List of levels for 191IR

Author: V.R. Vanin Et Al. | Citation: Nucl. Data Sheets 108, 2393 (2007) | Cutoff date: 1-Dec-2006

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
82.423	1/2+	4.08 ns 7	82.413 15	M1+E2	-0.873 20	10.54	B(E2)(W.u.)=20.9 7, B(M1)(W.u.)=0.000474 14, α=10.54, α(K)=5.32 12, α(L)=3.95 9, α(M)=0.994 23, α(N)=0.241 6, α(O)=0.0378 8, α(P)=0.000687 15, α(N+)=0.279 7
129.413	5/2+	89.9 ps 9	47.05 3	E2		143.5	B(E2)(W.u.)=10.4 13, α=143.5, α(L)=108.1 16, α(M)=27.7 4, α(N)=6.67 10, α(O)=1.010 15, α(P)=0.000955 14, α(N+)=7.69 11
129.413	5/2+	89.9 ps 9	129.416 16	M1+E2	-0.398 3	2.76	B(E2)(W.u.)=96.2 24, B(M1)(W.u.)=0.0259 6, α=2.76, α(K)=2.15 3, α(L)=0.463 7, α(M)=0.1098 16, α(N)=0.0269 4, α(O)=0.00458 7, α(P)=0.000265 4, α(N+)=0.0317 5
171.29	11/2-	4.899 s 23 % IT = 100	41.89 4	E3		1.69×10⁴	B(E3)(W.u.)=0.0299 5, α=1.69E4, α(L)=1.212E4 19, α(M)=3.71E3 6, α(N)=919 14, α(O)=135.6 21, α(P)=0.1446 22, α(N+)=1055 16
178.950	3/2+	43 ps 4	49.59 3	M1+E2	0.177 25	11.5	B(E2)(W.u.)=27 9, B(M1)(W.u.)=0.0053 11, α=11.5 10, α(L)=8.8 7, α(M)=2.09 18, α(N)=0.51 5, α(O)=0.086 7, α(P)=0.00472 8, α(N+)=0.60 5
	3/2+	43 ps 4	96.517 9	M1+E2	+0.145 7	6.75	B(E2)(W.u.)=58 9, B(M1)(W.u.)=0.066 8, α=6.75, α(K)=5.48 8, α(L)=0.972 15, α(M)=0.226 4, α(N)=0.0554 9, α(O)=0.00971 15, α(P)=0.000682 10, α(N+)=0.0658 10
	3/2+	43 ps 4	178.96 3	M1+E2	-0.79 4	0.916	B(E2)(W.u.)=15.7 20, B(M1)(W.u.)=0.00205 24, α=0.916 21, α(K)=0.682 21, α(L)=0.179 3, α(M)=0.0431 8, α(N)=0.01052 18, α(O)=0.00175 3, α(P)=8.2E-5 3, α(N+)=0.01235 21
343.23	(7/2)+	20.4 ps 8	213.76 7	M1+E2	-0.342 7	0.667	B(E2)(W.u.)=29.8 19, B(M1)(W.u.)=0.0296 15, α=0.667, α(K)=0.542 8, α(L)=0.0962 14, α(M)=0.0224 4, α(N)=0.00549 8, α(O)=0.000960 14, α(P)=6.64E-5 10, α(N+)=0.00652 10
343.23	(7/2)+	20.4 ps 8	343.32 8	(E2)		0.0641	B(E2)(W.u.)=41.9 20, α=0.0641, α(K)=0.0429 6, α(L)=0.01607 23, α(M)=0.00397 6, α(N)=0.000966 14, α(O)=0.0001560 22, α(P)=4.69E-6 7, α(N+)=0.001127 16
351.154	(5/2)+	18.8 ps 25	172.19 2	M1+E2	+0.072 6	1.301	B(E2)(W.u.)=3.9 9, B(M1)(W.u.)=0.056 8, α=1.301, α(K)=1.072 15, α(L)=0.1761 25, α(M)=0.0406 6, α(N)=0.00998 14, α(O)=0.001765 25, α(P)=0.0001322 19, α(N+)=0.01187 17
	(5/2)+	18.8 ps 25	221.74 8	(M1)		0.644	B(M1)(W.u.)=0.00095 16, α=0.644, α(K)=0.532 8, α(L)=0.0864 13, α(M)=0.0199 3, α(N)=0.00489 7, α(O)=0.000866 13, α(P)=6.54×10^-5 10, α(N+)=0.00582 9
	(5/2)+	18.8 ps 25	268.71 8	E2		0.1324	B(E2)(W.u.)=39 7, α=0.1324, α(K)=0.0795 12, α(L)=0.0401 6, α(M)=0.01004 15, α(N)=0.00244 4, α(O)=0.000387 6, α(P)=8.40E-6 12, α(N+)=0.00283 4
	(5/2)+	18.8 ps 25	351.17 3	M1+E2	-0.30 2	0.173	B(E2)(W.u.)=1.7 4, B(M1)(W.u.)=0.0060 9, α=0.173 3, α(K)=0.1427 23, α(L)=0.0236 4, α(M)=0.00545 8, α(N)=0.001340 20, α(O)=0.000236 4, α(P)=1.74E-5 3, α(N+)=0.001593 24
390.94	7/2-	240 ps 20	219.65 5	E2		0.252	B(E2)(W.u.)=56 5, α=0.252, α(K)=0.1335 19, α(L)=0.0897 13, α(M)=0.0227 4, α(N)=0.00550 8, α(O)=0.000862 12, α(P)=1.367E-5 20, α(N+)=0.00637 9
502.61	(9/2)+	13.4 ps 19	159.38 3	[M1,E2]		1.2	α=1.2 5, α(K)=0.8 6, α(L)=0.28 7, α(M)=0.070 20, α(N)=0.017 5, α(O)=0.0028 6, α(P)=0.00010 7, α(N+)=0.020 6
502.61	(9/2)+	13.4 ps 19	373.20 9	E2		0.0508	B(E2)(W.u.)=72 11, α=0.0508, α(K)=0.0350 5, α(L)=0.01198 17, α(M)=0.00295 5, α(N)=0.000717 10, α(O)=0.0001165 17, α(P)=3.86E-6 6, α(N+)=0.000838 12
538.854	3/2+	9.8 ps 8	187.69 4	M1+E2	0.54 11	0.89	B(E2)(W.u.)=10 4, B(M1)(W.u.)=0.0031 5, α=0.89 5, α(K)=0.70 5, α(L)=0.146 4, α(M)=0.0345 10, α(N)=0.00845 24, α(O)=0.00144 3, α(P)=8.5E-5 7, α(N+)=0.0100 3
	3/2+	9.8 ps 8	359.88 3	M1+E2	+0.023 9	0.1719	B(E2)(W.u.)=0.013 10, B(M1)(W.u.)=0.0080 7, α=0.1719, α(K)=0.1422 20, α(L)=0.0228 4, α(M)=0.00525 8, α(N)=0.001291 18, α(O)=0.000229 4, α(P)=1.734E-5 25, α(N+)=0.001537 22
	3/2+	9.8 ps 8	409.44 2	M1+E2	+0.19 1	0.1189	B(E2)(W.u.)=0.60 9, B(M1)(W.u.)=0.0071 8, α=0.1189, α(K)=0.0983 14, α(L)=0.01589 23, α(M)=0.00365 6, α(N)=0.000898 13, α(O)=0.0001590 23, α(P)=1.195E-5 17, α(N+)=0.001069 15
	3/2+	9.8 ps 8	456.47 5	M1+E2	-0.32 4	0.0856	B(E2)(W.u.)=0.39 10, B(M1)(W.u.)=0.00204 21, α=0.0856 18, α(K)=0.0707 16, α(L)=0.01152 21, α(M)=0.00265 5, α(N)=0.000652 12, α(O)=0.0001152 21, α(P)=8.56E-6 19, α(N+)=0.000776 14
	3/2+	9.8 ps 8	538.87 5	M1+E2	-0.68 2	0.0467	B(E2)(W.u.)=2.52 25, B(M1)(W.u.)=0.0040 4, α=0.0467 9, α(K)=0.0383 7, α(L)=0.00649 11, α(M)=0.001501 24, α(N)=0.000369 6, α(O)=6.47E-5 11, α(P)=4.59E-6 9, α(N+)=0.000438 7
587.95	3/2+,5/2+	≈ 0.3 ps	458.59 15	[M1,E2]		0.06	α=0.06 3, α(K)=0.05 3, α(L)=0.009 3, α(M)=0.0021 7, α(N)=0.00052 16, α(O)=9.E-5 3, α(P)=6.E-6 4, α(N+)=0.00061 20
587.95	3/2+,5/2+	≈ 0.3 ps	587.95 8	(M1)		0.0471	B(M1)(W.u.)≈0.17, α=0.0471, α(K)=0.0391 6, α(L)=0.00619 9, α(M)=0.001419 20, α(N)=0.000349 5, α(O)=6.19×10^-5 9, α(P)=4.72E-6 7, α(N+)=0.000415 6
624.07	(1/2+)	> 5 ps	85.15 8	[M1,E2]		9.4	α=9.4 4, α(K)=4 4, α(L)=3.8 25, α(M)=0.9 7, α(N)=0.23 16, α(O)=0.036 23, α(P)=0.0006 5, α(N+)=0.27 18
	(1/2+)	> 5 ps	445.13 8	[M1,E2]		0.06	α=0.06 4, α(K)=0.05 3, α(L)=0.010 4, α(M)=0.0023 7, α(N)=0.00056 17, α(O)=0.00010 4, α(P)=6.E-6 4, α(N+)=0.00067 21
	(1/2+)	> 5 ps	494.69 7	(E2)		0.0244	B(E2)(W.u.)<1.3, α=0.0244, α(K)=0.0181 3, α(L)=0.00478 7, α(M)=0.001154 17, α(N)=0.000281 4, α(O)=4.67E-5 7, α(P)=2.05E-6 3, α(N+)=0.000330 5
	(1/2+)	> 5 ps	541.64 10	(M1)		0.0583	B(M1)(W.u.)<0.0038, α=0.0583, α(K)=0.0484 7, α(L)=0.00767 11, α(M)=0.001761 25, α(N)=0.000433 6, α(O)=7.68×10^-5 11, α(P)=5.85E-6 9, α(N+)=0.000516 8
	(1/2+)	> 5 ps	624.06 6	(M1+E2)	0.40 22	0.037	B(E2)(W.u.)<2.7, B(M1)(W.u.)<0.0100, α=0.037 4, α(K)=0.030 4, α(L)=0.0049 4, α(M)=0.00113 9, α(N)=0.000277 23, α(O)=4.9E-5 5, α(P)=3.7E-6 4, α(N+)=0.00033 3
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
658.90	(3/2-)	< 0.12 ns	267.92 8	E2		0.1337	B(E2)(W.u.)>38, α=0.1337, α(K)=0.0801 12, α(L)=0.0406 6, α(M)=0.01016 15, α(N)=0.00247 4, α(O)=0.000391 6, α(P)=8.46E-6 12, α(N+)=0.00287 4
	(3/2-)	< 0.12 ns	479.95 7	[E1]		0.00869	α=0.00869, α(K)=0.00725 11, α(L)=0.001111 16, α(M)=0.000254 4, α(N)=6.19×10^-5 9, α(O)=1.079E-5 16, α(P)=7.47E-7 11, α(N+)=7.35E-5 11
	(3/2-)	< 0.12 ns	576.46 8	E1		0.00591	B(E1)(W.u.)>1.0E-6, α=0.00591, α(K)=0.00494 7, α(L)=0.000746 11, α(M)=0.0001700 24, α(N)=4.16E-5 6, α(O)=7.27E-6 11, α(P)=5.14E-7 8, α(N+)=4.93E-5 7
	(3/2-)	< 0.12 ns	658.75 15	[E1]		0.00450	α=0.00450, α(K)=0.00377 6, α(L)=0.000564 8, α(M)=0.0001285 18, α(N)=3.14×10^-5 5, α(O)=5.51E-6 8, α(P)=3.95E-7 6, α(N+)=3.73E-5 6
686.10	7/2+	2.7 ps 3	556.79 15	M1+E2	-1.11 10	0.0344	B(E2)(W.u.)=18 3, B(M1)(W.u.)=0.0117 18, α=0.0344 18, α(K)=0.0279 16, α(L)=0.00505 20, α(M)=0.00118 5, α(N)=0.000289 11, α(O)=5.02E-5 20, α(P)=3.31E-6 19, α(N+)=0.000342 13
686.10	7/2+	2.7 ps 3	686.02 17	E2		0.01141	B(E2)(W.u.)=8.9 11, α=0.01141, α(K)=0.00896 13, α(L)=0.00188 3, α(M)=0.000446 7, α(N)=0.0001090 16, α(O)=1.85E-5 3, α(P)=1.020E-6 15, α(N+)=0.0001285 18
747.77	(5/2)+		208.96 15	M1(+E2)	0.5 4	0.67	α=0.67 12, α(K)=0.53 12, α(L)=0.104 3, α(M)=0.0244 12, α(N)=0.0060 3, α(O)=0.001030 17, α(P)=6.5×10^-5 16, α(N+)=0.0071 3
	(5/2)+		396.7 2	[M1,E2]		0.09	α=0.09 5, α(K)=0.07 4, α(L)=0.014 4, α(M)=0.0032 9, α(N)=0.00079 21, α(O)=0.00014 4, α(P)=8.E-6 5, α(N+)=0.0009 3
	(5/2)+		568.81 8	(M1)		0.0513	α=0.0513, α(K)=0.0426 6, α(L)=0.00675 10, α(M)=0.001548 22, α(N)=0.000381 6, α(O)=6.75×10^-5 10, α(P)=5.14E-6 8, α(N+)=0.000453 7
	(5/2)+		618.7 4	[M1,E2]		0.028	α=0.028 14, α(K)=0.023 12, α(L)=0.0040 15, α(M)=0.0009 4, α(N)=0.00023 8, α(O)=3.9×10^-5 15, α(P)=2.7E-6 15, α(N+)=0.00027 10
	(5/2)+		747.75 13	[M1,E2]		0.017	α=0.017 8, α(K)=0.014 7, α(L)=0.0024 9, α(M)=0.00056 21, α(N)=0.00014 5, α(O)=2.4×10^-5 10, α(P)=1.7E-6 9, α(N+)=0.00016 6
762.54	3/2+		138.2 2	[M1,E2]		1.9	α=1.9 6, α(K)=1.2 8, α(L)=0.49 17, α(M)=0.12 5, α(N)=0.030 12, α(O)=0.0048 15, α(P)=0.00014 11, α(N+)=0.035 13
	3/2+		223.67 8	M1+E2	0.39 25	0.58	α=0.58 7, α(K)=0.47 7, α(L)=0.0842 12, α(M)=0.0196 4, α(N)=0.00482 9, α(O)=0.000840 14, α(P)=5.7×10^-5 8, α(N+)=0.00571 9
	3/2+		411.3 3	[M1,E2]		0.08	α=0.08 4, α(K)=0.06 4, α(L)=0.012 4, α(M)=0.0029 8, α(N)=0.00071 20, α(O)=0.00012 4, α(P)=8.E-6 5, α(N+)=0.00084 24
	3/2+		583.61 8	(M1)		0.0480	α=0.0480, α(K)=0.0398 6, α(L)=0.00631 9, α(M)=0.001447 21, α(N)=0.000356 5, α(O)=6.31×10^-5 9, α(P)=4.81E-6 7, α(N+)=0.000424 6
	3/2+		633.18 10	E2(+M1)	1.5 GT	0.018	α=0.018 4, α(K)=0.014 4, α(L)=0.0028 5, α(M)=0.00065 10, α(N)=0.000159 24, α(O)=2.7×10^-5 5, α(P)=1.6E-6 5, α(N+)=0.00019 3
	3/2+		680.0 2	[M1,E2]		0.022	α=0.022 11, α(K)=0.018 9, α(L)=0.0031 12, α(M)=0.0007 3, α(N)=0.00018 7, α(O)=3.1×10^-5 12, α(P)=2.1E-6 11, α(N+)=0.00021 8
	3/2+		762.60 15	[M1,E2]		0.017	α=0.017 8, α(K)=0.014 7, α(L)=0.0023 9, α(M)=0.00053 20, α(N)=0.00013 5, α(O)=2.3×10^-5 9, α(P)=1.6E-6 8, α(N+)=0.00015 6
799.79	(5/2)-		140.884 15	M1(+E2)	0.5 5	2.1	α=2.1 4, α(K)=1.6 5, α(L)=0.37 9, α(M)=0.09 3, α(N)=0.022 6, α(O)=0.0036 8, α(P)=0.00020 6, α(N+)=0.025 7
831.97	(11/2+)	3.15 ps 19	488.85 18			0.0253	B(E2)(W.u.)=70 4, α=0.0253

Calculations:

Magnetic properties of selected levels: 2002St11.

Levels and properties in rotor + 1 quasiparticle model: 2001Ro23.

Levels and properties in triaxial rotor and supersymmetry model: 2000Be07.

Levels, B(E2), with IBM, in ¹⁸⁵Ir-¹⁹⁵Ir: 1994He24, 1986Ar03.

Supersymmetry model: 1985Hu07.

Compilation, review: NMR in oriented nuclei: 1996Ha09.

Isotope shift and hyperfine structure measurements: 1989Sa31.

Levels: The rotational bands of ¹⁹¹Ir with axially asymmetric core are discussed in 1979Vi06, 1987Pr10, and 2001Ro23. The band assignments are based on assignments in ¹⁹¹Ir(n,n’γ) (1987Pr10) and ¹⁹²Os(³He,d) (1971Pr13). Spin(6) symmetry and U(6/4), U(6/20) supersymmetry are used to describe ¹⁹¹Ir (1984Mu19, 1986Mc01, 2000Be07).

Q-value: Note: Current evaluation has used the following Q record

Q(β-)=-1009 keV 4	S(n)= 8026.5 keV 4	S(p)= 5290.4 keV 12	Q(α)= 2082.8 keV 13
Reference: 2012WA38

References:
A	¹⁹¹Pt ε decay	B	¹⁹¹Os β^- decay (15.4 d)
C	¹⁹¹Ir IT decay (4.899 S)	D	Coulomb Excitation
E	¹⁹²Os(p,2nγ),(d,3nγ)	F	¹⁹¹Ir(γ,γ): MOSSBAUER
G	¹⁹⁰Os(³He,d),(α,t)	H	¹⁹¹Ir(d,d’)
I	¹⁹¹Ir(p,p’) E=50 MeV	J	¹⁹³Ir(p,t)
K	¹⁹¹Ir(γ,γ’)	L	¹⁹¹Ir(n,n’γ)

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A B C D E F G H I J L	3/2+	STABLE
82.423 12	A B C D E F G H I J L	1/2+	4.08 ns 7	82.413 15	100	M1+E2	0.0	3/2+
129.413 13	A B C D E F G H I J L	5/2+	89.9 ps 9	47.05 3 129.416 16	0.0094 11 100.00 15	E2 M1+E2	82.423 0.0	1/2+ 3/2+
171.29 4	A B C D E G H J L	11/2-	4.899 s 23 % IT = 100	41.89 4	100	E3	129.413	5/2+
178.950 12	A D E G H I J L	3/2+	43 ps 4	49.59 3 96.517 9 178.96 3	1.11 13 100 4 31.6 10	M1+E2 M1+E2 M1+E2	129.413 82.423 0.0	5/2+ 1/2+ 3/2+
300.4 4	E			121.5 5 300.4 5	100 8		178.950 0.0	3/2+ 3/2+
343.23 5	A D E G H I J L	(7/2)+	20.4 ps 8	213.76 7 343.32 8	63.7 17 100.0 17	M1+E2 (E2)	129.413 0.0	5/2+ 3/2+
351.154 17	A D E G I J L	(5/2)+	18.8 ps 25	172.19 2 221.74 8 268.71 8 351.17 3	100 3 3.6 3 48 5 99 3	M1+E2 (M1) E2 M1+E2	178.950 129.413 82.423 0.0	3/2+ 5/2+ 1/2+ 3/2+
390.94 6	A D E G L	7/2-	240 ps 20	219.65 5	100	E2	171.29	11/2-
502.61 5	D E H J L	(9/2)+	13.4 ps 19	159.38 3 373.20 9	8.9 5 100.0 23	[M1,E2] E2	343.23 129.413	(7/2)+ 5/2+
504.13 11	D E H I L	(7/2+)		152.9 3 161.2 5 325.2 5 374.83 15	58 5 200 80 100 5 52 11	(D(+Q))	351.154 343.23 178.950 129.413	(5/2)+ (7/2)+ 3/2+ 5/2+
538.854 17	A D E H J K L	3/2+	9.8 ps 8	187.69 4 196 1 359.88 3 409.44 2 456.47 5 538.87 5	2.83 12 0.022 6 40.3 9 55 3 23.2 11 100 3	M1+E2 M1+E2 M1+E2 M1+E2 M1+E2	351.154 343.23 178.950 129.413 82.423 0.0	(5/2)+ (7/2)+ 3/2+ 5/2+ 1/2+ 3/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
556.64 11	E L	(13/2-)		385.33 10	100	(D+Q)	171.29	11/2-
587.95 7	A D E G J K L	3/2+,5/2+	≈ 0.3 ps	244.6 2 458.59 15 587.95 8	69 7 38 3 100 5	[M1,E2] (M1)	343.23 129.413 0.0	(7/2)+ 5/2+ 3/2+
591.13 16	E L	(15/2-)		419.89 16	100	(Q)	171.29	11/2-
614 4	H
624.07 4	A D J K L	(1/2+)	> 5 ps	85.15 8 445.13 8 494.69 7 541.64 10 624.06 6	4.1 5 4.00 27 4.11 22 25 3 100 3	[M1,E2] [M1,E2] (E2) (M1) (M1+E2)	538.854 178.950 129.413 82.423 0.0	3/2+ 3/2+ 5/2+ 1/2+ 3/2+
653.99 9	D E H L	(9/2-)		263.08 7 482.5 5	79 17 100 13		390.94 171.29	7/2- 11/2-
658.90 5	A D E H K	(3/2-)	< 0.12 ns	267.92 8 479.95 7 576.46 8 658.75 15	100 10 7.2 4 16.4 5 2.01 15	E2 [E1] E1 [E1]	390.94 178.950 82.423 0.0	7/2- 3/2+ 1/2+ 3/2+
686.10 10	A D E G H I J L	7/2+	2.7 ps 3	556.79 15 686.02 17	100 3 76 3	M1+E2 E2	129.413 0.0	5/2+ 3/2+
747.77 6	A D E L	(5/2)+		208.96 15 396.7 2 404.1 3 568.81 8 618.7 4 747.75 13	100 6 8.0 25 9 4 41.7 18 6.7 25 2.76 25	M1(+E2) [M1,E2] (M1) [M1,E2] [M1,E2]	538.854 351.154 343.23 178.950 129.413 0.0	3/2+ (5/2)+ (7/2)+ 3/2+ 5/2+ 3/2+
762.54 5	A D E J L	3/2+		138.2 2 223.67 8 411.3 3 583.61 8 633.18 10 680.0 2 762.60 15	22 15 100 9 8.8 22 69 5 26.4 11 7.2 6 11.8 9	[M1,E2] M1+E2 [M1,E2] (M1) E2(+M1) [M1,E2] [M1,E2]	624.07 538.854 351.154 178.950 129.413 82.423 0.0	(1/2+) 3/2+ (5/2)+ 3/2+ 5/2+ 1/2+ 3/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
799.79 5	A D E L	(5/2)-		140.884 15 409.26 19	78 12 100 17	M1(+E2)	658.90 390.94	(3/2-) 7/2-
811.88 12	D E J L	(9/2+)		308.03 21 460.43 15 468.9 5	78 6 100 8 46 6	(D)	504.13 351.154 343.23	(7/2+) (5/2)+ (7/2)+
816.59 18	L			645.30 17	100		171.29	11/2-
825.10 17	E L	(7/2+,9/2+)		482.5 5 695.60 18	<220 100 11		343.23 129.413	(7/2)+ 5/2+
831.97 17	D E H J L	(11/2+)	3.15 ps 19	329.4 5 488.85 18	35.4 18 100 3	(D(+Q))	502.61 343.23	(9/2)+ (7/2)+
877.65 12	E G L	(9/2-,11/2+)		374.83 15 534.59 15	100 15 78 13		502.61 343.23	(9/2)+ (7/2)+
919.08 17	E L	(11/2-)		264.8 5 527.9 5 748.0 2	100 10 18 5 21 15	(Q)	653.99 390.94 171.29	(9/2-) 7/2- 11/2-
927.80 25	E L	(7/2+)		389.1 5 425.5 10 798.3 3			538.854 502.61 129.413	3/2+ (9/2)+ 5/2+
935.46 13	A L	(1/2+,3/2,5/2+)		756.4 5 806.4 3 853.4 4 935.33 15	13 3 34.2 21 9.0 7 100 5		178.950 129.413 82.423 0.0	3/2+ 5/2+ 1/2+ 3/2+
945.4 4	D E J L	(5/2+,7/2+,9/2+)		259.0 5 443 603 816.0 5	79 7 95 5 100 17 71 5		686.10 502.61 343.23 129.413	7/2+ (9/2)+ (7/2)+ 5/2+
963.2 4	E	(15/2-)		372.1 5 406.5 5			591.13 556.64	(15/2-) (13/2-)
977.04 8	E G L	(7/2-)		177.25 6 318.4 10 586.2 3	100 15 43 16		799.79 658.90 390.94	(5/2)- (3/2-) 7/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
991.28 16	E L	(11/2+)		178.7 5 487.1 5 489.0 5	9.4 18 100 3		811.88 504.13 502.61	(9/2+) (7/2+) (9/2)+
1003.6 3	D E J L	(13/2+)		172.0 500.9 3			831.97 502.61	(11/2+) (9/2)+
1034 3	G L	1/2+
1036.59 21	E L	(17/2-)		445.50 15 480 1	100 10 <25	(D+Q)	591.13 556.64	(15/2-) (13/2-)
1052.63 14	E L			366.56 11 549.8 3 709.4 5	100 16 23 5 9 3		686.10 502.61 343.23	7/2+ (9/2)+ (7/2)+
1070	G J	3/2+
1127.1 6	E	(19/2-)		536.0 5	100	(Q)	591.13	(15/2-)
1130	J
1135.23 24	E L	(7/2-,9/2,11/2-)		216.8 5 482.5 5 743.6 3	100 14 <166 41 4		919.08 653.99 390.94	(11/2-) (9/2-) 7/2-
1138	G H J
1206.57 18	D E L	(7/2+,9/2+,11/2+)		375.2 5 520.5 3 703.81 23	<180 100 13 67 12		831.97 686.10 502.61	(11/2+) 7/2+ (9/2)+
1206.89 20	E L	(9/2-)		229.85 18	100		977.04	(7/2-)
1210.5 4	E J L	(9/2,11/2)		332.5 5 556.8 5	100 20 <85		877.65 653.99	(9/2-,11/2+) (9/2-)
1244	G J
1253.5 4	E	(13/2-)		334.6 5 599.4 5	38 6 100 10		919.08 653.99	(11/2-) (9/2-)
1297.19 22	L			793.0 3 946.1 3	43 14 100 14		504.13 351.154	(7/2+) (5/2)+
1359	G
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1393	H
1397.7 3	D E L	(13/2+)		406.7 3 585.2 5	100 48 9 4		991.28 811.88	(11/2+) (9/2+)
1400.9 4	E	(5/2+,7/2-)		715 1 741.4 5 898.9 5			686.10 658.90 502.61	7/2+ (3/2-) (9/2)+
1418.1 3	D E L	(15/2+)		414.3 5 586.2 3	100 18 <300		1003.6 831.97	(13/2+) (11/2+)
1421.7 4	E	(17/2-)		385.6 5 458.6 5 864.6 5	<1350 <262 100 12		1036.59 963.2 556.64	(17/2-) (15/2-) (13/2-)
1433	G
1449	G	1/2-,3/2-
1461	J	3/2+
1507	H
1520	G	5/2-,7/2-
1596	J	3/2+
1600.1 6	D E	(17/2+)		596.5 5	100		1003.6	(13/2+)
1613	G
1642	G
1645.9 8	E	(21/2-)		518.8 5	100		1127.1	(19/2-)
1651.6 8	E			524.5 5	100		1127.1	(19/2-)
1660	G
1680.6 8	E	(23/2-)		553.5 5	100	(Q)	1127.1	(19/2-)
1711	G
2046.7 9	E			395.1 5			1651.6
2046.7+X	E		5.5 s 7 % IT = 100
2112.1 11	D	(19/2+)		694	100		1418.1	(15/2+)
2312.1 12	D	(21/2+)		712	100		1600.1	(17/2+)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - 3/2(402)
0.0	3/2+	STABLE
129.413 13	5/2+	89.9 ps 9	47.05 3 129.416 16	0.0094 11 100.00 15	E2 M1+E2	82.423 0.0	1/2+ 3/2+
343.23 5	(7/2)+	20.4 ps 8	213.76 7 343.32 8	63.7 17 100.0 17	M1+E2 (E2)	129.413 0.0	5/2+ 3/2+
502.61 5	(9/2)+	13.4 ps 19	159.38 3 373.20 9	8.9 5 100.0 23	[M1,E2] E2	343.23 129.413	(7/2)+ 5/2+
831.97 17	(11/2+)	3.15 ps 19	329.4 5 488.85 18	35.4 18 100 3	(D(+Q))	502.61 343.23	(9/2)+ (7/2)+
1003.6 3	(13/2+)		172.0 500.9 3			831.97 502.61	(11/2+) (9/2)+
1418.1 3	(15/2+)		414.3 5 586.2 3	100 18 <300		1003.6 831.97	(13/2+) (11/2+)
1600.1 6	(17/2+)		596.5 5	100		1003.6	(13/2+)
2112.1 11	(19/2+)		694	100		1418.1	(15/2+)
2312.1 12	(21/2+)		712	100		1600.1	(17/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - 1/2(400)
82.423 12	1/2+	4.08 ns 7
178.950 12	3/2+	43 ps 4	49.59 3 96.517 9 178.96 3	1.11 13 100 4 31.6 10	M1+E2 M1+E2 M1+E2	129.413 82.423 0.0	5/2+ 1/2+ 3/2+
351.154 17	(5/2)+	18.8 ps 25	172.19 2 221.74 8 268.71 8 351.17 3	100 3 3.6 3 48 5 99 3	M1+E2 (M1) E2 M1+E2	178.950 129.413 82.423 0.0	3/2+ 5/2+ 1/2+ 3/2+
504.13 11	(7/2+)		152.9 3 161.2 5 325.2 5 374.83 15	58 5 200 80 100 5 52 11	(D(+Q))	351.154 343.23 178.950 129.413	(5/2)+ (7/2)+ 3/2+ 5/2+
811.88 12	(9/2+)		308.03 21 460.43 15 468.9 5	78 6 100 8 46 6	(D)	504.13 351.154 343.23	(7/2+) (5/2)+ (7/2)+
991.28 16	(11/2+)		178.7 5 487.1 5 489.0 5	9.4 18 100 3		811.88 504.13 502.61	(9/2+) (7/2+) (9/2)+
1397.7 3	(13/2+)		406.7 3 585.2 5	100 48 9 4		991.28 811.88	(11/2+) (9/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - 1/2(411)
538.854 17	3/2+	9.8 ps 8
624.07 4	(1/2+)	> 5 ps	85.15 8 445.13 8 494.69 7 541.64 10 624.06 6	4.1 5 4.00 27 4.11 22 25 3 100 3	[M1,E2] [M1,E2] (E2) (M1) (M1+E2)	538.854 178.950 129.413 82.423 0.0	3/2+ 3/2+ 5/2+ 1/2+ 3/2+
747.77 6	(5/2)+		208.96 15 396.7 2 404.1 3 568.81 8 618.7 4 747.75 13	100 6 8.0 25 9 4 41.7 18 6.7 25 2.76 25	M1(+E2) [M1,E2] (M1) [M1,E2] [M1,E2]	538.854 351.154 343.23 178.950 129.413 0.0	3/2+ (5/2)+ (7/2)+ 3/2+ 5/2+ 3/2+
927.80 25	(7/2+)		389.1 5 425.5 10 798.3 3			538.854 502.61 129.413	3/2+ (9/2)+ 5/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - K^π=(7/2-)
390.94 6	7/2-	240 ps 20
653.99 9	(9/2-)		263.08 7 482.5 5	79 17 100 13		390.94 171.29	7/2- 11/2-
919.08 17	(11/2-)		264.8 5 527.9 5 748.0 2	100 10 18 5 21 15	(Q)	653.99 390.94 171.29	(9/2-) 7/2- 11/2-
1253.5 4	(13/2-)		334.6 5 599.4 5	38 6 100 10		919.08 653.99	(11/2-) (9/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - 11/2(505)
171.29 4	11/2-	4.899 s 23 % IT = 100
556.64 11	(13/2-)		385.33 10	100	(D+Q)	171.29	11/2-
591.13 16	(15/2-)		419.89 16	100	(Q)	171.29	11/2-
1036.59 21	(17/2-)		445.50 15 480 1	100 10 <25	(D+Q)	591.13 556.64	(15/2-) (13/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - K^π=(3/2-)
658.90 5	(3/2-)	< 0.12 ns
799.79 5	(5/2)-		140.884 15 409.26 19	78 12 100 17	M1(+E2)	658.90 390.94	(3/2-) 7/2-
977.04 8	(7/2-)		177.25 6 318.4 10 586.2 3	100 15 43 16		799.79 658.90 390.94	(5/2)- (3/2-) 7/2-
1206.89 20	(9/2-)		229.85 18	100		977.04	(7/2-)

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	3/2+	STABLE	Q=+0.816 9, μ=+0.1507 6 Nuclear charge radius: <r²>^1/2=5.40 11 fm (2004An14). E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
82.423	1/2+	4.08 ns 7	μ=+0.600 6 E(level): 1/2(400). From ¹⁹²Os(p,2nγ),(d,3nγ).
129.413	5/2+	89.9 ps 9	μ=+0.81 6 E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
171.29	11/2-	4.899 s 23 % IT = 100	μ=+6.03 4 E(level): 11/2(505).
178.950	3/2+	43 ps 4	μ=+1.4 4 E(level): 1/2(400). From ¹⁹²Os(p,2nγ),(d,3nγ).
343.23	(7/2)+	20.4 ps 8	μ=+1.40 6 E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
351.154	(5/2)+	18.8 ps 25	E(level): 1/2(400). From ¹⁹²Os(p,2nγ),(d,3nγ).
390.94	7/2-	240 ps 20	E(level): K^π=(7/2-). From ¹⁹¹Os β^- decay.
502.61	(9/2)+	13.4 ps 19	μ=+2.38 23 E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
504.13	(7/2+)		E(level): 1/2(400). From ¹⁹²Os(p,2nγ),(d,3nγ).
538.854	3/2+	9.8 ps 8	E(level): 1/2(411). From Coulomb excitation.
556.64	(13/2-)		E(level): 11/2(505).
587.95	3/2+,5/2+	≈ 0.3 ps	XREF: γ(591).
591.13	(15/2-)		E(level): 11/2(505).
624.07	(1/2+)	> 5 ps	E(level): 1/2(411). From Coulomb excitation.
653.99	(9/2-)		E(level): K^π=(7/2-). From ¹⁹¹Os β^- decay.
658.90	(3/2-)	< 0.12 ns	E(level): K^π=(3/2-).
747.77	(5/2)+		E(level): 1/2(411). From Coulomb excitation.
799.79	(5/2)-		E(level): K^π=(3/2-).
811.88	(9/2+)		E(level): 1/2(400). From ¹⁹²Os(p,2nγ),(d,3nγ).
831.97	(11/2+)	3.15 ps 19	E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
919.08	(11/2-)		E(level): K^π=(7/2-). From ¹⁹¹Os β^- decay.
927.80	(7/2+)		E(level): 1/2(411). From Coulomb excitation.
977.04	(7/2-)		E(level): K^π=(3/2-).
991.28	(11/2+)		E(level): 1/2(400). From ¹⁹²Os(p,2nγ),(d,3nγ).
E(level)	J^π(level)	T_1/2(level)	Comments
1003.6	(13/2+)		E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
1036.59	(17/2-)		E(level): 11/2(505).
1052.63			1987Pr10 from ¹⁹¹Ir(n,n’γ) and 1979Lu01 from ¹⁹²Ir(p,2nγ) suggest Jπ=(9/2⁺); γ-branching ratios in (n,n’γ) and (p,2nγ) do not match. E(level): 1987Pr10 from ¹⁹¹Ir(n,n’γ) and 1979Lu01 from ¹⁹²Ir(p,2nγ) suggest Jπ=(9/2⁺); γ-branching ratios in (n,n’γ) and (p,2nγ) do not match.
1138			L=1 or 2 in (³He,d) and (α,t). E(level): L=1 or 2 in (³He,d) and (α,t).
1206.57	(7/2+,9/2+,11/2+)		XREF: E(1207.3).
1206.89	(9/2-)		XREF: E(1206.0)L(1207.7). E(level): K^π=(3/2-).
1253.5	(13/2-)		E(level): K^π=(7/2-). From ¹⁹¹Os β^- decay.
1359			L=4 or 5 in (³He,d) and (α,t). E(level): L=4 or 5 in (³He,d) and (α,t).
1397.7	(13/2+)		E(level): 1/2(400). From ¹⁹²Os(p,2nγ),(d,3nγ).
1418.1	(15/2+)		E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
1433			L=3 or 4 (³He,d) and (α,t). E(level): L=3 or 4 (³He,d) and (α,t).
1600.1	(17/2+)		E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
2112.1	(19/2+)		E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
2312.1	(21/2+)		E(level): 3/2(402). Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.

E(level)	E(gamma)	Comments
82.423	82.413	E(γ): Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
129.413	47.05	E(γ): From ¹⁹¹Os β^- decay. I(γ): From ¹⁹¹Os β^- decay. M(γ): from ce data in ¹⁹¹Os β^- decay.
129.413	129.416	E(γ): Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay. I(γ): From ¹⁹¹Os β^- decay. M(γ): from ce data in ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay.
171.29	41.89	E(γ): Unweighted average from ¹⁹¹Os β^- decay and ¹⁹¹Pt ε decay. I(γ): From ¹⁹¹Os β^- decay. M(γ): from ce data in ¹⁹¹Os β^- decay.
300.4	121.5	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
300.4	300.4	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(p,2nγ).
343.23	213.76	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From Coulomb excitation. M(γ): from δ and RUL.
343.23	343.32	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From Coulomb excitation. M(γ): From Coulomb excitation.
351.154	268.71	M(γ): Mult=E2(+M1) with δ>3.6 from ¹⁹¹Pt ε decay, restricted by adopted spins.
390.94	219.65	M(γ): Mult=E2⁺(M1) with δ>3 in ¹⁹¹Pt ε decay; other level properties require multipolarity >1.
502.61	159.38	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): Weighted average of Coulomb excitation, ¹⁹²Os(p,2nγ) and ¹⁹¹Ir(n,n’γ).
502.61	373.20	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): Weighted average of Coulomb excitation, ¹⁹²Os(p,2nγ) and ¹⁹¹Ir(n,n’γ). M(γ): From Coulomb excitation.
504.13	152.9	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): See also comment on 161.2γ Iγ.. Weighted average of Coulomb excitation, ¹⁹²Os(p,2nγ) and ¹⁹¹Ir(n,n’γ). M(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
	161.2	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): Unweighted average of Iγ(161.2)/Iγ(325.2)=1.21 17 in ¹⁹²Os(p,2nγ) and 2.8 5 in ¹⁹¹Ir(n,n’γ); 161.2γ not seen in Coulomb excitation. Iγ(152.9γ)/Iγ(325.2γ) observed in all reactions in good agreement.
	325.2	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): See also comment on 161.2γ Iγ.. Weighted average of Coulomb excitation, ¹⁹²Os(p,2nγ) and ¹⁹¹Ir(n,n’γ).
	374.83	E(γ): Multiply placed with intensity suitably divided. From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): γ multiply placed in ¹⁹²Os(p,2nγ) and ¹⁹¹Ir(n,n’γ) but likely not in Coulomb excitation; see also comment on 161.2γ Iγ.. Multiply placed with intensity suitably divided. From Coulomb excitation.
556.64	385.33	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. M(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
587.95	244.6	E(γ): From Coulomb excitation. I(γ): Other: 2.4(6) in ¹⁹¹Pt ε decay.. From Coulomb excitation.
	458.59	I(γ): weighted average from ¹⁹¹Pt ε decay, ¹⁹¹Ir(n,n’γ), and Coulomb excitation.
	587.95	I(γ): weighted average from ¹⁹¹Pt ε decay, ¹⁹¹Ir(n,n’γ), and Coulomb excitation.
591.13	419.89	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. M(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
624.07	494.69	M(γ): (M1,E2) from ce data. Decay scheme requires E2.
653.99	263.08	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): Other: Iγ>150 in ¹⁹²Os(p,2nγ).. From Coulomb excitation.
653.99	482.5	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): This transition seems not to be a multiplet in Coulomb excitation; placed also from levels 825.4 and 1135.1 keV in other reactions.. From Coulomb excitation.
658.90	267.92	M(γ): Mult=E2(+M1) with δ>3 from ¹⁹¹Pt ε decay; see comment on 659 keV level Jπ for adopted multipolarity.
658.90	576.46	M(γ): RUL - see comment on 659 keV level Jπ.
E(level)	E(gamma)	Comments
686.10	556.79	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From Coulomb excitation. M(γ): From Coulomb excitation.
686.10	686.02	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From Coulomb excitation. M(γ): From Coulomb excitation.
762.54	411.3	I(γ): Other: 70(30) from ¹⁹¹Ir(n,n’γ).
762.54	583.61	I(γ): Other: 37(12) from ¹⁹¹Ir(n,n’γ).
799.79	409.26	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset.
811.88	308.03	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): weighted average from ¹⁹²Os(p,2nγ) and ¹⁹²Os(d,3nγ). M(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
	460.43	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): weighted average from ¹⁹²Os(p,2nγ) and ¹⁹²Os(d,3nγ).
	468.9	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): weighted average from ¹⁹²Os(p,2nγ) and ¹⁹²Os(d,3nγ).
816.59	645.30	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset.
825.10	482.5	E(γ): Multiply placed with undivided intensity. From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): Multiply placed with undivided intensity. From ¹⁹²Os(p,2nγ).
825.10	695.60	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From ¹⁹²Os(p,2nγ).
831.97	329.4	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From Coulomb excitation. M(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
831.97	488.85	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From Coulomb excitation.
877.65	374.83	E(γ): Multiply placed with intensity suitably divided. From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): Multiply placed with intensity suitably divided. From ¹⁹¹Ir(n,n’γ).
877.65	534.59	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From ¹⁹¹Ir(n,n’γ).
919.08	264.8	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(p,2nγ). M(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
	527.9	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(p,2nγ).
	748.0	E(γ): Other: 747.20 20, corrected value from ¹⁹¹Ir(n,n’γ). I(γ): Corrected for Iγ(747.8γ) from 747.8 keV level using Iγ(747.8γ)/Iγ(209.0γ) from ¹⁹¹Pt ε decay and Iγ(209.0γ) from ¹⁹²Os(p,2nγ).. From ¹⁹²Os(p,2nγ).
927.80	389.1	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
	425.5	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
	798.3	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset.
945.4	259.0	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): Weighted average of ¹⁹²Os(p,2nγ) and ¹⁹²Os(d,3nγ). See also comment on 816.0γ.
	443	E(γ): From Coulomb excitation. I(γ): Weighted average of Coulomb excitation and ¹⁹¹Ir(n,n’γ). See also comment on 816.0γ.
	603	E(γ): From Coulomb excitation. I(γ): See also comment on 816.0γ.. From Coulomb excitation.
	816.0	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): Weighted average of Coulomb excitation, ¹⁹²Os(p,2nγ), ¹⁹²Os(d,3nγ), and ¹⁹¹Ir(n,n’γ). α different set of γ-ray transitions was seen decaying from 945.4 level in each reaction, this being the only common transition; all available data embodied in the adopted branching-ratios.
E(level)	E(gamma)	Comments
963.2	372.1	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
963.2	406.5	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
977.04	177.25	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From ¹⁹¹Ir(n,n’γ).
	318.4	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
	586.2	E(γ): Multiply placed with intensity suitably divided. From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): In ¹⁹¹Ir(n,n’γ), 586.2γ is a multiplet whose intensity could be properly divided.. Multiply placed with intensity suitably divided. From ¹⁹¹Ir(n,n’γ).
991.28	178.7	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
	487.1	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From Coulomb excitation.
	489.0	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From Coulomb excitation.
1003.6	172.0	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
1003.6	500.9	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset.
1036.59	445.50	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): from ¹⁹²Os(d,3nγ), where it is a singlet (seen as a doublet in ¹⁹¹Ir(n,n’γ)) M(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
1036.59	480	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): from ¹⁹²Os(d,3nγ), where it is multiply placed.
1052.63	366.56	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From ¹⁹¹Ir(n,n’γ).
	549.8	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From ¹⁹¹Ir(n,n’γ).
	709.4	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): Not seen in ¹⁹¹Ir(n,n’γ); deduced from Iγ(709γ):Iγ(550γ) =38 11:100 11 in (p,2nγ), where Iγ(367γ) was not given.. From ¹⁹²Os(p,2nγ).
1127.1	536.0	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). M(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
1135.23	216.8	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(p,2nγ).
	482.5	E(γ): Multiply placed with undivided intensity. From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): Multiply placed with undivided intensity. From ¹⁹²Os(p,2nγ).
	743.6	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From ¹⁹²Os(p,2nγ).
1206.57	375.2	E(γ): Multiply placed with undivided intensity. From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): Multiply placed with undivided intensity. From ¹⁹²Os(p,2nγ).
	520.5	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): Weighted average of Coulomb excitation and ¹⁹¹Ir(n,n’γ).
	703.81	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): Weighted average of Coulomb excitation and ¹⁹¹Ir(n,n’γ).
1206.89	229.85	E(γ): Other: Eγ=228.6 5 in (p,2nγ).. From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset.
1210.5	332.5	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(p,2nγ).
1210.5	556.8	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(p,2nγ).
E(level)	E(gamma)	Comments
1253.5	334.6	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(d,3nγ).
1253.5	599.4	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(d,3nγ).
1297.19	793.0	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From ¹⁹¹Ir(n,n’γ).
1297.19	946.1	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From ¹⁹¹Ir(n,n’γ).
1397.7	406.7	E(γ): From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): From ¹⁹¹Ir(n,n’γ).
1397.7	585.2	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹¹Ir(n,n’γ).
1400.9	715	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
	741.4	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
	898.9	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
1418.1	414.3	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From Coulomb excitation.
1418.1	586.2	E(γ): Multiply placed with undivided intensity. From ¹⁹¹Ir(n,n’γ), multiplied by 0.99945 15; see note on Eγ in ¹⁹¹Ir(n,n’γ) dataset. I(γ): In Coulomb excitation, 586.2γ is a doublet and the intensity could not be divided; 414.3γ was not seen in ¹⁹¹Ir(n,n’γ), where 586.2γ intensity could be divided.. Multiply placed with undivided intensity. From Coulomb excitation.
1421.7	385.6	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(p,2nγ).
	458.6	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(p,2nγ).
	864.6	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). I(γ): From ¹⁹²Os(p,2nγ).
1600.1	596.5	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
1645.9	518.8	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
1651.6	524.5	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
1680.6	553.5	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ). M(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
2046.7	395.1	E(γ): From ¹⁹²Os(p,2nγ),(d,3nγ).
2112.1	694	E(γ): From Coulomb excitation.
2312.1	712	E(γ): From Coulomb excitation.