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Table 2

Line-of-sight properties and derived Quantities.

Source E(B–V) (mag) N(HI) (1021 cm−2) (1) N(HI)cl (1021 cm−2) (1) 2N(H2) (1021 cm−2) (2) WCO (K-km s−1) (3) N(DNM) (1021 cm−2) (1) 2N(H2)/N(HI) N(DNM)/N(HI) XCO (4)
J0203 + 1134 0.144 0.664 0.646 ≤0.193 0.201 ≤0.290 0.303
J0209+1352 0.094 0.696 0.686 0.144 0.00 0.206 0.00
J0211+1051 0.145 0.618 0.617 0.561 0.240 0.908 0.388
J0213 + 1820 0.130 0.933 0.911 ≤0.253 0.177 ≤0.271 0.190
J0231 + 1322 0.121 0.926 0.852 0.103 0.00 0.111 0.00
J0242+1742 0.077 0.820 0.819 ≤0.111 0.00 ≤0.135 0.00
J0252+1718 0.220 1.142 1.139 0.184 0.299 0.161 0.262
J0325 + 2224 0.213 0.999 0.926 0.742 2.82 0.180 0.743 0.180 1.314
J0329 + 3510 0.267 1.418 1.131 0.372 0.150 0.263 0.106
J0329 + 2756 0.198 1.129 1.002 ≤0.142 ≤1.97 0.00 ≤0.126 0.00
J0334+0800 0.391 1.893 1.855 0.322 0.223 0.170 0.118
J0336+ 3218 0.733 1.435 1.165 0.119 ≤2.60 0.606 0.082 0.423
J0356+ 2903 0.212 0.666 0.520 1.099 1.40 0.178 1.650 0.267 3.931
J0357 + 2319 0.185 1.022 0.944 0.205 ≤0.79 0.00 0.200 0.00
J0400+0550 0.266 1.266 1.210 0.182 0.238 0.144 0.188
J0401 + 0413 0.341 1.209 1.202 0.357 0.426 0.296 0.352
J0403 + 2600 0.201 0.830 0.667 0.438 1.99 0.00 0.528 0.00 1.101
J0406+0637 0.283 1.182 1.143 0.397 0.266 0.335 0.225
J0407 + 0742 0.265 1.033 1.006 0.387 0.258 0.374 0.250
J0426 + 0518 0.291 1.305 1.141 0.091 ≤1.40 0.414 0.070 0.317
J0426 + 2327 0.539 1.586 1.331 1.887 5.78 0.00 1.190 0.00 1.632
J0427 + 0457 0.335 1.361 1.192 0.457 2.49 0.590 0.336 0.433 0.918
J0437 + 2037 0.532 2.324 1.992 1.130 ≤1.61 0.00 0.486 0.00
J0431 + 1731 0.464 1.714 1.457 0.739 3.09 0.00 0.431 0.00 1.198
J0433 + 0521 0.298 1.159 0.950 0.255 ≤1.48 0.795 0.220 0.686
J0437 + 2940 0.979 1.320 0.936 4.345 11.98 0.126 3.292 0.095 1.814
J0438 + 3004 0.952 2.019 1.002 4.586 7.70 0.771 2.271 0.382 2.979
J0439 + 3045 0.867 2.361 0.745 3.701 9.42 0.00 1.567 0.00 1.964
J0440+ 1437 0.681 1.659 1.524 0.888 ≤1.97 1.230 0.535 0.741
J0445 + 0715 0.121 1.044 0.915 ≤0.061 0.00 ≤0.058 0.00
J0449 + 1121 0.504 1.416 1.347 0.476 0.791 0.336 0.558
J0502+1338 0.564 2.188 1.957 1.324 ≤1.90 0.672 0.605 0.307
J0510+ 1800 0.328 2.347 1.986 0.092 ≤2.00 0.00 0.039 0.00
J0942-7731 0.336 1.000 0.617 0.837 ≤1.50 0.382 0.838 0.382
J1058-8003 0.152 0.651 0.470 0.147 “ 0.371 0.226 0.570
J1136-6827 0.460 2.407 0.915 0.910 “ 0.172 0.378 0.071
J1145-6954 0.387 1.925 0.998 0.638 “ 0.223 0.331 0.116
J1147-7935 0.300 2.506 0.773 0.040 “ 0.00 0.016 0.00
J1152-8344 0.283 1.088 0.505 0.176 “ 0.515 0.162 0.473
J1224-8313 0.257 0.962 0.563 0.693 “ 0.335 0.720 0.348
J1254-7138 0.282 1.902 0.660 0.102 “ 0.00 0.053 0.00
J1312-7724 0.476 1.257 0.671 0.199 “ 0.396 0.158 0.315
J1550-8258 0.107 0.679 0.416 0.177 “ 0.027 0.261 0.039
J1617-7717 0.091 0.659 0.431 0.043 “ 0.045 0.065 0.068
J1723-7713 0.255 0.834 0.500 1.105 2.40 0.195 1.325 0.234 2.302
J1733-7935 0.139 0.792 0.525 0.041 ≤1.50 0.00 0.052 0.00

Notes. (1)HI and DNM column densities are from Planck Collaboration Int. XXVIII. (2015) and Remy et al. (2017, 2018).(2)N(H2) = N(HCO+)/3 × 10−9. (3)Integrated J = 1–0 CO emission used by Planck Collaboration Int. XXVIII. (2015) and Remy et al. (2017, 2018).(4)XCO = N(H2)/WCO.

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