Table 5
Parameters of CH3OH derived radialdensity ρdense(r) and multi-thermometer derived temperature profiles T(r).
| Source | ρ0 0.1 pc | Power-law slope qdense |  |
 |
Tin | rin | Tout | rout |
|---|---|---|---|---|---|---|---|---|
| × 106 (cm−3) | (pc) | (pc) | (K) | (pc) | (K) | (pc) | ||
| G18 | 2.9(0.2) | −0.26(0.07) | 0.08 | 0.10 | 64.7(1.1) | 0.016(e) | 19.2(0.1) | 0.25(0.05) |
| G28 | 6.3(0.4) | −0.83(0.07) | 0.20 | 0.30 | 96.1(1.2) | 0.02 | 21.5(0.1) | 0.80(0.10) |
| G19 | 5.3(0.3) | −0.61(0.05) | 0.20 | 0.25 | 119.5(2.5) | 0.008(e) | 21.2(0.1) | 0.25(0.03) |
| G08a | 10.3(1.2) | −1.33(0.12) | 0.30 | 0.50 | 128.6(1.8) | 0.008(e) | 22.4(0.1) | 1.1(0.14) |
| G31(c) | 8660 (3000) | –3.22(0.37) | 0.34 | 0.42 | 400.0(d) | 0.01(e) | 18.3(1.4) | 0.27(0.03) |
| G08b | 22.9(0.7) | −1.35(0.02) | 0.34 | 0.50 | 135.0(1.4) | 0.02 | 22.3(0.1) | 0.80(0.08) |
| G13 | 9.1(1.8) | −1.67(0.20) | 0.20 | 0.40 | 229.6(23.1) | 0.004(e) | 17.0(1.5) | 0.20(0.07) |
| G10 | 51.6(2.6) | −1.07(0.03) | 0.28 | 0.42 | 172.4(4.8) | 0.02 | 24.7(0.6) | 0.90(0.31) |
Notes. (a) Effective radius Reff is defined as π Reff2 = A, where the A is the CH3OH emission area in which n(H2) can be reliably derived. (b) The largest radius (distance to the center) of n(H2) map derived by CH3OH; this is due to the irregular shape of the emission area. (c)The density profile of source G31 is better described by a two-component power-law form consisting of a shallow slope in the inner region followed by a steep slope of −5.22(0.045) in the outer region. (d) Upper limit is set to 400 K in the fit. (e)For sources G18, G19, G08a, G31, and G13, rin is a re-adjusted parameter based on SED calculation and comparison presented in Fig. 11 (temperature profile shown as blue lines in Fig. 20).
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