List of levels for 58CU

Authors: Caroline D. Nesaraja, Scott D. Geraedts and Balraj Singh | Citation: Nucl. Data Sheets 111, 897 (2010) | Cutoff date: 12-Jan-2010

Structure calculations (levels, transition probabilities, etc.): 2008Na24, 2007BeZX (Gamow-Teller transitions) 2006Va21, 2004Ho08, 2004Va38, 1977Ko02, 1975Wa29, 1971Ru09

Levels: Isotopic spins t are from (p,nγ) and (³He,t)

Q-value: Note: Current evaluation has used the following Q record -9364 50 12423 16 2869.0 23-6077.6 16 2009AuZZ,2003Au03

Q-value: Q(εp)=393.2 15 (2009AuZZ,2003Au03)

Q-value: S(2n)=29200 140 (2009AuZZ,syst); S(2p)=10200.5 25 (2009AuZZ)

E(level): From least-squares fit to Eγ’s for levels populated in γ-ray studies. Other values are mostly from (³He,t)

T_1/2(level): From DSAM in (p,nγ), except where noted otherwise

M(γ): From γγ(θ) and γ(lin pol) in (p,nγ) and γγ(θ)(DCO) in (³⁶Ar,αpnγ) and RUL (for E2 and M2 transitions)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
202.99	0+		203.2 3	[M1]		0.00846	α=0.00846
443.64	3+	0.32 ns 6	443.5 2	E2(+M3)	-0.02 4		B(E2)(W.u.)=7.7 15
1051.5	1+	78 fs +19-13	848.6 2	[M1]			B(M1)(W.u.)=0.43 +8-11
1427.85	2+	> 0.66 ps	984.2	(M1+E2)	-0.8 +2-15		B(E2)(W.u.)<2.7, B(M1)(W.u.)<0.0019
	2+	> 0.66 ps	1225.1	[E2]			B(E2)(W.u.)<0.35
	2+	> 0.66 ps	1427.8 3	[M1+E2]			B(E2)(W.u.)<10, B(M1)(W.u.)<0.010
1549.5	(4+)	> 0.34 ps	1105.8 3	(M1+E2)	-0.77 5		B(E2)(W.u.)<30, B(M1)(W.u.)<0.032
1647.41	(3+)	> 0.90 ps	1203.5	(M1+E2)	+0.53 13		B(E2)(W.u.)<1.1, B(M1)(W.u.)<0.0023
1647.41	(3+)	> 0.90 ps	1647.4 2	(E2(+M3))	-0.06 +16-27		B(E2)(W.u.)<2.8
1652.5	2+	35 fs 7	601.4	(M1(+E2))	+0.02 5		B(M1)(W.u.)=0.15 4
	2+	35 fs 7	1208.2	(M1(+E2))	-0.02 2		B(M1)(W.u.)=0.31 7
	2+	35 fs 7	1449.5	[E2]			B(E2)(W.u.)=9 4
2065.0	(5+)		1621.2 4	(E2+M3)	-0.12 4
2750.2	(4+)		1103.1	(M1(+E2))	-0.07 +5-12
2750.2	(4+)		1200.6	(M1(+E2))	0.00 5
9747.2	(11+)	0.38 ps 4	830.2 3	E2			B(E2)(W.u.)=183 25
	(11+)	0.38 ps 4	1519 1	E2			B(E2)(W.u.)=2.0 6
	(11+)	0.38 ps 4	4171 3	E2			B(E2)(W.u.)=0.015 4
10944.5	(13+)	0.104 ps 14	1197.3 5	E2			B(E2)(W.u.)=166 23
12520.9	(15+)	0.035 ps 7	1576.4 4	E2			B(E2)(W.u.)=125 25

Q(β-)=-9.37×10³ keV 5	S(n)= 12430.2 keV 7	S(p)= 2872.9 keV 7	Q(α)= -6082.7 keV 6
Reference: 2012WA38

References:
A	⁵⁸Zn ε decay (86 MS)	B	²⁸Si(³⁶Ar,APNG)
C	⁵⁸Ni(p,n)	D	⁵⁸Ni(p,nγ)
E	⁵⁸Ni(³He,t),(³He,tγ)	F	⁵⁸Ni(⁶Li,⁶He)

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A B C D E F	1+	3.204 s 7 % ε = 100
202.99 24	A C D E	0+		203.2 3	100	[M1]	0.0	1+
443.64 18	B C D E F	3+	0.32 ns 6	443.5 2	100	E2(+M3)	0.0	1+
1051.5 3	A C D E F	1+	78 fs +19-13	607 848.6 2 1052	<5 100 <9	[M1]	443.64 202.99 0.0	3+ 0+ 1+
1427.85 25	C D E F	2+	> 0.66 ps	376.6 984.2 1225.1 1427.8 3	3.4 19 8.5 41 1.7 5 100	(M1+E2) [E2] [M1+E2]	1051.5 443.64 202.99 0.0	1+ 3+ 0+ 1+
1549.5 3	B C D E F	(4+)	> 0.34 ps	1105.8 3	100	(M1+E2)	443.64	3+
1647.41 18	B D F	(3+)	> 0.90 ps	220 596 1203.5 1445 1647.4 2	<4.3 <5 27 8 <19 100 8	(M1+E2) (E2(+M3))	1427.85 1051.5 443.64 202.99 0.0	2+ 1+ 3+ 0+ 1+
1652.5 5	C D E F	2+	35 fs 7	601.4 1208.2 1449.5 1653	5.9 2 100 3 5.3 18 <4.1	(M1(+E2)) (M1(+E2)) [E2]	1051.5 443.64 202.99 0.0	1+ 3+ 0+ 1+
2065.0 3	B D	(5+)		418 1 515.4 3 1621.2 4	13 2 43 2 100 3	D (E2+M3)	1647.41 1549.5 443.64	(3+) (4+) 3+
2070 20	E
2170 20	E
2249.2 8	D			596.7 821.3	100 6 12 6		1652.5 1427.85	2+ 2+
2270 20	E
2690 20	E F	4+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2750.2 6	D	(4+)		1103.1 1200.6 2306.4	73 15 100 15 8.9 33	(M1(+E2)) (M1(+E2))	1647.41 1549.5 443.64	(3+) (4+) 3+
2780 20	E
2815.2 6	D			1162.7 1387.2 2371.5	100 19 57 14 81 19		1652.5 1427.85 443.64	2+ 2+ 3+
2840 20	E
2920.6 5	B D F	(5+)		856 1274 1372 2477.5	<2.8 <2.8 <2.8 100 4	Q	2065.0 1647.41 1549.5 443.64	(5+) (3+) (4+) 3+
2930.9 8	D F	(0+:4+)		1278.3 1503.0	100 8 30 8		1652.5 1427.85	2+ 2+
2949 10	E	(1)+
3230 20	E
3280.2 8	D	(0+:4+)		1627.7 1852.2	100 6 19 6		1652.5 1427.85	2+ 2+
3310 20	E
3421.0 5	B D	(7+)		500.5 3 1355.6 4	8 1 100 3	Q Q	2920.6 2065.0	(5+) (5+)
3460.1 11	E F	(1)+		3257	100		202.99	0+
3512.6 7	B D			592.0 5	100		2920.6	(5+)
3570 20	E
3677.9 8	E F	(1)+		3234 3475			443.64 202.99	3+ 0+
3717 10	C E F	(1)+
3820 20	E
3890 20	E
4010	F
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4065.6 6	B	(7+)		1145.2 5 2000 1	60 7 100 7	Q	2920.6 2065.0	(5+) (5+)
4210 20	E
4441.4 6	B	(8+)		1020.4 4	100	D	3421.0	(7+)
4720 10	E F	(1)+
5065 20	E	(1)+
5160 20	C E F	(1)+
5190.6 23	B	(7+)		3125 3	100		2065.0	(5+)
5348.0 8	B	(9+)		906 1 1927 1	24 3 100 6	D Q	4441.4 3421.0	(8+) (7+)
5451 20	E F	(1)+
5574.9 8	B	(9+)		1509.3 5	100	Q	4065.6	(7+)
5645 20	E F	(1)+
6038 20	E	(1)+
6086 20	E	(1)+
6387.2 10	B	(10+)		1039 1 1946 1	21 4 100 8	D Q	5348.0 4441.4	(9+) (8+)
6497 20	C E	(1)+
6794.1 12	B	(9)		1446 1	100		5348.0	(9+)
6844 20	E	(1)+
7105 20	E	(1)+
7143 20	E	(1)+
7392.6 11	B	(11+)		1818 2044 2	16 5 100	Q	5574.9 5348.0	(9+) (9+)
7586 20	E	(1)+
7700 20	E	(1)+
7752 20	E	(1)+
7907 20	E	(1)+
7993 20	E	(1)+
8063 20	E	(1)+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
8127.3 13	B	(11)		1740 1	100	(D)	6387.2	(10+)
8159 20	E	(1)+
8199 20	E	(1)+
8228.2 13 ?	B	(9+)		2654 2 3037 3	100 25 50 25		5574.9 5190.6	(9+) (7+)
8282 20	E	(1)+
8370 10	E	(1)+
8421 10	E	(1)+
8487.3 16	B	(12+)		2100 2	100	(Q)	6387.2	(10+)
8520 10	E	(1)+
8566 10	E	(1)+
8614 10	E	(1)+
8725 10	E	(1)+
8837 10	E	(1)+
8881.6 13	B			1489 1 2087 2	100 20 80 20		7392.6 6794.1	(11+) (9)
8900	F		2.8 MeV
8916.9 11	B	(9+)	0.22 ps 18 % p = 96 4
8959 10	E	(1)+
9000 10	E	(1)+
9129 20	E	(1)+
9172 10	E	(1)+
9209 10	C E	(1)+
9307 10	E	(1)+
9371 10	E	(1)+
9444 20	E	(1)+
9567 10	E	(1)+
9645 10	E	(1)+
9680.7 23	B			2288 2	100		7392.6	(11+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
9747.2 11	B	(11+)	0.38 ps 4	830.2 3 1519 1 4171 3 4399	100 5 23 5 27 5 5 5	E2 E2 E2	8916.9 8228.2 5574.9 5348.0	(9+) (9+) (9+) (9+)
9783 10	E	(1)+
9804.3 15	B	(12)		1317 1 1677 1	50 12 100 12		8487.3 8127.3	(12+) (11)
9861 10	E	(1)+
9989 10	E	(1)+
10291 10	E	(1)+
10329 10	E	(1)+
10388 10	E	(1)+
10554 10	E	(1)+
10597 10	E	(1)+
10776.6 17	B			1895 1	100		8881.6
10825 10	E	(1)+
10944.5 12	B	(13+)	0.104 ps 14	1197.3 5	100	E2	9747.2	(11+)
11137 10	C E	(1)+
11358 10	E	(1)+
11553 4	B			3066 3	100		8487.3	(12+)
11562 20	E	(1)+
11815 20	E	(1)+
11842 3	B			2038 2	100		9804.3	(12)
11903 20	E	(1)+
12034 20	E	(1)+
12.45E3 15	E
12520.9 13	B	(15+)	0.035 ps 7	1576.4 4	100	E2	10944.5	(13+)
12880 20	C E	(1)+
13130 3	B			2353 2	100		10776.6
14475.9 16	B	(17+)		1955 1	100	Q	12520.9	(15+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
14881 4	B			3039 3	100		11842
16000	F		14 MeV
16818 3	B	(19+)		2342 2	100	Q	14475.9	(17+)
19566 4	B	(21+)		2748 2	100	Q	16818	(19+)
22747 5	B	(23+)		3181 3	100		19566	(21+)
24000	F		25 MeV

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - ν4¹π4¹ INTRUDER (SD) band.
8916.9 11	(9+)	0.22 ps 18 % p = 96 4
9747.2 11	(11+)	0.38 ps 4	830.2 3 1519 1 4171 3 4399	100 5 23 5 27 5 5 5	E2 E2 E2	8916.9 8228.2 5574.9 5348.0	(9+) (9+) (9+) (9+)
10944.5 12	(13+)	0.104 ps 14	1197.3 5	100	E2	9747.2	(11+)
12520.9 13	(15+)	0.035 ps 7	1576.4 4	100	E2	10944.5	(13+)
14475.9 16	(17+)		1955 1	100	Q	12520.9	(15+)
16818 3	(19+)		2342 2	100	Q	14475.9	(17+)
19566 4	(21+)		2748 2	100	Q	16818	(19+)
22747 5	(23+)		3181 3	100		19566	(21+)

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1+	3.204 s 7 % ε = 100	μ=+0.479 13 (2010Co01), T=0 From comparison of measured magnetic-dipole moment with calculated values from shell-model using GXPF1 interaction, proposed dominant configuration=πp_3/2~#νp_3/2 (2010Co01).
1652.5	2+	35 fs 7	XREF: C(1638).
2949	(1)+		J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
3421.0	(7+)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
3460.1	(1)+		J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
3677.9	(1)+		J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
3717	(1)+		J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
4065.6	(7+)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
4441.4	(8+)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
4720	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
5065	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
5160	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
5348.0	(9+)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
5451	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
5574.9	(9+)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
5645	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
6038	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
6086	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
6387.2	(10+)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
6497	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
6844	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
7105	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
7143	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
7392.6	(11+)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
7586	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
E(level)	J^π(level)	T_1/2(level)	Comments
7700	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
7752	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
7907	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
7993	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8063	(1)+		t=(1). J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8127.3	(11)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
8159	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8199	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8228.2	(9+)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
8282	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8370	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8421	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8487.3	(12+)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
8520	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8566	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8614	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8725	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8837	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
8916.9	(9+)	0.22 ps 18 % p = 96 4	α 2330γ from this level proposed earlier is not confirmed by 2002Ru09. E(level): α 2330γ from this level proposed earlier is not confirmed by 2002Ru09. ν4¹π4¹ INTRUDER (SD) band. J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
8959	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9000	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9129	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9172	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9209	(1)+		T=1 XREF: C(9200). J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9307	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
E(level)	J^π(level)	T_1/2(level)	Comments
9371	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9444	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9567	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9645	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9747.2	(11+)	0.38 ps 4	Q(transition)=2.75 +27-24 (2001Ru02). E(level): ν4¹π4¹ INTRUDER (SD) band. J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
9783	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9804.3	(12)		J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
9861	(1)+		T=2 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
9989	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
10291	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
10329	(1)+		T=1 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
10388	(1)+		T=2 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
10554	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
10597	(1)+		T=2 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
10825	(1)+		T=2 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
10944.5	(13+)	0.104 ps 14	Q(transition)=2.55 +19-15 (2001Ru02). E(level): ν4¹π4¹ INTRUDER (SD) band. J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
11137	(1)+		T=2 XREF: C(11200). J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
11358	(1)+		T=2 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
11562	(1)+		T=(2) J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
11815	(1)+		T=2 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
11903	(1)+		T=0 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
12034	(1)+		T=2 J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
12520.9	(15+)	0.035 ps 7	Q(transition)=2.21 +26-19 (2001Ru02). E(level): ν4¹π4¹ INTRUDER (SD) band. J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
12880	(1)+		T=2 XREF: C(13000). J^π(level): From L(³He,t)=0, interpreted as Gamow-Teller transition.
14475.9	(17+)		E(level): ν4¹π4¹ INTRUDER (SD) band. J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
E(level)	J^π(level)	T_1/2(level)	Comments
16818	(19+)		E(level): ν4¹π4¹ INTRUDER (SD) band. J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
19566	(21+)		E(level): ν4¹π4¹ INTRUDER (SD) band. J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
22747	(23+)		E(level): ν4¹π4¹ INTRUDER (SD) band. J^π(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in ²⁸Si(³⁶Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.