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Table 3

Results of our analysis of the H2 S(0) to S(7) pure rotational lines.

Model Ntot avg (cm2)$N_{{\rm{tot}}}^{{\rm{avg}}}\left( {{\rm{c}}{{\rm{m}}^{ - 2}}} \right)$ Ntotmax(cm2)$N_{{\rm{tot}}}^{\max }\left( {{\rm{c}}{{\rm{m}}^{ - 2}}} \right)$ nH2( cm3)${n_{{{\rm{H}}_2}}}\left( {{\rm{c}}{{\rm{m}}^{ - 3}}} \right)$ MH2(M)${M_{{{\rm{H}}_2}}}\left( {{M_ \odot }} \right)$ Tavg (K) χavg2$\chi _{{\rm{avg}}}^2$
Two-temperature, ‘warm’ 4.8 ± 0.3 × 1019 1.0 ± 0.1 × 1010 0.3−1.5 × 103 1.5 ± 0.3 970 ± 40 1.9
Two-temperature, ‘cold’ 4.0 ± 0.1 × 1010 1.1 ± 0.1 × 1011 0.1−1.1 × 104 14±1 430 ± 130 1.7
Thermal admixture, LTE 1.90.7+1.0×1022$1.9_{ - 0.7}^{ + 1.0} \times {10^{22}}$ 6.42.0+2.9×1022$6.4_{ - 2.0}^{ + 2.9} \times {10^{22}}$ 0.3-1 × 105 25090+130$250_{ - 90}^{ + 130}$ 60 ± 30 1.2
Thermal admixture, SE 1.70.6+0.9×1022$1.7_{ - 0.6}^{ + 0.9} \times {10^{22}}$ 6.01.7+2.5×1022$6.0_{ - 1.7}^{ + 2.5} \times {10^{22}}$ 0.1–1.5 × 105 22080+110$220_{ - 80}^{ + 110}$ 80 ± 40 0.9

Notes. The two-temperature models 'warm' and 'cold' refer respectively to the 'gray' and 'red' linear models in Fig. 5 (see Sect. 4.2). The thermal admixture models refer to the results presented in Fig. 9 (see Sect. 5.2). The terms Ntot    avg  and  Ntot max$N_{{\rm{tot}}\,\,\,}^{{\rm{avg}}}\,{\rm{and}}\,\,N_{{\rm{tat}}}^{\max }$ are respectively the average and peak column densities across the maps; nH2${n_{{{\rm{H}}_{\rm{2}}}}}$ is the local density inferred for a clump length l = 0.1–0.5 pc; MH2${M_{{{\rm{H}}_{\rm{2}}}}}$ is the molecular mass; Tavg is the average excitation temperature (LTE) or kinetic temperature (SE) across the map; and χavg 2$\chi _{{\rm{avg}}}^2$ is the average value returned by the chi-square test across the map.

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