List of levels for 140PM

Author: N. Nica | Citation: Nucl. Data Sheets 154, 1 (2018) | Cutoff date: 20-Nov-2018

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
139.95	(2)-		140.0 1	E1		0.1068	α=0.1068, α(K)=0.0907 13, α(L)=0.01273 18, α(M)=0.00270 4, α(N)=0.000601 9, α(O)=8.71×10^-5 13, α(P)=4.66E-6 7
225.47	0+,1+,2+		225.4 1	M1		0.1599	α=0.1599, α(K)=0.1360 20, α(L)=0.0188 3, α(M)=0.00401 6, α(N)=0.000905 13, α(O)=0.0001367 20, α(P)=8.70×10^-6 13
260.64	(1,2,3)+		35.2 2	(M1+E2)		80	α=80 75, α(L)=62 59, α(M)=14 14, α(N)=3.1 29, α(O)=0.38 36, α(P)=0.00110 68
260.64	(1,2,3)+		120.8 1	E1		0.1597	α=0.1597, α(K)=0.1353 20, α(L)=0.0192 3, α(M)=0.00409 6, α(N)=0.000908 13, α(O)=0.0001307 19, α(P)=6.82×10^-6 10
335.35	+		109.9 2	M1		1.182	α=1.182, α(K)=1.003 15, α(L)=0.1408 21, α(M)=0.0301 5, α(N)=0.00678 11, α(O)=0.001022 16, α(P)=6.45×10^-5 10
339.88	(1,2)+		114.6 2	M1		1.049	α=1.049, α(K)=0.891 14, α(L)=0.1249 19, α(M)=0.0267 4, α(N)=0.00601 9, α(O)=0.000907 14, α(P)=5.73×10^-5 9
	(1,2)+		199.9 2	E1		0.0408	α=0.0408, α(K)=0.0347 5, α(L)=0.00477 7, α(M)=0.001012 15, α(N)=0.000226 4, α(O)=3.31×10^-5 5, α(P)=1.86E-6 3
	(1,2)+		339.8 1	E2		0.0370	α=0.0370, α(K)=0.0295 5, α(L)=0.00588 9, α(M)=0.001294 19, α(N)=0.000287 4, α(O)=4.03×10^-5 6, α(P)=1.636E-6 23
344.94	+		84.4 1	M1		2.52	α=2.52, α(K)=2.14 3, α(L)=0.301 5, α(M)=0.0643 10, α(N)=0.01449 21, α(O)=0.00218 4, α(P)=0.0001376 20
	+		119.5 2	M1,E2		1.06	α=1.06 14, α(K)=0.75 4, α(L)=0.24 14, α(M)=0.054 31, α(N)=0.0120 67, α(O)=0.00160 80, α(P)=4.1×10^-5 10
	+		344.9 2	(E2)		0.0354	α=0.0354, α(K)=0.0283 4, α(L)=0.00559 8, α(M)=0.001229 18, α(N)=0.000273 4, α(O)=3.83×10^-5 6, α(P)=1.570E-6 23
415.15	1+		75.3 2	M1		3.50	α=3.50 6, α(K)=2.97 5, α(L)=0.419 7, α(M)=0.0895 15, α(N)=0.0202 4, α(O)=0.00304 5, α(P)=0.000191 3
481.18	+		136.4 2	M1		0.641	α=0.641, α(K)=0.544 8, α(L)=0.0762 12, α(M)=0.01626 24, α(N)=0.00366 6, α(O)=0.000553 8, α(P)=3.50×10^-5 6
	+		141.3 2	[M1,E2]		0.62	α=0.62 5, α(K)=0.46 3, α(L)=0.125 56, α(M)=0.028 14, α(N)=0.0061 29, α(O)=8.4×10^-4 34, α(P)=2.6E-5 6
	+		145.7 2	M1		0.533	α=0.533, α(K)=0.453 7, α(L)=0.0632 10, α(M)=0.01350 20, α(N)=0.00304 5, α(O)=0.000459 7, α(P)=2.91×10^-5 5
	+		220.7 1	(M1)		0.1693	α=0.1693, α(K)=0.1440 21, α(L)=0.0199 3, α(M)=0.00425 6, α(N)=0.000959 14, α(O)=0.0001448 21, α(P)=9.21×10^-6 13
	+		255.6 2	(M1)		0.1139	α=0.1139, α(K)=0.0970 14, α(L)=0.01337 19, α(M)=0.00285 4, α(N)=0.000643 9, α(O)=9.71×10^-5 14, α(P)=6.19E-6 9
503.39	0+,1+,2+		158.5 2	(M1)		0.421	α=0.421, α(K)=0.358 6, α(L)=0.0499 8, α(M)=0.01065 16, α(N)=0.00240 4, α(O)=0.000362 6, α(P)=2.30×10^-5 4
	0+,1+,2+		163.6 2	(M1)		0.386	α=0.386, α(K)=0.328 5, α(L)=0.0457 7, α(M)=0.00975 14, α(N)=0.00220 4, α(O)=0.000332 5, α(P)=2.10×10^-5 3
	0+,1+,2+		503.3 2	M1		0.0195	α=0.0195, α(K)=0.01668 24, α(L)=0.00225 4, α(M)=0.000478 7, α(N)=0.0001078 16, α(O)=1.633×10^-5 23, α(P)=1.053E-6 15
534.03	(+)		308.7 2	(M1)		0.0689	α=0.0689, α(K)=0.0587 9, α(L)=0.00805 12, α(M)=0.001715 25, α(N)=0.000387 6, α(O)=5.85×10^-5 9, α(P)=3.74E-6 6
534.03	(+)		533.9 2	(E2)		0.01033	α=0.01033, α(K)=0.00855 12, α(L)=0.001397 20, α(M)=0.000302 5, α(N)=6.75×10^-5 10, α(O)=9.80E-6 14, α(P)=4.99E-7 7
565.46	(1+,2+)		150.4 2	(M1)		0.487	α=0.487, α(K)=0.414 6, α(L)=0.0578 9, α(M)=0.01234 18, α(N)=0.00278 4, α(O)=0.000420 6, α(P)=2.66×10^-5 4
	(1+,2+)		220.6 1	(M1)		0.1695	α=0.1695, α(K)=0.1442 21, α(L)=0.0200 3, α(M)=0.00426 6, α(N)=0.000960 14, α(O)=0.0001450 21, α(P)=9.22×10^-6 13
	(1+,2+)		339.8 1	(E2)		0.0370	α=0.0370, α(K)=0.0295 5, α(L)=0.00588 9, α(M)=0.001294 19, α(N)=0.000287 4, α(O)=4.03×10^-5 6, α(P)=1.636E-6 23
	(1+,2+)		565.6 2	(M1)		0.01457	α=0.01457, α(K)=0.01245 18, α(L)=0.001672 24, α(M)=0.000356 5, α(N)=8.02×10^-5 12, α(O)=1.215E-5 17, α(P)=7.84E-7 11
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
572.11	(1+,2+)		237.0 2	(M1)		0.1396	α=0.1396, α(K)=0.1188 17, α(L)=0.01641 24, α(M)=0.00350 5, α(N)=0.000789 12, α(O)=0.0001192 17, α(P)=7.59×10^-6 11
	(1+,2+)		311.4 2	(M1)		0.0674	α=0.0674, α(K)=0.0574 8, α(L)=0.00786 11, α(M)=0.001676 24, α(N)=0.000378 6, α(O)=5.71×10^-5 8, α(P)=3.65E-6 6
	(1+,2+)		572.2 2	(M1)		0.01416	α=0.01416, α(K)=0.01210 17, α(L)=0.001624 23, α(M)=0.000345 5, α(N)=7.79×10^-5 11, α(O)=1.180E-5 17, α(P)=7.62E-7 11
576.27	(0-,1-,2-)		576.3 2	(E1)		0.00300	α=0.00300, α(K)=0.00258 4, α(L)=0.000336 5, α(M)=7.12×10^-5 10, α(N)=1.599E-5 23, α(O)=2.40E-6 4, α(P)=1.488E-7 21
670.17	(+)		409.5 2	(M1)		0.0330	α=0.0330, α(K)=0.0282 4, α(L)=0.00383 6, α(M)=0.000814 12, α(N)=0.000184 3, α(O)=2.78×10^-5 4, α(P)=1.78E-6 3
761.35	(+)		761.5 2	(E2)		0.00431	α=0.00431, α(K)=0.00363 5, α(L)=0.000535 8, α(M)=0.0001147 16, α(N)=2.57×10^-5 4, α(O)=3.80E-6 6, α(P)=2.16E-7 3
386.23+X	8+	1.0 ns +10-5	386.2 1	E1		0.00755	B(E1)(W.u.)=4.3E-6 +43-22, α=0.00755, α(K)=0.00647 9, α(L)=0.000859 12, α(M)=0.000182 3, α(N)=4.08E-5 6, α(O)=6.08E-6 9, α(P)=3.66E-7 6
407.28+X	9+		407.5 2	E1		0.00664	α=0.00664, α(K)=0.00569 8, α(L)=0.000754 11, α(M)=0.0001597 23, α(N)=3.58×10^-5 5, α(O)=5.34E-6 8, α(P)=3.23E-7 5
844.62	0+,1+,2+		279.0 2	(M1)		0.0902	α=0.0902, α(K)=0.0768 11, α(L)=0.01055 15, α(M)=0.00225 4, α(N)=0.000507 8, α(O)=7.67×10^-5 11, α(P)=4.89E-6 7
532.15+X	10+		124.8 1	M1+E2		0.93	α=0.93 11, α(K)=0.66 4, α(L)=0.20 11, α(M)=0.046 25, α(N)=0.0100 54, α(O)=0.00135 64, α(P)=3.7×10^-5 9
1065.80	(+)		725.8 2	(M1)		0.00788	α=0.00788, α(K)=0.00674 10, α(L)=0.000898 13, α(M)=0.000191 3, α(N)=4.30×10^-5 6, α(O)=6.52E-6 10, α(P)=4.23E-7 6
934.29+X	11+		402.1 1	(M1+E2)	+0.07 4	0.0346	α=0.0346, α(K)=0.0295 5, α(L)=0.00401 6, α(M)=0.000853 12, α(N)=0.000192 3, α(O)=2.91×10^-5 5, α(P)=1.87E-6 3
1670.11	1+		825.5 2	M1		0.00577	α=0.00577, α(K)=0.00494 7, α(L)=0.000655 10, α(M)=0.0001390 20, α(N)=3.14×10^-5 5, α(O)=4.76E-6 7, α(P)=3.09E-7 5
1301.5+X	11(-)		495.1	E2		0.01262	α=0.01262, α(K)=0.01040 15, α(L)=0.001745 25, α(M)=0.000379 6, α(N)=8.45×10^-5 12, α(O)=1.221E-5 17, α(P)=6.03E-7 9
1308.41+X	12+		374.1 1	M1(+E2)	+0.08 10	0.0416	α=0.0416 7, α(K)=0.0355 6, α(L)=0.00484 7, α(M)=0.001031 15, α(N)=0.000232 4, α(O)=3.51×10^-5 6, α(P)=2.25E-6 4
1308.41+X	12+		776.4 2	E2		0.00412	α=0.00412, α(K)=0.00348 5, α(L)=0.000509 8, α(M)=0.0001092 16, α(N)=2.45×10^-5 4, α(O)=3.62E-6 5, α(P)=2.07E-7 3
1601.65+X	11(-)		795.5 1	E2		0.00390	α=0.00390, α(K)=0.00329 5, α(L)=0.000480 7, α(M)=0.0001028 15, α(N)=2.30×10^-5 4, α(O)=3.41E-6 5, α(P)=1.96E-7 3
1690.2+X	12(+)		755.9 3	(M1+E2)		0.0058	α=0.0058 14, α(K)=0.0049 12, α(L)=0.00068 14, α(M)=0.00014 3, α(N)=3.3×10^-5 7, α(O)=4.9E-6 11, α(P)=3.01E-7 82
1873.4+X	13+		565.0 2	M1+E2	+0.13 6	0.01452	α=0.01452 23, α(K)=0.01240 20, α(L)=0.00167 3, α(M)=0.000355 6, α(N)=8.00×10^-5 12, α(O)=1.211E-5 19, α(P)=7.81E-7 13
1873.4+X	13+		938.7	E2		0.00270	α=0.00270, α(K)=0.00229 4, α(L)=0.000323 5, α(M)=6.90×10^-5 10, α(N)=1.548E-5 22, α(O)=2.31E-6 4, α(P)=1.374E-7 20
1948.3+X	12(+)		1014.0	(M1+E2)		0.0029	α=0.0029 7, α(K)=0.0025 6, α(L)=0.00033 7, α(M)=7.1×10^-5 14, α(N)=1.6E-5 3, α(O)=2.4E-6 5, α(P)=1.5E-7 4
2097.0+X	13(-)		495.4 2	E2		0.01260	α=0.01260, α(K)=0.01038 15, α(L)=0.001742 25, α(M)=0.000378 6, α(N)=8.43×10^-5 12, α(O)=1.218E-5 18, α(P)=6.02E-7 9
2097.0+X	13(-)		795.2	E2		0.00391	α=0.00391, α(K)=0.00330 5, α(L)=0.000480 7, α(M)=0.0001028 15, α(N)=2.31×10^-5 4, α(O)=3.42E-6 5, α(P)=1.97E-7 3
2209.2+X	12(+)		1274.8 3	(M1+E2)		0.0018	α=0.0018 4, α(K)=0.0015 3, α(L)=0.00020 4, α(M)=4.2×10^-5 8, α(N)=9.5E-6 17, α(O)=1.4E-6 3, α(P)=9.2E-8 19
2266.2+X	13(+)		576.0	(M1+E2)		0.011	α=0.011 3, α(K)=0.0095 25, α(L)=0.00136 24, α(M)=0.00029 5, α(N)=6.5×10^-5 12, α(O)=9.8E-6 19, α(P)=5.8E-7 17
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2332.1+X	14+		458.9	(M1+E2)		0.020	α=0.020 5, α(K)=0.017 5, α(L)=0.0025 4, α(M)=0.00054 7, α(N)=0.000122 16, α(O)=1.8×10^-5 3, α(P)=1.03E-6 30
2332.1+X	14+		1023.6	E2		0.00225	α=0.00225, α(K)=0.00191 3, α(L)=0.000265 4, α(M)=5.65×10^-5 8, α(N)=1.270E-5 18, α(O)=1.90E-6 3, α(P)=1.147E-7 16
2354.2+X	14+		1045.8	E2		0.00215	α=0.00215, α(K)=0.00183 3, α(L)=0.000253 4, α(M)=5.38×10^-5 8, α(N)=1.210E-5 17, α(O)=1.81E-6 3, α(P)=1.097E-7 16
2444.1+X	12(+)		1509.5	(M1+E2)		0.00130	α=0.00130 20, α(K)=0.00105 17, α(L)=0.000137 21, α(M)=2.9×10^-5 5, α(N)=6.5E-6 10, α(O)=9.9E-7 16, α(P)=6.4E-8 11
2557.1+X	14+		1248.6 2	E2		1.51×10^-3	α=1.51×10^-3, α(K)=0.001277 18, α(L)=0.0001721 25, α(M)=3.66E-5 6, α(N)=8.23E-6 12, α(O)=1.236E-6 18, α(P)=7.68E-8 11
2570.7+X	14+		697.4 2	(M1+E2)		0.0070	α=0.0070 17, α(K)=0.0059 15, α(L)=0.00083 17, α(M)=0.00018 4, α(N)=4.0×10^-5 8, α(O)=6.0E-6 13, α(P)=3.7E-7 11
2570.7+X	14+		1262.5 7	E2		1.48×10^-3	α=1.48×10^-3, α(K)=0.001249 18, α(L)=0.0001681 24, α(M)=3.57E-5 5, α(N)=8.04E-6 12, α(O)=1.207E-6 17, α(P)=7.51E-8 11
2595.5+X	13(+)		905.1	(M1+E2)		0.0038	α=0.0038 9, α(K)=0.0032 8, α(L)=0.00044 9, α(M)=9.3×10^-5 18, α(N)=2.1E-5 5, α(O)=3.2E-6 7, α(P)=1.98E-7 50
2625.2+X	14(-)		528.2 2	(M1+E2)		0.014	α=0.014 4, α(K)=0.0118 30, α(L)=0.0017 3, α(M)=0.00037 6, α(N)=8.3×10^-5 13, α(O)=1.23E-5 22, α(P)=7.2E-7 21
2664.7+X	13(+)		455.2	(M1+E2)		0.021	α=0.021 5, α(K)=0.017 5, α(L)=0.0026 4, α(M)=0.00055 7, α(N)=0.000124 16, α(O)=1.8×10^-5 3, α(P)=1.05E-6 31
2664.7+X	13(+)		974.3	(M1+E2)		0.0032	α=0.0032 7, α(K)=0.0027 6, α(L)=0.00037 8, α(M)=7.8×10^-5 15, α(N)=1.8E-5 4, α(O)=2.7E-6 6, α(P)=1.7E-7 4
2747.8+X	15(-)		177.1 3	[E1]		0.0565	α=0.0565, α(K)=0.0480 7, α(L)=0.00664 10, α(M)=0.001409 21, α(N)=0.000314 5, α(O)=4.59×10^-5 7, α(P)=2.54E-6 4
2747.8+X	15(-)		190.6 3	[E1]		0.0463	α=0.0463, α(K)=0.0395 6, α(L)=0.00543 8, α(M)=0.001152 17, α(N)=0.000257 4, α(O)=3.76×10^-5 6, α(P)=2.10E-6 3
2776.7+X	13(+)		1468.4 3	(M1+E2)		0.00136	α=0.00136 21, α(K)=0.00111 18, α(L)=0.000145 23, α(M)=3.1×10^-5 5, α(N)=6.9E-6 11, α(O)=1.05E-6 17, α(P)=6.8E-8 12
2830.0+X	15(-)		732.8	E2		0.00472	α=0.00472, α(K)=0.00397 6, α(L)=0.000589 9, α(M)=0.0001265 18, α(N)=2.83×10^-5 4, α(O)=4.18E-6 6, α(P)=2.36E-7 4
2905.7+X	14(+)		240.9 3	(M1+E2)		0.121	α=0.121 13, α(K)=0.098 16, α(L)=0.0181 25, α(M)=0.0040 7, α(N)=0.00088 13, α(O)=0.000126 13, α(P)=5.8×10^-6 15
2905.7+X	14(+)		310.1 3	(M1+E2)		0.059	α=0.059 10, α(K)=0.048 10, α(L)=0.00803 14, α(M)=0.00174 6, α(N)=0.000389 9, α(O)=5.65×10^-5 15, α(P)=2.90E-6 80
2992.5+X	16(-)		244.8 2	(M1+E2)		0.116	α=0.116 13, α(K)=0.094 15, α(L)=0.0172 22, α(M)=0.0038 6, α(N)=0.00084 12, α(O)=0.000120 11, α(P)=5.5×10^-6 15
3132.6+X	15(+)		226.9 2	(M1+E2)		0.145	α=0.145 13, α(K)=0.117 17, α(L)=0.022 4, α(M)=0.0049 10, α(N)=0.00108 20, α(O)=0.000154 20, α(P)=6.8×10^-6 17
3285.9+X	(15+)		297.4	(M1+E2)		0.066	α=0.066 11, α(K)=0.054 11, α(L)=0.0092 3, α(M)=0.00199 10, α(N)=0.000444 18, α(O)=6.43×10^-5 10, α(P)=3.25E-6 88
3372.8+X	16(-)		747.6 2	E2		0.00450	α=0.00450, α(K)=0.00379 6, α(L)=0.000560 8, α(M)=0.0001202 17, α(N)=2.69×10^-5 4, α(O)=3.98E-6 6, α(P)=2.26E-7 4
3386.6+X	16(+)		254.0 2	(M1+E2)		0.104	α=0.104 12, α(K)=0.085 15, α(L)=0.0152 17, α(M)=0.0033 5, α(N)=0.00074 9, α(O)=0.000106 8, α(P)=5.0×10^-6 13
3498.4+X	17(-)		505.9	(M1+E2)		0.016	α=0.016 4, α(K)=0.0131 34, α(L)=0.0019 3, α(M)=0.00041 6, α(N)=9.3×10^-5 14, α(O)=1.38E-5 24, α(P)=8.1E-7 24
3519.0+X	17(-)		688.8	E2		0.00546	α=0.00546, α(K)=0.00458 7, α(L)=0.000691 10, α(M)=0.0001486 21, α(N)=3.33×10^-5 5, α(O)=4.90E-6 7, α(P)=2.72E-7 4
3652.3+X	17(+)		265.8	(M1+E2)		0.091	α=0.091 12, α(K)=0.074 13, α(L)=0.0131 11, α(M)=0.0029 3, α(N)=0.00064 6, α(O)=9.2×10^-5 5, α(P)=4.4E-6 12
3652.3+X	17(+)		519.7	E2		0.01109	α=0.01109, α(K)=0.00917 13, α(L)=0.001511 22, α(M)=0.000327 5, α(N)=7.31×10^-5 11, α(O)=1.059E-5 15, α(P)=5.34E-7 8
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
3887.2+X	18(-)		894.7	E2		0.00300	α=0.00300, α(K)=0.00254 4, α(L)=0.000361 5, α(M)=7.72×10^-5 11, α(N)=1.733E-5 25, α(O)=2.58E-6 4, α(P)=1.522E-7 22
3935.2+X	18(-)		416.2	(M1+E2)		0.026	α=0.026 6, α(K)=0.022 6, α(L)=0.0033 4, α(M)=0.00072 7, α(N)=0.000161 16, α(O)=2.4×10^-5 3, α(P)=1.33E-6 39
4043.0+X	18(+)		390.7	(M1+E2)		0.031	α=0.031 7, α(K)=0.026 6, α(L)=0.0040 4, α(M)=0.00086 6, α(N)=0.000193 15, α(O)=2.8×10^-5 3, α(P)=1.57E-6 45
4128.2+X	18(-)		755.4	E2		0.00439	α=0.00439, α(K)=0.00370 6, α(L)=0.000546 8, α(M)=0.0001170 17, α(N)=2.62×10^-5 4, α(O)=3.88E-6 6, α(P)=2.20E-7 3
4393.0+X	19(-)		894.6 3	E2		0.00300	α=0.00300, α(K)=0.00254 4, α(L)=0.000361 5, α(M)=7.72×10^-5 11, α(N)=1.733E-5 25, α(O)=2.58E-6 4, α(P)=1.522E-7 22
4484.4+X	19(-)		597.2	(M1+E2)		0.0102	α=0.0102 25, α(K)=0.0087 23, α(L)=0.00124 23, α(M)=0.00026 5, α(N)=5.9×10^-5 11, α(O)=8.9E-6 18, α(P)=5.3E-7 16
4486.0+X	18(-)		892.5	E2		0.00302	α=0.00302, α(K)=0.00256 4, α(L)=0.000363 5, α(M)=7.77×10^-5 11, α(N)=1.743E-5 25, α(O)=2.59E-6 4, α(P)=1.530E-7 22
4486.0+X	18(-)		966.9	(M1+E2)		0.0032	α=0.0032 8, α(K)=0.0028 7, α(L)=0.00037 8, α(M)=8.0×10^-5 16, α(N)=1.8E-5 4, α(O)=2.7E-6 6, α(P)=1.7E-7 5
4508.0+X	19(+)		465.0	(M1+E2)		0.019	α=0.019 5, α(K)=0.016 4, α(L)=0.0024 4, α(M)=0.00052 7, α(N)=0.000117 15, α(O)=1.7×10^-5 3, α(P)=1.00E-6 29
4721.2+X	20(-)		785.9	E2		0.00401	α=0.00401, α(K)=0.00338 5, α(L)=0.000494 7, α(M)=0.0001059 15, α(N)=2.37×10^-5 4, α(O)=3.52E-6 5, α(P)=2.02E-7 3
4864.5+X	19(-)		736.3	(M1+E2)		0.0061	α=0.0061 15, α(K)=0.0052 13, α(L)=0.00072 15, α(M)=0.00015 3, α(N)=3.5×10^-5 7, α(O)=5.2E-6 11, α(P)=3.21E-7 88
4956.4+X	19(-)		828.2	(M1+E2)		0.0046	α=0.0046 11, α(K)=0.0040 10, α(L)=0.00054 11, α(M)=0.000115 23, α(N)=2.6×10^-5 6, α(O)=3.9E-6 9, α(P)=2.43E-7 64
5012.4+X	20(+)		504.4	(M1+E2)		0.016	α=0.016 4, α(K)=0.0132 34, α(L)=0.0019 3, α(M)=0.00042 6, α(N)=9.4×10^-5 14, α(O)=1.39E-5 24, α(P)=8.1E-7 24
5019.8+X	20(-)		891.6	E2		0.00302	α=0.00302, α(K)=0.00256 4, α(L)=0.000364 5, α(M)=7.79×10^-5 11, α(N)=1.747E-5 25, α(O)=2.60E-6 4, α(P)=1.533E-7 22
5356.4+X	21(+)		344.0	(M1+E2)		0.044	α=0.044 9, α(K)=0.036 8, α(L)=0.00584 22, α(M)=0.00126 3, α(N)=0.000283 9, α(O)=4.1×10^-5 3, α(P)=2.20E-6 62
5525.2+X	21(-)		505.4	(M1+E2)		0.016	α=0.016 4, α(K)=0.0132 34, α(L)=0.0019 3, α(M)=0.00041 6, α(N)=9.3×10^-5 14, α(O)=1.38E-5 24, α(P)=8.1E-7 24
6391.5+X	23(-)		866.3	E2		0.00322	α=0.00322, α(K)=0.00273 4, α(L)=0.000390 6, α(M)=8.34×10^-5 12, α(N)=1.87E-5 3, α(O)=2.78E-6 4, α(P)=1.631E-7 23

Other experimental papers: 2011Ti05 (production σ for ^natW and ¹⁸¹Ta targets irradiated with 0.04-2.6 GeV protons) 1995Ve08, 1995VeZX (β-decay energy)

Above the 8- isomer, the levels schemes proposed in (HI,xnγ) and (¹⁹F,5nγ) are discrepant, of which the E(level)’s and γ-rays placements of (¹⁹F,5nγ) are preferred.

Q(β-)=-2758 keV 27	S(n)= 8785 keV 28	S(p)= 3490 keV 40	Q(α)= 702 keV 27
Reference: 2017WA10

References:
A	¹⁴⁰Sm ε decay	B	¹²⁶Te(¹⁹F,5nγ)
C	(HI,xnγ)

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A	1+	9.2 s 2 % ε = 100
139.95 7	A	(2)-		140.0 1	100	E1	0.0	1+
225.47 6	A	0+,1+,2+		225.4 1	100	M1	0.0	1+
260.64 8	A	(1,2,3)+		35.2 2 120.8 1 260.6 2	2.7 9 100 9.4	(M1+E2) E1	225.47 139.95 0.0	0+,1+,2+ (2)- 1+
335.35 9	A	+		109.9 2 195.4 2 335.5 2	100 20.4 10.2	M1	225.47 139.95 0.0	0+,1+,2+ (2)- 1+
339.88 7	A	(1,2)+		114.6 2 199.9 2 339.8 1	53.3 38.9 100	M1 E1 E2	225.47 139.95 0.0	0+,1+,2+ (2)- 1+
344.94 8	A	+		84.4 1 119.5 2 204.9 2 344.9 2	100 20.8 7.7 73.9	M1 M1,E2 (E2)	260.64 225.47 139.95 0.0	(1,2,3)+ 0+,1+,2+ (2)- 1+
415.15 11	A	1+		75.3 2 189.6 2 415.3 2	100 10.3 38.5	M1	339.88 225.47 0.0	(1,2)+ 0+,1+,2+ 1+
0.0+X	A B C	8-	5.95 m 5 % ε = 100
481.18 9	A	+		136.4 2 141.3 2 145.7 2 220.7 1 255.6 2 481.1 2	45 37.5 32.5 100 22.5 12.5	M1 [M1,E2] M1 (M1) (M1)	344.94 339.88 335.35 260.64 225.47 0.0	+ (1,2)+ + (1,2,3)+ 0+,1+,2+ 1+
503.39 11	A	0+,1+,2+		158.5 2 163.6 2 503.3 2	100 14.3 90.5	(M1) (M1) M1	344.94 339.88 0.0	+ (1,2)+ 1+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
534.03 15	A	(+)		308.7 2 533.9 2	60 100	(M1) (E2)	225.47 0.0	0+,1+,2+ 1+
565.46 8	A	(1+,2+)		150.4 2 220.6 1 339.8 1 425.6 2 565.6 2	20 100 20 22 66	(M1) (M1) (E2) (M1)	415.15 344.94 225.47 139.95 0.0	1+ + 0+,1+,2+ (2)- 1+
572.11 11	A	(1+,2+)		237.0 2 311.4 2 431.9 2 572.2 2	33 83 20 100	(M1) (M1) (M1)	335.35 260.64 139.95 0.0	+ (1,2,3)+ (2)- 1+
576.27 14	A	(0-,1-,2-)		436.3 2 576.3 2	15 100	(E1)	139.95 0.0	(2)- 1+
652.36 10	A			312.4 2 427.0 2 652.5 2	100 59 100		339.88 225.47 0.0	(1,2)+ 0+,1+,2+ 1+
670.17 16	A	(+)		409.5 2	100	(M1)	260.64	(1,2,3)+
761.35 13	A	(+)		421.6 2 761.5 2	100	(E2)	339.88 0.0	(1,2)+ 1+
386.23+X 10	B C	8+	1.0 ns +10-5	386.2 1	100	E1	0.0+X	8-
808.16 21	A			468.5 3 668.2 2 808.3?	36 6 100 18		339.88 139.95 0.0	(1,2)+ (2)- 1+
407.28+X 16	B C	9+		21.3S 407.5 2	100	E1	386.23+X 0.0+X	8+ 8-
844.62 11	A	0+,1+,2+		279.0 2 341.3 2 844.8 2	23 100 30	(M1)	565.46 503.39 0.0	(1+,2+) 0+,1+,2+ 1+
855.81 11	A			520.5 2 630.5 2 855.8 2	100 40 67		335.35 225.47 0.0	+ 0+,1+,2+ 1+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
874.29 15	A			648.9 2 874.2 2	52 100		225.47 0.0	0+,1+,2+ 1+
926.33 15	A			586.3 2 701.0 2 926.3 2 ?	61 100 32		339.88 225.47 0.0	(1,2)+ 0+,1+,2+ 1+
532.15+X 17	B C	10+		124.8 1	100	M1+E2	407.28+X	9+
951.30 16	A			951.1 2	100		0.0	1+
1065.80 16	A	(+)		725.8 2 1065.5 5 ?	100 13	(M1)	339.88 0.0	(1,2)+ 1+
1088.99 20	A			863.5 2 1089.1 5	46 100		225.47 0.0	0+,1+,2+ 1+
1173.91 16	A			608.3 2	100		565.46	(1+,2+)
806.15+X 16	B C	9(-)		273.7 2 399.4 2 419.8 2 805.7 4	76 3 31 5 100 11 55 8	D D	532.15+X 407.28+X 386.23+X 0.0+X	10+ 9+ 8+ 8-
1278.8 5	A			1018.2 5 1053.5 5 ?	100 60		260.64 225.47	(1,2,3)+ 0+,1+,2+
934.29+X 20	B C	11+		402.1 1	100	(M1+E2)	532.15+X	10+
1594.6 3	A			1022.6 5 1249.5 5 1254.7 5 1594.7 5 ?	55 100 62 12		572.11 344.94 339.88 0.0	(1+,2+) + (1,2)+ 1+
1618.2 4	A			1278.1 5 1283.0 5	100 95		339.88 335.35	(1,2)+ +
1619.25 11	A	1+		445.2 2 774.7 2 858.0 5 967.0 2 1046.9 5 1116.0 5 1138.1 3 1274.2 3 1393.5 3 1479.9 5 1619.1 5 ?	7.8 22.8 2.2 10 10 12.8 100 88.9 66.7 6.1 3.3		1173.91 844.62 761.35 652.36 572.11 503.39 481.18 344.94 225.47 139.95 0.0	0+,1+,2+ (+) (1+,2+) 0+,1+,2+ + + 0+,1+,2+ (2)- 1+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1623.09 15	A	1+		671.6 2 862.0 2 1119.6 5 1278.1 5 1283.0 5 1397.5 5 1623.0 5 ?	7.1 36 43 100 95 27 5.4		951.30 761.35 503.39 344.94 339.88 225.47 0.0	(+) 0+,1+,2+ + (1,2)+ 0+,1+,2+ 1+
1670.11 10	A	1+		604.2 2 814.5 2 825.5 2 999.9 2 1017.8 2 1093.9 5 1098.0 5 1166.7 5 1188.9 5 1324.9 5 1330.0 5 1444.4 5 1530.2 3 1670.0 5	16.9 23.9 57.7 9.2 11.5 9.2 40 53 10.8 33.9 23.9 10.8 100 33.9	M1	1065.80 855.81 844.62 670.17 652.36 576.27 572.11 503.39 481.18 344.94 339.88 225.47 139.95 0.0	(+) 0+,1+,2+ (+) (0-,1-,2-) (1+,2+) 0+,1+,2+ + + (1,2)+ 0+,1+,2+ (2)- 1+
1301.5+X 8	B	11(-)		495.1	100	E2	806.15+X	9(-)
1308.41+X 21	B C	12+		374.1 1 776.4 2	100 3 8.5 21	M1(+E2) E2	934.29+X 532.15+X	11+ 10+
1601.65+X 19 ?	C	11(-)		795.5 1	100	E2	806.15+X	9(-)
2017.4 5	A			1677.5 5	100		339.88	(1,2)+
1690.2+X 4	B C	12(+)		755.9 3	100	(M1+E2)	934.29+X	11+
1873.4+X 3	B C	13+		565.0 2 938.7	100 5 12 3	M1+E2 E2	1308.41+X 934.29+X	12+ 11+
1948.3+X 11	B	12(+)		1014.0	100	(M1+E2)	934.29+X	11+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2097.0+X 3	B C	13(-)		495.4 2 ? 795.2		E2 E2	1601.65+X 1301.5+X	11(-) 11(-)
2209.2+X 4	B C	12(+)		1274.8 3	100	(M1+E2)	934.29+X	11+
2266.2+X 11	B	13(+)		576.0	100	(M1+E2)	1690.2+X	12(+)
2332.1+X 8	B	14+		458.9 1023.6	100 9 50 23	(M1+E2) E2	1873.4+X 1308.41+X	13+ 12+
2354.2+X 11	B	14+		1045.8	100	E2	1308.41+X	12+
2444.1+X 8	B	12(+)		1509.5	100	(M1+E2)	934.29+X	11+
2557.1+X 3	B C	14+		1248.6 2	100	E2	1308.41+X	12+
2570.7+X 3	B C	14+		697.4 2 1262.5 7	100 7 60 8	(M1+E2) E2	1873.4+X 1308.41+X	13+ 12+
2595.5+X 5	B C	13(+)		386.0 905.1	71 14 100 14	D+Q (M1+E2)	2209.2+X 1690.2+X	12(+) 12(+)
2625.2+X 4	B C	14(-)		528.2 2	100	(M1+E2)	2097.0+X	13(-)
2664.7+X 5	B C	13(+)		220.2 455.2 974.3	20 4 41 6 100 14	(M1+E2) (M1+E2)	2444.1+X 2209.2+X 1690.2+X	12(+) 12(+) 12(+)
2747.8+X 4	B C	15(-)		177.1 3 190.6 3	100 7 24 2	[E1] [E1]	2570.7+X 2557.1+X	14+ 14+
2776.7+X 4	B C	13(+)		1468.4 3	100	(M1+E2)	1308.41+X	12+
2830.0+X 9	B	15(-)		732.8	100	E2	2097.0+X	13(-)
2905.7+X 4	B C	14(+)		129.1 3 240.9 3 310.1 3	40 10 80 20 100 30	D+Q (M1+E2) (M1+E2)	2776.7+X 2664.7+X 2595.5+X	13(+) 13(+) 13(+)
2988.5+X 8	B	(14+)		324.0 1115.0	<7 100 21		2664.7+X 1873.4+X	13(+) 13+
2992.5+X 4	B C	16(-)		244.8 2	100	(M1+E2)	2747.8+X	15(-)
3132.6+X 5	B C	15(+)		226.9 2	100	(M1+E2)	2905.7+X	14(+)
3285.9+X 13	B	(15+)		297.4	100	(M1+E2)	2988.5+X	(14+)
3372.8+X 4	B C	16(-)		747.6 2	100	E2	2625.2+X	14(-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3386.6+X 5	B C	16(+)		254.0 2	100	(M1+E2)	3132.6+X	15(+)
3498.4+X 8	B C	17(-)		505.9 750.6	100 8 11 4	(M1+E2)	2992.5+X 2747.8+X	16(-) 15(-)
3519.0+X 10	B	17(-)		688.8	100	E2	2830.0+X	15(-)
3593.5+X 9	B	(16-)		220.8	100		3372.8+X	16(-)
3610.0+X 16	B	(16+)		324.1	100		3285.9+X	(15+)
3652.3+X 8	B C	17(+)		265.8 519.7	100 4 6 1	(M1+E2) E2	3386.6+X 3132.6+X	16(+) 15(+)
3887.2+X 9	B	18(-)		388.8 894.7	100 10 67 10	E2	3498.4+X 2992.5+X	17(-) 16(-)
3935.2+X 12	B	18(-)		416.2	100	(M1+E2)	3519.0+X	17(-)
4002.8+X 19	B	(17+)		392.8	100		3610.0+X	(16+)
4043.0+X 9	B C	18(+)		390.7 656.5	100 5 2.3 6	(M1+E2)	3652.3+X 3386.6+X	17(+) 16(+)
4128.2+X 9	B C	18(-)		534.6 755.4	9.2 25 100 9	E2	3593.5+X 3372.8+X	(16-) 16(-)
4393.0+X 8 ?	C	19(-)		894.6 3	100	E2	3498.4+X	17(-)
4484.4+X 10	B	19(-)		597.2 986.0	100 13 13 8	(M1+E2)	3887.2+X 3498.4+X	18(-) 17(-)
4486.0+X 11	B	18(-)		892.5 966.9	20 8 100 25	E2 (M1+E2)	3593.5+X 3519.0+X	(16-) 17(-)
4508.0+X 10	B C	19(+)		465.0 855.7	100 6 7.0 12	(M1+E2)	4043.0+X 3652.3+X	18(+) 17(+)
4721.2+X 12	B	20(-)		593.1 785.9	<5.3 100 21	E2	4128.2+X 3935.2+X	18(-) 18(-)
4864.5+X 14	B	19(-)		736.3	100	(M1+E2)	4128.2+X	18(-)
4956.4+X 14	B	19(-)		828.2	100	(M1+E2)	4128.2+X	18(-)
5012.4+X 11	B	20(+)		504.4 969.4	100 8 15 7	(M1+E2)	4508.0+X 4043.0+X	19(+) 18(+)
5019.8+X 14	B C	20(-)		891.6	100	E2	4128.2+X	18(-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5356.4+X 12	B	21(+)		344.0 848.4	100 13 <4.4	(M1+E2)	5012.4+X 4508.0+X	20(+) 19(+)
5525.2+X 17	B	21(-)		505.4	100	(M1+E2)	5019.8+X	20(-)
5786.2+X 17	B	(21-)		921.7	100		4864.5+X	19(-)
5941.4+X 16	B	(22+)		585.0	100		5356.4+X	21(+)
6391.5+X 20	B	23(-)		866.3	100	E2	5525.2+X	21(-)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - Band based on 15(+).
3132.6+X 5	15(+)
3386.6+X 5	16(+)		254.0 2	100	(M1+E2)	3132.6+X	15(+)
3652.3+X 8	17(+)		265.8 519.7	100 4 6 1	(M1+E2) E2	3386.6+X 3132.6+X	16(+) 15(+)
4043.0+X 9	18(+)		390.7 656.5	100 5 2.3 6	(M1+E2)	3652.3+X 3386.6+X	17(+) 16(+)
4508.0+X 10	19(+)		465.0 855.7	100 6 7.0 12	(M1+E2)	4043.0+X 3652.3+X	18(+) 17(+)
5012.4+X 11	20(+)		504.4 969.4	100 8 15 7	(M1+E2)	4508.0+X 4043.0+X	19(+) 18(+)
5356.4+X 12	21(+)		344.0 848.4	100 13 <4.4	(M1+E2)	5012.4+X 4508.0+X	20(+) 19(+)
5941.4+X 16	(22+)		585.0	100		5356.4+X	21(+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - Band based on (14⁺).
2988.5+X 8	(14+)
3285.9+X 13	(15+)		297.4	100	(M1+E2)	2988.5+X	(14+)
3610.0+X 16	(16+)		324.1	100		3285.9+X	(15+)
4002.8+X 19	(17+)		392.8	100		3610.0+X	(16+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - Probable πh_11/2~#νh_11/2 band.
407.28+X 16	9+
532.15+X 17	10+		124.8 1	100	M1+E2	407.28+X	9+
934.29+X 20	11+		402.1 1	100	(M1+E2)	532.15+X	10+
1308.41+X 21	12+		374.1 1 776.4 2	100 3 8.5 21	M1(+E2) E2	934.29+X 532.15+X	11+ 10+
1873.4+X 3	13+		565.0 2 938.7	100 5 12 3	M1+E2 E2	1308.41+X 934.29+X	12+ 11+
2332.1+X 8	14+		458.9 1023.6	100 9 50 23	(M1+E2) E2	1873.4+X 1308.41+X	13+ 12+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - Band based on 15(-).
2747.8+X 4	15(-)
2992.5+X 4	16(-)		244.8 2	100	(M1+E2)	2747.8+X	15(-)
3498.4+X 8	17(-)		505.9 750.6	100 8 11 4	(M1+E2)	2992.5+X 2747.8+X	16(-) 15(-)
3887.2+X 9	18(-)		388.8 894.7	100 10 67 10	E2	3498.4+X 2992.5+X	17(-) 16(-)
4484.4+X 10	19(-)		597.2 986.0	100 13 13 8	(M1+E2)	3887.2+X 3498.4+X	18(-) 17(-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - Possible πh_11/2~#ν1/2[411]
806.15+X 16	9(-)
1301.5+X 8	11(-)		495.1	100	E2	806.15+X	9(-)
2097.0+X 3	13(-)		495.4 2 ? 795.2		E2 E2	1601.65+X 1301.5+X	11(-) 11(-)
2830.0+X 9	15(-)		732.8	100	E2	2097.0+X	13(-)
3519.0+X 10	17(-)		688.8	100	E2	2830.0+X	15(-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - Band based on 14(-).
2625.2+X 4	14(-)
3372.8+X 4	16(-)		747.6 2	100	E2	2625.2+X	14(-)
4128.2+X 9	18(-)		534.6 755.4	9.2 25 100 9	E2	3593.5+X 3372.8+X	(16-) 16(-)
5019.8+X 14	20(-)		891.6	100	E2	4128.2+X	18(-)

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1+	9.2 s 2 % ε = 100	J^π(level): log ft\|<5.7 via 0⁺ parent.
407.28+X	9+		E(level): Probable πh_11/2~#νh_11/2 band.
532.15+X	10+		E(level): Probable πh_11/2~#νh_11/2 band.
806.15+X	9(-)		E(level): Possible πh_11/2~#ν1/2[411].
934.29+X	11+		E(level): Probable πh_11/2~#νh_11/2 band.
1619.25	1+		J^π(level): log ft\|<5.7 via 0⁺ parent.
1623.09	1+		J^π(level): log ft\|<5.7 via 0⁺ parent.
1670.11	1+		J^π(level): log ft\|<5.7 via 0⁺ parent.
1301.5+X	11(-)		E(level): Possible πh_11/2~#ν1/2[411].
1308.41+X	12+		E(level): Probable πh_11/2~#νh_11/2 band.
1690.2+X	12(+)		E(level): Possible member of a 4-qp configuration.
1873.4+X	13+		E(level): Probable πh_11/2~#νh_11/2 band.
1948.3+X	12(+)		E(level): Possible member of a 4-qp configuration.
2097.0+X	13(-)		E(level): Possible πh_11/2~#ν1/2[411].
2209.2+X	12(+)		E(level): Possible member of a 4-qp configuration.
2266.2+X	13(+)		E(level): Possible member of a 4-qp configuration.
2332.1+X	14+		E(level): Probable πh_11/2~#νh_11/2 band.
2354.2+X	14+		E(level): Possible member of a 4-qp configuration.
2444.1+X	12(+)		E(level): Possible member of a 4-qp configuration.
2557.1+X	14+		E(level): Possible member of a 4-qp configuration.
2570.7+X	14+		E(level): Possible member of a 4-qp configuration.
2595.5+X	13(+)		E(level): Possible member of a 4-qp configuration.
2625.2+X	14(-)		E(level): Band based on 14(-).
2664.7+X	13(+)		E(level): Possible member of a 4-qp configuration.
2747.8+X	15(-)		E(level): Band based on 15(-).
E(level)	J^π(level)	T_1/2(level)	Comments
2776.7+X	13(+)		E(level): Possible member of a 4-qp configuration.
2830.0+X	15(-)		E(level): Possible πh_11/2~#ν1/2[411].
2905.7+X	14(+)		E(level): Possible member of a 4-qp configuration.
2988.5+X	(14+)		E(level): Band based on (14⁺).
2992.5+X	16(-)		E(level): Band based on 15(-).
3132.6+X	15(+)		E(level): Band based on 15(+).
3285.9+X	(15+)		E(level): Band based on (14⁺).
3372.8+X	16(-)		E(level): Band based on 14(-).
3386.6+X	16(+)		E(level): Band based on 15(+).
3498.4+X	17(-)		E(level): Band based on 15(-).
3519.0+X	17(-)		E(level): Possible πh_11/2~#ν1/2[411].
3593.5+X	(16-)		E(level): Possible member of a 6-qp configuration.
3610.0+X	(16+)		E(level): Band based on (14⁺).
3652.3+X	17(+)		E(level): Band based on 15(+).
3887.2+X	18(-)		E(level): Band based on 15(-).
3935.2+X	18(-)		E(level): Possible member of a 6-qp configuration.
4002.8+X	(17+)		E(level): Band based on (14⁺).
4043.0+X	18(+)		E(level): Band based on 15(+).
4128.2+X	18(-)		E(level): Band based on 14(-).
4484.4+X	19(-)		E(level): Band based on 15(-).
4486.0+X	18(-)		E(level): Possible member of a 6-qp configuration.
4508.0+X	19(+)		E(level): Band based on 15(+).
4721.2+X	20(-)		E(level): Possible member of a 6-qp configuration.
4864.5+X	19(-)		E(level): Possible member of a 6-qp configuration.
4956.4+X	19(-)		E(level): Possible member of a 6-qp configuration.
E(level)	J^π(level)	T_1/2(level)	Comments
5012.4+X	20(+)		E(level): Band based on 15(+).
5019.8+X	20(-)		E(level): Band based on 14(-).
5356.4+X	21(+)		E(level): Band based on 15(+).
5525.2+X	21(-)		E(level): Possible member of a 6-qp configuration.
5786.2+X	(21-)		E(level): Possible member of a 6-qp configuration.
5941.4+X	(22+)		E(level): Band based on 15(+).
6391.5+X	23(-)		E(level): Possible member of a 6-qp configuration.

E(level)	E(gamma)	Comments
806.15+X	273.7	I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
	399.4	I(γ): From ¹²⁶Te(¹⁹F,5nγ)
	419.8	I(γ): From ¹²⁶Te(¹⁹F,5nγ)
	805.7	I(γ): From ¹²⁶Te(¹⁹F,5nγ)
1301.5+X	495.1	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
1308.41+X	776.4	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
1690.2+X	755.9	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
1873.4+X	565.0	I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
1873.4+X	938.7	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
1948.3+X	1014.0	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2097.0+X	795.2	E(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2209.2+X	1274.8	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2266.2+X	576.0	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2332.1+X	458.9	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2332.1+X	1023.6	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2354.2+X	1045.8	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2444.1+X	1509.5	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2557.1+X	1248.6	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2570.7+X	697.4	I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2570.7+X	1262.5	I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2595.5+X	386.0	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ)
2595.5+X	905.1	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2625.2+X	528.2	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2664.7+X	220.2	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ)
	455.2	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
	974.3	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
E(level)	E(gamma)	Comments
2747.8+X	177.1	I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): relatively pure stretched d, Δπ=yes E1 based on proposed configuration in (¹⁹F,5nγ) (2010Wa37). From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2747.8+X	190.6	I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): relatively pure stretched d, Δπ=yes E1 based on proposed configuration in (¹⁹F,5nγ) (2010Wa37). From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2776.7+X	1468.4	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2830.0+X	732.8	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2905.7+X	240.9	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2905.7+X	310.1	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
2988.5+X	324.0	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ)
2988.5+X	1115.0	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ)
2992.5+X	244.8	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
3132.6+X	226.9	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
3285.9+X	297.4	E(γ): From ¹²⁶Te(¹⁹F,5nγ) I(γ): From ¹²⁶Te(¹⁹F,5nγ) M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).
3372.8+X	747.6	M(γ): From ¹²⁶Te(¹⁹F,5nγ) based on measurements of DCO ratios (2010Wa37), γ(θ), and linear pol ((1981PoZV, 1982PoZX) , from in ¹²⁶Te(¹⁹F,5nγ). When linear pol is not available Q transitions are most likely E2 based on heavy ion reaction type, deformation, and rotational character of the bands; and admixed D+Q transitions are tentatively M1⁺E2 (combined with level scheme arguments). Few pure d transitions were adopted as E1 (also combined with level scheme arguments).