List of levels for 48CA

Author: Jun Chen | Citation: Nucl. Data Sheets 179, 1 (2022) | Cutoff date: 30-Nov-2021

Mass measurements: 2016Ko45, 2014Kw04, 2013Bu12, 2012Re17, 2006Fr27

Measurements of hyperfine structure and isotope shift: 2019Kn01, 2017Ga02, 2015Go24

$ See ⁴⁸Ca(pol p,p’):GDR,GQR for information on the giant dipole, giant quadrupole, spin dipole, and spin quadrupole resonances

$ See ⁴⁸Ca(e,e’n):GMR,GDR,GQR,IAR for information on the giant monopole, giant dipole, and giant quadrupole resonances.

Levels: B(M1)|^ given under comments are from (p,p’), unless otherwise noted.

Levels: %β^-,%2β^- of g.s.: the small β^- decay probability together with the rather large phase space available for the 2β^- process have made ⁴⁸Ca a favorite for the study of the process. See the Nuclear Science References File for theoretical studies, compilations, and reviews. See 1990Al19 for a measurement of σ(θ) from the ⁴⁸Ti(n,p) reaction at E=198 MeV and its possible implications for ⁴⁸Ca 2β^- decay.

Q-value: S(2n)=17227.9 22, S(2p)=29031.6 23 (2021Wa16)

E(level): From a least-squares fit to γ-ray energies for levels connected with γ transitions except for those from (p,p’γ), and from (p,p’) for other levels where available, unless otherwise noted. In the least-squares fit, where ΔEγ is not available, the following assumptions have been made: 0.05 keV for Eγ quoted to ¹⁰⁰Th keV, 0.5 keV for Eγ quoted to 10th keV and 1.0 keV for quoted to keV. The reduced χ² of the fitting is 2.65, compared to the critical χ²=1.83, after adjustments of ΔEγ for some poor-fit Eγ values, as noted.

T_1/2(level): From DSAM in (n,n’γ) (1992Va06), unless otherwise noted.

E(γ): Values with uncertainties are from (n,n’γ) and those without uncertainties are from level-energy differences for transitions reported in (p,p’γ) , unless otherwise noted. Note that values without uncertainties from (p,p’γ) are deduced from E(level) values reported in 1969Te03 only, while adopted E(level) values from (p,p’) are mostly from 1988Fu01 or average of all available measurements. Therefore, for those transitions, Eγ values quoted here have been re-deduced by the evaluator from the adopted level energies.

I(γ): From (n,n’γ), unless otherwise noted.

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
3831.96	2+	36 fs 3	3831.4 3	E2		1.12×10^-3	B(E2)(W.u.)=1.84 +17-14, α=1.12E-3 2, α(K)=6.68E-6 9, α(L)=5.71E-7 8, α(M)=6.78E-8 9, α(N)=3.86E-9 5
4283.56	0+	223 ps 11	451.6 1	[E2]		0.000934	B(E2)(W.u.)=10.1 5, α=0.000934 13, α(K)=0.000851 12, α(L)=7.37E-5 10, α(M)=8.73E-6 12, α(N)=4.89E-7 7
4503.74	4+	1.53 ns 3	671.8 4	E2		0.000268	B(E2)(W.u.)=0.261 5, α=0.000268 4, α(K)=0.0002441 34, α(L)=2.106E-5 30, α(M)=2.498E-6 35, α(N)=1.408E-7 20
4507.05	3-	6.1 ps +38-20	675.1 1	(E1(+M2))	0.00 3	9.18×10^-5	B(E1)(W.u.)=0.00021 +10-8, α=9.18E-5 13, α(K)=8.37E-5 12, α(L)=7.19E-6 10, α(M)=8.53E-7 12, α(N)=4.83E-8 7
4507.05	3-	6.1 ps +38-20	4507.3 5	E3		1.05×10^-3	B(E3)(W.u.)=8.4 +43-35, α=1.05E-3 2, α(K)=6.86E-6 10, α(L)=5.87E-7 8, α(M)=6.97E-8 10, α(N)=3.97E-9 6
4612.24	3(+)	2.5 ps 14	780.2 1	(M1)		0.0001108	B(M1)(W.u.)=0.019 +17-7, α=0.0001108 16, α(K)=0.0001010 14, α(L)=8.68×10^-6 12, α(M)=1.031E-6 14, α(N)=5.85E-8 8
5260.81	4(-)	5.1 ps +14-8	648.4 1	(E1)		0.0001008	B(E1)(W.u.)=5.3E-5 +10-12, α=0.0001008 14, α(K)=9.19E-5 13, α(L)=7.89E-6 11, α(M)=9.37E-7 13, α(N)=5.30E-8 7
5260.81	4(-)	5.1 ps +14-8	753.8 1	(M1)		0.0001188	B(M1)(W.u.)=0.0086 +16-19, α=0.0001188 17, α(K)=0.0001083 15, α(L)=9.31×10^-6 13, α(M)=1.106E-6 15, α(N)=6.28E-8 9
5312.2	2	232 fs +28-13	1480.2 1	D+Q	+0.7 6
5369.90	3-	1.80 ps 14	757.5 1	(E1)		7.10×10^-5	B(E1)(W.u.)=0.000102 15, α=7.10E-5 10, α(K)=6.47E-5 9, α(L)=5.56E-6 8, α(M)=6.59E-7 9, α(N)=3.74E-8 5
	3-	1.80 ps 14	862.7 1	[M1,E2]		0.000112	B(E2)(W.u.)=10.3 +15-14, B(M1)(W.u.)=0.00308 +46-43, α=0.000112 22, α(K)=0.000102 20, α(L)=8.8E-6 17, α(M)=1.04E-6 20, α(N)=5.9E-8 11
	3-	1.80 ps 14	866.9 1	(E1)		5.33×10^-5	B(E1)(W.u.)=6.2E-5 +9-8, α=5.33E-5 7, α(K)=4.86E-5 7, α(L)=4.17E-6 6, α(M)=4.95E-7 7, α(N)=2.81E-8 4
	3-	1.80 ps 14	1537.8 1	(E1)		0.000312	B(E1)(W.u.)=4.2E-5 4, α=0.000312 4, α(K)=1.715E-5 24, α(L)=1.468E-6 21, α(M)=1.743E-7 24, α(N)=9.91E-9 14
5729.64	5-	0.90 ps +49-21	468.7 1	[M1]		0.000324	B(M1)(W.u.)=0.14 5, α=0.000324 5, α(K)=0.000295 4, α(L)=2.55×10^-5 4, α(M)=3.03E-6 4, α(N)=1.713E-7 24
5729.64	5-	0.90 ps +49-21	1226.0 1	[E1]		0.0001000	B(E1)(W.u.)=0.00012 +4-5, α=0.0001000 14, α(K)=2.511E-5 35, α(L)=2.151E-6 30, α(M)=2.55E-7 4, α(N)=1.451E-8 20
6105.00	(2+)	139 fs +17-28	1597.8 1	[E1]		0.000359	B(E1)(W.u.)=0.00079 +19-9, α=0.000359 5, α(K)=1.613E-5 23, α(L)=1.381E-6 19, α(M)=1.640E-7 23, α(N)=9.32E-9 13
6105.00	(2+)	139 fs +17-28	2273.1 1	[M1,E2]		0.00042	B(E2)(W.u.)=0.78 +24-14, B(M1)(W.u.)=0.0016 +5-3, α=0.00042 4, α(K)=1.49E-5 6, α(L)=1.28E-6 5, α(M)=1.52E-7 6, α(N)=8.63E-9 32
6336.8	2+	191 fs 29	6336.4 20	E2			B(E2)(W.u.)=0.028 +5-4
6612.19	1-	1.87 fs 14	6611.7 1	E1			B(E1)(W.u.)=0.00095 +8-7
6648.99	4+	114 fs +42-28	2036.8 1	(M1)		0.000283	B(M1)(W.u.)=0.0053 +19-15, α=0.000283 4, α(K)=1.724×10^-5 24, α(L)=1.476E-6 21, α(M)=1.753E-7 25, α(N)=9.98E-9 14
6648.99	4+	114 fs +42-28	2145.1 1	(M1)		0.000327	B(M1)(W.u.)=0.009 3, α=0.000327 5, α(K)=1.583×10^-5 22, α(L)=1.354E-6 19, α(M)=1.609E-7 23, α(N)=9.16E-9 13
6685.64	2(-)	69 fs +56-52	1315.8 1	[M1,E2]		7.3×10^-5	B(E2)(W.u.)=1.5E2 +19-7, B(M1)(W.u.)=0.10 +13-5, α=7.3E-5 9, α(K)=4.1E-5 4, α(L)=3.49E-6 33, α(M)=4.2E-7 4, α(N)=2.36E-8 22
	2(-)	69 fs +56-52	2073.9 1	(E1)		0.000705	B(E1)(W.u.)=1.0E-4 +13-5, α=0.000705 10, α(K)=1.089E-5 15, α(L)=9.31E-7 13, α(M)=1.106E-7 15, α(N)=6.29E-9 9
	2(-)	69 fs +56-52	2178.30	[M1,E2]		0.00038	B(E2)(W.u.)=2.2 +28-11, B(M1)(W.u.)=0.0041 +52-21, α=0.00038 4, α(K)=1.60E-5 6, α(L)=1.37E-6 5, α(M)=1.63E-7 7, α(N)=9.3E-9 4
6805.7	2+	83 fs +44-38	2301.9 1	[E2]		0.000478	B(E2)(W.u.)=5.9 +48-22, α=0.000478 7, α(K)=1.510E-5 21, α(L)=1.292E-6 18, α(M)=1.535E-7 21, α(N)=8.73E-9 12
6805.7	2+	83 fs +44-38	2974.8 5	[M1,E2]		0.00073	B(E2)(W.u.)=1.2 +10-5, B(M1)(W.u.)=0.0042 +36-17, α=0.00073 6, α(K)=9.64E-6 26, α(L)=8.24E-7 22, α(M)=9.79E-8 26, α(N)=5.58E-9 15
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
6895.87	(2-)	55 fs +83-55	1525.7 1	(M1)		0.0001032	B(M1)(W.u.)>0.0065, α=0.0001032 14, α(K)=2.83×10^-5 4, α(L)=2.426E-6 34, α(M)=2.88E-7 4, α(N)=1.640E-8 23
	(2-)	55 fs +83-55	2283.15	[E1]		0.000843	B(E1)(W.u.)>2.8E-5, α=0.000843 12, α(K)=9.50E-6 13, α(L)=8.12E-7 11, α(M)=9.65E-8 14, α(N)=5.49E-9 8
	(2-)	55 fs +83-55	2389.0 1	(M1)		0.000428	B(M1)(W.u.)>0.0053, α=0.000428 6, α(K)=1.329×10^-5 19, α(L)=1.137E-6 16, α(M)=1.350E-7 19, α(N)=7.69E-9 11
7007.6	3-	69 fs +18-14	3175.5 5	[E1]		1.33×10^-3	B(E1)(W.u.)=0.00023 +6-5, α=1.33E-3 2, α(K)=6.12E-6 9, α(L)=5.23E-7 7, α(M)=6.21E-8 9, α(N)=3.54E-9 5
7296.1	(2+)	< 6.9 fs	7298 2	(E2)			B(E2)(W.u.)>0.051
7298.50	1-	0.201 fs 14	7297.9 2	E1			B(E1)(W.u.)=0.0065 5
7440.6	2,3-	177.4 fs 70	7440 2	Q,E3			B(E3)(W.u.)=39.7 +17-15
7655.66	1-	1.87 fs 7	7655.0 2	E1			B(E1)(W.u.)=6.11E-4 +24-23
7915.4	2+	22 fs +4-3	7914.7 9	E2			B(E2)(W.u.)=0.080 +13-12
8027.6	2+	11.4 fs 12	8026.9 4	E2			B(E2)(W.u.)=0.144 +17-14
8386.1	1-	0.159 fs 21	4554.2 12	(E1)		1.88×10^-3	B(E1)(W.u.)=0.0031 +6-4, α=1.88E-3 3, α(K)=3.93E-6 5, α(L)=3.35E-7 5, α(M)=3.98E-8 6, α(N)=2.269E-9 32
8386.1	1-	0.159 fs 21	8385.3 5	E1			B(E1)(W.u.)=0.0050 +8-6
8883.3	1-	0.42 fs 14	5050.6 9	(E1)		2.04×10^-3	B(E1)(W.u.)=0.00036 +30-14, α=2.04E-3 3, α(K)=3.48E-6 5, α(L)=2.97E-7 4, α(M)=3.52E-8 5, α(N)=2.008E-9 28
8883.3	1-	0.42 fs 14	8882.6 5	E1			B(E1)(W.u.)=0.0017 +9-4
9033.9	1-	0.242 fs 14	5200.9 15	(E1)		2.08×10^-3	B(E1)(W.u.)=0.00033 13, α=2.08E-3 3, α(K)=3.36E-6 5, α(L)=2.87E-7 4, α(M)=3.41E-8 5, α(N)=1.940E-9 27
9033.9	1-	0.242 fs 14	9033.0 4	E1			B(E1)(W.u.)=0.0028 2
9295.3	1-	0.236 fs 14	9294.3	E1			B(E1)(W.u.)=0.00270 +17-15
9472.8	1-	0.250 fs 21	9471.8 8	E1			B(E1)(W.u.)=0.00241 +22-19
9545.72	1-	0.139 fs 7	9544.7 2	E1			B(E1)(W.u.)=0.00424 +23-21

Q(β-)=279 keV 5	S(n)= 9951.5 keV 22	S(p)= 15801.9 keV 14	Q(α)= -13976.5 keV 16
Reference: 2021WA16

References:
A	⁴⁸K β^- decay	B	⁴⁹K β^-n decay
C	⁴⁶Ca(t,p)	D	⁴⁸Ca(γ,γ’),(pol γ,γ’)
E	⁴⁸Ca(E,E’)	F	⁴⁸Ca(E,E’n):GMR,GDR,GQR,IAR
G	⁴⁸Ca(π^-,π^-’),(π⁺,π⁺’)	H	⁴⁸Ca(n,n’γ)
I	⁴⁸Ca(p,p’),(pol p,p’)	J	⁴⁸Ca(pol p,p’):GDR,GQR
K	⁴⁸Ca(p,p’γ)	L	⁴⁸Ca(d,d’),(pol d,d’)
M	⁴⁸Ca(³He,³He’),(pol ³He,³He’)	N	⁴⁸Ca(α,α’)
O	⁴⁸Ca(α,α’):GIANT resonance	P	⁴⁸Ca(α,α’γ)
Q	⁴⁸Ca(⁶Li,⁶Li’)	R	⁴⁸Ca(¹⁶O,¹⁶O’)
S	⁴⁸Ca(⁴⁸Ca,⁴⁸Ca’γ)

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	0+	2.9×10¹⁹ y +42-11 % β^- = 22 +30-22 % 2β^- = 78 +22-30	Nuclear rms charge radius=3.4771 fm 20 (2013An02). E(level): Nuclear rms charge radius=3.4771 fm 20 (2013An02). T_1/2(level): Estimated by the evaluator from the following partial T_1/2 and limits: T_1/2(β^-)>1.6×10²⁰ y, >2.5×10²⁰ y, >1.9×10²⁰ y for single β^- decay to g.s., 131 and 252 levels in ⁴⁸Sc, respectively (2002Bb03, 90% C.L.), T_1/2(2ν2β^-)=5.6×10¹⁹ y +14-11 (2016Ar19,2000Br63,1996Ba80) and T_1/2(0ν2β^-)>5.8×10²² y (2008Um05, 90% C.L.), for 2β^- to g.s. in ⁴⁸Ti, and T_1/2(2β^-)>1.8×10²⁰ y, >1.5×10²⁰ y, and >1.5×10²⁰ y (2002Bb03, 90% C.L.), for (0ν+2ν)2β^- to 984, 2421, and 2997 levels in ⁴⁸Ti, respectively. Estimate was obtained by taking decay constant \|l=\|l_upper/2 with Δ\|l=\|l for partial T_1/2 given as lower limit (for \|l_upper). See the ⁴⁸Ca β^- and ⁴⁸Ca 2β^- decay datasets for experimental details.
3831.96	2+	36 fs 3	B(E2)\|^=0.0082 5 from (e,e’) (1985Wi06), but it is discrepant with 0.0140 15 from (α,α’):giant res (2011Lu07) and 0.0131 12 from (⁶Li,⁶Li’) (2010Kr06). E(level): B(E2)\|^=0.0082 5 from (e,e’) (1985Wi06), but it is discrepant with 0.0140 15 from (α,α’):giant res (2011Lu07) and 0.0131 12 from (⁶Li,⁶Li’) (2010Kr06).
4283.56	0+	223 ps 11	XREF: α(?).
4503.74	4+	1.53 ns 3	XREF: M(?).
4507.05	3-	6.1 ps +38-20	B(E3)\|^=0.0069 10, unweighted average of 0.0065 10 from (e,e’), 0.0054 8 from (α,α’):giant res, 0.0087 8 from (⁶Li,⁶Li’). E(level): B(E3)\|^=0.0069 10, unweighted average of 0.0065 10 from (e,e’), 0.0054 8 from (α,α’):giant res, 0.0087 8 from (⁶Li,⁶Li’).
4612.24	3(+)	2.5 ps 14	XREF: n(?).
4695.4	1	32.6 fs +25-22	T_1/2(level): From Γ_γ0 in (γ,γ’) assuming Γ_γ0/Γ=1 (2002Ha13).
5260.81	4(-)	5.1 ps +14-8	XREF: α(?).
5311	(1)-		XREF: K(5322). J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
5461	0+		XREF: n(?).
6345.72	4+	180 fs +35-13	XREF: K(6351).
6612.19	1-	1.87 fs 14	T_1/2(level): From Γ_γ0 in (γ,γ’) assuming Γ_γ0/Γ=1 (2002Ha13).
6648.99	4+	114 fs +42-28	XREF: n(?).
6685.64	2(-)	69 fs +56-52	J^π(level): From DWBA analysis in (p,p’) with unnatural parity due to peak not observed in (α,α’) spectra (1988Fu01). Natural parity is distinguished from unnatural parity based on observation of one-to-one correspondences of levels in (p,p’) and (α,α’) spectra (1988Fu01).
6805.7	2+	83 fs +44-38	XREF: C(6793)I(6794)p(6800).
7007.6	3-	69 fs +18-14	J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
7032.0	(3)-		XREF: n(7050). J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
7298.50	1-	0.201 fs 14	T_1/2(level): From Γ_γ0 in (γ,γ’) assuming Γ_γ0/Γ=1 (2002Ha13).
7401.22	(2-)		XREF: E(7397). J^π(level): From DWBA analysis in (p,p’) with unnatural parity due to peak not observed in (α,α’) spectra (1988Fu01). Natural parity is distinguished from unnatural parity based on observation of one-to-one correspondences of levels in (p,p’) and (α,α’) spectra (1988Fu01). In (⁴⁸Ca,⁴⁸Ca’γ), 2001Br35 suggest that these states are near yrast states with J>5 and must involve two-particle two-hole core excitations, which is manifested by their large energy separation from lower lying states.
7536.4	3-		J^π(level): In (⁴⁸Ca,⁴⁸Ca’γ), 2001Br35 suggest that these states are near yrast states with J>5 and must involve two-particle two-hole core excitations, which is manifested by their large energy separation from lower lying states. Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
7652	3-		J^π(level): From DWBA fit to the Coulomb form factors and RPA calculations in (e,e’); unnatural parity state from absence of longitudinal form factor.
7655.66	1-	1.87 fs 7	BM1=0.008 5 XREF: p(7651). T_1/2(level): From Γ_γ0 in (γ,γ’) assuming Γ_γ0/Γ=1 (2002Ha13).
7659	3-		B(E3)\|^≈0.0014 from (e,e’). E(level): B(E3)\|^≈0.0014 from (e,e’). J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
7696	(1+,2+)		B(M1)\|^<0.05 from (e,e’). E(level): B(M1)\|^<0.05 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
7789	3-		XREF: n(7760).
E(level)	J^π(level)	T_1/2(level)	Comments
7797	4+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
7911	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
7915.4	2+	22 fs +4-3	T_1/2(level): From Γ_γ0 in (γ,γ’) assuming Γ_γ0/Γ=1 (2002Ha13).
7953	(2-,6-)		J^π(level): From DWBA fit to the Coulomb form factors and RPA calculations in (e,e’); unnatural parity state from absence of longitudinal form factor.
7957	(4)+		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
8027.6	2+	11.4 fs 12	T_1/2(level): From Γ_γ0 in (γ,γ’) assuming Γ_γ0/Γ=1 (2002Ha13).
8065	5-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8150	(1+,2+)		B(M1)\|^<0.05 from (e,e’). E(level): B(M1)\|^<0.05 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
8178	4+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8248	4+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8279.1	4+		J^π(level): In (⁴⁸Ca,⁴⁸Ca’γ), 2001Br35 suggest that these states are near yrast states with J>5 and must involve two-particle two-hole core excitations, which is manifested by their large energy separation from lower lying states. Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8356	5-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8386.1	1-	0.159 fs 21	XREF: p(8400). J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’). T_1/2(level): From Γ_γ0 in (γ,γ’) (2002Ha13) and adopted Γ_γ0/Γ.
8437	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8523	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8563	(6-)		J^π(level): From DWBA fit to the Coulomb form factors and RPA calculations in (e,e’); unnatural parity state from absence of longitudinal form factor.
8607	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8664.6	(3,4,5)		J^π(level): In (⁴⁸Ca,⁴⁸Ca’γ), 2001Br35 suggest that these states are near yrast states with J>5 and must involve two-particle two-hole core excitations, which is manifested by their large energy separation from lower lying states.
8680	(3+)		J^π(level): From DWBA analysis in (p,p’) with unnatural parity due to peak not observed in (α,α’) spectra (1988Fu01). Natural parity is distinguished from unnatural parity based on observation of one-to-one correspondences of levels in (p,p’) and (α,α’) spectra (1988Fu01).
8797	4+&(6+)		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8883.3	1-	0.42 fs 14	XREF: p(8900). T_1/2(level): From Γ_γ0 in (γ,γ’) (2002Ha13) and adopted Γ_γ0/Γ.
8886	2+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
8890.7			J^π(level): In (⁴⁸Ca,⁴⁸Ca’γ), 2001Br35 suggest that these states are near yrast states with J>5 and must involve two-particle two-hole core excitations, which is manifested by their large energy separation from lower lying states.
8982	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
9033.9	1-	0.242 fs 14	T_1/2(level): From Γ_γ0 in (γ,γ’) (2002Ha13) and adopted Γ_γ0/Γ.
E(level)	J^π(level)	T_1/2(level)	Comments
9047	2+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
9094.6			J^π(level): In (⁴⁸Ca,⁴⁸Ca’γ), 2001Br35 suggest that these states are near yrast states with J>5 and must involve two-particle two-hole core excitations, which is manifested by their large energy separation from lower lying states.
9123.1	(1+,2+,3+)		J^π(level): In (⁴⁸Ca,⁴⁸Ca’γ), 2001Br35 suggest that these states are near yrast states with J>5 and must involve two-particle two-hole core excitations, which is manifested by their large energy separation from lower lying states.
9158	(4)+		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
9176	2+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
9211	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
9288	(2+)		J^π(level): From DWBA fit to the Coulomb form factors and RPA calculations in (e,e’); unnatural parity state from absence of longitudinal form factor.
9295.3	1-	0.236 fs 14	XREF: p(9300). J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’). T_1/2(level): From Γ_γ0 in (γ,γ’) assuming Γ_γ0/Γ=1 (2002Ha13).
9295.7	(8-)		XREF: E(9276). J^π(level): In (⁴⁸Ca,⁴⁸Ca’γ), 2001Br35 suggest that these states are near yrast states with J>5 and must involve two-particle two-hole core excitations, which is manifested by their large energy separation from lower lying states.
9383	(1+,2+)		BM1=0.020 2 B(M1)\|^<0.07 from (e,e’). E(level): B(M1)\|^<0.07 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
9472.8	1-	0.250 fs 21	J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’). T_1/2(level): From Γ_γ0 in (γ,γ’) assuming Γ_γ0/Γ=1 (2002Ha13).
9545.72	1-	0.139 fs 7	T_1/2(level): From Γ_γ0 in (γ,γ’) assuming Γ_γ0/Γ=1 (2002Ha13).
9550	(3-)		J^π(level): From DWBA fit to the Coulomb form factors and RPA calculations in (e,e’); unnatural parity state from absence of longitudinal form factor.
9621	4+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
9765	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
9816	(1)-		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
9862	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
9885	(1+,2+)		B(M1)\|^<0.09 from (e,e’). E(level): B(M1)\|^<0.09 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
9921	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
9.95E3	(8-)		J^π(level): From DWBA fit to the Coulomb form factors and RPA calculations in (e,e’); unnatural parity state from absence of longitudinal form factor.
9954	(1+,2+)		B(M1)\|^<0.10 from (e,e’). E(level): B(M1)\|^<0.10 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
9993	4+		XREF: α(9985). J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10065	(4)+		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
10081	(3)-		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
10108	4+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
E(level)	J^π(level)	T_1/2(level)	Comments
10126	1-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10138	(1+,2+)		BM1=0.148 13 B(M1)\|^=0.12 3 from (e,e’). E(level): B(M1)\|^=0.12 3 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
10151	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10178	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10191	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10224	1+		B(M1)\|^=3.9 3 from (e,e’). E(level): B(M1)\|^=3.9 3 from (e,e’).
10319	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10330	(1+,2+)		B(M1)\|^=0.09 4 from (e,e’). E(level): B(M1)\|^=0.09 4 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
10345	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10350	(1+,2+)		BM1=0.040 13 B(M1)\|^=0.08 4 from (e,e’). E(level): B(M1)\|^=0.08 4 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
10370	(2)+		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
10483	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10521	(2)+		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
10586	(4)+		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
10611	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10648	(3)-		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
10686	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10731	2+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10782	(1+,2+)		B(M1)\|^=0.12 4 from (e,e’). E(level): B(M1)\|^=0.12 4 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
10803	(3-)		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10822	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10857	2+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10883	(2+)		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
10916	(3)-		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
10935	(1+,2+)		BM1=0.011 8 B(M1)\|^=0.05 2 from (e,e’). E(level): B(M1)\|^=0.05 2 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
E(level)	J^π(level)	T_1/2(level)	Comments
10955	4+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11037	(2+)		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11098	2+&4+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11183	(5-)		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11248	(4)+		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
11281	2+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11329	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11376	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11421	(1+,2+)		B(M1)\|^<0.09 from (e,e’). E(level): B(M1)\|^<0.09 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
11490	(1+,2+)		B(M1)\|^=0.15 3 from (e,e’). E(level): B(M1)\|^=0.15 3 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
11508	2+		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11530	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11622	(4+)		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11693	5-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11725	(1+,2+)		BM1=0.014 9 B(M1)\|^=0.12 4 from (e,e’). E(level): B(M1)\|^=0.12 4 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
11752	(2)+		J^π(level): Likely spin but not clearly observed in (α,α’) spectra measured by 1988Fu01 in (p,p’).
11913	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
11945	(0)+		J^π(level): σ(θ) in (p,p’) show oscillatory patterns and are well fitted by DWBA assuming 0⁺.
11967	(0)+		J^π(level): σ(θ) in (p,p’) show oscillatory patterns and are well fitted by DWBA assuming 0⁺.
12009	(3-)		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
12029	3-		J^π(level): Natural parity state due to presence in the (α,α’) spectra measured by 1988Fu01 in (p,p’).
12055	(1+,2+)		B(M1)\|^=0.08 3 from (e,e’). E(level): B(M1)\|^=0.08 3 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
12275	(1+,2+)		BM1=0.035 19 B(M1)\|^=0.10 5 from (e,e’). E(level): B(M1)\|^=0.10 5 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
12318	(0)+		B(M1)\|^=0.11 3 from (e,e’). E(level): B(M1)\|^=0.11 3 from (e,e’). J^π(level): σ(θ) in (p,p’) show oscillatory patterns and are well fitted by DWBA assuming 0⁺.
12499	(1+,2+)		B(M1)\|^=0.09 4 from (e,e’). E(level): B(M1)\|^=0.09 4 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
E(level)	J^π(level)	T_1/2(level)	Comments
12565	(0)+		J^π(level): σ(θ) in (p,p’) show oscillatory patterns and are well fitted by DWBA assuming 0⁺.
12693	(1+,2+)		BM1=0.035 5 B(M1)\|^=0.10 5 from (e,e’). E(level): B(M1)\|^=0.10 5 from (e,e’). Poor-fit and uncertainty multiplied by a factor of 3 in the fitting. J^π(level): (M1) transition in (e,e’) gives (1⁺); E2 giving 2⁺ may not be excluded due to the weakness of the transition.
12869	(0+)		J^π(level): σ(θ) in (p,p’) show oscillatory patterns and are well fitted by DWBA assuming 0⁺.
16.69E3		6.2 MeV +15-1	E1 resonance. E(level): E1 resonance.
16.79E3		6.95 MeV +11-35	E2 resonance. E(level): E2 resonance.
19.88E3		6.68 MeV +31-36	E0 (ISGMR) resonance. E(level): E0 (ISGMR) resonance.
20.90E3		9.34 MeV 16	E3⁺E4 resonance. E(level): E3⁺E4 resonance.
37.3E3		14.9 MeV +35-1	E1 resonance. E(level): E1 resonance.

E(level)	E(gamma)	Comments
3831.96	3831.4	E(γ): weighted average of 3831.3 2 from (γ,γ’) and 3832.2 5 from (n,n’γ). M(γ): Q from pγ(θ) in (p,p’γ) and M2 ruled out by RUL.
4283.56	451.6	E(γ): from (n,n’γ). Other: 451.9 5 from (p,p’γ). I(γ): from (p,p’γ). Other: 100 13 from ⁴⁹K β^-n decay.. From (p,p’γ), except as noted.
4283.56	4283	M(γ): from observation of E0 e+/e- pair emission to g.s.
4503.74	671.8	E(γ): unweighted average of 671.4 1 from (n,n’γ) and 672.1 2 from (p,p’γ). M(γ): Q from γ(θ) in (n,n’γ); M2 ruled out by RUL.
4507.05	675.1	E(γ): from (n,n’γ). Other: 675.0 1 from (p,p’γ). I(γ): from (p,p’γ). Others: 100 4 from ⁴⁸K β^- decay and 100 8 from (n,n’γ).
4507.05	4507.3	I(γ): unweighted average of 22 6 from ⁴⁸K β^- decay, 25.0 28 from (n,n’γ), and 37.0 28 from (p,p’γ).. Iγ(4507γ)/Iγ(675γ)=0.37 3 from (p,p’γ) discrepant, 0.22 6 from β^- decay consistent. M(γ): O from pγ(θ) in (p,p’γ); M3 ruled out by RUL.
4612.24	780.2	E(γ): weighted average of 780.1 1 from (n,n’γ) and 780.4 2 from (p,p’γ). M(γ): d from γγ(θ) in (p,p’γ) and γ(θ) in (n,n’γ); Δπ=(no) from level scheme.
4695.4	4695.2	E(γ): From (γ,γ’).
5146.42	642.7	E(γ): other: 642.9 2 from (p,p’γ).
5260.81	648.4	I(γ): other: I(648γ)/I(754γ)=100 20/41 20 from (p,p’γ) is discrepant. M(γ): d from γ(θ) in (n,n’γ); Δπ=(yes) from level scheme.
	753.8	E(γ): other: 753.9 from (⁴⁸Ca,⁴⁸Ca’γ). M(γ): d from γ(θ) in (n,n’γ); Δπ=(no) from level scheme.
	757.7	E(γ): from (⁴⁸Ca,⁴⁸Ca’γ).. From (⁴⁸Ca,⁴⁸Ca’γ)
5311	804	E(γ): original 810 from (p,p’γ) I(γ): From (p,p’γ), except as noted.
5311	1479	E(γ): original 1490 from (p,p’γ) I(γ): From (p,p’γ), except as noted.
5312.2	803.9	E(γ): level-energy difference=805.17. Very poor-fit and omitted in the fitting.
	1480.2	E(γ): Poor-fit and uncertainty multiplied by a factor of 3 in the fitting
	5312.2	M(γ): M2 or E2 both allowed by RUL.
5369.90	757.5	I(γ): other: 6.3 4 from ⁴⁸K β^- decay is discrepant. M(γ): d from γ(θ) in (n,n’γ); Δπ=yes from level scheme.
	862.7	I(γ): weighted average of 29 4 from ⁴⁸K β^- decay and 30 4 from (n,n’γ). Other: 67 17 from (p,p’γ) is discrepant.
	866.9	E(γ): level-energy difference=866.16. Poor-fit and uncertainty multiplied by a factor of 3 in the fitting I(γ): weighted average of 23 4 from ⁴⁸K β^- decay and 28.6 32 from (n,n’γ). M(γ): d from γ(θ) in (n,n’γ); Δπ=yes from level scheme.
	1537.8	I(γ): from ⁴⁸K β^- decay. Others: 100 9 from (n,n’γ) and 100 17 from (p,p’γ). M(γ): d from γ(θ) in (n,n’γ); Δπ=yes from level scheme.
5729.64	468.7	I(γ): from (n,n’γ). Other: 100 17 from (p,p’γ). M(γ): assumed based on comparions with RUL
5729.64	1226.0	I(γ): weighted average of 63 14 from (n,n’γ) and 67 17 from (p,p’γ).
6345.72	1841.2	E(γ): level-energy difference=1841.94. Poor-fit and uncertainty multiplied by a factor of 3 in the fitting
6612.19	6611.7	E(γ): From (γ,γ’). M(γ): γ(θ) and γ asymmetry in (γ,γ’).
E(level)	E(gamma)	Comments
6648.99	1504.0	E(γ): level-energy difference=1502.54. Very poor-fit and omitted in the fitting.
	2036.8	M(γ): d from γ(θ) in (n,n’γ); Δπ=no from level scheme.
	2145.1	M(γ): d from γ(θ) in (n,n’γ); Δπ=no from level scheme.
6685.64	1315.8	I(γ): from ⁴⁸K β^- decay. Other: 100 10 from (n,n’γ).
	2073.9	E(γ): level-energy difference=2073.35. Poor-fit and uncertainty multiplied by a factor of 3 in the fitting I(γ): weighted average of 15 4 from ⁴⁸K β^- decay and 26 9 from (n,n’γ). M(γ): d from comparison to RUL; Δπ=yes from level scheme.
	2178.30	E(γ): From β^- decay. I(γ): From β^- decay.
6895.87	1525.7	I(γ): from ⁴⁸K β^- decay. Other: 35 8 from (n,n’γ). M(γ): d from γ(θ) in (n,n’γ); Δπ=(no) from level scheme.
	2283.15	E(γ): From β^- decay. I(γ): From β^- decay.
	2389.0	I(γ): from ⁴⁸K β^- decay. Other: 100 14 from (n,n’γ). M(γ): d from γ(θ) in (n,n’γ); Δπ=(no) from level scheme.
	3063.27	E(γ): From β^- decay. I(γ): From β^- decay.
7032.0	1771	E(γ): level-energy difference=1763 from (p,p’γ)
7296.1	7298	M(γ): (Q) from γ(θ) in (n,n’γ); M2 ruled out by RUL.
7298.50	1929	E(γ): 1932 from level-energy difference in ⁴⁸K β^- decay. From β^- decay. I(γ): From β^- decay.
	2686	E(γ): 2689 from level-energy difference in ⁴⁸K β^- decay. From β^- decay. I(γ): From β^- decay.
	7297.9	E(γ): from (γ,γ’). Other: 7300.9 from ⁴⁸K β^- decay. I(γ): from ⁴⁸K β^- decay. M(γ): from γ(θ) and γ asymmetry in (γ,γ’).
7401.22	715.61	E(γ): From β^- decay. I(γ): From β^- decay.
	2031.23	E(γ): From β^- decay. I(γ): From β^- decay.
	2788.90	E(γ): From β^- decay. I(γ): From β^- decay.
	2894	E(γ): From β^- decay. I(γ): From β^- decay.
	3569	E(γ): From β^- decay. I(γ): From β^- decay.
	7400	E(γ): From β^- decay. I(γ): From β^- decay.
7407.3	793.11	E(γ): From β^- decay.
7536.4	2389.8	E(γ): From (⁴⁸Ca,⁴⁸Ca’γ)
7536.4	3032.7	E(γ): From (⁴⁸Ca,⁴⁸Ca’γ)
7652	3146	E(γ): level-energy difference=3140 from (p,p’γ). Multiply placed
7652	3146	E(γ): level-energy difference=3140 from (p,p’γ). Multiply placed
E(level)	E(gamma)	Comments
7655.66	7655.0	E(γ): From (γ,γ’). M(γ): from γ(θ) and α asymmetry in (γ,γ’).
7789	958	E(γ): level-energy difference=964 from (p,p’γ)
7915.4	7914.7	E(γ): From (γ,γ’).
7957	1126	E(γ): level-energy difference=1137 from (p,p’γ)
8027.6	8026.9	E(γ): From (γ,γ’). M(γ): Q from γ(θ) in (γ,γ’); M2 ruled out by RUL.
8045	3544	E(γ): level-energy difference=3529 from (p,p’γ). Multiply placed
	3544	E(γ): level-energy difference=3529 from (p,p’γ). Multiply placed
	8044	E(γ): level-energy difference=8040 from (p,p’γ)
8248	3740	E(γ): level-energy difference=3735 from (p,p’γ). Multiply placed
8248	3740	E(γ): level-energy difference=3735 from (p,p’γ). Multiply placed
8276	1445	E(γ): level-energy difference=1456 from (p,p’γ)
	3770	E(γ): level-energy difference=3764 from (p,p’γ). Multiply placed
	3770	E(γ): level-energy difference=3764 from (p,p’γ). Multiply placed
8279.1	3133	E(γ): From (⁴⁸Ca,⁴⁸Ca’γ)
8386.1	1555	E(γ): level-energy difference=1564 from (p,p’γ)
	4554.2	E(γ): From (γ,γ’). I(γ): From (γ,γ’). M(γ): d from γ(θ) in (γ,γ’); Δπ=yes from level scheme.
	8385.3	E(γ): From (γ,γ’). I(γ): From (γ,γ’). M(γ): from γ(θ) and γ asymmetry in (γ,γ’).
8467	4635	E(γ): From β^- decay. I(γ): From β^- decay.
8467	8466	E(γ): From β^- decay. I(γ): From β^- decay.
8478	3972	E(γ): level-energy difference=3976 from (p,p’γ). Multiply placed
8478	3972	E(γ): level-energy difference=3976 from (p,p’γ). Multiply placed
8517.9	8517.1	E(γ): From (γ,γ’).
8523	4017	E(γ): level-energy difference=4015 from (p,p’γ). Multiply placed
8523	4017	E(γ): level-energy difference=4015 from (p,p’γ). Multiply placed
8531	4247	E(γ): From β^- decay. I(γ): From β^- decay.
	4699	E(γ): From β^- decay. I(γ): From β^- decay.
	8530	E(γ): From β^- decay. I(γ): From β^- decay.
E(level)	E(gamma)	Comments
8586	4080	E(γ): level-energy difference=4073 from (p,p’γ). Multiply placed
8586	4080	E(γ): level-energy difference=4073 from (p,p’γ). Multiply placed
8664.6	386	E(γ): From (⁴⁸Ca,⁴⁸Ca’γ)
8680	4174	E(γ): level-energy difference=4159 from (p,p’γ). Multiply placed
8680	4174	E(γ): level-energy difference=4159 from (p,p’γ). Multiply placed
8788	4282	E(γ): level-energy difference=4277 from (p,p’γ). Multiply placed
8788	4282	E(γ): level-energy difference=4277 from (p,p’γ). Multiply placed
8883.3	5050.6	M(γ): d from γ(θ) in (γ,γ’); Δπ=yes from level scheme.
8890.7	3160.8	E(γ): From (⁴⁸Ca,⁴⁸Ca’γ)
8967	8966	E(γ): From β^- decay.
9033.9	5200.9	E(γ): From (γ,γ’). I(γ): From (γ,γ’). M(γ): d from γ(θ) in (γ,γ’); Δπ=yes from level scheme.
9033.9	9033.0	E(γ): From (γ,γ’). I(γ): From (γ,γ’). M(γ): from γ(θ) and γ asymmetry in (γ,γ’).
9094.6	430	E(γ): From (⁴⁸Ca,⁴⁸Ca’γ)
9123.1	232	E(γ): From (⁴⁸Ca,⁴⁸Ca’γ)
9123.1	459	E(γ): From (⁴⁸Ca,⁴⁸Ca’γ)
9295.3	9294.3	E(γ): other: 9300 from (α,α’γ) and ⁴⁸K β^- decay. M(γ): from γ(θ) and γ asymmetry in (γ,γ’) and αγ(θ) in (α,α’γ).
9295.7	405	E(γ): From (⁴⁸Ca,⁴⁸Ca’γ)
9472.8	9471.8	E(γ): From (γ,γ’). M(γ): from γ(θ) and γ asymmetry in (γ,γ’).
9545.72	9544.7	E(γ): From (γ,γ’). M(γ): from γ(θ) and γ asymmetry in (γ,γ’).

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 G H I K L M N P Q R S	0+	2.9×10¹⁹ y +42-11 % β^- = 22 +30-22 % 2β^- = 78 +22-30
3831.96 22	A B C D E G H I K L M N O P Q R S	2+	36 fs 3	3831.4 3	100	E2	0.0	0+
4283.56 24	A B C E H I K N S	0+	223 ps 11	451.6 1 4283S	100.0 10	[E2] E0	3831.96 0.0	2+ 0+
4503.74 24	A C H K M S	4+	1.53 ns 3	671.8 4	100	E2	3831.96	2+
4507.05 23	A C E G H I K L M N O P Q R S	3-	6.1 ps +38-20	675.1 1 4507.3 5	100.0 28 28 5	(E1(+M2)) E3	3831.96 0.0	2+ 0+
4612.24 23	A E H I K N S	3(+)	2.5 ps 14	780.2 1	100	(M1)	3831.96	2+
4695.4 3	D	1	32.6 fs +25-22	4695.2 3	100	D	0.0	0+
5146.42 25	E H I K N R S	3,4,5	< 0.69 ns	642.7 1	100	D	4503.74	4+
5260.81 23	A E H I K S	4(-)	5.1 ps +14-8	648.4 1 753.8 1 757.7?	16.8 17 100 9	(E1) (M1)	4612.24 4507.05 4503.74	3(+) 3- 4+
5311 6	I K N	(1)-		804 1479	25 13 100 13		4507.05 3831.96	3- 2+
5312.2 3	H N	2	232 fs +28-13	803.9 1 1480.2 1 5312.2 5	5.7 10 100 8 15.4 18	D D+Q Q	4507.05 3831.96 0.0	3- 2+ 0+
5369.90 23	A E H I K N	3-	1.80 ps 14	757.5 1 862.7 1 866.9 1 1537.8 1	29 4 30 4 26.4 32 100 6	(E1) [M1,E2] (E1) (E1)	4612.24 4507.05 4503.74 3831.96	3(+) 3- 4+ 2+
5461 7	C I N	0+
5729.64 24	E G H I K N S	5-	0.90 ps +49-21	468.7 1 1226.0 1	100 9 65 14	[M1] [E1]	5260.81 4503.74	4(-) 4+
6105.00 23	E H I K N	(2+)	139 fs +17-28	1597.8 1 2273.1 1	100 10 13.7 20	[E1] [M1,E2]	4507.05 3831.96	3- 2+
6336.8 20	C H	2+	191 fs 29	6336.4 20	100	E2	0.0	0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6345.72 24	E H I K N	4+	180 fs +35-13	1199.3 1 1733.5 1 1841.2 1	17 8 20 5 100 11		5146.42 4612.24 4503.74	3,4,5 3(+) 4+
6.48E+3?	N
6612.19 10	A D I K P	1-	1.87 fs 14	6611.7 1	100	E1	0.0	0+
6648.99 24	C E H I K N	4+	114 fs +42-28	1278? 1504.0 1 2036.8 1 2145.1 1	68 8 51 5 100 16	D (M1) (M1)	5369.90 5146.42 4612.24 4503.74	3- 3,4,5 3(+) 4+
6685.64 23	A E H I K	2(-)	69 fs +56-52	1315.8 1 2073.9 1 2178.30?	100 8 17 4 18 4	[M1,E2] (E1) [M1,E2]	5369.90 4612.24 4507.05	3- 3(+) 3-
6755	I N	2+
6791.5 20	E H	1	< 6.9 fs	6791.0 20	100	D	0.0	0+
6805.7 3	C E H I N P	2+	83 fs +44-38	2301.9 1 2974.8 5	100 14 72 24	[E2] [M1,E2]	4503.74 3831.96	4+ 2+
6830.8 6	H I K N	(3-)		2998.7 5	100	D	3831.96	2+
6895.87 24	A E H K	(2-)	55 fs +83-55	1525.7 1 2283.15? 2389.0 1 3063.27?	36 6 23 4 100 7 35 7	(M1) [E1] (M1)	5369.90 4612.24 4507.05 3831.96	3- 3(+) 3- 2+
6896 7	E I	(5+)
7007.6 6	E H I	3-	69 fs +18-14	3175.5 5	100	[E1]	3831.96	2+
7019 7	E I
7032.0 6	E H I K N	(3)-		1771? 2524.9 5	100	D+Q	5260.81 4507.05	4(-) 3-
7.16E+3?	N
7296.1 5	H	(2+)	< 6.9 fs	3463.9 5 7298 2	100 11 21 4	(E2)	3831.96 0.0	2+ 0+
7298.50 20	A D E I K P	1-	0.201 fs 14	1929 2686 7297.9 2	0.52 0.52 100 26	E1	5369.90 4612.24 0.0	3- 3(+) 0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7370.6 20	H	(1,2)		7370 2	100		0.0	0+
7385 10	I	3-,(1-)
7401.22 23	A E I K S	(2-)		715.61 2031.23 2788.90 2894 3569 7400	8.2 24 17.9 24 100 6 5.3 6.6 1.30		6685.64 5369.90 4612.24 4507.05 3831.96 0.0	2(-) 3- 3(+) 3- 2+ 0+
7407.3 5 ?	A	(0,1,2,3-)		793.11 6 ?	100		6612.19	1-
7440.6 20	H I K	2,3-	177.4 fs 70	7440 2	100	Q,E3	0.0	0+
7471 5	E I	4+
7497.5 3	H I	(3-)		1767.8 1	100		5729.64	5-
7536.4 4	I N S	3-		2389.8 3032.7			5146.42 4503.74	3,4,5 4+
7568.7 6	H			3736.6 5	100		3831.96	2+
7580 7	I
7652 10	A C E G I K	3-		3146? 3146? 7651			4503.74 4507.05 0.0	4+ 3- 0+
7655.66 20	C D P	1-	1.87 fs 7	7655.0 2	100	E1	0.0	0+
7659 3	C E G I	3-
7696	E	(1+,2+)
7789 7	E K N	3-		958			6830.8	(3-)
7797 8	I	4+
7911 7	I	3-
7915.4 9	D	2+	22 fs +4-3	7914.7 9	100	E2	0.0	0+
7953 15 ?	E	(2-,6-)
7957 10	I K	(4)+		1126			6830.8	(3-)
8001 8	C I
8027.6 4	C D E I	2+	11.4 fs 12	8026.9 4	100	E2	0.0	0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
8045 8	C E I K	(1)		3544? 3544? 8044?			4503.74 4507.05 0.0	4+ 3- 0+
8050	E P	2		8050			0.0	0+
8065 8	I	5-
8082 10	I
8116 8	E I	1+,2+,3+
8150	E	(1+,2+)
8178 8	I	4+
8236 8	C I	4-,5-,6-
8248 8	C I K	4+		3740? 3740?			4503.74 4507.05	4+ 3-
8276?	C K	(1-,2,3)		1445 3770? 3770? 8275			6830.8 4507.05 4503.74 0.0	(3-) 3- 4+ 0+
8279.1 9	C E I N S	4+		3133			5146.42	3,4,5
8356 8	I N	5-
8385 18 ?	E	(3-)
8386 8	I P	(6)+
8386.1 5	A D I K P	1-	0.159 fs 21	1555? 4554.2 12 8385.3 5	9.9 3 100 9	(E1) E1	6830.8 3831.96 0.0	(3-) 2+ 0+
8437 5	E I	3-
8467?	A C	(1,2)		4635? 8466?	100 15.7		3831.96 0.0	2+ 0+
8478 8	C E I K	3+,4+,5+		3972? 3972?			4503.74 4507.05	4+ 3-
8517.9 8	C D	(1-,2+)		8517.1 8	100		0.0	0+
8523 5	C E I K	3-		4017? 4017?			4503.74 4507.05	4+ 3-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
8531?	A C	(1,2+)		4247? 4699? 8530?	39 100 61		4283.56 3831.96 0.0	0+ 2+ 0+
8563 7	E I	(6-)
8586 10 ?	I K			4080? 4080?			4503.74 4507.05	4+ 3-
8607 6	C E I	3-
8664.6 11	S	(3,4,5)		386			8279.1	4+
8680 7	C I K	(3+)		4174? 4174?			4503.74 4507.05	4+ 3-
8698 8	C I
8788 8	C I K			4282? 4282?			4503.74 4507.05	4+ 3-
8797 8	I	4+&(6+)
8805 5	E I	5-
8831 8	I	2-,3-,4-
8866 8	I	4-,5-,6-
8883.3 5	D E P	1-	0.42 fs 14	5050.6 9 8882.6 5	4.0 10 100 30	(E1) E1	3831.96 0.0	2+ 0+
8886 6	E I	2+
8890.7 6	S			3160.8			5729.64	5-
8920 8	I
8947 8	I
8967?	A I	(1,2,3)		8966?	100		0.0	0+
8982 8	I	3-
9033.9 4	D E I	1-	0.242 fs 14	5200.9 15 9033.0 4	2.2 9 100 4	(E1) E1	3831.96 0.0	2+ 0+
9047 9	E I	2+
9050	E P	1		9050		D	0.0	0+
9079 9	I
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
9094.6 15	S			430			8664.6	(3,4,5)
9123.1 10	I S	(1+,2+,3+)		232 459			8890.7 8664.6	(3,4,5)
9138 22	E
9158 9	I	(4)+
9176 9	I	2+
9211 9	I	3-
9229	I	(7-)
9232 9	I	(0-,1-,2-)
9288 9	E I	(2+)
9295.3 5	A D I P	1-	0.236 fs 14	9294.3	100	E1	0.0	0+
9295.7 11	E I S	(8-)		405			8890.7
9307	I	8
9334 9	I
9366 9	I	5+,6+,7+
9383 10	E I	(1+,2+)
9430 9	I	2-,3-,4-
9472.8 8	D I P	1-	0.250 fs 21	9471.8 8	100	E1	0.0	0+
9496 9	I
9545.72 20	D I P	1-	0.139 fs 7	9544.7 2	100	E1	0.0	0+
9550 20 ?	E	(3-)
9568 9	I	(5+,6+,7+)
9621 9	I	4+
9645 9	I	2-,3-,4-
9691 9	I	(0-,1-,2-)
9728 9	I	2-,3-,4-
9765 9	I	3-
9784 9	I	(3+,4+,5+)
9816 9	I	(1)-
9862 9	I	3-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
9885	E	(1+,2+)
9894 7	I
9921 9	I	3-
9942 9	E I	2-,3-,4-
9.95E3 3	E	(8-)
9954	E	(1+,2+)
9973 10	I	1+
9993 9	A I	4+
10065 10	A I	(4)+
10081 10	A I	(3)-
10108 10	I	4+
10126 10	A I	1-
10138 10	E I	(1+,2+)
10151 10	E I	3-
10178 10	A I	3-
10191 10	I	3-
10224 7	E G I	1+
10240?	A
10265 10	A I	(-)
10288 10	I
10319 10	I	3-
10330 10 ?	E	(1+,2+)
10345 10	I	3-
10350 10	A E I	(1+,2+)
10370 10	A I	(2)+
10390 10	I
10399 10	I	3+,4+,5+
10433 10	I	1+,2+,3+
10483 10	I	3-
10521 10	I	(2)+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
10535 10	I	(0-,1-,2-)
10571 10	I
10586 10	I	(4)+
10610 10	I
10611 10	A I	3-
10623 10	I
10645 10	I
10648 10	A I	(3)-
10686 10	A I	3-
10708 10	I
10731 10	I	2+
10764 10	I
10782 10	E I	(1+,2+)
10803 10	I	(3-)
10822 10	A I	3-
10857 10	I	2+
10872 10	I	5+,6+,7+
10883 10	I	(2+)
10916 10	A I	(3)-
10935 10	E I	(1+,2+)
10955 10	I	4+
11013 11	A I
11032?	A	(-)
11037 11	I	(2+)
11050 11	I	(3+,4+,5+)
11098 11	I	2+&4+
11125 11	I	3+,4+,5+
11153 11	I
11183 11	I	(5-)
11219 11	I
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
11227 10	I
11248 11	I	(4)+
11281 11	I	2+
11329 11	I	3-
11376 11	I	3-
11383 10	I
11421 11	E I	(1+,2+)
11433 11	I	1+,2+,3+
11447 11	I	2-,3-,4-
11466 11	I
11485 11	I	(2-,3-,4-)
11490	E	(1+,2+)
11508 11	I	2+
11513 10	I
11530 11	I	3-
11550 11	I
11563 10	I
11589 11	I	0-,1-,2-
11622 11	I	(4+)
11639 11	I	(1+,2+,3+)
11671 11	I	(4-,5-,6-)&(8-)
11693 11	I	5-
11695 10	I
11715 11	I	(1+,2+,3+)
11725 10	E I	(1+,2+)
11752 11	I	(2)+
11773 11	I
11816 11	I	2-,3-,4-
11828 11	I
11843 10	I
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
11848 11	I
11913 11	I	3-
11945 11	I	(0)+
11967 11	I	(0)+
11990 10	I
12009 12	I	(3-)
12029 12	I	3-
12051 12	I	(0-,1-,2-)
12055	E	(1+,2+)
12090 12	I	(2-,3-,4-)
12107 12	I	4-,5-,6-
12121 10	I	0-,1-,2-
12162 12	I	3+,4+,5+
12176 12	I
12216 12	I	4-,5-,6-
12271 12	E I	(3+,4+,5+)
12275 10	E I	(1+,2+)
12318 12	E I	(0)+
12338 10	I	(1,2)+
12369 12	I	(3+,4+,5+)
12422 12	I	1+,2+,3+
12441 12	I	2-,3-,4-
12478 10	I
12499 12	E I	(1+,2+)
12540 12	I	1+,2+,3+
12565 12	I	(0)+
12620 12	I	1+,2+,3+
12623 10	I
12659 10	I
12667 12	I
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
12693 10	E I	(1+,2+)
12704 12	I
12757 12	I	1+,2+,3+
12798 12	I	1+,2+,3+
12846 12	I
12869 12	I	(0+)
12918 10	I
12925 12	I	1+,2+,3+
12968 12	I	(2-,3-,4-)
13030 13	I	4-,5-,6-
13065 13	I	(1+,2+,3+)
13098 13	I	1+,2+,3+
13169 13	I	0-,1-,2-
13223 13	I
13256 13	I	2-,3-,4-
13290 13	I
13360 13	I	1+,2+,3+
13403 13	I	1+,2+,3+
13439 13	I
13475 13	I	1+,2+,3+
13493 13	I
16.69E3 19	O		6.2 MeV +15-1
16.79E3 14	O		6.95 MeV +11-35
19.88E3 18	O		6.68 MeV +31-36
20.90E3 14	O		9.34 MeV 16
24.2E3	F	(1-)	% n = 100
37.3E3 20	O		14.9 MeV +35-1