9 2427.1	(21/2-) (19/2-)
3072 12	H
3094 12	H
3159.3 7	E	(25/2)		325 967			2834.3 2192.2	(27/2)+ (23/2)+
3160 12	H
3181.3 4	E	(29/2+)		644.0	100	(E2)	2537.2	(25/2)+
3181.0+X	E	(25/2 TO 33/2)	4 ns 1
3194 12	H
3218 12	H
3220.3 9	E	(25/2)		1028			2192.2	(23/2)+
3257 12	H
3303 13	H
3324 13	H
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3328.0 8	E	(27/2-)		626 791			2701.7 2537.2	(23/2-) (25/2)+
3360	O
3361.2 4	E	(29/2-)		519.0 526.9		E1	2842.2 2834.3	(25/2-) (27/2)+
3364.8 5	E	(29/2+)		489.4 530 828			2875.5 2834.3 2537.2	(25/2+) (27/2)+ (25/2)+
3377 13	H
3384.0 9	E	(25/2-)		329 649			3055.1 2734.9	(23/2-) (21/2-)
3393 14	H
3419 14	H
3436 14	H
3461 14	H
3478 14	H
3533 14	H
3545 15	H
3564.1 5	E	(29/2-)		203.1 730			3361.2 2834.3	(29/2-) (27/2)+
3575 15	H
3595 15	H
3623 15	H
3636 15	H
3651.8 5	E	(31/2+)		291 817.0 7	<29 100 8	E2	3361.2 2834.3	(29/2-) (27/2)+
3661 15	H
3687 15	H
3700 15	H
3734 15	H
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3765 15	H
3777.3 8	E	(29/2)		557 618 943			3220.3 3159.3 2834.3	(25/2) (25/2) (27/2)+
3806 15	H
3859.6 5	E	(33/2+)		678.0	100	(E2)	3181.3	(29/2+)
3880.3 11	E	(31/2-)		699			3181.3	(29/2+)
3953.3 11	E	(31/2-)		772			3181.3	(29/2+)
3968.4 6	E	(33/2-)		316.6 607			3651.8 3361.2	(31/2+) (29/2-)
4005.9 5	E	(33/2-)		354.0 442.0 644			3651.8 3564.1 3361.2	(31/2+) (29/2-) (29/2-)
4054.7 6	E	(33/2+)		691 875			3364.8 3181.3	(29/2+) (29/2+)
4486.8 12	E	(33/2)		835			3651.8	(31/2+)
4543.8 6	E	(35/2-)		489.4 684.0			4054.7 3859.6	(33/2+) (33/2+)
4575.1 9	E	(35/2+)		607 923			3968.4 3651.8	(33/2-) (31/2+)
4597.3 6	E	(37/2+)		737.7	100		3859.6	(33/2+)
4606.6 10	E	(37/2-)		601			4005.9	(33/2-)
4686.4 7	E	(37/2-)		718.0		(E2)	3968.4	(33/2-)
4799.0 10	E	(37/2+)		744			4054.7	(33/2+)
5140.6 9	E	(39/2-)		543 597			4597.3 4543.8	(37/2+) (35/2-)
5173.4 11	E	(39/2+)		374 567			4799.0 4606.6	(37/2+) (37/2-)
5325.4 12	E	(39/2)		639			4686.4	(37/2-)
5361.3 12	E	(41/2+)		764			4597.3	(37/2+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5372.5 12	E	(41/2-)		199 766			5173.4 4606.6	(39/2+) (37/2-)
5477.4 12	E	(41/2-)		791			4686.4	(37/2-)
5600	O
5791.5 16	E	(43/2)		419			5372.5	(41/2-)
5801.6 14	E	(43/2-)		661			5140.6	(39/2-)
6189.5 19	E	(45/2)		398			5791.5	(43/2)