192IR 191IR(N,G) E=THERMAL 1991KE10 192IR C Secondary 1991KE10. Others: 1989DU03, 1988BA49, 1980SIZT, 1976RA25. 192IR2C See also the reference list with 191IR(N,G) E=thermal: Primary. 192IR C All secondary EG and IG data in this data set are from (N,G) E=thermal; 192IR2C however, documentation for E=resonance (several) and E=reactor spectrum 192IR3C studies yielding secondary G information, and additional data 192IR4C available from those sources, are also included in this data set (as 192IR5C indicated). 192IR C 1976RA25 (E=thermal): measured precise EG in 40-600-KEV range 192IR2C (curved crystal spect); report EG values for a few placed 192IR3C transitions, plus EG for G's in the 155-165-KEV range. 192IR C 1980SIZT (E=reactor spectrum): measured ECE, ICE (mag spect); 192IR2C report multipolarities, but do not describe measurements. 192IR C 1988BA49 (E=thermal): measured EG, IG (curved crystal spect 192IR2C (to 640 KEV)), ECE, ICE (mag spect (to 215 KEV)). 192IR C 1989DU03 (E=thermal): measured EG, IG in 20-60-KEV range 192IR2C (SILI, FWHM=300 EV at 17 KEV, 350 EV at 30 KEV). 192IR C 1991KE10 (E=thermal). EG, IG data: curved-crystal spectrometer (FWHM=5 192IR2C arcsec), COMPTON-suppression spectrometer and GELI detectors (for 192IR3C isotopic identification and IG calibration, natural IR, 86% and 88.8% 192IR4C 191IR targets. Conversion electron data: magnetic spectrometer 192IR5C (momentum resolution 0.19% at 30 KEV, 0.06% at 190 KEV), 94.3% 191IR 192IR6C target, measured E(ce) (19-280 KEV), I(ce); calibration based on 192IR7C ten unspecified transitions. GG coin data: HP Ge (FWHM AP 500 EV at 192IR8C 60 KEV) and GELI spectrometer (FWHM=2.5 KEV at 100 KEV), timing 192IR9C resolution FWHM=35 NS, deduced level T from GG(T) or centroid shift. 192IRAC Supersedes earlier reports by some of the same authors in 1988BA49, 192IRBC 1980SIZT, 1976RA25. See also 1997BAZV for suggested placement of 192IRCC some transitions which were reported but not placed by 1991KE10. 192IR C 1991KE10 (E=resonance): E(resonance)=0.655 EV (J=1), 5.36 EV (J=1), 192IR2C 6.13 EV (J=2); pulsed n beam, TOF, natural IR target, GELI detector, 192IR3C measured E(n), EG (secondaries), IG; deduced level JPI from population 192IR4C ratios of secondary gammas, defined as RI(at J=2 resonance)/RI(at J=1 192IR5C resonance) (expected ratios are 1.1 (J=2), 2.4 (J=3), assuming J=1 192IR6C for 236 level whose ratio is 0.85). 192IR C The level scheme is from 1991KE10, with the addition of fourteen levels 192IR2C defined by G placements suggested in 1997BAZV, the addition of four 192IR3C transitions deexciting previously established levels (1997BAZV), and 192IR4C relocation of the 126.958G as suggested in 1997BAZV. Since the levels 192IR5C introduced by 1997BAZV seem somewhat speculative and have not yet been 192IR6C published, the evaluator shows all but the 441 level (supported 192IR7C by GG coin) as tentative. 192IR CL E From least-squares adjustment of EG. 192IR CL T From GG(T) or centroid shift (1991KE10). 192IR CL J From adopted levels. See 1991KE10 for authors' JPI based on 192IR2CL G multipolarities and decay patterns in (N,G) E=thermal, 192IR3CL reduced intensities of primary gammas in average 192IR4CL resonance capture, population ratios for secondary gammas following 192IR5CL capture in isolated J=1 and J=2 resonances, level population 192IR6CL in (D,P) and (D,T) reactions (i.e., all data from 1991KE10). 192IR CG RI$Secondary photon intensity (for E=thermal) relative to 192IR2CG IG(84.3)=100 10 (1991KE10), except as noted. 192IR CG M,MR$Secondary from ce data of 1991KE10. Note that, in most cases, some 192IR2CG E2 admixture is possible for multipolarities designated as M1. 192IR CG E(A),RI(A)$Secondary from 1989DU03 (E=thermal). 192IR CG E(E),RI(E)$May be a |g in 193IR arising from double neutron capture 192IR2CG (1991KE10). 192IR CG E(F) From 1971KR09; unconfirmed by 1991KE10, so probably does not 192IR2CG belong in 192IR. 192IR CL E(G),J(G) Level introduced by 1997BAZV; based on NILSSON model 192IR2CL calculations, G decay patterns and mult. 192IR CG E(G) Placement from 1997BAZV. 192IR CL BAND(U) |g BAND (1991KE10). 192IR CL BAND(V) POSSIBLE CONF=((|p 11/2[505])-(|n 9/2[505])) (1991KE10). 192IR CL BAND(W) POSSIBLE CONF=((|p 3/2[402])-(|n 3/2[512])) (1991KE10). 192IR2CL The levels assigned to this band by 1991KE10 differ from those assigned 192IR3CL in adopted levels on the basis of later transfer reaction data. 192IR CL BAND(X) POSSIBLE CONF=((|p 1/2[400])-(|n 3/2[512])) (1991KE10). 192IR2CL The levels assigned to this band by 1991KE10 differ from those assigned 192IR3CL in adopted levels on the basis of later transfer reaction data. 192IR CL BAND(Y) POSSIBLE CONF=((|p 3/2[402])-(|n 1/2[510])) (1991KE10). 192IR C Primary 1991KE10, 1971KR09. Others: 1959BA05, 1959KN63, 1966WA02, 192IR2C 1967DO08, 1973PRZI, 1975PRZP, 1978COZD, 1979SIZU, 1983MUZU, 1988MU26. 192IR C All primary EG and IG data in this data set are from (N,G) E=thermal, 192IR2C with the exception of the 6112G (as noted). However, 192IR3C documentation for E=resonance (several) and E=reactor spectrum studies 192IR4C is also included in this data set, for completeness. 192IR C 1971KR09 (E=thermal): measured EG, IG (GELI-scin pair spect). 192IR C 1983MUZU (E=resonance: avg): measured averaged intensities 192IR2C of primary G's (GELI); determined JPI for low-lying states. 192IR C 1988MU26 (E=reactor spectrum, filtered beam): measured EG, IG 192IR2C (GELI-NAI-NAI 3-crystal pair spect). 192IR C 1991KE10 (E=thermal): natural IR, 86% 191IR and 98.1% 193IR targets, 192IR2C pair spectrometer (EG calibration based on 14N(N,G)); measured EG, IG. 192IR C The level scheme and all data are from 1991KE10, unless noted 192IR2C otherwise. 1988MU26 favor an alternative level scheme, with capture 192IR3C state at 6169 KEV and JPI=4- for ground state. 192IR CG E$Primary from 1991KE10, unless noted otherwise. 192IR CG RI$Primary relative values from 1991KE10 for E=thermal, normalized so 192IR2CG RI(5668.6G)=100.0, except as noted. See comment with 192IR3CG normalization to obtain absolute intensities. 192IR CL E(A) Adopted value. 192IR CL E(B) Probable doublet (see adopted levels, gammas), 192IR2CL with JPI components indicated. 192IR CG E(A),RI(A)$Numerically resolved from overlapping peaks. 192IR CG E(B) Observed in epithermal capture (1971KR09); because of poor 192IR2CG energy precision, transition was not used to establish a 192IR3CG corresponding level. 192IR CG E(Z),RI(Z)$From 1971KR09. Primary intensities have been scaled so 192IR2CG I(6092G+6081G) in 1971KR09 is the same as I(6093G+6082G+6079G) in 192IRxCG 1991KE10. 192IR N 0.023 3 192IR CN NR$Secondary from IG(58.84)=1.20 3 per 100 neutron captures (E=thermal, 192IR2CN 1989DU03); values were calibrated to SIGMAN=954 10 (1984MUZY). The 192IR3CN listed uncertainties in IG do not include an 11% uncertainty due to 192IR4CN absolute calibration. This uncertainty is included in the normalization 192IR5CN factor. With this normalization, SUMOF(TI to GS+13+16+57) AP 71%. 192IR CN NR$Primary from I(6079G+6082G+i6093g)=9.1 per 1000 captures if 192IR2CN SIGMAN=924 53 (1971KR09), revised by evaluator assuming SIGMAN=954 10 192IR3CN (1984MUZY). With this normalization, SUMOF IG(primary) AP 15%. 192IR4CN Placed on same scale as secondary. 192IR cN SIGMAN=954 43 192IR G 19.71 3 0.25 4 (M1) A 192IR CG EM1C=38 11 for (19.7G+20.0G) doublet (1991KE10); authors do 192IR2CG not state the subshell measured, but their deduced mult suggests the 192IR3CG M1 subshell. M1C(M1 theory)=20. 192IR G 19.96 2 0.34 4 (M1) A 192IR CG EM1C=38 11 for (19.7G+20.0G) doublet (1991KE10); authors do 192IR2CG not state the subshell measured, but their deduced mult suggests the 192IR3CG M1 subshell. M1C(M1)=20. 192IR G 47.443 16 2.70 19 M1 192IR2 G EL1C=8.0 25 (1991KE10) 192IR G 68.443 20 0.7 4 192IR G 83.371 11 1.4 7 M1 192IR2 G EL1C=3.5 25 (1991KE10) 192IR G 90.66 4 0.8 4 192IR G 90.794 25 1.8 5 192IR G 98.410 25 0.9 5 192IR G 99.62 3 3.0 6 M1 192IR2 G EKC=3.3 18 (1991KE10) 192IR G 100.76 8 E0 192IR CG M 1991KE10 observe ce but no G; they estimate IG<2. 192IR G 102.29 3 1.4 4 M1 192IR2 G EKC=9 5 (1991KE10) 192IR G 105.497 20 3.0 6 192IR2 G EKC=1.2 6 (1991KE10) 192IR G 120.153 5 2.0 4 192IR G 122.748 15 1.9 6 M1 192IR2 G EKC=4.2 16 (1991KE10) 192IR G 124.771 5 10.7 11 M1 192IR2 G EKC=1.9 5 (1991KE10) 192IR CG Population ratio>1.5 in (N,G) E=resonance (1991KE10) favors 192IR2CG J=3,4 or possibly 2 for parent level. 192IR G 126.586 9 1.8 5 192IR G 128.59 4 1.2 6 192IR G 130.90 9 1.5 8 192IR G 133.083 8 2.1 5 M1 192IR2 G EKC=2.0 11 (1991KE10) 192IR G 134.157 10 2.4 6 M1 192IR2 G EKC=1.8 10 (1991KE10) 192IR G 138.942 5 5.7 7 M1 E 192IR2 G EKC=1.9 3 (1991KE10) 192IR G 140.17 5 1.4 7 192IR G 142.210 25 2.1 5 M1 192IR2 G EKC=2.4 13 (1991KE10) 192IR G 144.356 7 3.0 6 192IR G 146.902 6 3.3 5 M1 192IR2 G EKC=1.8 9 (1991KE10) 192IR G 149.953 5 2.4 6 192IR G 151.275 20 1.1 6 192IR G 151.754 4 4.3 6 M1 192IR2 G EKC=2.5 10 (1991KE10) 192IR G 155.354 17 1.8 5 192IR G 159.495 3 7.6 8 E2 192IR2 G EKC=0.5 3 (1991KE10) 192IR G 161.966 11 1.4 4 192IR G 162.370 8 2.2 5 M1 192IR2 G EKC=1.4 7 (1991KE10) 192IR G 165.084 18 2.9 4 M1 192IR2 G EKC=1.3 7 (1991KE10) 192IR G 165.417 11 2.3 5 M1 192IR2 G EKC=1.3 6 (1991KE10) 192IR G 165.568 4 9.3 11 M1 192IR2 G EKC=1.3 4 (1991KE10) 192IR G 172.18 5 1.0 5 192IR G 173.707 13 1.3 7 M1 192IR2 G EKC=1.2 7 (1991KE10) 192IR G 175.11 7 0.50 25 192IR G 175.376 25 1.6 4 192IR G 177.052 25 1.3 7 192IR G 177.395 20 1.4 7 192IR G 178.21 5 0.50 25 192IR G 180.724 4 10.8 11 M1 192IR2 G EKC=1.1 2 (1991KE10) 192IR CG Population ratio=0.91 20 in (N,G) E=resonance (1991KE10) 192IR2CG favors J=1 or possibly 2 for parent level. 192IR G 181.32 3 1.0 3 192IR G 181.80 4 0.7 4 E 192IR G 182.74 4 1.0 3 192IR G 183.310 15 0.8 4 192IR G 185.051 18 1.6 5 192IR G 185.50 4 0.8 4 192IR G 188.60 7 0.6 3 192IR G 190.216 5 5.2 6 M1 192IR2 G EKC=0.9 3 (1991KE10) 192IR CG Population ratio>2.0 in (N,G) E=resonance (1991KE10) favors 192IR2CG J=3,4 for parent level. 192IR G 192.676 25 1.8 5 192IR G 193.93 4 1.5 8 192IR G 195.09 4 1.5 5 192IR G 195.656 25 2.3 6 192IR G 195.94 3 2.2 7 192IR G 196.725 25 1.5 5 192IR G 197.95 3 1.3 4 192IR G 201.246 12 8.5 9 M1 192IR2 G EKC=0.94 18 (1991KE10) 192IR G 202.255 9 4.6 6 M1 192IR2 G EKC=0.80 26 (1991KE10) 192IR G 203.676 14 2.7 4 192IR G 204.078 11 4.8 6 M1 192IR2 G EKC=0.63 20 (1991KE10) 192IR G 204.469 25 4.5 7 M1 192IR2 G EKC=0.44 23 (1991KE10) 192IR G 211.194 6 15.1 12 M1 192IR2 G EKC=0.47 16 (1991KE10) 192IR G 219.160 4 20.3 20 E1 E 192IR2 G EKC=0.044 10 (1991KE10) 192IR G 219.72 8 0.8 4 192IR G 222.180 10 5.6 7 M1 192IR2 G EKC=0.68 14 (1991KE10) 192IR CG Population ratio=0.87 17 in (N,G) E=resonance (1991KE10) 192IR2CG favors J=1 or possibly 2 for parent level. 192IR G 222.42 10 0.8 4 192IR G 225.21 8 1.1 3 192IR G 228.228 25 1.6 3 192IR G 230.235 20 1.6 5 192IR G 231.40 5 3.7 6 192IR G 234.602 20 1.2 4 E 192IR G 238.561 20 1.4 4 192IR G 245.162 20 1.5 4 192IR G 245.671 10 4.7 6 M1 192IR2 G EKC=0.43 17 (1991KE10) 192IR G 245.83 4 1.6 5 192IR G 247.81 4 1.6 5 192IR G 248.56 12 0.4 2 192IR G 250.750 6 11.5 12 M1 192IR2 G EKC=0.37 10 (1991KE10) 192IR CG Population ratio=1.35 26 in (N,G) E=resonance (1991KE10) 192IR2CG favors J=2 for parent level. 192IR G 255.375 20 1.8 5 192IR G 255.74 3 4.4 7 E1,E2 192IR2 G EKC<0.23 (1991KE10) 192IR G 259.336 8 9.8 12 M1 192IR2 G EKC=0.38 7 (1991KE10) 192IR CG Population ratio=1.6 5 in (N,G) E=resonance (1991KE10) favors 192IR2CG J=2,3 for parent level. 192IR G 261.743 25 2.7 7 192IR G 262.48 4 2.2 6 192IR G 267.99 6 0.50 25 192IR G 269.56 10 2.0 4 192IR G 270.363 17 6.2 9 M1 192IR2 G EKC=0.32 14 (1991KE10) 192IR G 271.30 6 3.2 6 192IR G 274.57 4 1.6 5 192IR G 276.93 4 1.7 5 192IR G 278.50 4 1.9 5 192IR G 280.56 8 2.8 6 E 192IR G 289.838 16 4.4 7 M1 192IR2 G EKC=0.23 12 (1991KE10) 192IR G 296.622 20 4.5 14 M1 192IR2 G EKC=0.33 16 (1991KE10) 192IR G 297.78 10 1.1 3 192IR G 298.849 18 3.7 7 E 192IR G 300.279 15 6.2 9 E2 192IR2 G EKC=0.11 5 (1991KE10) 192IR G 302.57 6 1.8 5 192IR G 303.73 4 2.3 5 192IR G 313.671 25 4.3 9 192IR CG EKC=0.24 9, mult=M1 (1991KE10) for 313.7G+314.4G doublet. 192IR G 314.402 16 6.0 9 192IR CG EKC=0.24 9, mult=M1 (1991KE10) for 313.7G+314.4G doublet. 192IR G 318.46 4 4.5 9 192IR G 319.68 10 0.9 5 192IR G 323.75 4 4.4 9 192IR G 330.876 17 10.4 16 M1 192IR2 G EKC=0.19 6 (1991KE10) 192IR G 337.408 25 5.8 12 192IR G 339.93 4 3.5 9 192IR G 341.22 8 1.2 4 192IR G 345.272 25 4.7 12 192IR G 347.32 4 9.2 18 M1 192IR2 G EKC=0.16 5 (1991KE10) 192IR G 352.80 5 3.2 10 192IR G 355.70 15 0.6 3 192IR G 357.82 6 6.0 12 E 192IR G 359.42 15 2.5 8 192IR G 361.85 6 2.8 8 E 192IR G 364.54 6 5.5 11 192IR G 366.47 4 7.0 14 192IR G 367.454 25 9.8 15 192IR G 371.34 3 6.3 9 192IR G 374.60 7 4.5 14 192IR G 380.67 6 3.8 11 192IR G 381.86 6 4.9 15 192IR G 382.914 25 10.0 15 E 192IR G 389.06 4 5.8 15 192IR G 392.78 11 4.0 10 192IR G 398.59 6 4.9 10 192IR G 401.24 14 8.5 12 192IR G 405.30 13 7.7 19 192IR G 406.18 15 7.5 19 192IR G 409.24 8 5.1 15 192IR G 414.48 8 7.1 21 192IR G 425.36 8 8.5 21 192IR G 440.98 8 6.7 20 E 192IR G 449.73 7 16.0 24 192IR G 452.42 12 6.6 20 192IR G 466.5 15 F 192IR G 482.93 15 7.7 23 192IR G 490.44 6 17.6 26 192IR G 504.6 3 3.7 19 192IR G 509.64 15 8.1 24 192IR G 521.60 17 5.3 27 192IR G 525.54 14 5.1 26 192IR G 534.81 13 8.0 24 192IR G 557.5 15 F 192IR G 574.78 18 13 6 192IR G 599.51 14 19 8 192IR G 618.60 20 18 9 192IR G 622.6 15 F 192IR G 632.9 3 20 10 192IR G 692.5 15 F 192IR L 0.0 4+ 192IR CL Probable 192IR2CL CONF=((|p 3/2[402])-(|n 11/2[615]))+((|p 11/2[505])-(|n 3/2[512])) 192IR3CL (1991KE10). 192IR L 12.987 9 (6+) G ? 192IR L 16.041 10 (6-) G ? 192IR L 56.719 5 1- Y 192IR G 56.71 3 0.69 9 E3 2840 192IR2 G EL2C=1070 160 (1991KE10) 192IR CG From subshell ratios of 1991KE10, viz., 192IR2CG L1:L2:L3:M2:M3:M4+M5:N2+N3=2.7 13:100 8:92 11:28 4:22.5 23:2.9 5:17 3. 192IR CG E from ce data (1991KE10). Other EG: 56.67 2 (1989DU03). 192IR CG RI from 1989DU03. 192IR L 66.823 12 (4-) 15 NS 4 192IR G 50.78010 1.6410 E2 100.2 A ? 192IR2 G EL2C=33 4 (1991KE10) 192IRF G FLAG=G 192IR CG M from L1:L2:L3:M2:M3:N2+N3=7 4:100 10:111 17:26 8:26 8:18 9 192IR2CG (1991KE10). 192IR G 66.83 2 16.213 [E1] 0.234 192IR L 84.274 3 3- 1.9 NS 4 192IR CL Possible bandhead for CONF=((|p 3/2[402])-(|n 9/2[505])) 192IR2CL (1991KE10). 192IR G 84.276 3 10010 E1 0.624 192IR2 G EL1C=0.113 25 (1991KE10) 192IR CG M from L1:L2:L3:M1=100 20:45 13:53 13:26 8 (1991KE10). 192IR2CG Mult=E1+M2, MR=+0.055 +10-13 from EL1C alone is considered less 192IR3CG reliable than results based on subshell ratios. 192IR L 104.776 5 (1)- 17.4 NS 26 X 192IR G 48.0568 8 79 4 M1+E2 0.163 10 12.6 3 192IR2 G EL1C=6.2 7 (1991KE10) 192IR CG M,MR from L1:L2:L3:M1:M2:N1=100 10:29 4:23 3:24 5:8.9 26:8.1 16 192IR2CG (authors' analysis, 1991KE10) 192IR CG RI from 1989DU03. 192IR L 115.563 5 (2)- Y 192IR G 58.843810 51.816 M1+E2 0.227 5 7.39 7 192IR2 G EL1C=2.8 7 (1991KE10) 192IR CG RI from 1989DU03. 192IR CG MR from authors' analysis of unenumerated subshell ratios 192IR2CG (L1, L2, L3, M1, M2, M3, N1 shells). 192IR L 118.7824 17 3- 15 NS GT 192IR CL Possible bandhead for CONF=((|p 3/2[402])+(|n 3/2[512])) 192IR2CL (1991KE10). 192IR G 34.52010 0.30021 M1 25.2 A 192IR2 G EL1C=16 5 (1991KE10) 192IR G 118.781718 6.9 8 E1 0.260 192IR2 G EKC<0.5 (1991KE10) 192IR CG Population ratio>1.5 in (N,G) E=resonance (1991KE10) favors 192IR2CG J=3,4 for parent level. 192IR L 128.742 5 (0)- W 192IR G 23.970 6 2.1113 M1 A 192IR2 G EM1C=16 3 (1991KE10) 192IR G 72.025 3 7.619 M1 192IR2 G EL1C=1.3 5 (1991KE10) 192IR G 128.73625 1.3 7 ? 192IR L 139.945 10 (5+) G ? 192IR G 126.958 3 24.024 M1 3.20 G ? 192IR2 G EKC=2.8 7 (1991KE10) 192IR CG Population ratio>6.0 in (N,G) E=resonance (1991KE10); from 192IR2CG this ratio 1997BAZV and 1991KE10 favor J=5 and 4, respectively, for 192IR3CG parent level. Therefore, the evaluator does not adopt 192IR4CG the placement of the 127G from the J=2, 320 level suggested 192IR5CG in 1991KE10. 192IR L 143.554 5 (1)- W 192IR G 28.01010 0.22018 M1 A 192IR2 G EL1C=31 13 (1991KE10) 192IR G 38.80 2 0.32 3 M1 A 192IR2 G EL1C=12 6 (1991KE10) 192IR G 86.837 5 10 2 M1 192IR2 G EL1C=1.2 3 (1991KE10) 192IR L 144.904 5 (5+) G ? 192IR G 144.904 5 38 4 (M1) 2.195 G ? 192IR CG M EKC=1.6 3 (1991KE10) for (144.8G+144.9G) doublet dominated by 192IR2CG the latter G. 192IR L 173.2 7 192IR L 192.932 5 (2)- 192IR G 49.39010 1.51 9 M1 A 192IR2 G EL1C=7 3 (1991KE10) 192IR G 77.368 4 4.714 M1 192IR2 G EL1C=1.4 6 (1991KE10) 192IR G 108.66812 1.4 4 M1 192IR2 G EKC=5 3 (1991KE10) 192IR G 136.210 6 49 6(M1,E2) 192IR CG EKC=1.8 3, mult=M1 (1991KE10) for (136.2G+136.1G) favors 192IR2CG mult=M1,E2 for this transition. 192IR L 193.509 5 (1)+ 2.7 NS 6 V 192IR G 49.97010 1.42 9 D A 192IR2 G EL1C=8.3 21 (1991KE10) 192IR CG M EL1C allows mult=M1 or E1+M2 (MR=0.21 3); the latter is 192IR2CG required by level scheme, but MR violates RUL. 192IR G 77.9466 8 5010 E1 0.760 192IR2 G EL1C=0.16 5 (1991KE10) 192IR G 88.7335 8 53 5 E1 0.547 192IR2 G EL1C=0.18 4 (1991KE10) 192IR CG M from L1:L2:L3:M1=100 20:38 18:38 18:27 13 (1991KE10). 192IR2CG Mult=E1+M2, MR=+0.091 +13-15 from EL1C alone is considered less 192IR3CG reliable than result based on subshell ratios. 192IR G 136.792 2 27.322 E1 0.181 192IR2 G EKC=0.26 9 (1991KE10) 192IR L 203.2 8 LE 3 192IR L 212.805 5 (1,2)- W 192IR G 69.252 6 3.1 9 M1 192IR2 G EL1C=2.6 11 (1991KE10) 192IR G 108.031816 31.525 M1 192IR2 G EKC=3.6 4 (1991KE10) 192IR CG M from K:L1:M1=100 10:13.2 26:7 3 192IR2CG mult=M1+E2, MR=+0.45 +18-22 from EKC alone is considered less 192IR3CG reliable than result based on subshell ratios. 192IR G 156.081 3 12.613 M1 192IR2 G EKC=1.1 3 (1991KE10) 192IR L 216.905 4 (4+) G ? 192IR G 216.905 4 46 4 M1 0.708 G ? 192IR2 G EKC=0.61 11 (1991KE10) 192IR CG Population ratio=3.0 10 in (N,G) E=resonance (1991KE10); from 192IR2CG this ratio 1997BAZV and 1991KE10 favor J=4 and 3, respectively, for 192IR3CG parent level. 192IR L 223.341 10 (6+) G ? 192IR G 207.302 6 6.2 7 E1 0.063 G ? 192IR2 G EKC<0.16 (1991KE10) 192IR G 210.353 5 9.3 9 [E2] 0.770 & ? 192IRF G FLAG=G 192IR CG EKC=0.45 16 (1991KE10), mult=M1(+E2) for multiply-placed G. 192IR L 225.915 5 (2)- 192IR G 32.981 7 0.70 4 M1 A 192IR2 G EL1C=13 4 (1991KE10) 192IR G 107.12910 2.8 7 M1 192IR2 G EKC=3.6 16 (1991KE10) 192IR G 110.358 4 6.6 8 M1 192IR2 G EKC=4.8 13 (1991KE10) 192IR G 121.136 7 2.0 4 M1 192IR2 G EKC=5.0 18 (1991KE10) 192IR G 169.202 7 23.023 E2 192IR2 G EKC=0.43 12 (1991KE10) 192IR CG M from 1991KE10, presumably based on K:L2:L3. mult=E2+M1, 192IR2CG MR=2.1 +21-6 based on EKC alone. 192IR L 226.261 6 (LE 2-) G ? 192IR G 169.541 5 6.5 8 & ? 192IRF G FLAG=G 192IR CG EKC=1.7 7, mult=M1 (1991KE10) for doubly-placed G. 192IR L 235.758 5 (1-) ? 192IR G 107.025 8 2.5 8 M1 E ? 192IR2 G EKC=4.0 18 (1991KE10) 192IR G 179.038 2 25.020 M1+E2 1.1 3 ? 192IR2 G EKC=0.58 10 (1991KE10) 192IR CG Population ratio=0.85 9 in (N,G) E=resonance (1991KE10); 192IR2CG J=1 assumed for parent level in order to normalize measured ratios. 192IR L 239.767 6 (1)- G ? 192IR G 26.96010 0.24017 A ? 192IR2 G EL1C=81 25 (1991KE10) 192IRF G FLAG=G 192IR CG EL1C is much larger than expected from M1 theory. 192IR G 111.025 3 12.212 M1 G ? 192IR2 G EKC=5.6 9 (1991KE10) 192IR L 240.900 5 (2)- X 192IR G 97.351 6 3.1 6 & 192IR CG EKC=5.5 18 (1991KE10), mult=M1 for doubly-placed G. 192IR G 136.124815 8010 M1 192IR CG EKC=1.8 3 (1991KE10) for (136.2G+136.1G) doublet in 192IR2CG which this transition is major component implies mult=M1 for this 192IR3CG transition. 192IR L 265.159 8 (0-) G ? 192IR G 208.437 7 3.8 6 M1 G ? 192IR2 G EKC=0.92 24 (1991KE10) 192IR L 267.126 5 (3)- W 192IR G 26.231 6 1.64 8 M1 A 192IR2 G EM1C=7.2 22 (1991KE10) 192IR G 54.324 4 3.8323 M1 192IR2 G EL1C=3.6 10 (1991KE10) 192IR CG RI from 1989DU03. 192IR CG Other EG: 54.340 8 (1989DU03). 192IR G 151.561 3 25.025 M1 192IR2 G EKC=1.5 3 (1991KE10) 192IR CG Population ratio=2.3 5 in (N,G) E=resonance (1991KE10) favors 192IR2CG J=3 for parent level. 192IR L 277.992 5 (4)- 192IR G 193.718 4 10.312 M1 192IR2 G EKC=0.78 25 (1991KE10) 192IR CG Population ratio>2.5 in (N,G) E=resonance (1991KE10) favors 192IR2CG J=3,4 for parent level. 192IR L 284.213 5 (2,3)+ V 192IR G 90.703515 16.425 M1 192IR2 G EKC=5.9 13 (1991KE10) 192IR CG M from K:L1:M1=100 16:22 3:6.2 21 (1991KE10). 192IR L 288.402 6 (2)- 192IR G 95.47 4 2.2 4 M1 192IR2 G EKC=6.6 24 (1991KE10) 192IR G 144.82811 7.011 192IR CG EKC=1.6 3 (1991KE10) for (144.8G+144.9G) doublet. 192IR G 172.841 4 5.9 6 M1 192IR2 G EKC=1.1 3 (1991KE10) 192IR G 183.624 6 9.311 M1 192IR2 G EKC=1.1 3 (1991KE10) 192IR CG Population ratio=1.5 4 in (N,G) E=resonance (1991KE10) favors 192IR2CG J=2 or possibly 3 for parent level. 192IR G 231.67 3 5.6 7 M1 192IR2 G EKC=0.36 15 (1991KE10) 192IR L 292.374 6 (2)- 192IR G 66.47214 1.2 6 M1 192IR2 G EL1C=4.2 27 (1991KE10) 192IR G 148.822 3 13.413 & 192IR CG EKC=1.6 3 (1991KE10), mult=M1 for doubly-placed G. 192IR G 176.82625 2.5 5 M1 192IR2 G EKC=1.4 7 (1991KE10) 192IR G 292.35 6 1.7 5 ? 192IR L 310.996 6 2- 192IR G 195.42614 3.3 8 192IR G 206.219 4 29.424 M1 192IR2 G EKC=0.63 11 (1991KE10) 192IR CG Population ratio=1.08 20 in (N,G) E=resonance (1991KE10) 192IR2CG favors J=2 or possibly 1 for parent level. 192IR G 226.74 4 2.3 5 M1 192IR2 G EKC=0.9 5 (1991KE10) 192IR G 254.27715 13.914 M1 192IR2 G EKC=0.28 13 (1991KE10) 192IR CG Population ratio=0.97 16 in (N,G) E=resonance (1991KE10) 192IR2CG favors J=2 or possibly 1 for parent level. 192IR L 319.892 7 (2)- 192IR G 191.16 4 0.8 4 ? 192IR G 201.10820 2.6 7 M1 192IR2 G EKC=1.3 6 (1991KE10) 192IR G 215.09112 2.9 4 M1 192IR2 G EKC=0.7 4 (1991KE10) 192IR L 331.074 5 (2)- 192IR G 105.15512 1.7 5 M1 192IR2 G EKC=7 4 (1991KE10) 192IR G 118.270 6 1.9 4 M1 192IR2 G EKC=3.7 20 (1991KE10) 192IR G 187.521 6 5.3 6 M1 192IR2 G EKC=0.8 2 (1991KE10) 192IR CG Population ratio=1.1 4 in (N,G) E=resonance (1991KE10) favors 192IR2CG J<3 for parent level. 192IR G 212.31 5 0.9 5 192IR G 215.519 8 3.0 5 M1 192IR2 G EKC=0.7 3 (1991KE10) 192IR G 226.297 3 30.024 M1 192IR2 G EKC=0.56 12 (1991KE10) 192IR CG Population ratio=1.08 12 in (N,G) E=resonance (1991KE10) 192IR2CG favors J=2 for parent level. 192IR G 246.80114 1.8 5 192IR L 331.757 5 (1)- 192IR G 90.854 5 2.5 5 M1 ? 192IR2 G EL1C=1.4 5 (1991KE10) 192IR G 138.247 4 6.6 8 E1,E2 192IR2 G EKC=0.45 23 (1991KE10) 192IR G 188.19 4 1.6 5 192IR G 203.018 8 3.3 5 M1 192IR2 G EKC=0.70 20 (1991KE10) 192IR G 216.196 4 8.010 M1 192IR2 G EKC=0.61 17 (1991KE10) 192IR G 275.04220 4.0 8 192IR L 351.690 4 (2)+ U 192IR G 158.17910 1.8 5 192IR G 232.89116 2.5 5 192IR G 267.41610 7.8 9 E1,E2 192IR2 G EKC<0.13 (1991KE10) 192IR CG Population ratio=1.25 35 in (N,G) E=resonance (1991KE10) 192IR2CG favors J=2 or possibly 1 for parent level. 192IR G 351.691 5 13516 E2 0.060 192IR2 G EKC=0.037 13 (1991KE10) 192IR L 365.651 6 (2-,3-) G ? 192IR G 98.524 4 4.0 6 M1 G ? 192IR2 G EKC=3.5 12 (1991KE10) 192IR G 139.736 9 3.4 5 M1 G ? 192IR2 G EKC=3.2 12 (1991KE10) 192IR L 366.730 7 (2)- 192IR G 140.83015 2.0 6 192IR G 223.18 3 2.2 4 192IR G 261.951 6 25.025 M1 192IR2 G EKC=0.30 5 (1991KE10) 192IR CG Population ratio=1.35 21 in (N,G) E=resonance (1991KE10) 192IR2CG favors J=2 for parent level. 192IR G 310.01 4 3.210 192IR L 368.352 7 (2)- 192IR G 101.22115 1.3 4 192IR G 263.571 8 10.711 M1 192IR2 G EKC=0.33 10 (1991KE10) 192IR G 284.07212 13.911 M1 192IR2 G EKC=0.26 4 (1991KE10) 192IR G 311.70 5 2.8 7 192IR L 380.3 5 192IR L 389.722 5 (2)- X 192IR G 97.351 6 3.1 6 & 192IR CG EKC=5.5 18 (1991KE10), mult=M1 for doubly-placed G. 192IR G 122.59910 2.3 7 M1 192IR2 G EKC=3.0 13 (1991KE10) 192IR G 148.822 3 13.413 & 192IR CG EKC=1.6 3 (1991KE10), mult=M1 for doubly-placed G. 192IR CG Population ratio=1.0 4 in (N,G) E=resonance (1991KE10) favors 192IR2CG J=1,2 for parent level. 192IR G 246.15212 1.8 5 192IR G 284.93914 6.4 8 M1+E2 1.1 +31-7 192IR2 G EKC=0.16 8 (1991KE10) 192IR G 305.45 5 2.7 5 192IR L 392.349 6 (1,2,3)- 192IR G 72.46412 1.1 6 192IR G 151.44425 3.2 6 192IR G 166.086 6 11.011 M1 G ? 192IR2 G EKC=1.2 2 (1991KE10) 192IR G 166.439 6 3.0 5 192IR G 199.41 4 1.7 5 M1 192IR2 G EKC=1.1 5 (1991KE10) 192IR G 273.57 4 2.2 7 192IR G 276.76216 6.610 E2 192IR2 G EKC=0.15 7 (1991KE10) 192IR L 415.038 9 1-,2-,3- 192IR G 83.95615 2.211 M1 192IR2 G EL1C=2.3 16 (1991KE10) 192IR G 104.02025 1.6 5 192IR G 174.14410 2.6 5 M1 192IR2 G EKC=2.1 11 (1991KE10) 192IR G 299.50 5 1.6 5 192IR G 358.34 8 2.7 8 192IR L 418.140 6 (3+,4+) U ? 192IR G 133.934 9 2.4 6 M1 ? 192IR2 G EKC=2.3 13 (1991KE10) 192IR G 273.25 3 6.1 9 & ? 192IRF G FLAG=G 192IR CG EKC=0.16 9, mult=E2 (1991KE10) for doubly-placed G. 192IR G 278.19916 5.2 6 E1,E2 G ? 192IR2 G EKC<0.19 (1991KE10) 192IR G 333.866 9 16.725 E1 ? 192IR2 G EKC=0.024 12 (1991KE10) 192IR G 418.11425 29 4 ? 192IR L 440.867 6 (3+) G 192IR G 156.653 3 22.218 (M1) G 192IR CG EKC=0.9 19 (1991KE10) obviously includes a typographical 192IR2CG error, presumably in the uncertainty (authors assign M1(+E2)). 192IR CG Placement supported by GG coin data. 192IR L 451.250 7 (1,2)- 192IR G 140.23714 4.0 6 M1 192IR2 G EKC=2.3 6 (1991KE10) 192IR G 162.82615 1.7 4 M1 ? 192IR2 G EKC=2.4 13 (1991KE10) 192IR G 210.353 5 9.3 9 & 192IR CG EKC=0.45 16 (1991KE10), mult=M1(+E2) for multiply-placed G. 192IR G 258.33825 3.0 6 M1 192IR2 G EKC=0.65 26 (1991KE10) 192IR G 322.55 4 4.7 9 192IR L 470.9 4 1-,2-,3- 192IR L 489.436 7 1-,2-,3- ? 192IR G 169.541 5 6.5 8 & ? 192IR CG EKC=1.7 7, mult=M1 (1991KE10) for doubly-placed G. 192IR G 197.072 8 4.5 9 M1 ? 192IR2 G EKC=0.8 3 (1991KE10) 192IR G 384.64 8 3.410 ? 192IR G 432.64 4 16.124 ? 192IR L 508.990 8 (2,3)- 192IR G 140.61015 1.2 6 192IR G 177.92612 3.5 7 M1 192IR2 G EKC=1.0 5 (1991KE10) 192IR G 189.09910 2.4 5 192IR G 220.57 4 1.0 3 192IR G 241.87215 2.6 5 M1 192IR2 G EKC=0.9 5 (1991KE10) 192IR G 273.25 3 6.1 9 & ? 192IR CG EKC=0.16 9, mult=E2 (1991KE10) for doubly-placed G. 192IR G 316.0210 2111 192IR2 G EKC=0.12 7 (1991KE10) 192IR G 365.44 4 6.413 192IR L 513.195 7 (4+) U ? 192IRF L FLAG=G 192IR G 72.326 5 3.511 M1 G ? 192IR2 G EL1C=2.0 8 (1991KE10) 192IR G 95.06812 3.0 6 M1 G ? 192IR2 G EKC=4.8 17 (1991KE10) 192IR L 516.5 5 1-,2-,3- 192IR L 529.166 9 (1-) G ? 192IR G 264.003 9 7.0 8 M1,E2 G ? 192IR2 G EKC=0.21 11 (1991KE10) 192IR G 302.91110 7.211 M1 G ? 192IR2 G EKC=0.28 9 (1991KE10) 192IR L 530.248 8 1-,2-,3- ? 192IR G 199.19012 4.910 M1 ? 192IR2 G EKC=0.65 18 (1991KE10) 192IR G 210.353 5 9.3 9 & ? 192IR CG EKC=0.45 16 (1991KE10), mult=M1(+E2) for multiply-placed G. 192IR L 537.3 4 192IR L 543.84 19 0- TO 3- 192IR L 560.5 4 192IR L 585.54 17 192IR L 602.56 21 0- TO 3- 192IR L 612.6 6 0- TO 3- 192IR L 628.9 3 1-,2-,3- 192IR L 633.71 24 192IR L 645.9 3 0- TO 3- 192IR L 657.8 8 192IR L 663.31 17 192IR L 670.637 12 (4+) G ? 192IR G 229.76911 4.0 6 M1 G ? 192IR2 G EKC=0.40 20 (1991KE10) 192IR G 252.54 6 4.1 6 M1,E2 G ? 192IR2 G EKC=0.24 12 (1991KE10) 192IR L 681.4 4 1-,2-,3- 192IR L 702.7 4 0- TO 3- 192IR L 707.9 6 192IR L 714.1 5 0- TO 3- 192IR L 734.0 5 192IR L 739.2 3 1-,2-,3- 192IR L 749.51 21 192IR L 766.72 19 1-,2-,3- 192IR L 777.5 4 0- TO 3- 192IR L 787.9 7 192IR L 797.1 3 192IR L 813.3 4 1-,2-,3- 192IR L 822.01 21 192IR L 841.06 21 0- TO 3- 192IR L 851.1 5 0- TO 3- 192IR L 865.5 4 0- TO 3- 192IR L 870.6 4 192IR L 884.5 4 1-,2-,3- 192IR L 893.65 19 192IR L 906.4 24 1-,2-,3- 192IR L 914.45 21 192IR L 937.3 3 0- TO 3- 192IR L 944.4 5 192IR L 950.0 4 192IR L 962.6 13 0- TO 3- 192IR L 977.9 3 192IR L 999.3 3 192IR L 1003.5 4 192IR L 1013.7 3 0- TO 3- 192IR L 1020 3 1-,2-,3- ? 192IR L 1031.21 24 192IR L 1045.6 5 192IR L 1050.56 19 1-,2-,3- 192IR L 1059.92 21 192IR L 1068.83 19 192IR L 1075.0 5 192IR L 1088.5 7 192IR L 1092.8 7 192IR L 1106.97 21 192IR L 1112.5 4 192IR L 1131.2 5 192IR L 1144.5 6 192IR L 1151.6 7 192IR L 1155.8 3 192IR L 1160.4 5 192IR L 1169.4 3 192IR L 1177.71 24 192IR L 1195.2 5 192IR L 1204.71 24 192IR L 1212.11 24 192IR L 1217.2 3 192IR L 1226.1 3 192IR L 1232.1 5 192IR L 1242.9 3 192IR L 1249.0 4 192IR L 1254.9 3 192IR L 1259.2 3 192IR L 1265.2 4 192IR L 1273.2 11 192IR L 1282.2 5 192IR L 1290.7 6 192IR L 1299.4 3 192IR L 1304.1 4 192IR L 1323.0 3 192IR L 1331.12 19 192IR L 1338.8 5 192IR L 1343.3 6 192IR L 1348.3 4 192IR L 1359.8 5 192IR L 1365.9 6 192IR L 1372.0 5 192IR L 1380.0 6 192IR L 1387.4 6 192IR L 1396.4 4 192IR L 1409.0 7 192IR L 1418.28 24 192IR L 1432.5 3 192IR L 1436.7 6 192IR L 1441.7 7 192IR L 1448.02 24 192IR L 1463.9 3 192IR L 1469.2 5 192IR L 1486.3 4 192IR L 1494.9 7 192IR L 1502.1 7 192IR L 1514.4 5 192IR L 1529.9 3 192IR L 1534.8 3 192IR L 1552.2 5 192IR L 1558.0 7 192IR L 1571.0 5 192IR L 1586.3 7 192IR L 1596.6 7 192IR L 1607.9 4 192IR L 1625.8 4 192IR L 1634.4 10 192IR L 1641.1 9 192IR L 1648.1 6 192IR L 1658.6 5 192IR L 1666.9 4 192IR L 1676.4 5 192IR L 1692.0 5 192IR L 1702.6 5 192IR L 6198.10 5 1+,2+ S 192IR cL E$6198.08 20 from 1995Au04. 192IR2cL Observed deexcitation intensity is 25% of GS feeding. 192IR G 4495.1 7 2.5 4 Z 192IR G 4505.7 7 2.5 4 Z 192IR G 4521.3 7 2.1 4 A 192IRF G FLAG=Z 192IR G 4530.8 6 7.514 A 192IRF G FLAG=Z 192IR G 4539.1 7 3.3 8 A 192IRF G FLAG=Z 192IR G 4549.6 9 2.2 8 A 192IRF G FLAG=Z 192IR G 4556.613 2.2 8 A 192IRF G FLAG=Z 192IR G 4563.314 1.714 A 192IRF G FLAG=Z 192IR G 4571.9 6 5.6 8 Z 192IR G 4589.8 6 6.414 Z 192IR G 4601.110 1.4 8 Z 192IR G 4611.410 1.4 8 Z 192IR G 4626.7 7 1.7 4 Z 192IR G 4640.010 1.9 7 192IR G 4645.8 7 2.9 6 192IR G 4663.2 5 2.8 8 192IR G 4668.2 5 3.911 192IR G 4683.6 8 1.1 7 192IR G 4695.610 0.8 4 Z 192IR G 4702.810 0.8 4 Z 192IR G 4711.4 6 2.1 4 Z 192IR G 4728.8 7 1.6 7 192IR G 4734.1 5 5.611 192IR G 4750.0 4 3.9 8 192IR G 4756.310 1.0 6 192IR G 4761.410 1.2 7 192IR G 4765.6 6 4.4 8 192IR G 4779.8 4 5.3 6 192IR G 4789.010 1.3 7 192IR G 4801.6 6 1.7 4 192IR G 4810.6 9 4.8 6 192IR G 4818.0 9 2.8 8 192IR G 4826.0 8 1.4 4 192IR G 4832.2 9 1.3 4 192IR G 4838.2 8 1.9 5 192IR G 4849.7 6 2.5 8 192IR G 4854.710 3.5 6 192IR G 4859.2 8 6.7 8 192IR G 4866.9 3 8.9 8 192IR G 4875.1 5 4.4 8 192IR G 4893.9 5 4.211 192IR G 4898.7 6 5.011 192IR G 4907.0 8 1.3 4 Z 192IR G 4915.5 7 7.517 Z 192IR G 4924.515 1.4 8 Z 192IR G 4932.8 6 2.9 7 192IR G 4938.9 6 3.111 192IR G 4943.2 5 5.314 192IR G 4949.0 6 3.111 192IR G 4955.2 5 1.9 8 192IR G 4966.0 7 1.7 8 192IR G 4971.9 5 3.1 5 192IR G 4980.8 4 7.5 8 192IR G 4985.9 4 6.9 8 192IR G 4993.3 4 3.5 6 192IR G 5002.8 7 4.4 6 192IR G 5020.3 4 5.8 8 192IR G 5028.6 4 3.1 8 192IR G 5037.6 7 1.9 8 192IR G 5042.2 4 7.214 192IR G 5046.411 1.5 4 192IR G 5053.5 9 2.6 7 192IR G 5066.8 8 1.2 4 192IR G 5085.5 5 2.8 7 192IR G 5091.1 3 4.6 5 192IR G 5105.210 1.3 5 192IR G 5109.610 1.4 8 192IR G 5123.0 7 1.4 8 192IR G 5129.2 3 8.1 8 192IR G 5138.1 3 4.3 6 192IR G 5147.5 3 14.514 192IR G 5152.5 8 2.5 8 192IR G 5166.8 4 11.411 192IR G 5178 4 0.817 A ? 192IRF G FLAG=Z 192IR G 5184.4 4 2.5 7 192IR G 5194.5 7 4.411 192IR G 5198.7 6 4.711 192IR G 5220.1 5 7.514 192IR G 5235.118 0.4 4 Z 192IR G 5248.0 5 1.4 8 192IR G 5253.6 8 1.4 8 192IR G 5260.7 6 2.8 6 192IR G 5283.6 4 9.214 192IR G 5291 4 0.817 Z 192IR G 5304.4 3 8.9 8 192IR G 5313.6 6 1.911 192IR G 5327.5 6 8.117 192IR G 5332.5 6 5.611 192IR G 5346.9 7 2.2 8 192IR G 5357.0 3 8.914 192IR G 5376.0 3 3.7 4 192IR G 5384.7 6 3.5 4 192IR G 5400.9 5 3.8 4 192IR G 5409.810 0.3 8 Z 192IR G 5420.5 5 2.2 8 192IR G 5431.3 3 10.6 8 192IR G 5448.5 3 6.0 6 192IR G 5458.8 5 5.811 192IR G 5464.0 8 5.014 192IR G 5483.9 7 2.1 7 192IR G 5490.1 9 2.3 3 192IR G 5495.3 5 2.2 8 192IR G 5516.7 5 6.7 7 192IR G 5534.7 3 16.414 192IR G 5540.213 0.6 5 192IR G 5552.2 5 2.5 7 192IR G 5564.3 4 15.314 192IR G 5569.1 4 5.011 192IR G 5585.1 8 1.3 4 Z 192IR G 5595.5 3 7.8 6 192IR G 5612.5 3 12.211 192IR G 5637.5 7 1.0 5 192IR G 5654.2 3 6.1 8 192IR G 5660.7 5 4.4 7 192IR G 5667.6625 28. 192IR G 5681.5 7 1.9 5 192IR G 5689.0525 18.114 192IR G 5708.3 5 1.6 4 192IR G 5727.2 5 3.4 4 192IR G 5746.8 4 2.4 6 192IR G 5758.2 3 6.1 6 192IR G 5782.8 3 16.119 192IR G 5808.0 4 5.814 192IR G 5817.7 7 1.4 3 192IR G 5830.0 5 2.0 6 192IR G 5846.410 0.9 4 192IR G 5866.6 3 9.0 6 192IR G 5880.7 7 0.7 3 192IR G 5905.8 6 4.211 192IR G 5910.2 6 4.711 192IR G 5957.9 4 20.622 192IR G 5962.1 5 7.814 192IR G 5972.4 8 2.9 6 192IR G 5985.510 1.1 3 192IR G 5994.511 0.6 4 Z 192IR G 6004.4 4 3.0 5 192IR G 6024.812 0.7 3 192IR G 6055.1 5 0.7 3 192IR G 6067.211 0.6 3 192IR G 6078.512 3.611 192IR G 6082.1 3 27.519 192IR G 6093.0 4 7.2 6 192IR G 6112 D 192IR G 6130.115 0.4 4 Z ? 192IR G 6141.1 8 1.4 3