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 2.68114 1.0 192IR cN SIGMAN=954 43 192IR G 19.71 3 0.25 4 (M1) 133 A 192IRS G LC= 102 $MC= 23.7 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) 128 A 192IRS G LC= 98.4 $MC= 22.8 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 9.84 192IRS G LC= 7.58 $MC= 1.74 192IR G 68.443 20 0.7 4 192IR G 83.371 11 1.4 7 M1 10.7 192IRS G KC= 8.82 $LC= 1.45 $MC= 0.336 $NC+= 0.1000 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 6.42 192IRS G KC= 5.29 $LC= 0.869 $MC= 0.200 $NC+= 0.0625 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 5.95 192IRS G KC= 4.90 $LC= 0.805 $MC= 0.185 $NC+= 0.0582 192IR G 105.497 20 3.0 6 192IR G 120.153 5 2.0 4 192IR G 122.748 15 1.9 6 M1 3.52 192IRS G KC= 2.90 $LC= 0.476 $MC= 0.109 $NC+= 0.0346 192IR G 124.771 5 10.7 11 M1 3.36 192IRS G KC= 2.77 $LC= 0.455 $MC= 0.104 $NC+= 0.0329 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 2.80 192IRS G KC= 2.31 $LC= 0.378 $MC= 0.0861 $NC+= 0.0273 192IR G 134.157 10 2.4 6 M1 2.73 192IRS G KC= 2.25 $LC= 0.369 $MC= 0.0842 $NC+= 0.0266 192IR G 138.942 5 5.7 7 M1 2.47 E 192IRS G KC= 2.04 $LC= 0.334 $MC= 0.0763 $NC+= 0.0240 192IR G 140.17 5 1.4 7 192IR G 142.210 25 2.1 5 M1 2.31 192IRS G KC= 1.91 $LC= 0.312 $MC= 0.0715 $NC+= 0.0225 192IR G 144.356 7 3.0 6 192IR G 146.902 6 3.3 5 M1 2.11 192IRS G KC= 1.74 $LC= 0.285 $MC= 0.0654 $NC+= 0.0205 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 1.92 192IRS G KC= 1.59 $LC= 0.260 $MC= 0.0599 $NC+= 0.0187 192IR G 155.354 17 1.8 5 192IR G 159.495 3 7.6 8 E2 0.775 192IRS G KC= 0.303 $LC= 0.353 $MC= 0.0915 $NC+= 0.0275 192IR G 161.966 11 1.4 4 192IR G 162.370 8 2.2 5 M1 1.59 192IRS G KC= 1.31 $LC= 0.214 $MC= 0.0501 $NC+= 0.0155 192IR G 165.084 18 2.9 4 M1 1.52 192IRS G KC= 1.25 $LC= 0.204 $MC= 0.0480 $NC+= 0.0148 192IR G 165.417 11 2.3 5 M1 1.51 192IRS G KC= 1.25 $LC= 0.203 $MC= 0.0478 $NC+= 0.0147 192IR G 165.568 4 9.3 11 M1 1.51 192IRS G KC= 1.24 $LC= 0.203 $MC= 0.0477 $NC+= 0.0147 192IR G 172.18 5 1.0 5 192IR G 173.707 13 1.3 7 M1 1.32 192IRS G KC= 1.09 $LC= 0.177 $MC= 0.0421 $NC+= 0.0129 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 1.18 192IRS G KC= 0.975 $LC= 0.158 $MC= 0.0380 $NC+= 0.0115 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 1.02 192IRS G KC= 0.843 $LC= 0.137 $MC= 0.0333 $NC+= 0.00990 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 0.873 192IRS G KC= 0.719 $LC= 0.117 $MC= 0.0288 $NC+= 0.00831 192IR G 202.255 9 4.6 6 M1 0.861 192IRS G KC= 0.709 $LC= 0.115 $MC= 0.0284 $NC+= 0.00818 192IR G 203.676 14 2.7 4 192IR G 204.078 11 4.8 6 M1 0.840 192IRS G KC= 0.691 $LC= 0.113 $MC= 0.0277 $NC+= 0.00795 192IR G 204.469 25 4.5 7 M1 0.835 192IRS G KC= 0.688 $LC= 0.112 $MC= 0.0276 $NC+= 0.00790 192IR G 211.194 6 15.1 12 M1 0.763 192IRS G KC= 0.629 $LC= 0.102 $MC= 0.0253 $NC+= 0.00710 192IR G 219.160 4 20.3 20 E1 0.0547 E 192IRS G KC= 0.0450 $LC= 0.00737 $MC= 0.00180 $NC+= 0.000489 192IR G 219.72 8 0.8 4 192IR G 222.180 10 5.6 7 M1 0.663 192IRS G KC= 0.547 $LC= 0.0889 $MC= 0.0220 $NC+= 0.00596 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 0.502 192IRS G KC= 0.414 $LC= 0.0673 $MC= 0.0164 $NC+= 0.00415 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 0.475 192IRS G KC= 0.392 $LC= 0.0636 $MC= 0.0154 $NC+= 0.00385 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 192IR G 259.336 8 9.8 12 M1 0.432 192IRS G KC= 0.357 $LC= 0.0580 $MC= 0.0139 $NC+= 0.00341 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 0.385 192IRS G KC= 0.318 $LC= 0.0517 $MC= 0.0121 $NC+= 0.00292 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 0.318 192IRS G KC= 0.263 $LC= 0.0427 $MC= 0.00953 $NC+= 0.00228 192IR G 296.622 20 4.5 14 M1 0.298 192IRS G KC= 0.247 $LC= 0.0401 $MC= 0.00877 $NC+= 0.00210 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 0.0944 192IRS G KC= 0.0603 $LC= 0.0266 $MC= 0.00609 $NC+= 0.00139 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 0.221 192IRS G KC= 0.184 $LC= 0.0297 $MC= 0.00586 $NC+= 0.00146 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 0.194 192IRS G KC= 0.162 $LC= 0.0260 $MC= 0.00492 $NC+= 0.00126 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 L 12.987 6 (6+) 192IR L 16.040 6 (6-) 192IR L 56.7189 23 1- 1.45 M 5 192IR G 56.7189 23 E3 2977 192IRS G LC= 2107 $MC= 613 $NC+= 257 192IR L 66.822 8 (4-) 15 NS 4 192IR G 50.782 8 0.132 11 E2 100.6 192IRS G LC= 75.2 $MC= 19.2 $NC+= 6.16 192IR G 66.822 8 1.31 13 [E1] 0.234 192IRS G LC= 0.180 $MC= 0.0417 $NC+= 0.0127 192IR L 84.2742 24 3- 1.9 NS 4 192IR G 84.2742 24 7.7 4 E1 0.623 192IRS G KC= 0.500 $LC= 0.0954 $MC= 0.0220 $NC+= 0.00632 192IR L 104.7758 23 (1)- 17.4 NS 26 192IR G 48.0569 7 5.7 4 M1+E2 0.163 10 12.4 4 192IRS G LC= 9.66 24$MC= 2.28 6 192IR L 115.5628 24 (2)- 192IR G 58.8439 8 5.3 3 M1+E2 0.227 5 7.47 192IRS G LC= 5.64 $MC= 1.34 $NC+= 0.488 192IR L 118.7824 13 3- 15 NS GT 192IR G 34.508 3 0.0242 21 M1 25.2 192IRS G LC= 19.4 $MC= 4.47 192IR G 118.7823 13 0.56 7 E1 0.260 192IRS G KC= 0.211 $LC= 0.0374 $MC= 0.00856 $NC+= 0.00263 192IR L 128.743 3 (0)- 192IR G 23.9668 23 0.170 14 M1 74.4 192IRS G LC= 57.3 $MC= 13.2 192IR G 72.0237 23 0.6 3 M1 2.90 192IRS G LC= 2.23 $MC= 0.513 $NC+= 0.156 192IR L 139.945 7 (5+) 192IR G 126.958 3 1.86 10 M1 3.20 192IRS G KC= 2.64 $LC= 0.432 $MC= 0.0985 $NC+= 0.0313 192IR L 143.553 3 (1)- 192IR G 27.990 3 0.0178 17 M1 46.9 192IRS G LC= 36.1 $MC= 8.31 192IR G 38.7774 25 0.026 3 M1 17.9 192IRS G LC= 13.7 $MC= 3.17 192IR G 86.8343 25 0.65 13 M1 9.54 192IRS G KC= 7.86 $LC= 1.29 $MC= 0.298 $NC+= 0.0896 192IR L 144.904 5 (5+) 192IR G 144.903 5 3.1 4 (M1) 2.19 192IRS G KC= 1.81 $LC= 0.296 $MC= 0.0679 $NC+= 0.0213 192IR L 173.2 6 192IR L 192.932 3 (2)- 192IR G 49.379 4 0.122 10 M1 8.75 192IRS G LC= 6.74 $MC= 1.55 192IR G 77.369 3 0.38 11 M1 13.4 192IRS G KC= 11.0 $LC= 1.81 $MC= 0.417 $NC+= 0.124 192IR G 108.658 4 0.11 3 M1 5.00 192IRS G KC= 4.12 $LC= 0.676 $MC= 0.155 $NC+= 0.0492 192IR G 136.213 3 4.0 5(M1,E2) 2.0 6 192IRS G KC= 1.3 9$LC= 0.5 3$MC= 0.13 6$NC+= 0.041 15 192IR G 192.932 3 D 0.983 192IRS G KC= 0.810 $LC= 0.132 $MC= 0.0321 $NC+= 0.00948 192IR L 193.5095 24 (1)+ 2.7 NS 6 192IR G 49.9563 25 0.115 9 E1 0.508 192IRS G LC= 0.401 $MC= 0.0931 192IR G 77.9467 7 4.8 4 E1 0.759 192IRS G KC= 0.605 $LC= 0.118 $MC= 0.0273 $NC+= 0.00778 192IR G 88.7337 7 3.67 24 E1 0.547 192IRS G KC= 0.439 $LC= 0.0829 $MC= 0.0191 $NC+= 0.00556 192IR G 136.7906 8 2.20 21 192IR L 203.3 7 LE 3 192IR L 212.806 3 (1,2)- 192IR G 69.252 3 0.25 7 M1 3.26 192IRS G LC= 2.50 $MC= 0.575 $NC+= 0.179 192IR G 108.0297 17 2.62 12 M1 5.08 192IRS G KC= 4.18 $LC= 0.688 $MC= 0.158 $NC+= 0.0500 192IR G 156.0866 18 1.02 12 M1 1.78 192IRS G KC= 1.46 $LC= 0.239 $MC= 0.0556 $NC+= 0.0173 192IR L 216.905 4 (4+) 192IR G 216.905 4 5.57 24 E1 0.0562 192IRS G KC= 0.0462 $LC= 0.00757 $MC= 0.00185 $NC+= 0.000505 192IR L 223.341 6 (6+) 192IR G 207.301 5 0.50 6 [E2] 0.313 192IRS G KC= 0.157 $LC= 0.115 $MC= 0.0321 $NC+= 0.00862 192IR G 210.354 5 0.75 8 M1 0.772 192IRS G KC= 0.636 $LC= 0.103 $MC= 0.0256 $NC+= 0.00719 192IR L 225.915 3 (2)- 192IR G 32.983 3 0.057 4 M1 28.9 192IRS G LC= 22.2 $MC= 5.11 192IR G 107.132 4 0.23 6 M1 5.20 192IRS G KC= 4.29 $LC= 0.705 $MC= 0.162 $NC+= 0.0512 192IR G 110.352 3 0.53 7 E2 3.15 192IRS G KC= 0.665 $LC= 1.86 $MC= 0.475 $NC+= 0.148 192IR G 121.139 3 0.17 7 192IR G 169.196 3 3.05 13 M1 1.42 192IRS G KC= 1.17 $LC= 0.190 $MC= 0.0451 $NC+= 0.0138 192IR L 226.261 4 (LE 2-) 192IR G 169.542 4 0.52 7 M1+E2 1.1 3 0.98 12 192IRS G KC= 0.67 14$LC= 0.23 3$MC= 0.059 8$NC+= 0.0178 12 192IR L 235.757 3 (1-) 192IR G 107.015 3 0.20 7 M1 5.22 192IRS G KC= 4.30 $LC= 0.707 $MC= 0.162 $NC+= 0.0514 192IR G 179.0383 20 2.1 5 [M1] 1.21 192IRS G KC= 1.001 $LC= 0.162 $MC= 0.0390 $NC+= 0.0118 192IR L 239.767 4 (1)- 192IR G 26.962 4 0.0194 17 M1 52.4 192IRS G LC= 40.4 $MC= 9.29 192IR G 111.025 3 0.99 11 M1 4.70 192IRS G KC= 3.87 $LC= 0.636 $MC= 0.145 $NC+= 0.0463 192IR L 240.9006 25 (2)- 192IR G 97.347 3 0.25 5 M1 6.86 192IRS G KC= 5.65 $LC= 0.929 $MC= 0.214 $NC+= 0.0665 192IR G 136.1247 13 6.5 9 M1 2.62 192IRS G KC= 2.16 $LC= 0.354 $MC= 0.0808 $NC+= 0.0255 192IR G 240.9005 25 M1 0.530 192IRS G KC= 0.437 $LC= 0.0710 $MC= 0.0174 $NC+= 0.00446 192IR L 265.159 7 (0-) 192IR G 208.440 6 0.70 9 M1 0.792 192IRS G KC= 0.652 $LC= 0.106 $MC= 0.0262 $NC+= 0.00741 192IR L 267.126 3 (3)- 192IR G 26.2259 24 0.132 9 M1 56.9 192IRS G LC= 43.8 $MC= 10.09 192IR G 54.3209 25 0.54 20 192IR G 151.5636 22 2.89 20 M1 1.93 192IRS G KC= 1.59 $LC= 0.260 $MC= 0.0601 $NC+= 0.0187 192IR L 277.992 4 (4)- 192IR G 193.718 3 0.83 11 M1 0.972 192IRS G KC= 0.801 $LC= 0.130 $MC= 0.0318 $NC+= 0.00936 192IR L 284.213 3 (2,3)+ 192IR G 90.7035 15 1.25 15 M1 8.40 192IRS G KC= 6.92 $LC= 1.14 $MC= 0.263 $NC+= 0.0799 192IR L 288.402 4 (2)- 192IR G 95.470 4 0.9 3[M1] 7.25 192IRS G KC= 5.97 $LC= 0.982 $MC= 0.226 $NC+= 0.0700 192IR G 144.849 4 0.57 9 M1 2.20 192IRS G KC= 1.81 $LC= 0.296 $MC= 0.0680 $NC+= 0.0213 192IR G 172.839 3 0.53 24[M1] 1.34 192IRS G KC= 1.10 $LC= 0.179 $MC= 0.0427 $NC+= 0.0130 192IR G 183.626 3 1.0 4[M1] 1.13 192IRS G KC= 0.932 $LC= 0.151 $MC= 0.0365 $NC+= 0.0110 192IR G 231.683 3 0.95 13 M1 0.591 192IRS G KC= 0.487 $LC= 0.0791 $MC= 0.0195 $NC+= 0.00514 192IR L 292.375 4 (2)- 192IR G 66.460 4 0.10 5 M1 3.68 192IRS G LC= 2.82 $MC= 0.648 $NC+= 0.209 192IR G 148.821 3 1.08 12 M1 2.03 192IRS G KC= 1.68 $LC= 0.274 $MC= 0.0631 $NC+= 0.0197 192IR G 176.812 3 0.6 4 [M1] 1.26 192IRS G KC= 1.04 $LC= 0.168 $MC= 0.0402 $NC+= 0.0122 192IR G 292.374 4 0.42 12 M1 0.310 192IRS G KC= 0.257 $LC= 0.0417 $MC= 0.00924 $NC+= 0.00221 192IR L 310.996 4 2- 192IR G 195.433 4 0.27 7 M1 0.948 192IRS G KC= 0.781 $LC= 0.127 $MC= 0.0311 $NC+= 0.00912 192IR G 206.220 4 3.70 18 M1 0.816 192IRS G KC= 0.672 $LC= 0.109 $MC= 0.0270 $NC+= 0.00768 192IR G 226.722 5 0.19 4 M1 0.627 192IRS G KC= 0.517 $LC= 0.0840 $MC= 0.0208 $NC+= 0.00555 192IR G 254.277 4 1.08 11 M1 0.457 192IRS G KC= 0.377 $LC= 0.0612 $MC= 0.0148 $NC+= 0.00366 192IR L 319.893 5 (2)- 192IR G 191.151 5 0.06 3 192IR G 201.111 5 0.21 6 M1 0.875 192IRS G KC= 0.720 $LC= 0.117 $MC= 0.0288 $NC+= 0.00833 192IR G 215.117 5 0.23 4 M1 0.725 192IRS G KC= 0.598 $LC= 0.0972 $MC= 0.0241 $NC+= 0.00667 192IR L 331.074 3 (2)- 192IR G 105.159 3 0.14 6 M1 5.49 192IRS G KC= 4.52 $LC= 0.743 $MC= 0.171 $NC+= 0.0539 192IR G 118.268 3 0.15 3 E1,E2 192IR G 187.521 3 0.43 5 192IR G 212.291 3 0.07 4 M1 0.753 192IRS G KC= 0.620 $LC= 0.1008 $MC= 0.0249 $NC+= 0.00697 192IR G 215.5111 24 0.24 4 M1 0.722 192IRS G KC= 0.595 $LC= 0.0967 $MC= 0.0239 $NC+= 0.00662 192IR G 226.2980 23 4.0 4 192IR G 246.800 4 0.32 9 192IR L 331.757 3 (1)- 192IR G 90.857 3 0.20 4 192IR G 138.2477 24 0.53 7 E1,E2 192IR G 188.204 3 0.52 23 E2 0.434 192IRS G KC= 0.200 $LC= 0.173 $MC= 0.0472 $NC+= 0.0134 192IR G 203.015 3 0.27 4 M1 0.852 192IRS G KC= 0.702 $LC= 0.114 $MC= 0.0281 $NC+= 0.00808 192IR G 216.1943 24 0.65 9 M1 0.716 192IRS G KC= 0.589 $LC= 0.0959 $MC= 0.0237 $NC+= 0.00655 192IR G 275.0381 24 0.74 16 192IR L 351.689 4 (2)+ 192IR G 158.180 4 0.15 4 192IR G 232.907 4 0.20 4 M1 0.582 192IRS G KC= 0.480 $LC= 0.0780 $MC= 0.0193 $NC+= 0.00504 192IR G 267.415 4 0.93 21 192IR G 351.689 4 10.9 4 192IR L 365.651 5 (2-,3-) 192IR G 98.524 4 0.32 5 M1 6.63 192IRS G KC= 5.46 $LC= 0.897 $MC= 0.206 $NC+= 0.0644 192IR G 139.736 5 0.27 4 M1 2.43 192IRS G KC= 2.01 $LC= 0.329 $MC= 0.0751 $NC+= 0.0236 192IR L 366.729 6 (2)- 192IR G 99.603 6 0.24 13 192IR G 140.814 6 0.16 5 192IR G 223.176 6 0.18 3 192IR G 261.953 6 2.02 23 M1 0.420 192IRS G KC= 0.347 $LC= 0.0564 $MC= 0.0135 $NC+= 0.00328 192IR G 310.010 6 0.26 8 192IR L 366.80 10 (2)- 192IR G 221.90 10 0.83 16 192IR G 262.03 10 3.05 18 M1+E2 1.1 +31-7 0.28 14 192IRS G KC= 0.22 13$LC= 0.051 23$MC= 0.013 6$NC+= 0.0030 3 192IR G 310.08 10 0.61 10 192IR L 368.349 6 192IR G 101.222 6 0.10 3 192IR G 263.573 6 0.86 10 192IR G 284.074 6 1.95 15 M1 0.336 192IRS G KC= 0.278 $LC= 0.0451 $MC= 0.0102 $NC+= 0.00245 192IR G 311.630 6 0.23 6 192IR L 380.3 4 (2)- 192IR G 380.3 4 M1 0.152 192IRS G KC= 0.127 $LC= 0.0204 $MC= 0.00364 $NC+= 0.000990 192IR L 389.723 4 (1,2,3)- 192IR G 97.348 4 0.36 14 192IR G 122.596 3 0.41 7 E2 2.08 192IRS G KC= 0.547 $LC= 1.15 $MC= 0.291 $NC+= 0.0907 192IR G 148.822 3 1.08 12 M1 2.03 192IRS G KC= 1.68 $LC= 0.274 $MC= 0.0631 $NC+= 0.0197 192IR G 246.169 3 0.15 4 192IR G 284.947 3 0.52 7 M1 0.333 192IRS G KC= 0.276 $LC= 0.0447 $MC= 0.01013 $NC+= 0.00242 192IR G 305.448 4 0.45 10 192IR L 392.350 5 1-,2-,3- 192IR G 72.457 6 0.09 5 192IR G 151.450 5 0.26 5 M1 1.93 192IRS G KC= 1.59 $LC= 0.261 $MC= 0.0602 $NC+= 0.0188 192IR G 166.089 5 0.89 10 192IR G 166.435 4 0.24 4 E1,E2 192IR G 199.418 5 0.14 4 E1 0.0694 192IRS G KC= 0.0570 $LC= 0.00942 $MC= 0.00228 $NC+= 0.000650 192IR G 273.568 5 0.18 6 192IR G 276.787 4 0.55 12 (M1) 0.361 192IRS G KC= 0.299 $LC= 0.0485 $MC= 0.0112 $NC+= 0.00269 192IR L 415.039 8 (3+,4+) 192IR G 83.965 8 0.18 9 M1 10.5 192IRS G KC= 8.65 $LC= 1.42 $MC= 0.329 $NC+= 0.0980 192IR G 104.043 9 0.13 4 M1 5.66 192IRS G KC= 4.66 $LC= 0.767 $MC= 0.176 $NC+= 0.0556 192IR G 174.139 8 0.21 4 192IR G 296.257 8 0.65 17 M1 0.299 192IRS G KC= 0.248 $LC= 0.0402 $MC= 0.00881 $NC+= 0.00211 192IR G 299.476 8 0.13 4 192IR G 358.320 8 0.34 9 192IR L 418.139 6 (3+) 192IR G 133.925 6 0.19 5 192IR G 273.235 8 0.49 8 M1 0.374 192IRS G KC= 0.309 $LC= 0.0502 $MC= 0.0117 $NC+= 0.00281 192IR G 278.193 8 0.42 5 192IR G 333.864 6 1.53 10 192IR G 418.138 6 3.45 15 192IR L 440.867 4 (1,2)- 192IR G 156.654 3 2.76 12 M1 1.76 192IRS G KC= 1.45 $LC= 0.237 $MC= 0.0551 $NC+= 0.0171 192IR L 451.253 5 1-,2-,3- 192IR G 140.257 6 0.32 5 192IR G 162.850 6 0.14 3 192IR G 210.352 5 0.75 8 M1 0.772 192IRS G KC= 0.636 $LC= 0.103 $MC= 0.0256 $NC+= 0.00719 192IR G 258.320 5 0.24 5 192IR G 322.510 5 0.51 11 192IR L 470.9 3 1-,2-,3- 192IR G 470.9 3 192IR L 489.436 6 (2,3)- 192IR G 169.542 5 0.52 7 M1 1.41 192IRS G KC= 1.16 $LC= 0.189 $MC= 0.0448 $NC+= 0.0138 192IR G 197.061 7 0.73 19 M1 0.926 192IRS G KC= 0.763 $LC= 0.124 $MC= 0.0304 $NC+= 0.00888 192IR G 384.659 6 0.50 12 192IR G 432.716 6 1.85 7 M1,E2 192IR L 508.994 7 (4+) 192IR G 140.645 9 0.10 5 M1 2.39 192IRS G KC= 1.97 $LC= 0.323 $MC= 0.0737 $NC+= 0.0232 192IR G 177.919 7 0.28 6 M1 1.24 192IRS G KC= 1.019 $LC= 0.165 $MC= 0.0396 $NC+= 0.0120 192IR G 189.100 7 0.47 18 192IR G 220.591 7 0.081 25 192IR G 241.867 7 0.65 13 192IR G 273.236 7 0.72 17 192IR G 316.061 7 2.4 4 192IR G 365.440 7 1.15 10 192IR L 513.195 5 1-,2-,3- 192IR G 72.328 4 0.28 9 192IR G 95.056 6 0.24 5 192IR G 513.194 5 192IR L 517.0 3 (1-) 192IR G 517.0 3 192IR L 529.167 8 1-,2-,3- 192IR G 264.008 7 0.57 7 192IR G 302.905 8 1.20 11 192IR L 530.248 7 192IR G 199.174 7 1.07 18 M1 0.899 192IRS G KC= 0.740 $LC= 0.120 $MC= 0.0296 $NC+= 0.00859 192IR G 210.354 5 2.1 4 M1,E2 0.53 24 192IRS G KC= 0.39 24$LC= 0.11 5$MC= 0.028 12$NC+= 0.0076 4 192IR L 537.06 20 0- TO 3- 192IR G 537.06 20 192IR L 543.78 14 192IR G 543.78 14 192IR L 560.5 4 192IR G 560.5 4 192IR L 585.51 12 0- TO 3- 192IR G 585.51 12 192IR L 602.42 13 0- TO 3- 192IR G 602.42 13 192IR L 612.7 5 1-,2-,3- 192IR G 612.7 5 192IR L 628.6 3 192IR G 628.6 3 192IR L 633.52 14 0- TO 3- 192IR G 633.52 14 192IR L 645.88 21 192IR G 645.87 21 192IR L 657.8 7 192IR G 657.8 7 192IR L 663.33 12 (4+) 192IR G 663.32 12 192IR L 670.638 11 1-,2-,3- 192IR G 229.771 11 0.48 11 192IR G 252.499 12 0.5 3 192IR L 681.02 17 0- TO 3- 192IR G 681.02 17 192IR L 702.79 23 192IR G 702.79 23 192IR L 707.9 5 0- TO 3- 192IR G 707.9 5 192IR L 714.1 4 192IR G 714.1 4 192IR L 734.1 4 1-,2-,3- 192IR G 734.1 4 192IR L 739.15 18 192IR G 739.15 18 192IR L 749.46 17 1-,2-,3- 192IR G 749.46 17 192IR L 766.72 13 0- TO 3- 192IR G 766.72 13 192IR L 777.49 23 192IR G 777.49 23 192IR L 788.0 6 192IR G 788.0 6 192IR L 797.28 16 1-,2-,3- 192IR G 797.28 16 192IR L 813.24 20 192IR G 813.24 20 192IR L 821.96 14 0- TO 3- 192IR G 821.95 14 192IR L 840.97 16 0- TO 3- 192IR G 840.97 16 192IR L 851.0 3 0- TO 3- 192IR G 851.0 3 192IR L 865.57 20 192IR G 865.57 20 192IR L 870.53 19 1-,2-,3- 192IR G 870.53 19 192IR L 884.5 3 192IR G 884.5 3 192IR L 893.63 13 1-,2-,3- 192IR G 893.62 13 192IR L 906.6 21 192IR G 906.6 21 192IR L 914.46 13 0- TO 3- 192IR G 914.46 13 192IR L 936.93 18 192IR G 936.93 18 192IR L 944.3 3 192IR G 944.3 3 192IR L 950.05 23 0- TO 3- 192IR G 950.05 23 192IR L 962.7 11 192IR G 962.7 11 192IR L 978.14 17 192IR G 978.14 17 192IR L 999.43 21 192IR G 999.42 21 192IR L 1003.55 24 0- TO 3- 192IR G 1003.54 24 192IR L 1013.69 25 1-,2-,3- 192IR G 1013.69 25 192IR L 1020.0 24 192IR G 1020.0 24 192IR L 1031.15 14 192IR G 1031.15 14 192IR L 1044.9 3 1-,2-,3- 192IR G 1044.9 3 192IR L 1050.56 12 192IR G 1050.56 12 192IR L 1060.01 14 192IR G 1060.01 14 192IR L 1068.86 12 192IR G 1068.85 12 192IR L 1074.8 3 192IR G 1074.8 3 192IR L 1088.5 6 192IR G 1088.5 6 192IR L 1093.5 4 192IR G 1093.4 4 192IR L 1106.97 18 192IR G 1106.97 18 192IR L 1112.62 20 192IR G 1112.61 20 192IR L 1131.6 3 192IR G 1131.6 3 192IR L 1144.93 23 192IR G 1144.92 23 192IR L 1151.6 6 192IR G 1151.6 6 192IR L 1155.73 23 192IR G 1155.72 23 192IR L 1160.6 3 192IR G 1160.6 3 192IR L 1169.56 15 192IR G 1169.55 15 192IR L 1177.56 15 192IR G 1177.56 15 192IR L 1194.7 3 192IR G 1194.7 3 192IR L 1204.75 15 192IR G 1204.75 15 192IR L 1212.14 15 192IR G 1212.14 15 192IR L 1217.50 15 192IR G 1217.50 15 192IR L 1225.95 17 192IR G 1225.95 17 192IR L 1231.6 3 192IR G 1231.6 3 192IR L 1242.9 3 192IR G 1242.9 3 192IR L 1248.67 24 192IR G 1248.67 24 192IR L 1255.16 18 192IR G 1255.15 18 192IR L 1259.2 3 192IR G 1259.2 3 192IR L 1265.2 3 192IR G 1265.2 3 192IR L 1272.6 9 192IR G 1272.6 9 192IR L 1281.6 3 192IR G 1281.6 3 192IR L 1290.7 4 192IR G 1290.7 4 192IR L 1299.55 19 192IR G 1299.55 19 192IR L 1304.26 23 192IR G 1304.25 23 192IR L 1323.04 18 192IR G 1323.04 18 192IR L 1331.11 13 192IR G 1331.10 13 192IR L 1338.78 23 192IR G 1338.77 23 192IR L 1343.3 5 192IR G 1343.3 5 192IR L 1348.5 3 192IR G 1348.5 3 192IR L 1359.8 4 192IR G 1359.8 4 192IR L 1365.9 5 192IR G 1365.9 5 192IR L 1372.0 4 192IR G 1372.0 4 192IR L 1380.7 3 192IR G 1380.7 3 192IR L 1388.36 23 192IR G 1388.36 23 192IR L 1396.7 3 192IR G 1396.7 3 192IR L 1409.0 6 192IR G 1409.0 6 192IR L 1418.26 15 192IR G 1418.25 15 192IR L 1432.42 17 192IR G 1432.41 17 192IR L 1436.9 3 192IR G 1436.9 3 192IR L 1442.80 20 192IR G 1442.79 20 192IR L 1447.90 15 192IR G 1447.89 15 192IR L 1463.9 3 192IR G 1463.9 3 192IR L 1468.9 3 192IR G 1468.9 3 192IR L 1486.4 4 192IR G 1486.4 4 192IR L 1495.0 6 192IR G 1495.0 6 192IR L 1502.2 6 192IR G 1502.2 6 192IR L 1514.4 4 192IR G 1514.4 4 192IR L 1529.99 17 192IR G 1529.99 17 192IR L 1534.73 21 192IR G 1534.72 21 192IR L 1551.61 14 192IR G 1551.61 14 192IR L 1558.0 6 192IR G 1558.0 6 192IR L 1571.4 3 192IR G 1571.4 3 192IR L 1586.4 6 192IR G 1586.4 6 192IR L 1596.44 25 192IR G 1596.44 25 192IR L 1606.78 17 192IR G 1606.77 17 192IR L 1626.3 5 192IR G 1626.3 5 192IR L 1634.5 9 192IR G 1634.5 9 192IR L 1641.2 8 192IR G 1641.2 8 192IR L 1648.3 5 192IR G 1648.3 5 192IR L 1658.5 4 192IR G 1658.5 4 192IR L 1666.81 20 192IR G 1666.80 20 192IR L 1676.8 4 192IR G 1676.8 4 192IR L 1692.1 4 192IR G 1692.1 4 192IR L 1702.21 21 1+,2+ 192IR G 1702.20 21 192IR L 6198.14 3 192IR G 4495.88 21 0.44 4 192IR G 4505.9 4 0.20 3 192IR G 4521.3 4 0.12 4 192IR G 4531.28 19 0.61 5 192IR G 4539.5 4 0.06 3 192IR G 4549.8 5 0.06 3 192IR G 4556.8 8 0.18 7 192IR G 4563.5 9 0.14 11 192IR G 4571.8 5 0.23 4 192IR G 4591.30 17 0.57 4 192IR G 4601.64 24 0.22 4 192IR G 4611.6 6 0.11 7 192IR G 4626.7 3 0.10 3 192IR G 4640.0 6 0.15 6 192IR G 4646.47 13 0.26 5 192IR G 4663.36 21 0.18 3 192IR G 4668.09 17 0.36 3 192IR G 4683.7 4 0.09 6 192IR G 4695.8 6 0.06 3 192IR G 4703.0 6 0.06 3 192IR G 4711.6 4 0.17 3 192IR G 4729.1 3 0.167 25 192IR G 4734.2 3 0.45 9 192IR G 4750.18 15 0.38 3 192IR G 4755.28 20 0.39 3 192IR G 4761.1 3 0.106 20 192IR G 4765.66 17 0.245 24 192IR G 4779.82 15 0.32 3 192IR G 4789.0 6 0.10 6 192IR G 4801.4 3 0.12 3 192IR G 4809.72 23 0.44 4 192IR G 4817.3 3 0.28 4 192IR G 4826.1 4 0.11 3 192IR G 4832.2 5 0.10 3 192IR G 4838.3 4 0.15 4 192IR G 4849.6 3 0.15 3 192IR G 4854.8 5 0.28 5 192IR G 4859.30 23 0.45 4 192IR G 4866.97 12 0.68 4 192IR G 4875.03 18 0.33 4 192IR G 4893.82 23 0.35 3 192IR G 4898.53 19 0.41 4 192IR G 4907.4 4 0.07 4 192IR G 4916.5 3 0.29 5 192IR G 4925.5 9 0.06 3 192IR G 4932.9 3 0.11 4 192IR G 4938.9 3 0.25 9 192IR G 4942.92 18 0.52 4 192IR G 4949.40 24 0.31 4 192IR G 4955.2 3 0.15 7 192IR G 4966.5 3 0.20 3 192IR G 4972.12 17 0.35 3 192IR G 4980.57 15 0.82 4 192IR G 4985.93 14 0.58 3 192IR G 4993.32 15 0.40 4 192IR G 5003.4 3 0.35 4 192IR G 5020.51 15 0.66 6 192IR G 5028.52 15 0.67 6 192IR G 5037.5 3 0.22 4 192IR G 5042.35 23 0.57 6 192IR G 5046.4 6 0.12 3 192IR G 5053.15 23 0.26 3 192IR G 5066.5 3 0.15 3 192IR G 5085.45 20 0.266 25 192IR G 5091.10 18 0.37 5 192IR G 5104.6 4 0.14 3 192IR G 5109.6 6 0.11 7 192IR G 5123.3 3 0.20 3 192IR G 5129.21 12 0.90 5 192IR G 5138.06 14 0.39 4 192IR G 5147.51 12 1.29 6 192IR G 5153.1 3 0.26 3 192IR G 5166.92 13 0.96 6 192IR G 5178.0 24 192IR G 5184.38 25 0.20 6 192IR G 5194.52 24 0.34 5 192IR G 5198.64 21 0.38 4 192IR G 5219.92 17 0.72 5 192IR G 5235.3 11 0.03 3 192IR G 5248.02 23 0.20 3 192IR G 5253.7 3 0.091 22 192IR G 5261.14 17 0.51 4 192IR G 5283.60 13 0.85 6 192IR G 5291.5 21 192IR G 5304.44 13 0.73 5 192IR G 5313.6 3 0.15 4 192IR G 5327.53 19 0.71 5 192IR G 5332.49 20 0.54 5 192IR G 5347.1 3 0.18 3 192IR G 5357.09 16 1.03 6 192IR G 5376.11 14 0.288 24 192IR G 5384.82 20 0.224 22 192IR G 5400.78 16 0.40 3 192IR G 5410.0 6 192IR G 5420.57 23 0.201 22 192IR G 5431.34 12 0.78 4 192IR G 5448.60 17 0.51 4 192IR G 5458.91 18 0.60 5 192IR G 5463.9 4 0.31 7 192IR G 5483.9 4 0.17 6 192IR G 5490.1 5 0.19 3 192IR G 5495.27 23 0.22 3 192IR G 5517.04 17 0.76 4 192IR G 5534.73 12 1.39 6 192IR G 5540.2 7 0.05 4 192IR G 5552.18 21 0.163 22 192IR G 5564.54 14 1.71 8 192IR G 5569.4 3 0.67 4 192IR G 5585.3 5 0.10 3 192IR G 5595.63 13 0.72 4 192IR G 5612.55 12 1.06 5 192IR G 5637.5 4 0.08 4 192IR G 5654.27 14 0.39 3 192IR G 5661.00 20 0.38 3 192IR G 5667.81 3 2.68 10 192IR G 5681.1 3 0.165 19 192IR G 5689.06 3 1.73 7 192IR G 5708.62 3 0.122 17 192IR G 5727.2 3 0.27 4 192IR G 5746.80 3 0.190 18 192IR G 5757.18 3 0.49 6 192IR G 5783.01 3 1.34 6 192IR G 5808.33 3 0.48 3 192IR G 5817.7 4 0.113 25 192IR G 5829.70 3 0.16 5 192IR G 5846.36 3 0.045 14 192IR G 5866.29 3 0.73 6 192IR G 5866.97 3 0.79 5 192IR G 5878.15 3 0.057 24 192IR G 5905.67 3 0.45 4 192IR G 5909.64 3 0.23 3 192IR G 5958.28 3 1.79 8 192IR G 5962.29 3 0.75 4 192IR G 5972.13 3 0.254 21 192IR G 5985.24 3 0.089 25 192IR G 5994.7 7 0.05 3 192IR G 6004.53 3 0.257 21 192IR G 6024.8 6 0.057 24 192IR G 6054.49 3 0.054 13 192IR G 6069.30 3 0.048 24 192IR G 6079.26 3 0.29 9 192IR G 6082.48 3 2.62 11 192IR G 6093.26 3 0.56 4 192IR G 6113.76 3 192IR G 6131.22 3 0.03 3 192IR G 6141.32 3 0.072 8