List of levels for 100MO

ADOPTED LEVELS, GAMMAS for ¹⁰⁰Mo

Authors: Balraj Singh and Jun Chen | Citation: Nucl. Data Sheets 172, 1 (2021) | Cutoff date: 31-Jan-2021

Full ENSDF file | Adopted Levels (PDF version)

Q(β-)=-172.1 keV 14	S(n)= 8294.2 keV 4	S(p)= 11147 keV 12	Q(α)= -3179.1 keV 3
Reference: 2017WA10

References:
A	¹⁰⁰Nb β^- decay (1.4 S)	B	¹⁰⁰Nb β^- decay (2.99 S)
C	¹⁰⁰Tc ε decay (15.65 S)	D	⁹Be(¹⁰⁹Tc,xγ)
E	⁹⁶Zr(⁷Li,p2nγ)	F	⁹⁸Mo(t,p),(t,pγ)
G	¹⁰⁰Mo(γ,γ’)	H	¹⁰⁰Mo(n,n’)
I	¹⁰⁰Mo(n,n’γ)	J	¹⁰⁰Mo(p,p’)
K	¹⁰⁰Mo(α,α’)	L	¹⁰⁰Mo(d,d’)
M	Coulomb Excitation	N	¹⁰⁰Mo(¹³⁶Xe,xγ)
O	¹⁰²Ru(¹⁴C,¹⁶O)	P	¹⁰⁴Ru(d,⁶Li)
Q	¹¹⁰Pd(⁸⁶Kr,xγ)	R	¹⁶⁸Er(³⁰Si,xγ)

Other reactions:

Giant-dipole resonances, (γ,X) reactions: 1980St26, 1974Be33, 1974Ca05. (p,p’) reaction at E(p)=200 MeV (1982Dj04).

Giant-quadrupole resonances, ¹⁰⁰Mo(α,α’), ¹⁰⁰Mo(³He,³He’): 1976Yo02, 1978Mo10, 1979Mo12. Resonance at 13.76 MeV with Γ=5.2 MeV

Low energy octupole resonances, ¹⁰⁰Mo(α,α’): 1978Mo10

¹⁰⁰Mo(²⁰Ne,F) E=146 MeV: 1984Na12

¹⁰⁰Mo(⁵⁸Ni,⁵⁸Ni) E=137.5 MeV: 1995Re06, measured σ(θ)

¹⁰⁰Mo(³²S,³²S): 1995He17, measured cross section

¹⁰⁰Mo(¹⁴C,¹⁴C’) E=71 MeV: 1982Ma30, σ(θ) for g.s. and first 2⁺

¹⁰⁰Mo(¹²C,¹²C’) E=48 MeV: 1981Vi01, 1980Lo01

¹⁰⁰Mo(e,e’) E=120, 200, 274 MeV: 1975Dr06, charge radii and charge distributions deduced. Other: 1972EhZZ

¹⁰⁰Mo(t,t) E=12 MeV: 2006Ch64, measured σ(θ), deduced optical model parameters.

Mesic atoms, ¹⁰⁰Mo(μ^-,X): 1978Du21, 1980Sc01. Theory: 1980Ba56, 1976Le08

Antiprotonic atoms, ¹⁰⁰Mo(antiproton,x): 1999Sc35, 1994Ha51, 1986Ka08, 1985Kl02

Isotope-shift measurements: 1986Ol03, 1985Go10, 1984Br09, 1978Au05

Mass measurements: 2015Gu09, 2012Ka13, 2008Ra09, 2006Jo14, 2004Ko42, 1963Bi12, 1963Ri07.

-----------------------------------------------------------------

Measurements of half-life of ββ decay of ¹⁰⁰Mo:

T_1/2(2νββ)(to ¹⁰⁰Ru g.s.): 7.12×10¹⁸ y +21-17 (2020Ar09, CUPID-Mo, Modane, earlier value of 6.90×10¹⁸ y 15(stat) 37(syst) in 2017Ar18); 6.81×10¹⁸ y 1(stat) +38-40(syst) (2019Ar04, earlier value: 7.17×10¹⁸ y 1(stat) 54(syst) in 2011Fl06, NEMO-3, also 2006Ar01,2005Ar27,2005Sa07, 2005Si06, 2004Ar29); 7.15×10¹⁸ y 37(stat) 66(syst) (2014Ca46, NIIC, Russia); 2.1×10¹⁸ y 3 (2004Hi19, geochemical); 7.6×10¹⁸ y +22-14 (1997Al02); 11.5×10¹⁸ y +30-20 (1991Ej05,1996Ej04, 1991Ej02); 9.5×10¹⁸ y 4 (stat) 9 (syst) (1995Da37, NEMO-2); 11.6×10¹⁸ y +34-8 (1991El04, also 1987El13); 0.33×10¹⁹ y +20-10 (1990Va10). α small contribution of ≈1% to total half-life is made by T_1/2(2νββ)(to 1130,0⁺ level in ¹⁰⁰Ru)=7.5×10²⁰ y 6(stat) 6(syst) (2014Ar08); 6.9×10²⁰ y +10-8(stat) 7(syst) (2010Be34); 5.7×10²⁰ y +15-12 (2007Ar02); 6.0×10²⁰ y +20-13 (2009Ki04,2006Ho17,2006Ba35); 6.1×10²⁰ y +18-11 (1995Ba29). Decay modes of 2νββ to other excited states in ¹⁰⁰Ru, and 0νββ modes make almost no contributions.

T_1/2(0ν,ββ to g.s.): >2.6×10²² y (2017Ar18); >1.1×10²⁴ y (2014Ar08,2011Ba55,NEMO-3, 90% εL; also >1.0×10²⁴ y in 2012Si23 and 2011Fl06), >4.6×10²³ y (2005Ar27,NEMO-3); >5.5×10²² y (2002Fu05,2001Ej03,ELEGANT-5); >4.9×10²¹ y (2001As06, 2001As05); >2.2×10²² y (1997Al02); >5.2×10²² y (1996Ej04); >1.2×10²² y (1995Da37)

T_1/2(0ν,ββ, Majorana neutrino to g.s.)>5.4×10²¹ y (1996Ej04,1991Ej02), >7.5×10²⁰ y (1995Da37).

Planned T_1/2(0ν,ββ) experiment: CROSS collaboration at Canfranc Underground Laboratory described in a review article by 2020Ce04, and by I.C. Bandac et al., Jour. High Energy Physics 1, 18 (2020)

T_1/2(0ν,ββ,Majorana neutrino emission)>2.7×10²⁷ y (2006Ar01).

T_1/2(2ν+0ν,ββ to 539,2⁺ level)>25×10²⁰ y (2014Ar08)

T_1/2(2ν,ββ to 539.5,2⁺ level)>11×10²⁰ y (2007Ar02) (90% confidence limit); >16×10²⁰ y (1995Ba29); >5×10²⁰ y (1992Bl06)

T_1/2(0ν,ββ to 539.5,2⁺ level)>1.6×10²³ y (2007Ar02) (90% confidence limit); >1.1×10²¹ y (1995Da37)

T_1/2(2ν,ββ to 1130,0⁺ level)=7.5×10²⁰ y 6(stat) 6(syst) (2014Ar08)

T_1/2(2ν+0ν,ββ to 1130,0⁺ level)=6.9×10²⁰ y +10-8(stat) 7(syst) (2010Be34).

T_1/2(0ν+2ν)=6.0×10²⁰ y +20-13 (2009Ki04,2006Ho17) for decay to the 1130, 0⁺ state. The statistical uncertainty of +1.9-1.1 and systematic uncertainty of 0.6 have been combined in quadrature. Earlier value from the same group=5.9×10²⁰ y +18-13 in 2001De17

T_1/2(2ν,ββ to 1130,0⁺ level)=5.7×10²⁰ y +15-12 (2007Ar02) (90% confidence limit); 6.1×10²⁰ y +18-11 (1995Ba29); >12×10²⁰ y (1992Bl06)

T_1/2(0ν,ββ to 1130,0⁺ level)>8.9×10²² y (2007Ar02) (90% confidence limit); >1.7×10²¹ y (1995Da37)

T_1/2(2ν+0ν,ββ to 1362,2⁺ level)>108×10²⁰ y (2014Ar08)

T_1/2(ββ)>44×10²⁰ y at 90% confidence level for decay to 1362.2 keV 2⁺ level (2009Ki04,2006Ho17).

T_1/2(2ν,ββ to 1362,2⁺ level)>13×10²⁰ y (1995Ba29); >6×10²⁰ y (1992Bl06)

T_1/2(2ν+0ν,ββ to 1741,0⁺ level)>40×10²⁰ y (2014Ar08)

T_1/2(ββ)>48×10²⁰ y at 90% confidence level for decay to 1741.0 keV 0⁺ level (2009Ki04,2006Ho17).

T_1/2(2ν,ββ to 1741,0⁺ level)>13×10²⁰ y (1995Ba29)

T_1/2(2ν+0ν,ββ to 1865,2⁺ level)>49×10²⁰ y (2014Ar08)

T_1/2(2ν+0ν,ββ to 2051,0⁺ level)>43×10²⁰ y (2014Ar08)

T_1/2(ββ)>38×10²⁰ y at 90% confidence level for decay to 2051.7 keV 0⁺ level (2009Ki04,2006Ho17).

T_1/2(ββ)>40×10²⁰ y at 90% confidence level for decay to 2387.2 keV 0⁺ level (2009Ki04,2006Ho17).

Measurements of ββ decay of ¹⁰⁰Mo: 2020Ar09, 2019Ar04, 2017Ar18, 2014Ar05, 2014Ar08, 2014Ca46, 2012Si23, 2011Ba55, 2011Fl06, 2010Be34, 2010Si06, 2009Da25, 2009Ki04, 2009KoZY, 2008KoZV, 2007Ar02, 2006Ho17, 2006Ba35, 2006Ar01 (also 2005Ar27,2005Ba01,2005Ba33,2005Sa07,2005Si06, 2004Ar29,2004Ba27,2004Ba97,2004Ko61,2003Ba22,2003Oh07,2002As05, 2002Ba52,2001As05,2001As06,2001Va34,2000Ar16,1999As01,1999As09, 1999Bb18,1999Bb19,1999Pi08,1999Sa02,1998As04); 2004Hi19 (geochemical method); 2002Fu05 (also 2002Ej05,2001Ej01, 2001Ej03,2000Ej01,2000Ku21,1998Ku09,1997Ej01); 2001Be19 (also 2000Be57); 1997Al02 (also 1993Al11,1989Al20), 1996Ej04 (also 1996Ej06, 1992Ku18,1991Wa31,1991Ej05,1991Ej02,1988Ok01), 1995Ba29 (also 1996Bb02,1990Ba63,1990Ba52), 1995Da37 (also 1994La42,1992Bl06), 1991El04 (also 1987El13), 1990Va10. Others: 1997De40, 1993Ko28, 1984Fi16 (also 1982Be20), 1983Zd01, 1955Wi33, 1954Se93, 1952Fr23.

Theory references: consult the NSR database (www.nndc.bnl.gov/nsr/) for 342 primary references, 136 dealing with nuclear structure calculations and 206 with double-beta decay nuclear matrix elements and half-life for ¹⁰⁰Mo 2β decay

Q-value: S(2n)=14219.7 3, S(2p)=19484 8, Q(2β^-)=3034.36 17 (2017Wa10)

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A B C D E F G H I J K L M N O P Q R	0+	7.01×10⁺¹⁸ y +21-17 % 2β^- = 100
535.59 4	A B D E F G H I J K L M N O P Q R	2+	12.4 ps 3	535.61 6	100	E2	0.0	0+
695.13 4	A B F G H I J L M P	0+	1.62 ns 4	159.547 13 695.1	100 1	E2 E0	535.59 0.0	2+ 0+
1063.82 4	A B F G H I J K L M R	2+	6.6 ps 6	369.1 1 528.248 18 1063.78 5	1.76 20 100.0 16 38.0 4	[E2] E2+M1 E2	695.13 535.59 0.0	0+ 2+ 0+
1136.02 4	A B D E F H I J K L M N Q R	4+	3.8 ps 3	600.40 2	100	(E2)	535.59	2+
1463.93 5	A B F G H I J L M	2+	2.9 ps 7	327 1 400.17 9 768.77 3 928.34 3	3.5 15 5.2 7 100.0 10 72.9 9	[E2] E2 M1+E2	1136.02 1063.82 695.13 535.59	4+ 2+ 0+ 2+
1504.66 6	A F I J L	0+		440.84 5 969.07 7	37 4 100 8	(E2)	1063.82 535.59	2+ 2+
1607.37 5	A B I J L R	(3+)		471.37 9 543.58 8 1071.77 3	17 2 100 7 74 1		1136.02 1063.82 535.59	4+ 2+ 2+
1766.52 11	H I J L	(2+)		702.7 1 1071.77 3 ?	100		1063.82 695.13	2+ 0+
1771.44 5	B H I L M	(4+)	2.5 ps 4	635.31 4 707.68 3	55 3 100 2	(E2)	1136.02 1063.82	4+ 2+
1847.17 8	B E I J M N Q R	6+	1.20 ps 17	711.15 6	100	(E2)	1136.02	4+
1908.19 6	F H I J K L M P R	3-	14 ps 3	844.37 4 1372.1 7 1908.2 5	100.0 10 46 4 4.6 10	[E1] [E1] [E3]	1063.82 535.59 0.0	2+ 2+ 0+
1977.34 7	A G I	(1,2+)		513.2 2 913.70 9 1281.8 5 1441.67 7	74 19 79 4 52 15 100 5		1463.93 1063.82 695.13 535.59	2+ 2+ 0+ 2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2037.60 17	A F G I J K L	0+		573.6 2 1502.2 3	6.6 9 100 7	(E2)	1463.93 535.59	2+ 2+
2042.78 7	G I J	(2)+		435.5 2 578.8 1 978.95 9 1507.5 4 2042.9 2	24 5 100 10 71 5 29 7 68 10		1607.37 1463.93 1063.82 535.59 0.0	(3+) 2+ 2+ 2+ 0+
2082 10	F H J
2086.33 15	A I	0+		622.5 2 1022.5 3 1550.5 3	31 6 100 12 14 2	(E2) (E2)	1463.93 1063.82 535.59	2+ 2+ 2+
2103.13 9	B F I J K L	4+		495.4 9 ? 639.1 2 967.1 1 1567.7 2	3.5 23 25 3 100 4 53 18		1607.37 1463.93 1136.02 535.59	(3+) 2+ 4+ 2+
2156 2	J L	1-
2189.56 15	A F I J K	(0+,1,2)		1125.8 2 1653.9 2	25 5 100 8		1063.82 535.59	2+ 2+
2201.22 11	F I J K L	(2-)		1137.4 1 1665.4 1 ?	100 7 84 7		1063.82 535.59	2+ 2+
2286.47 17	F I J L	2+		822.7 3 1750.8 2	32 4 100 6		1463.93 535.59	2+ 2+
2289.5 4	B R	(4,5+)		682.1 4	100		1607.37	(3+)
2310 2	J L	6+
2310.12 20	B	(4+)		538.6 4 702.7 3 1246.4 3	27 9 100 14 48 7		1771.44 1607.37 1063.82	(4+) (3+) 2+
2320.3 3	A F	(0+,1,2)		856.3 3 1257.0 6	44 18 100 9		1463.93 1063.82	2+ 2+
2339.8 4	F H J K L Q R	(5-)		431.5 5 1203.6 5	100 14 82 9		1908.19 1136.02	3- 4+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2369.68 11	F I J L	3-		1305.9 1 1833.7 3	100 12 56 9		1063.82 535.59	2+ 2+
2397.0 3	F I J K L	(1-)		1861.4 3 ?	100		535.59	2+
2416.58 22	B F I J K L	(4+)		952.5 3 1280.7 3	21 3 100 11	(M1+E2)	1463.93 1136.02	2+ 4+
2432 2	J K	1-
2464 20	K	4+
2514 5	F J L	(4+)
2527 5	F J L	(2+)
2564.20 14	B F I J K L	(4)+		461.1 2 792.8 2 1428.0 3 1500.2 3 ?	100 6 51 7 51 6 50 17		2103.13 1771.44 1136.02 1063.82	4+ (4+) 4+ 2+
2580.89 22	I	(1,2+)		1516.8 3 1886.0 3	100 20 80 13		1063.82 695.13	2+ 0+
2607 5	F J K L P	(4+,5-)
2627.5 5	E M N Q R	8+	0.58 ps 9	780.3 5	100	(E2)	1847.17	6+
2628 5	J L	(2+)
2632.4 3	G	(1)	0.51 ps 10	2632.4 3	100	(D)	0.0	0+
2652.87 21	B	(4+,5+)		549.7 3 1045.8 6 1516.8 3	50 10 25 10 100 15		2103.13 1607.37 1136.02	4+ (3+) 4+
2659 5	F J K L	(1-)
2662.6 3 ?	I			1598.8 3 ?	100		1063.82	2+
2725 5	J L
2738.02 22	F I K P	(2+)		1674.3 3 2202.3 3	53 11 100 11		1063.82 535.59	2+ 2+
2747 5	J L	4+
2791.3 5	R			944.1 5	100		1847.17	6+
2807 5	F J K L	(4+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2822.21 11	I J L	2+		1358.3 1 ?	100		1463.93	2+
2838 5	F J K P
2843.2 4	Q R	(7-)		503.2 5 996.3 5	100 14 88 8		2339.8 1847.17	(5-) 6+
2858 5	F J K L	(3-)
2901 5	J K	4+
2901.05 10	G	(1)	0.32 ps 4	2901.0 1	100	(D)	0.0	0+
2905.75 10	G	(1)	0.37 ps 4	2905.7 1	100	(D)	0.0	0+
2924 5	J L	4+
2928.7 5	R	(7-)		588.8 5	100		2339.8	(5-)
2934.8 10	A F J	(4+)		1871 1	100		1063.82	2+
2961.2 3	I J L	2+		1897.4 3 ?	100		1063.82	2+
2970.1 4	A F I K	4+		1362.5 10 1906.6 5 2434.1 5	7 5 28 10 100 8		1607.37 1063.82 535.59	(3+) 2+ 2+
2984 5	J L	(6+)
2996.31 21	I J L	(4+,3-)		1532.4 2 ?	100		1463.93	2+
3004.4 10	A F I J L	(4+,3-)		1397 1	100		1607.37	(3+)
3021 5	J K	(4+)
3039.4 10	A F K	(4+)		1432 1	100		1607.37	(3+)
3041 5	J L	(5-)
3042.2 6 ?	I			1978.4 6 ?	100		1063.82	2+
3053.70 21	F I	(LE 4)		1989.9 2 ?	100		1063.82	2+
3062.60 25	A F	(0+,1,2)		1598.7 3 2526.9 4	62 15 100 15		1463.93 535.59	2+ 2+
3066.25 20	G	(1)	0.207 ps 19	3066.2 2	100		0.0	0+
3068 5	J L	(5-)
3070.2 4	A	(0+,1,2)		2534.6 4	100		535.59	2+
3085 5	F J K L	(4+)
3112 5	F J K L	(3-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3129.6 4	A	(0+,1,2)		1665.7 4	100		1463.93	2+
3140 5	J L	(1-)
3143.0 8	R			351.7 5	100		2791.3
3154 5	F J K L	(3-)
3172 5	J L	(3-)
3190 5	J K L	(4+)
3198.4 4	G	(1)	0.23 ps 4	3198.3 4	100	(D)	0.0	0+
3217 5	J	(1-)
3237 5	F J K L	(3-)
3242.76 10	G	1	0.138 ps 7	3242.7 1	100	D	0.0	0+
3265 5	J L	(3-)
3282 5	F J K L	(3-)
3290.27 9	G	1(+)	43 fs 6	2595.3 3 2755.4 3 3290.1 1	21 6 21 4 100 6	(D) (D) D	695.13 535.59 0.0	0+ 2+ 0+
3294 5	F J L	(2+)
3299.2 6	R	(9-)		370.5 5 456.1 5	66 13 100 17		2928.7 2843.2	(7-) (7-)
3311 5	J L
3324 5	F J L
3342.06 10	G	(1)	0.175 ps 20	3342.0 1	100	(D)	0.0	0+
3354 15	F	(2+)
3367.0 8	E N Q R	(10+)		739.5 5	100		2627.5	8+
3376 5	J	(3-)
3406 5	F J K L	(4+)
3437 5	J	(5-)
3448 5	F J L	(0+)
3468 5	J L	(2+)
3479 5	F J L	(2+)
3483.82 7	G	(1+)	8.3 fs 8	2419.8 1 2948.2 1 3483.9 1	11.1 12 12.4 12 100.0 20	(D)	1063.82 535.59 0.0	2+ 2+ 0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3529 5	J	(3-)
3537 5	J L	(2+)
3557 5	F J L	(3-)
3557 15	F	(2+)
3570.77 10	G	(1)	18.9 fs 15	3570.7 1	100	(D)	0.0	0+
3586 5	J L
3595 5	J L	(3-)
3599.87 20	G	(1)	0.18 ps 3	3599.8 2	100		0.0	0+
3606 5	F J K L	(4+)
3615.57 20	G	1	56 fs 6	3615.5 2	100	D	0.0	0+
3626.5 5	B J L	(4+,5,6)		1779.3 5	100		1847.17	6+
3627.3 3	G	(1)	32 fs 3	3627.2 3	100	(D)	0.0	0+
3647.3 6	B F J L	(5-)		1800.1 6	100		1847.17	6+
3658.96 22	G	1(+)	18 fs 3	2595.3 3 3658.7 3	20 5 100 5	D D	1063.82 0.0	2+ 0+
3682 5	F J K L	(5-)
3718 5	J	(4+)
3726 5	J L	(3-)
3743 5	J	(4+)
3747 5	J L	(5-)
3773 5	F J L	(3-)
3783.5 9	R			640.5 5	100		3143.0
3797 5	J	(4+)
3810 5	J L	(4+)
3823 5	J L	(5-)
3887.98 10	G	1		3887.9 1		D	0.0	0+
3894 5	J L
3896.68 10	G	(1)		3896.6 1		(D)	0.0	0+
3915 5	J L
3925 5	J L	(2+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3925.98 10	G	(1)		3925.9 1		(D)	0.0	0+
3947 5	J L
4026 5	J L	(3-)
4032.7 8	R	(11-)		733.5 5	100		3299.2	(9-)
4043 5	J L	(4+)
4062.6 9	E N Q R	(12+)		695.6 5	100		3367.0	(10+)
4081.59 10	G	1		4081.5 1		D	0.0	0+
4156.5 3	G	1		4156.4 3		D	0.0	0+
4158 5	L	(3-)
4205 5	J L	(2+)
4217.60 10	G	1		4217.5 1		D	0.0	0+
4232.10 20	G	(1)		4232.0 2		(D)	0.0	0+
4243 5	J L
4260 5	L	(3-)
4329.90 20	G	1		4329.8 2		D	0.0	0+
4516.81 10	G	1		4516.7 1		D	0.0	0+
4565.51 10	G	1		4565.4 1		D	0.0	0+
4583.11 10	G	1		4583.0 1		D	0.0	0+
4594.91 10	G	1		4594.8 1		D	0.0	0+
4689.02 10	G	1		4688.9 1		D	0.0	0+
4730.32 20	G	1		4730.2 2		D	0.0	0+
4875.2 10	N Q R	(14+)		812.6 5	100		4062.6	(12+)
4939.8 9	R	(13-)		907.1 5	100		4032.7	(11-)
4989.63 20	G	1		4989.5 2		D	0.0	0+
5007.33 20	G	1		5007.2 2		D	0.0	0+
5034.54 20	G	1		5034.4 2		D	0.0	0+
5062.9 3	G	(2)		5062.8 3		(Q)	0.0	0+
5071.24 20	G	(1)		5071.1 2		(D)	0.0	0+
5101.3 6	G	1		5101.2 6		D	0.0	0+
5109.3 9	G	(1)		5109.2 9		(D)	0.0	0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5136.04 10	G	(1)		5135.9 1		(D)	0.0	0+
5158.3 3	G	1		5158.2 3		D	0.0	0+
5169.6 3	G	1		5169.5 3		D	0.0	0+
5181.8 3	G	1		5181.7 3		D	0.0	0+
5186.9 15	G	1		4651 2 5187 2	84 13 100 15	D	535.59 0.0	2+ 0+
5190.4 5	G	1		5190.3 5		D	0.0	0+
5204.6 4	G	(1)		5204.5 4		(D)	0.0	0+
5216.0 8	G	(1)		5215.9 8		(D)	0.0	0+
5271.2 6	G	1		5271.1 6		D	0.0	0+
5277.6 3	G	1		5277.5 3		D	0.0	0+
5310.5 4	G	1		5310.3 4		D	0.0	0+
5335.65 20	G	1		5335.5 2		D	0.0	0+
5347.85 10	G	1		5347.7 1		D	0.0	0+
5359.8 3	G	1		5359.6 3		D	0.0	0+
5369.6 6	G	1		5369.4 6		D	0.0	0+
5382.5 10	G	1		5382.3 10		D	0.0	0+
5390.3 6	G	1		5390.1 6		D	0.0	0+
5402.26 10	G	1		5402.1 1		D	0.0	0+
5412.6 8	G	1		5412.4 8		D	0.0	0+
5435.5 6	G	1		5435.3 6		D	0.0	0+
5442.9 6	G	1		5442.7 6		D	0.0	0+
5449.6 6	G	(1)		5449.4 6		(D)	0.0	0+
5502.7 4	G	1		5502.5 4		D	0.0	0+
5519.4 4	G	1		5519.2 4		D	0.0	0+
5532.2 5	G	1		5532.0 5		D	0.0	0+
5547.9 3	G	1		5547.7 3		D	0.0	0+
5554.4 11	G	1		5554.2 11		D	0.0	0+
5584.9 4	G	1		5584.7 4		D	0.0	0+
5596.8 7	G	1		5596.6 7		D	0.0	0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5604.7 12	G	1		5604.5 12		D	0.0	0+
5612.67 10	G	1		5612.5 1		D	0.0	0+
5618.6 3	G	1		5618.4 3		D	0.0	0+
5656.5 5	G	(2)		5656.3 5		(Q)	0.0	0+
5670.67 10	G	1		5670.5 1		D	0.0	0+
5680.9 7	G	(1)		5680.7 7		(D)	0.0	0+
5686.5 5	G	1		5686.3 5		D	0.0	0+
5715.9 3	G	1		5715.7 3		D	0.0	0+
5725.3 3	G	1		5725.1 3		D	0.0	0+
5732.9 3	G	1		5732.7 3		D	0.0	0+
5742.6 7	G	1		5742.4 7		D	0.0	0+
5764.0 15	G	(1)		5763.8 15		(D)	0.0	0+
5770.4 4	G	1		5770.2 4		D	0.0	0+
5798.2 3	G	1		5798.0 3		D	0.0	0+
5808.98 10	G	1		5808.8 1		D	0.0	0+
5826.5 6	G	(2)		5826.3 6		(Q)	0.0	0+
5840.2 15	N R	(16+)		965 1	100		4875.2	(14+)
5840.7 6	G	1		5840.5 6		D	0.0	0+
5879.39 20	G	1		5879.2 2		D	0.0	0+
5901.0 6	G	1		5900.8 6		D	0.0	0+
5947.79 20	G	1		5947.6 2		D	0.0	0+
5957.2 6	G	1		5957.0 6		D	0.0	0+
5964.0 6	G	1		5963.8 6		D	0.0	0+
5972.99 20	G	1		5972.8 2		D	0.0	0+
5988.9 4	G	1		5988.7 4		D	0.0	0+
6009.6 4	G	1		6009.4 4		D	0.0	0+
6019.5 11	G	(1)		6019.3 11		(D)	0.0	0+
6035.5 8	G	1		6035.3 8		D	0.0	0+
6061.3 9	G	(2)		6061.1 9		(Q)	0.0	0+
6065.9 7	G	1		6065.7 7		D	0.0	0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6082.9 3	G	1		6082.7 3		D	0.0	0+
6089.3 4	G	1		6089.1 4		D	0.0	0+
6122.5 5	G	1		6122.3 5		D	0.0	0+
6133.6 7	G	1		6133.4 7		D	0.0	0+
6147.1 9	G	1		6146.9 9		D	0.0	0+
6174.0 5	G	1		6173.8 5		D	0.0	0+
6194.51 10	G	(1)		6194.3 1		(D)	0.0	0+
6249.4 5	G	1		6249.2 5		D	0.0	0+
6257.61 20	G	1		6257.4 2		D	0.0	0+
6270.5 8	G	1		6270.3 8		D	0.0	0+
6278.71 10	G	1		6278.5 1		D	0.0	0+
6293.1 4	G	1		6292.9 4		D	0.0	0+
6310.3 15	G	(1)		6310.1 15		(D)	0.0	0+
6321.2 9	G	1		6321.0 9		D	0.0	0+
6327.6 9	G	1		6327.4 9		D	0.0	0+
6337.5 4	G	1		6337.3 4		D	0.0	0+
6354.32 20	G	1		6354.1 2		D	0.0	0+
6365.6 19	G	(1)		6365.4 19		(D)	0.0	0+
6375.6 5	G	1		6375.4 5		D	0.0	0+
6402.0 8	G	1		6401.8 8		D	0.0	0+
6414.3 4	G	1		6414.1 4		D	0.0	0+
6419.4 18	G	1-	9 fs 6	3788 4 ? 4385 4 4444 4 ? 5355 4 5723 4 5883 4 6418 4	7 2 19 4 6 2 11 3 0.8 4 1.2 6 100 15	(E1+M2) E1	2632.4 2037.60 1977.34 1063.82 695.13 535.59 0.0	(1) 0+ (1,2+) 2+ 0+ 2+ 0+
6421.4 6	G	1		6421.2 6		D	0.0	0+
6426.6 9	G	(1)		6426.4 9		(D)	0.0	0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6434.1 5	G	1		6433.9 5		D	0.0	0+
6459.0 6	G	1		6458.8 6		D	0.0	0+
6473.5 6	G	1		6473.3 6		D	0.0	0+
6483.2 20	G	(1)		6483 2		(D)	0.0	0+
6497.6 6	G	1		6497.4 6		D	0.0	0+
6518.5 13	G	1-	2.5 fs 14	3445 3 ? 4477 3 5055 3 5455 3 5823 3 5982 3 6517 3	18 3 23 5 28 5 8 2 10 2 32 5 100 15	E1	3066.25 2042.78 1463.93 1063.82 695.13 535.59 0.0	(1) (2)+ 2+ 2+ 0+ 2+ 0+
6519.1 5	G	1		6518.9 5		D	0.0	0+
6526.6 3	G	1		6526.4 3		D	0.0	0+
6570.2 4	G	1		6570.0 4		D	0.0	0+
6597.0 4	G	(2)		6596.8 4		(Q)	0.0	0+
6622.3 4	G	(1)		6622.1 4		(D)	0.0	0+
6628.3 5	G	(2)		6628.1 5		(Q)	0.0	0+
6641.0 3	G	1		6640.8 3		D	0.0	0+
6658.2 4	G	1		6658.0 4		D	0.0	0+
6669.14 20	G	1		6668.9 2		D	0.0	0+
6685.3 4	G	1		6685.1 4		D	0.0	0+
6764.1 8	G	1		6763.9 8		D	0.0	0+
6772.7 8	G	1		6772.5 8		D	0.0	0+
6790.6 10	G	1		6790.4 10		D	0.0	0+
6797.5 9	G	(1)		6797.3 9		(D)	0.0	0+
6807.9 10	G	(2)		6807.7 10		(Q)	0.0	0+
6829.5 3	G	(1)		6829.2 3		(D)	0.0	0+
6844.6 11	G	(2)		6844.3 11		(Q)	0.0	0+
6851.3 15	G	1		6851.0 15		D	0.0	0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6870.0 8	G	(1)		6869.7 8		(D)	0.0	0+
6886.5 8	G	1		6886.2 8		D	0.0	0+
6893.2 4	G	1		6892.9 4		D	0.0	0+
6906.1 6	G	1		6905.8 6		D	0.0	0+
6912.9 11	G	(1)		6912.6 11		(D)	0.0	0+
6919.5 13	G	1		6919.2 13		D	0.0	0+
6924.9 10	G	(1)		6924.6 10		(D)	0.0	0+
6934.2 12	G	(1)		6933.9 12		(D)	0.0	0+
6949.2 18	N	(18+)		1109 1	100		5840.2	(16+)
6949.9 11	G	1		6949.6 11		D	0.0	0+
6957.7 11	G	(2)		6957.4 11		(Q)	0.0	0+
6974.2 8	G	1		6973.9 8		D	0.0	0+
6981.1 12	G	(2)		6980.8 12		(Q)	0.0	0+
6994.5 5	G	(2)		6994.2 5		(Q)	0.0	0+
7001.2 5	G	1		7000.9 5		D	0.0	0+
7018.3 6	G	1		7018.0 6		D	0.0	0+
7032.1 5	G	1		7031.8 5		D	0.0	0+
7037.8 10	G	(1)		7037.5 10		(D)	0.0	0+
7060.2 11	G	1		7059.9 11		D	0.0	0+
7068.1 3	G	1		7067.8 3		D	0.0	0+
7095.4 5	G	1		7095.1 5		D	0.0	0+
7103.5 7	G	(1)		7103.2 7		(D)	0.0	0+
7115.3 3	G	1		7115.0 3		D	0.0	0+
7136.6 5	G	1		7136.3 5		D	0.0	0+
7171.7 7	G	(1)		7171.4 7		(D)	0.0	0+
7181.5 9	G	(1)		7181.2 9		(D)	0.0	0+
7194.4 3	G	1		7194.1 3		D	0.0	0+
7204.0 7	G	1		7203.7 7		D	0.0	0+
7219.4 9	G	(2)		7219.1 9		(Q)	0.0	0+
7225.4 13	G	(1)		7225.1 13		(D)	0.0	0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7299.6 5	G	1		7299.3 5		D	0.0	0+
7312.3 3	G	1		7312.0 3		D	0.0	0+
7330.8 3	G	1		7330.5 3		D	0.0	0+
7357.7 6	G	1		7357.4 6		D	0.0	0+
7380.3 7	G	(1)		7380.0 7		(D)	0.0	0+
7403.3 8	G	1		7403.0 8		D	0.0	0+
7450.6 10	G	1		7450.3 10		D	0.0	0+
7471.0 4	G	1		7470.7 4		D	0.0	0+
7487.2 7	G	1		7486.9 7		D	0.0	0+
7494.8 11	G	(1)		7494.5 11		(D)	0.0	0+
7503.5 12	G	(2)		7503.2 12		(Q)	0.0	0+
7526.1 6	G	1		7525.8 6		D	0.0	0+
7546.3 20	G	1		7546 2		D	0.0	0+
7559.1 15	G	(1)		7558.8 15		(D)	0.0	0+
7577.2 9	G	1		7576.9 9		D	0.0	0+
7606.9 4	G	1		7606.6 4		D	0.0	0+
7638.6 10	G	1-	3.3 fs 9	4569 4 ? 5007 2 ? 5597 4 5604 4 6176 2 6574 2 7102 2 7637 2	4 1 6 2 5 1 5 1 4 1 15 3 101 15 100 15	(E1+M2) E1	3066.25 2632.4 2042.78 2037.60 1463.93 1063.82 535.59 0.0	(1) (1) (2)+ 0+ 2+ 2+ 2+ 0+
7744.5 8	G	1		7744.2 8		D	0.0	0+
7758.4 10	G	(1)		7758.1 10		(D)	0.0	0+
7771.5 12	G	1		7771.2 12		D	0.0	0+
7796.9 14	G	1		7796.6 14		D	0.0	0+
7831.2 8	G	1		7830.9 8		D	0.0	0+
7863.1 7	G	(1)		7862.8 7		(D)	0.0	0+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7875.4 6	G	1		7875.1 6		D	0.0	0+
7887.2 10	G	1		7886.9 10		D	0.0	0+
7935.7 10	G	1		7935.4 10		D	0.0	0+
7955.7 6	G	1		7955.4 6		D	0.0	0+
7988.0 7	G	1		7987.7 7		D	0.0	0+
8002.0 6	G	1		8001.7 6		D	0.0	0+
8033.5 8	G	1		8033.2 8		D	0.0	0+
8052.2 6	G	1		8051.9 6		D	0.0	0+
8063.7 9	G	1		8063.4 9		D	0.0	0+
8083.3 16	G	1		8082.9 16		D	0.0	0+
8095.9 11	G	1		8095.5 11		D	0.0	0+
8108.1 12	G	1		8107.7 12		D	0.0	0+
8114.2 20	N	(20+)		1165 1	100		6949.2	(18+)
8127.7 10	G	1		8127.3 10		D	0.0	0+
8194.4 9	G	1		8194.0 9		D	0.0	0+
8208.8 6	G	1		8208.4 6		D	0.0	0+
8218.2 6	G	(1)		8217.8 6		(D)	0.0	0+
8238.6 9	G	1		8238.2 9		D	0.0	0+
8257.1 14	G	1		8256.7 14		D	0.0	0+
8269.6 6	G	1		8269.2 6		D	0.0	0+
8283.6 6	G	1		8283.2 6		D	0.0	0+
8294.5 13	G	(1)		8294.1 13		(D)	0.0	0+
13.0E3 3	K	1-	11.6 MeV 12
13.2E3 4	K	0+	2.6 MeV 6
13.60E3 26	K	2+	4.75 MeV 38
16.8E3 4	K	0+	2.5 MeV 5
21.5E3 4	K	3-	3.7 MeV 3
30.1E3 7	K	1-	12.5 MeV 38

E(level): From least-squares fit to Eγ data, for levels seen in γ-ray studies. In other cases weighted averages of available values

J^π(level): Above≈3 MeV excitation, the assignments are generally from L(p,p’), L(d,d’) or L(α,α’). These assignments are given in parentheses due to tentative level associations (in different reactions) and some possibility of S=1 transfer in (p,p’) and (d,d’) at higher excitation energies.

T_1/2(level): For excited states, values are from recoil-distance Doppler-shift (RDDS) method and/or B(E2) values determined from excitation yields in Coulomb excitation unless otherwise stated. For levels populated in (γ,γ’), level half-lives are deduced (by evaluators) from total widths given in different experiments.

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - Jπ=0⁺ band.
0.0	0+	7.01×10⁺¹⁸ y +21-17 % 2β^- = 100
535.59 4	2+	12.4 ps 3	535.61 6	100	E2	0.0	0+
1136.02 4	4+	3.8 ps 3	600.40 2	100	(E2)	535.59	2+
1847.17 8	6+	1.20 ps 17	711.15 6	100	(E2)	1136.02	4+
2627.5 5	8+	0.58 ps 9	780.3 5	100	(E2)	1847.17	6+
3367.0 8	(10+)		739.5 5	100		2627.5	8+
4062.6 9	(12+)		695.6 5	100		3367.0	(10+)
4875.2 10	(14+)		812.6 5	100		4062.6	(12+)
5840.2 15	(16+)		965 1	100		4875.2	(14+)
6949.2 18	(18+)		1109 1	100		5840.2	(16+)
8114.2 20	(20+)		1165 1	100		6949.2	(18+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - 3- octupole band
1908.19 6	3-	14 ps 3
2339.8 4	(5-)		431.5 5 1203.6 5	100 14 82 9		1908.19 1136.02	3- 4+
2843.2 4	(7-)		503.2 5 996.3 5	100 14 88 8		2339.8 1847.17	(5-) 6+
3299.2 6	(9-)		370.5 5 456.1 5	66 13 100 17		2928.7 2843.2	(7-) (7-)
4032.7 8	(11-)		733.5 5	100		3299.2	(9-)
4939.8 9	(13-)		907.1 5	100		4032.7	(11-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - Possible Kπ=2⁺, γ band.
1063.82 4	2+	6.6 ps 6
1607.37 5	(3+)		471.37 9 543.58 8 1071.77 3	17 2 100 7 74 1		1136.02 1063.82 535.59	4+ 2+ 2+
2310.12 20	(4+)		538.6 4 702.7 3 1246.4 3	27 9 100 14 48 7		1771.44 1607.37 1063.82	(4+) (3+) 2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - Possible Kπ=0⁺ band.
695.13 4	0+	1.62 ns 4
1463.93 5	2+	2.9 ps 7	327 1 400.17 9 768.77 3 928.34 3	3.5 15 5.2 7 100.0 10 72.9 9	[E2] E2 M1+E2	1136.02 1063.82 695.13 535.59	4+ 2+ 0+ 2+

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
535.59	2+	12.4 ps 3	535.61 6	E2		0.004	B(E2)(W.u.)=37.6 9, α=0.004
695.13	0+	1.62 ns 4	159.547 13	E2		0.223	B(E2)(W.u.)=89 3, α=0.223
1063.82	2+	6.6 ps 6	369.1 1	[E2]		0.0122	B(E2)(W.u.)=5.7 +14-11, α=0.0122
	2+	6.6 ps 6	528.248 18	E2+M1	+4.4 +15-9	0.004	B(E2)(W.u.)=52 7, B(M1)(W.u.)=0.0008 +6-4, α=0.004
	2+	6.6 ps 6	1063.78 5	E2			B(E2)(W.u.)=0.62 6
1136.02	4+	3.8 ps 3	600.40 2	(E2)		0.003	B(E2)(W.u.)=69 6, α=0.003
1463.93	2+	2.9 ps 7	327 1	[E2]		0.0181	B(E2)(W.u.)=36 +34-20, α=0.0181 4
	2+	2.9 ps 7	768.77 3	E2			B(E2)(W.u.)=15 +5-3
	2+	2.9 ps 7	928.34 3	M1+E2	-0.27 2		B(E2)(W.u.)=0.28 +15-9, B(M1)(W.u.)=0.0036 +13-8
1771.44	(4+)	2.5 ps 4	707.68 3	(E2)			B(E2)(W.u.)=30 +7-5
1847.17	6+	1.20 ps 17	711.15 6	(E2)			B(E2)(W.u.)=94 +16-12
1908.19	3-	14 ps 3	844.37 4	[E1]			B(E1)(W.u.)=2.5E-5 +8-5
	3-	14 ps 3	1372.1 7	[E1]			B(E1)(W.u.)=2.7E-6 +10-6
	3-	14 ps 3	1908.2 5	[E3]			B(E3)(W.u.)=48 +29-18
2086.33	0+		622.5 2	(E2)		0.003	α=0.003
2416.58	(4+)		1280.7 3	(M1+E2)	-0.7 +10-13
2627.5	8+	0.58 ps 9	780.3 5	(E2)			B(E2)(W.u.)=122 +23-17
6419.4	1-	9 fs 6	5355 4	(E1+M2)	+0.21 12		B(E1)(W.u.)=1.7E-6 +60-11
6419.4	1-	9 fs 6	6418 4	E1			B(E1)(W.u.)=9E-5 +22-4
6518.5	1-	2.5 fs 14	6517 3	E1			B(E1)(W.u.)=21E-5 +35-10
7638.6	1-	3.3 fs 9	7102 2	(E1+M2)	-0.06 2		B(E1)(W.u.)=11E-5 +7-4, B(M2)(W.u.)=0.04 +7-3
7638.6	1-	3.3 fs 9	7637 2	E1			B(E1)(W.u.)=9E-5 +6-3

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	0+	7.01×10⁺¹⁸ y +21-17 % 2β^- = 100	From experimental studies of one-neutron removal reactions (d,p), (p,d), (³He,α) and proton removing reaction (³He,d) on ¹⁰⁰Mo target, 2017Fr08 deduced following values of neutron and proton vacancies in the g.s. of ¹⁰⁰Mo: 0.33 2 for ν2s_1/2, 3.40 7 for ν1d, 2.48 19 for ν0g_7/2, 1.89 13 for ν0h_11/2, 1.49 7 for π1p, 0.47 2 for π0f_5/2 and 5.94 30 for π0g_9/2 orbitals, with a total vacancy of 8.09 29 for neutrons and 7.89 31 for protons, compared with expected value of 8 for each. E(level): From experimental studies of one-neutron removal reactions (d,p), (p,d), (³He,α) and proton removing reaction (³He,d) on ¹⁰⁰Mo target, 2017Fr08 deduced following values of neutron and proton vacancies in the g.s. of ¹⁰⁰Mo: 0.33 2 for ν2s_1/2, 3.40 7 for ν1d, 2.48 19 for ν0g_7/2, 1.89 13 for ν0h_11/2, 1.49 7 for π1p, 0.47 2 for π0f_5/2 and 5.94 30 for π0g_9/2 orbitals, with a total vacancy of 8.09 29 for neutrons and 7.89 31 for protons, compared with expected value of 8 for each. Jπ=0⁺ band.
535.59	2+	12.4 ps 3	μ=+0.94 7 (2001Ma17,2014StZZ), Q=-0.25 7 (2011Wr01,2016St14) β₂=0.20 (from (p,p’) and (α,α’)). E(level): Jπ=0⁺ band.
695.13	0+	1.62 ns 4	E(level): Possible Kπ=0⁺ band.
1063.82	2+	6.6 ps 6	β₂=0.037 (from (p,p’) and (α,α’)). E(level): Placement considered uncertain by evaluators since no such transition is reported in ¹⁰⁰Nb β^- decay. Possible Kπ=2⁺, γ band.
1136.02	4+	3.8 ps 3	β₄=-0.027 (from (p,p’)). B(E4)(W.u.)=0.99 21 (from (p,p’) and (d,d’) 1992Pi08). E(level): Jπ=0⁺ band.
1463.93	2+	2.9 ps 7	E(level): Possible Kπ=0⁺ band.
1504.66	0+		XREF: J(1510)L(1510).
1607.37	(3+)		XREF: J(?). E(level): Placement considered uncertain by evaluators since no such transition is reported in ¹⁰⁰Nb β^- decay. Possible Kπ=2⁺, γ band.
1766.52	(2+)		XREF: J(1770).
1847.17	6+	1.20 ps 17	XREF: I(?). E(level): Jπ=0⁺ band. J^π(level): Member of g.s. band from γ cascade in (⁷Li,p2nγ), ¹⁰⁰Mo(¹³⁶Xe,Xγ), ¹¹⁰Pd(⁸⁶Kr,Xγ) and ¹⁶⁸Er(³⁰Si,Xγ).
1908.19	3-	14 ps 3	β₃=0.17 ((p,p’) and (α,α’)). E(level): 3- octupole band.
1977.34	(1,2+)		XREF: γ(?).
2037.60	0+		XREF: F(2035)γ(2033)I(?)J(2040).
2042.78	(2)+		XREF: γ(2040)J(2046).
2082			XREF: F(2082)H(2100)J(2070?).
2103.13	4+		XREF: K(2121).
2189.56	(0+,1,2)		XREF: I(?)J(2192?).
2201.22	(2-)		XREF: J(2200).
2310.12	(4+)		E(level): Placement considered uncertain by evaluators since no such transition is reported in ¹⁰⁰Nb β^- decay. Possible Kπ=2⁺, γ band.
2320.3	(0+,1,2)		XREF: F(2312).
2339.8	(5-)		XREF: F(2334)H(2330)K(2330). E(level): 3- octupole band.
2397.0	(1-)		XREF: F(2392)I(?)K(2384).
2432	1-		XREF: K(2444).
2607	(4+,5-)		XREF: F(2602)p(2600).
2627.5	8+	0.58 ps 9	E(level): Jπ=0⁺ band. J^π(level): Member of g.s. band from γ cascade in (⁷Li,p2nγ), ¹⁰⁰Mo(¹³⁶Xe,Xγ), ¹¹⁰Pd(⁸⁶Kr,Xγ) and ¹⁶⁸Er(³⁰Si,Xγ).
E(level)	J^π(level)	T_1/2(level)	Comments
2632.4	(1)	0.51 ps 10	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
2659	(1-)		XREF: F(2652)K(2656).
2738.02	(2+)		XREF: K(2707)p(2730).
2807	(4+)		XREF: F(2803)K(2790).
2822.21	2+		XREF: I(?).
2838			XREF: F(2835)J(?)K(2852)p(2830).
2843.2	(7-)		E(level): 3- octupole band.
2858	(3-)		XREF: F(2873)K(2869).
2901	4+		XREF: K(2882).
2901.05	(1)	0.32 ps 4	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
2905.75	(1)	0.37 ps 4	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
2934.8	(4+)		XREF: F(2923).
2961.2	2+		XREF: I(?).
2970.1	4+		XREF: I(?)K(2970).
2996.31	(4+,3-)		XREF: I(?).
3004.4	(4+,3-)		XREF: F(2994)I(?).
3021	(4+)		XREF: K(3029).
3039.4	(4+)		XREF: F(3039)K(3041).
3053.70	(LE 4)		XREF: I(?). E(level): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ). J^π(level): γ to 2⁺.
3066.25	(1)	0.207 ps 19	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3085	(4+)		XREF: F(3106)K(3085).
3112	(3-)		XREF: F(3119)K(3114).
3154	(3-)		XREF: F(3148)K(3153).
3190	(4+)		XREF: K(3196).
3198.4	(1)	0.23 ps 4	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
3237	(3-)		XREF: F(3235)K(3216).
3242.76	1	0.138 ps 7	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3282	(3-)		XREF: F(3263)K(3276).
3290.27	1(+)	43 fs 6	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3294	(2+)		XREF: F(3282).
3299.2	(9-)		E(level): 3- octupole band.
3324			XREF: F(3306).
3342.06	(1)	0.175 ps 20	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3367.0	(10+)		E(level): Jπ=0⁺ band. J^π(level): Member of g.s. band from γ cascade in (⁷Li,p2nγ), ¹⁰⁰Mo(¹³⁶Xe,Xγ), ¹¹⁰Pd(⁸⁶Kr,Xγ) and ¹⁶⁸Er(³⁰Si,Xγ).
3406	(4+)		XREF: F(3409)K(3398).
3448	(0+)		XREF: F(3445).
3479	(2+)		XREF: F(3475).
3483.82	(1+)	8.3 fs 8	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3557	(3-)		XREF: F(3535).
3570.77	(1)	18.9 fs 15	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3599.87	(1)	0.18 ps 3	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3606	(4+)		XREF: F(3587)K(3603).
3615.57	1	56 fs 6	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3627.3	(1)	32 fs 3	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3647.3	(5-)		XREF: J(3652)L(3652).
3658.96	1(+)	18 fs 3	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3682	(5-)		XREF: F(3674)K(3701).
3773	(3-)		XREF: F(3771).
3887.98	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
3896.68	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
3925.98	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4032.7	(11-)		E(level): 3- octupole band.
4062.6	(12+)		E(level): Jπ=0⁺ band. J^π(level): Member of g.s. band from γ cascade in (⁷Li,p2nγ), ¹⁰⁰Mo(¹³⁶Xe,Xγ), ¹¹⁰Pd(⁸⁶Kr,Xγ) and ¹⁶⁸Er(³⁰Si,Xγ).
4081.59	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4156.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4217.60	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4232.10	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4329.90	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4516.81	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4565.51	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4583.11	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4594.91	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4689.02	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4730.32	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
4875.2	(14+)		E(level): Jπ=0⁺ band. J^π(level): Member of g.s. band from γ cascade in (⁷Li,p2nγ), ¹⁰⁰Mo(¹³⁶Xe,Xγ), ¹¹⁰Pd(⁸⁶Kr,Xγ) and ¹⁶⁸Er(³⁰Si,Xγ).
4939.8	(13-)		E(level): 3- octupole band.
4989.63	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5007.33	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5034.54	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5062.9	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5071.24	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5101.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5109.3	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5136.04	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5158.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
5169.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5181.8	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5190.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5204.6	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5216.0	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5271.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5277.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5310.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5335.65	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5347.85	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5359.8	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5369.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5382.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5390.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5402.26	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5412.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5435.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5442.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5449.6	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5502.7	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5519.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5532.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5547.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5554.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5584.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
5596.8	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5604.7	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5612.67	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5618.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5656.5	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5670.67	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5680.9	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5686.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5715.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5725.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5732.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5742.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5764.0	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5770.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5798.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5808.98	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5826.5	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5840.2	(16+)		E(level): Jπ=0⁺ band. J^π(level): Member of g.s. band from γ cascade in (⁷Li,p2nγ), ¹⁰⁰Mo(¹³⁶Xe,Xγ), ¹¹⁰Pd(⁸⁶Kr,Xγ) and ¹⁶⁸Er(³⁰Si,Xγ).
5840.7	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5879.39	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5901.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5947.79	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5957.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5964.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
5972.99	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
5988.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6009.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6019.5	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6035.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6061.3	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6065.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6082.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6089.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6122.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6133.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6147.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6174.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6194.51	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6249.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6257.61	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6270.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6278.71	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6293.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6310.3	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6321.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6327.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6337.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6354.32	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6365.6	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6375.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
6402.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6414.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6419.4	1-	9 fs 6	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6421.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6426.6	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6434.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6459.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6473.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6483.2	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6497.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6518.5	1-	2.5 fs 14	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6519.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6526.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6570.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6597.0	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6622.3	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6628.3	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6641.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6658.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6669.14	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6685.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6764.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6772.7	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6790.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6797.5	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
6807.9	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6829.5	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6844.6	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6851.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6870.0	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6886.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6893.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6906.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6912.9	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6919.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6924.9	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6934.2	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6949.2	(18+)		E(level): Jπ=0⁺ band. J^π(level): Member of g.s. band from γ cascade in (⁷Li,p2nγ), ¹⁰⁰Mo(¹³⁶Xe,Xγ), ¹¹⁰Pd(⁸⁶Kr,Xγ) and ¹⁶⁸Er(³⁰Si,Xγ).
6949.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6957.7	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6974.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6981.1	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
6994.5	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7001.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7018.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7032.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7037.8	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7060.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7068.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7095.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
7103.5	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7115.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7136.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7171.7	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7181.5	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7194.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7204.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7219.4	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7225.4	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7299.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7312.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7330.8	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7357.7	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7380.3	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7403.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7450.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7471.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7487.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7494.8	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7503.5	(2)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7526.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7546.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7559.1	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7577.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7606.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
7638.6	1-	3.3 fs 9	J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7744.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7758.4	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7771.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7796.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7831.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7863.1	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7875.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7887.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7935.7	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7955.7	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
7988.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8002.0	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8033.5	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8052.2	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8063.7	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8083.3	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8095.9	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8108.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8114.2	(20+)		E(level): Jπ=0⁺ band. J^π(level): Member of g.s. band from γ cascade in (⁷Li,p2nγ), ¹⁰⁰Mo(¹³⁶Xe,Xγ), ¹¹⁰Pd(⁸⁶Kr,Xγ) and ¹⁶⁸Er(³⁰Si,Xγ).
8127.7	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8194.4	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8208.8	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8218.2	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8238.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
E(level)	J^π(level)	T_1/2(level)	Comments
8257.1	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8269.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8283.6	1		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
8294.5	(1)		J^π(level): Dipole γ to g.s. from γ(θ) measurements in (γ,γ’). Also in (γ,γ’) nuclear resonance fluorescence reaction from 0⁺ g.s., main population is expected via dipole (E1 or M1) transitions to J=1 states, through scissors mode (for M1) and pygmy dipole resonances (for E1).
13.0E3	1-	11.6 MeV 12	%E1 EWSR=18 3 for ISGDR in (α,α’) (2015Yo04).
13.2E3	0+	2.6 MeV 6	%E0 EWSR=32 4 for ISGMR in (α,α’) (2020Ho11).
13.60E3	2+	4.75 MeV 38	%E2 EWSR=79 14 for ISGQR in (α,α’) (2015Yo04).
16.8E3	0+	2.5 MeV 5	%E0 EWSR=60 3 for ISGMR in (α,α’) (2020Ho11).
21.5E3	3-	3.7 MeV 3	%E3 EWSR=53 7 for ISGOR in (α,α’) (2015Yo04).
30.1E3	1-	12.5 MeV 38	%E1 EWSR=47 10 for ISGDR in (α,α’) (2015Yo04).

E(level)	E(gamma)	Comments
535.59	535.61	E(γ): unweighted average 535.666 14 from ¹⁰⁰Nb β^- decay and 535.547 13 from (n,n’γ). Others: 535.3 5 in (t,pγ), 535.6 5 in (³⁰Si,Xγ), 536 1 in (¹³⁶Xe,Xγ). M(γ): ΔJ=2, Q from γ(θ) in (n,n’γ); M2 ruled out by RUL
695.13	159.547	E(γ): from (n,n’γ). Others: 159.5 1 in ¹⁰⁰Nb β^- decay, 159.1 5 in (t,pγ) I(γ): from Coulomb excitation. M(γ): ΔJπ and T_1/2_1/2(level) are consistent with only E2, not M2.
695.13	695.1	E(γ): from level energy difference. Transition observed only in ce data
1063.82	369.1	E(γ): weighted average of 368.6 5 from ¹⁰⁰Nb β^- decay (1.5 s) and 369.1 1 from (n,n’γ) I(γ): weighted average of 1.4 3 from ¹⁰⁰Nb β^- decay (1.5 s), 2.01 21 from (n,n’γ), and 1.70 20 from Coulomb excitation
	528.248	E(γ): weighted average of 528.263 18 from ¹⁰⁰Nb β^- decay (1.5 s), 528.263 18 from ¹⁰⁰Nb β^- decay (2.99 s), 528.4 5 from (t,p), 528.21 2 from (n,n’γ), and 528.4 5 from (³⁰Si,Xγ) I(γ): from (n,n’γ). Others: 100.0 20 from Coul. ex., 100.0 22 from ¹⁰⁰Nb β^- decay (1.5 s), 100 13 from ¹⁰⁰Nb β^- decay (2.99 s) M(γ): from γγ(θ) in ¹⁰⁰Nb β^- decay, γ(θ) in (n,n’γ); M2 ruled out by RUL
	1063.78	E(γ): weighted average of 1063.7 1 from ¹⁰⁰Nb β^- decay (1.5 s), 1063.7 2 from ¹⁰⁰Nb β^- decay (2.99 s), 1064.1 1 from (γ,γ’), 1063.76 3 from (n,n’γ), and 1064 1 from (³⁰Si,Xγ) I(γ): weighted average of 36.3 22 from ¹⁰⁰Nb β^- decay (1.5 s), 42 9 from ¹⁰⁰Nb β^- decay (2.99 s), 38.1 4 from (n,n’γ), 58 25 from (³⁰Si,Xγ), and 38.0 10 from Coulomb excitation M(γ): Q from γ(θ) in (n,n’γ) and γγ(θ) in ¹⁰⁰Nb β^- decay (1.5 s); M2 ruled out by RUL
1136.02	600.40	E(γ): weighted average of 600.5 1 from ¹⁰⁰Nb β^- decay (1.5 s), 600.5 1 from ¹⁰⁰Nb β^- decay (2.99 s), and 600.39 2 from (n,n’γ). Others: 599.8 5 from (t,p), 601 1 from (¹³⁶Xe,Xγ), and 600.3 5 from (³⁰Si,Xγ) M(γ): from T_1/2(level), ΔJπ and RUL
1463.93	327	E(γ): from ¹⁰⁰Nb β^- decay (1.5 s) I(γ): from Coulomb excitation.
	400.17	E(γ): from (n,n’γ). Other: 400 1 from ¹⁰⁰Nb β^- decay (1.5 s) I(γ): weighted average of 5 3 from ¹⁰⁰Nb β^- decay (1.5 s), 4.9 7 from (n,n’γ), and 5.8 11 from Coulomb excitation
	768.77	E(γ): weighted average of 768.7 1 from ¹⁰⁰Nb β^- decay (1.5 s), 768.8 2 from ¹⁰⁰Nb β^- decay (2.99 s), and 768.77 3 from (n,n’γ) I(γ): from Coulomb excitation. Other: 100.0 13 from (n,n’γ), 100 9 from ¹⁰⁰Nb β^- decay (1.5 s) M(γ): Q from γ(θ) in (n,n’γ) and γγ(θ) in ¹⁰⁰Nb β^- decay (1.5 s); M2 ruled out by RUL
	928.34	E(γ): weighted average of 928.3 1 from ¹⁰⁰Nb β^- decay (1.5 s), 928.4 2 from ¹⁰⁰Nb β^- decay (2.99 s), and 928.34 3 from (n,n’γ) I(γ): weighted average of 74 3 from ¹⁰⁰Nb β^- decay (1.5 s), 71 8 from ¹⁰⁰Nb β^- decay (2.99 s), 72.8 9 from (n,n’γ), and 73.0 10 from Coulomb excitation
1504.66	440.84	E(γ): weighted average of 440.9 1 from ¹⁰⁰Nb β^- decay (1.5 s) and 440.83 5 from (n,n’γ) I(γ): unweighted average of 41.2 19 from ¹⁰⁰Nb β^- decay (1.5 s) and 33.6 21 from (n,n’γ)
1504.66	969.07	E(γ): weighted average of 969.1 1 from ¹⁰⁰Nb β^- decay (1.5 s) and 969.06 7 from (n,n’γ) M(γ): γγ(θ) in ¹⁰⁰Nb β^- decay (1.5 s), ΔJπ and RUL (βγ coin in ¹⁰⁰Nb β^- decay (1.5 s) suggests 1504.6 level has T_1/2<50 ns)
1607.37	471.37	E(γ): weighted average of 471 1 from ¹⁰⁰Nb β^- decay (1.5 s), 471.2 3 from ¹⁰⁰Nb β^- decay (2.99 s), and 471.39 9 from (n,n’γ) I(γ): weighted average of 23 14 from ¹⁰⁰Nb β^- decay (1.5 s), 18 7 from ¹⁰⁰Nb β^- decay (2.99 s), and 16.8 20 from (n,n’γ)
	543.58	E(γ): weighted average of 543.4 2 from ¹⁰⁰Nb β^- decay (1.5 s), 543.2 2 from ¹⁰⁰Nb β^- decay (2.99 s), 543.62 6 from (n,n’γ), and 544.1 5 from (³⁰Si,Xγ) I(γ): from ¹⁰⁰Nb β^- decay (1.5 s). Others: 100 8 from (n,n’γ), 100 15 from ¹⁰⁰Nb β^- decay (2.99 s)
	1071.77	E(γ): weighted average of 1071.6 2 from ¹⁰⁰Nb β^- decay (1.5 s) and 1071.77 3 from (n,n’γ). Others: 1071.6 3 from ¹⁰⁰Nb β^- decay (2.99 s) and 1071.9 5 from (³⁰Si,Xγ). Multiply placed I(γ): weighted average of 69 13 from ¹⁰⁰Nb β^- decay (2.99 s), 74.0 12 from (n,n’γ), and 52 16 from (³⁰Si,Xγ); the transition mainly deexcites the 1607 level. Other: 116 19 from ¹⁰⁰Nb β^- decay (1.5 s) is in disagreement.
1766.52	702.7	E(γ): from (n,n’γ)
1766.52	1071.77	E(γ): from (n,n’γ). Multiply placed
1771.44	635.31	E(γ): from (n,n’γ). Other: 635.4 3 from ¹⁰⁰Nb β^- decay (2.99 s) I(γ): weighted average of 53 8 from ¹⁰⁰Nb β^- decay (2.99 s), 55 3 from (n,n’γ), and 55 3 from Coulomb excitation
1771.44	707.68	E(γ): weighted average of 707.5 2 from ¹⁰⁰Nb β^- decay (2.99 s) and 707.68 3 from (n,n’γ) I(γ): from (n,n’γ) and Coulomb excitation. Other: 100 14 from ¹⁰⁰Nb β^- decay (2.99 s) M(γ): from T_1/2(level), ΔJπ and RUL
1847.17	711.15	E(γ): weighted average of 711.0 2 from ¹⁰⁰Nb β^- decay (2.99 s), 711.16 6 from (n,n’γ), 711 1 from (¹³⁶Xe,Xγ), and 711.1 5 from (³⁰Si,Xγ) M(γ): from T_1/2, ΔJπ and RUL
1908.19	844.37	E(γ): from (n,n’γ). Other: 844.5 5 from (³⁰Si,Xγ) I(γ): from Coulomb excitation. Others: 100 14 from (³⁰Si,Xγ), ≈100 in (n,n’γ)
	1372.1	E(γ): unweighted average of 1372.73 4 from (n,n’γ) and 1371.4 5 from (³⁰Si,Xγ) I(γ): from Coulomb excitation. Other: 20 6 in ¹⁶⁸Er(³⁰Si,Xγ), 36.1 15 from (n,n’γ)
	1908.2	E(γ): from (n,n’γ) I(γ): from Coulomb excitation. Other: 3.6 7 from (n,n’γ)
1977.34	513.2	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	913.70	E(γ): weighted average of 913.2 5 from ¹⁰⁰Nb β^- decay (1.5 s) and 913.72 9 from (n,n’γ) I(γ): from (n,n’γ). Other: 70 30 from ¹⁰⁰Nb β^- decay (1.5 s)
	1281.8	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	1441.67	E(γ): weighted average of 1441.5 2 from ¹⁰⁰Nb β^- decay (1.5 s) and 1441.69 7 from (n,n’γ) I(γ): from (n,n’γ). Other: 100 22 from ¹⁰⁰Nb β^- decay (1.5 s)
E(level)	E(gamma)	Comments
2037.60	573.6	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
2037.60	1502.2	E(γ): unweighted average of 1501.9 1 from ¹⁰⁰Nb β^- decay (1.5 s) and 1502.4 2 from (n,n’γ) M(γ): γγ(θ) in ¹⁰⁰Nb β^- decay (1.5 s), ΔJπ and RUL (βγ coin in ¹⁰⁰Nb β^- decay (1.5 s) suggests 1504.6 level has T_1/2<50 ns)
2042.78	435.5	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
	578.8	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
	978.95	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
	1507.5	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
	2042.9	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2086.33	622.5	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ) M(γ): see comment for 1022.5γ
	1022.5	M(γ): γγ(θ) in ¹⁰⁰Nb β^- decay (1.5 s), ΔJπ and RUL (βγ coin in ¹⁰⁰Nb β^- decay (1.5 s) suggests 1504.6 level has T_1/2<50 ns)
	1550.5	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
2103.13	495.4	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	639.1	E(γ): weighted average of 639.0 3 from ¹⁰⁰Nb β^- decay (2.99 s) and 639.2 2 from (n,n’γ) I(γ): weighted average of 22 3 from ¹⁰⁰Nb β^- decay (2.99 s) and 29 4 from (n,n’γ)
	967.1	E(γ): weighted average of 966.9 2 from ¹⁰⁰Nb β^- decay (2.99 s) and 967.1 1 from (n,n’γ) I(γ): from (n,n’γ). Other: 100 11 from ¹⁰⁰Nb β^- decay (2.99 s)
	1567.7	E(γ): weighted average of 1567.4 3 from ¹⁰⁰Nb β^- decay (2.99 s) and 1567.8 2 from (n,n’γ) I(γ): unweighted average of 35 5 from ¹⁰⁰Nb β^- decay (2.99 s) and 70 4 from (n,n’γ)
2189.56	1125.8	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
2286.47	822.7	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2286.47	1750.8	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2289.5	682.1	E(γ): weighted average of 681.8 4 from ¹⁰⁰Nb β^- decay (2.99 s) and 682.5 5 from (³⁰Si,Xγ)
2310.12	538.6	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	702.7	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	1246.4	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
2320.3	856.3	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
2320.3	1257.0	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
2369.68	1305.9	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2369.68	1833.7	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
E(level)	E(gamma)	Comments
2397.0	1861.4	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2416.58	952.5	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
2416.58	1280.7	E(γ): weighted average of 1280.4 2 from ¹⁰⁰Nb β^- decay (2.99 s) and 1280.9 2 from (n,n’γ) I(γ): from ¹⁰⁰Nb β^- decay (2.99 s)
2564.20	461.1	E(γ): weighted average of 461.2 2 from ¹⁰⁰Nb β^- decay (2.99 s) and 461.0 2 from (n,n’γ) I(γ): from ¹⁰⁰Nb β^- decay (2.99 s). Other: 100 21 from (n,n’γ)
	792.8	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	1428.0	E(γ): weighted average of 1427.9 3 from ¹⁰⁰Nb β^- decay (2.99 s) and 1428.1 3 from (n,n’γ) I(γ): from ¹⁰⁰Nb β^- decay (2.99 s). Other: 120 20 in (n,n’γ)
	1500.2	E(γ): Placement considered uncertain by evaluators since no such transition is reported in ¹⁰⁰Nb β^- decay. From (n,n’γ) only I(γ): From (n,n’γ) only
2580.89	1516.8	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2580.89	1886.0	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2627.5	780.3	E(γ): weighted average of 781 1 from (¹³⁶Xe,Xγ) and 780.1 5 from (³⁰Si,Xγ) M(γ): from T_1/2, ΔJπ and RUL
2632.4	2632.4	M(γ): From γ(θ) in (γ,γ’)
2652.87	549.7	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	1045.8	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	1516.8	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
2662.6	1598.8	E(γ): placement considered uncertain since a transition of similar energy is assigned to the 3062 level in ¹⁰⁰Nb β^- decay. From (n,n’γ) only I(γ): From (n,n’γ) only
2738.02	1674.3	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2738.02	2202.3	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2791.3	944.1	E(γ): from (³⁰Si,Xγ) only
2822.21	1358.3	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2901.05	2901.0	M(γ): From γ(θ) in (γ,γ’)
2905.75	2905.7	M(γ): From γ(θ) in (γ,γ’)
2928.7	588.8	E(γ): from (³⁰Si,Xγ)
2934.8	1871	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
2961.2	1897.4	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
2970.1	1362.5	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	1906.6	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
	2434.1	E(γ): weighted average of 2434.6 5 from ¹⁰⁰Nb β^- decay (1.5 s) and 2434.0 2 from (n,n’γ)
E(level)	E(gamma)	Comments
2996.31	1532.4	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
3004.4	1397	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
3039.4	1432	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
3042.2	1978.4	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
3053.70	1989.9	E(γ): From (n,n’γ) only I(γ): From (n,n’γ) only
3062.60	1598.7	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
3062.60	2526.9	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
3066.25	3066.2	E(γ): from (γ,γ’) only
3070.2	2534.6	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
3129.6	1665.7	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
3143.0	351.7	E(γ): from (³⁰Si,Xγ) only
3198.4	3198.3	M(γ): From γ(θ) in (γ,γ’)
3242.76	3242.7	M(γ): From γ(θ) in (γ,γ’)
3290.27	2595.3	M(γ): From γ(θ) in (γ,γ’)
	2755.4	M(γ): From γ(θ) in (γ,γ’)
	3290.1	M(γ): From γ(θ) in (γ,γ’)
3342.06	3342.0	M(γ): From γ(θ) in (γ,γ’)
3367.0	739.5	E(γ): from (³⁰Si,Xγ)
3483.82	3483.9	M(γ): From γ(θ) in (γ,γ’)
3570.77	3570.7	M(γ): From γ(θ) in (γ,γ’)
3599.87	3599.8	E(γ): from (γ,γ’) only
3615.57	3615.5	M(γ): From γ(θ) in (γ,γ’)
3626.5	1779.3	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
3627.3	3627.2	M(γ): From γ(θ) in (γ,γ’)
3647.3	1800.1	E(γ): γ reported in ¹⁰⁰Nb β^- decay, but not in (n,n’γ)
E(level)	E(gamma)	Comments
3658.96	2595.3	M(γ): From γ(θ) in (γ,γ’)
3658.96	3658.7	M(γ): From γ(θ) in (γ,γ’)
3783.5	640.5	E(γ): from (³⁰Si,Xγ) only
3887.98	3887.9	M(γ): From γ(θ) in (γ,γ’)
3896.68	3896.6	M(γ): From γ(θ) in (γ,γ’)
3925.98	3925.9	M(γ): From γ(θ) in (γ,γ’)
4032.7	733.5	E(γ): from (³⁰Si,Xγ) only
4062.6	695.6	E(γ): weighted average of 696 1 from (¹³⁶Xe,Xγ) and 695.5 5 from (³⁰Si,Xγ)
4081.59	4081.5	M(γ): From γ(θ) in (γ,γ’)
4156.5	4156.4	M(γ): From γ(θ) in (γ,γ’)
4217.60	4217.5	M(γ): From γ(θ) in (γ,γ’)
4232.10	4232.0	M(γ): From γ(θ) in (γ,γ’)
4329.90	4329.8	M(γ): From γ(θ) in (γ,γ’)
4516.81	4516.7	M(γ): From γ(θ) in (γ,γ’)
4565.51	4565.4	M(γ): From γ(θ) in (γ,γ’)
4583.11	4583.0	M(γ): From γ(θ) in (γ,γ’)
4594.91	4594.8	M(γ): From γ(θ) in (γ,γ’)
4689.02	4688.9	M(γ): From γ(θ) in (γ,γ’)
4730.32	4730.2	M(γ): From γ(θ) in (γ,γ’)
4875.2	812.6	E(γ): weighted average of 813 1 from (¹³⁶Xe,Xγ) and 812.5 5 from (³⁰Si,Xγ)
4939.8	907.1	E(γ): from (³⁰Si,Xγ) only
4989.63	4989.5	M(γ): From γ(θ) in (γ,γ’)
5007.33	5007.2	M(γ): From γ(θ) in (γ,γ’)
5034.54	5034.4	M(γ): From γ(θ) in (γ,γ’)
5062.9	5062.8	M(γ): From γ(θ) in (γ,γ’)
E(level)	E(gamma)	Comments
5071.24	5071.1	M(γ): From γ(θ) in (γ,γ’)
5101.3	5101.2	M(γ): From γ(θ) in (γ,γ’)
5109.3	5109.2	M(γ): From γ(θ) in (γ,γ’)
5136.04	5135.9	M(γ): From γ(θ) in (γ,γ’)
5158.3	5158.2	M(γ): From γ(θ) in (γ,γ’)
5169.6	5169.5	M(γ): From γ(θ) in (γ,γ’)
5181.8	5181.7	M(γ): From γ(θ) in (γ,γ’)
5186.9	5187	M(γ): From γ(θ) in (γ,γ’)
5190.4	5190.3	M(γ): From γ(θ) in (γ,γ’)
5204.6	5204.5	M(γ): From γ(θ) in (γ,γ’)
5216.0	5215.9	M(γ): From γ(θ) in (γ,γ’)
5271.2	5271.1	M(γ): From γ(θ) in (γ,γ’)
5277.6	5277.5	M(γ): From γ(θ) in (γ,γ’)
5310.5	5310.3	M(γ): From γ(θ) in (γ,γ’)
5335.65	5335.5	M(γ): From γ(θ) in (γ,γ’)
5347.85	5347.7	M(γ): From γ(θ) in (γ,γ’)
5359.8	5359.6	M(γ): From γ(θ) in (γ,γ’)
5369.6	5369.4	M(γ): From γ(θ) in (γ,γ’)
5382.5	5382.3	M(γ): From γ(θ) in (γ,γ’)
5390.3	5390.1	M(γ): From γ(θ) in (γ,γ’)
5402.26	5402.1	M(γ): From γ(θ) in (γ,γ’)
5412.6	5412.4	M(γ): From γ(θ) in (γ,γ’)
5435.5	5435.3	M(γ): From γ(θ) in (γ,γ’)
5442.9	5442.7	M(γ): From γ(θ) in (γ,γ’)
5449.6	5449.4	M(γ): From γ(θ) in (γ,γ’)
E(level)	E(gamma)	Comments
5502.7	5502.5	M(γ): From γ(θ) in (γ,γ’)
5519.4	5519.2	M(γ): From γ(θ) in (γ,γ’)
5532.2	5532.0	M(γ): From γ(θ) in (γ,γ’)
5547.9	5547.7	M(γ): From γ(θ) in (γ,γ’)
5554.4	5554.2	M(γ): From γ(θ) in (γ,γ’)
5584.9	5584.7	M(γ): From γ(θ) in (γ,γ’)
5596.8	5596.6	M(γ): From γ(θ) in (γ,γ’)
5604.7	5604.5	M(γ): From γ(θ) in (γ,γ’)
5612.67	5612.5	M(γ): From γ(θ) in (γ,γ’)
5618.6	5618.4	M(γ): From γ(θ) in (γ,γ’)
5656.5	5656.3	M(γ): From γ(θ) in (γ,γ’)
5670.67	5670.5	M(γ): From γ(θ) in (γ,γ’)
5680.9	5680.7	M(γ): From γ(θ) in (γ,γ’)
5686.5	5686.3	M(γ): From γ(θ) in (γ,γ’)
5715.9	5715.7	M(γ): From γ(θ) in (γ,γ’)
5725.3	5725.1	M(γ): From γ(θ) in (γ,γ’)
5732.9	5732.7	M(γ): From γ(θ) in (γ,γ’)
5742.6	5742.4	M(γ): From γ(θ) in (γ,γ’)
5764.0	5763.8	M(γ): From γ(θ) in (γ,γ’)
5770.4	5770.2	M(γ): From γ(θ) in (γ,γ’)
5798.2	5798.0	M(γ): From γ(θ) in (γ,γ’)
5808.98	5808.8	M(γ): From γ(θ) in (γ,γ’)
5826.5	5826.3	M(γ): From γ(θ) in (γ,γ’)
5840.2	965	E(γ): from (³⁰Si,Xγ) and (¹³⁷Xe,Xγ)
5840.7	5840.5	M(γ): From γ(θ) in (γ,γ’)
E(level)	E(gamma)	Comments
5879.39	5879.2	M(γ): From γ(θ) in (γ,γ’)
5901.0	5900.8	M(γ): From γ(θ) in (γ,γ’)
5947.79	5947.6	M(γ): From γ(θ) in (γ,γ’)
5957.2	5957.0	M(γ): From γ(θ) in (γ,γ’)
5964.0	5963.8	M(γ): From γ(θ) in (γ,γ’)
5972.99	5972.8	M(γ): From γ(θ) in (γ,γ’)
5988.9	5988.7	M(γ): From γ(θ) in (γ,γ’)
6009.6	6009.4	M(γ): From γ(θ) in (γ,γ’)
6019.5	6019.3	M(γ): From γ(θ) in (γ,γ’)
6035.5	6035.3	M(γ): From γ(θ) in (γ,γ’)
6061.3	6061.1	M(γ): From γ(θ) in (γ,γ’)
6065.9	6065.7	M(γ): From γ(θ) in (γ,γ’)
6082.9	6082.7	M(γ): From γ(θ) in (γ,γ’)
6089.3	6089.1	M(γ): From γ(θ) in (γ,γ’)
6122.5	6122.3	M(γ): From γ(θ) in (γ,γ’)
6133.6	6133.4	M(γ): From γ(θ) in (γ,γ’)
6147.1	6146.9	M(γ): From γ(θ) in (γ,γ’)
6174.0	6173.8	M(γ): From γ(θ) in (γ,γ’)
6194.51	6194.3	M(γ): From γ(θ) in (γ,γ’)
6249.4	6249.2	M(γ): From γ(θ) in (γ,γ’)
6257.61	6257.4	M(γ): From γ(θ) in (γ,γ’)
6270.5	6270.3	M(γ): From γ(θ) in (γ,γ’)
6278.71	6278.5	M(γ): From γ(θ) in (γ,γ’)
6293.1	6292.9	M(γ): From γ(θ) in (γ,γ’)
6310.3	6310.1	M(γ): From γ(θ) in (γ,γ’)
E(level)	E(gamma)	Comments
6321.2	6321.0	M(γ): From γ(θ) in (γ,γ’)
6327.6	6327.4	M(γ): From γ(θ) in (γ,γ’)
6337.5	6337.3	M(γ): From γ(θ) in (γ,γ’)
6354.32	6354.1	M(γ): From γ(θ) in (γ,γ’)
6365.6	6365.4	M(γ): From γ(θ) in (γ,γ’)
6375.6	6375.4	M(γ): From γ(θ) in (γ,γ’)
6402.0	6401.8	M(γ): From γ(θ) in (γ,γ’)
6414.3	6414.1	M(γ): From γ(θ) in (γ,γ’)
6419.4	5355	M(γ): From γ(θ,lin pol) in (γ,γ’)
6419.4	6418	M(γ): From γ(θ,lin pol) in (γ,γ’)
6421.4	6421.2	M(γ): From γ(θ) in (γ,γ’)
6426.6	6426.4	M(γ): From γ(θ) in (γ,γ’)
6434.1	6433.9	M(γ): From γ(θ) in (γ,γ’)
6459.0	6458.8	M(γ): From γ(θ) in (γ,γ’)
6473.5	6473.3	M(γ): From γ(θ) in (γ,γ’)
6483.2	6483	M(γ): From γ(θ) in (γ,γ’)
6497.6	6497.4	M(γ): From γ(θ) in (γ,γ’)
6518.5	6517	M(γ): From γ(θ,lin pol) in (γ,γ’)
6519.1	6518.9	M(γ): From γ(θ) in (γ,γ’)
6526.6	6526.4	M(γ): From γ(θ) in (γ,γ’)
6570.2	6570.0	M(γ): From γ(θ) in (γ,γ’)
6597.0	6596.8	M(γ): From γ(θ) in (γ,γ’)
6622.3	6622.1	M(γ): From γ(θ) in (γ,γ’)
6628.3	6628.1	M(γ): From γ(θ) in (γ,γ’)
6641.0	6640.8	M(γ): From γ(θ) in (γ,γ’)
E(level)	E(gamma)	Comments
6658.2	6658.0	M(γ): From γ(θ) in (γ,γ’)
6669.14	6668.9	M(γ): From γ(θ) in (γ,γ’)
6685.3	6685.1	M(γ): From γ(θ) in (γ,γ’)
6764.1	6763.9	M(γ): From γ(θ) in (γ,γ’)
6772.7	6772.5	M(γ): From γ(θ) in (γ,γ’)
6790.6	6790.4	M(γ): From γ(θ) in (γ,γ’)
6797.5	6797.3	M(γ): From γ(θ) in (γ,γ’)
6807.9	6807.7	M(γ): From γ(θ) in (γ,γ’)
6829.5	6829.2	M(γ): From γ(θ) in (γ,γ’)
6844.6	6844.3	M(γ): From γ(θ) in (γ,γ’)
6851.3	6851.0	M(γ): From γ(θ) in (γ,γ’)
6870.0	6869.7	M(γ): From γ(θ) in (γ,γ’)
6886.5	6886.2	M(γ): From γ(θ) in (γ,γ’)
6893.2	6892.9	M(γ): From γ(θ) in (γ,γ’)
6906.1	6905.8	M(γ): From γ(θ) in (γ,γ’)
6912.9	6912.6	M(γ): From γ(θ) in (γ,γ’)
6919.5	6919.2	M(γ): From γ(θ) in (γ,γ’)
6924.9	6924.6	M(γ): From γ(θ) in (γ,γ’)
6934.2	6933.9	M(γ): From γ(θ) in (γ,γ’)
6949.9	6949.6	M(γ): From γ(θ) in (γ,γ’)
6957.7	6957.4	M(γ): From γ(θ) in (γ,γ’)
6974.2	6973.9	M(γ): From γ(θ) in (γ,γ’)
6981.1	6980.8	M(γ): From γ(θ) in (γ,γ’)
6994.5	6994.2	M(γ): From γ(θ) in (γ,γ’)
7001.2	7000.9	M(γ): From γ(θ) in (γ,γ’)
E(level)	E(gamma)	Comments
7018.3	7018.0	M(γ): From γ(θ) in (γ,γ’)
7032.1	7031.8	M(γ): From γ(θ) in (γ,γ’)
7037.8	7037.5	M(γ): From γ(θ) in (γ,γ’)
7060.2	7059.9	M(γ): From γ(θ) in (γ,γ’)
7068.1	7067.8	M(γ): From γ(θ) in (γ,γ’)
7095.4	7095.1	M(γ): From γ(θ) in (γ,γ’)
7103.5	7103.2	M(γ): From γ(θ) in (γ,γ’)
7115.3	7115.0	M(γ): From γ(θ) in (γ,γ’)
7136.6	7136.3	M(γ): From γ(θ) in (γ,γ’)
7171.7	7171.4	M(γ): From γ(θ) in (γ,γ’)
7181.5	7181.2	M(γ): From γ(θ) in (γ,γ’)
7194.4	7194.1	M(γ): From γ(θ) in (γ,γ’)
7204.0	7203.7	M(γ): From γ(θ) in (γ,γ’)
7219.4	7219.1	M(γ): From γ(θ) in (γ,γ’)
7225.4	7225.1	M(γ): From γ(θ) in (γ,γ’)
7299.6	7299.3	M(γ): From γ(θ) in (γ,γ’)
7312.3	7312.0	M(γ): From γ(θ) in (γ,γ’)
7330.8	7330.5	M(γ): From γ(θ) in (γ,γ’)
7357.7	7357.4	M(γ): From γ(θ) in (γ,γ’)
7380.3	7380.0	M(γ): From γ(θ) in (γ,γ’)
7403.3	7403.0	M(γ): From γ(θ) in (γ,γ’)
7450.6	7450.3	M(γ): From γ(θ) in (γ,γ’)
7471.0	7470.7	M(γ): From γ(θ) in (γ,γ’)
7487.2	7486.9	M(γ): From γ(θ) in (γ,γ’)
7494.8	7494.5	M(γ): From γ(θ) in (γ,γ’)
E(level)	E(gamma)	Comments
7503.5	7503.2	M(γ): From γ(θ) in (γ,γ’)
7526.1	7525.8	M(γ): From γ(θ) in (γ,γ’)
7546.3	7546	M(γ): From γ(θ) in (γ,γ’)
7559.1	7558.8	M(γ): From γ(θ) in (γ,γ’)
7577.2	7576.9	M(γ): From γ(θ) in (γ,γ’)
7606.9	7606.6	M(γ): From γ(θ) in (γ,γ’)
7638.6	7102	M(γ): From γ(θ,lin pol) in (γ,γ’)
7638.6	7637	M(γ): From γ(θ,lin pol) in (γ,γ’)
7744.5	7744.2	M(γ): From γ(θ) in (γ,γ’)
7758.4	7758.1	M(γ): From γ(θ) in (γ,γ’)
7771.5	7771.2	M(γ): From γ(θ) in (γ,γ’)
7796.9	7796.6	M(γ): From γ(θ) in (γ,γ’)
7831.2	7830.9	M(γ): From γ(θ) in (γ,γ’)
7863.1	7862.8	M(γ): From γ(θ) in (γ,γ’)
7875.4	7875.1	M(γ): From γ(θ) in (γ,γ’)
7887.2	7886.9	M(γ): From γ(θ) in (γ,γ’)
7935.7	7935.4	M(γ): From γ(θ) in (γ,γ’)
7955.7	7955.4	M(γ): From γ(θ) in (γ,γ’)
7988.0	7987.7	M(γ): From γ(θ) in (γ,γ’)
8002.0	8001.7	M(γ): From γ(θ) in (γ,γ’)
8033.5	8033.2	M(γ): From γ(θ) in (γ,γ’)
8052.2	8051.9	M(γ): From γ(θ) in (γ,γ’)
8063.7	8063.4	M(γ): From γ(θ) in (γ,γ’)
8083.3	8082.9	M(γ): From γ(θ) in (γ,γ’)
8095.9	8095.5	M(γ): From γ(θ) in (γ,γ’)
E(level)	E(gamma)	Comments
8108.1	8107.7	M(γ): From γ(θ) in (γ,γ’)
8127.7	8127.3	M(γ): From γ(θ) in (γ,γ’)
8194.4	8194.0	M(γ): From γ(θ) in (γ,γ’)
8208.8	8208.4	M(γ): From γ(θ) in (γ,γ’)
8218.2	8217.8	M(γ): From γ(θ) in (γ,γ’)
8238.6	8238.2	M(γ): From γ(θ) in (γ,γ’)
8257.1	8256.7	M(γ): From γ(θ) in (γ,γ’)
8269.6	8269.2	M(γ): From γ(θ) in (γ,γ’)
8283.6	8283.2	M(γ): From γ(θ) in (γ,γ’)
8294.5	8294.1	M(γ): From γ(θ) in (γ,γ’)