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Table 4

Dust and free-free parameters for each source in Sgr B2(N).

Source Tdust (K) NH,dust (cm−2) βdust γdust (%) Te (K) EM (pc cm−6) γff (%)
Envelope

A01 39 ± 21
A02 35 ± 0
A03 48 ± 23
A04 59 ± 20
A05 58 ± 3
A06 63 ± 12
A07 58 ± 16
A08(*) 62 ± 29
A09 43 ± 31
A10(*) 68 ± 20
A11(*) 68 ± 13
A12(*) 77 ± 0
A13(*) 53 ± 22
A14 70 ± 24
A15 86 ± 5
A16(*) 58 ± 22
A17 60 ± 17
A18 77 ± 0
A19 56 ± 24
A20(*) 45 ± 23

Core

A01 248 ± 64
A02 221 ± 69
A03 240 ± 74
A04 210 ± 53
A05 223 ± 109
A06 196 ± 49
A07 208 ± 54
A08(*) 225 6.1(+24) 0.7
A09 190 ± 26
A10(*) 225 6.1(+24) 0.7
A11(*) 225 6.1(+24) 0.7
A12(*) 225 6.1(+24) 0.7
A13(*) 225 6.1(+24) 0.7
A14 282 ± 45
A15 231 ± 39
A16(*) 225 6.1(+24) 0.7
A17 203 ± 51
A18 267 ± 132
A19 206 ± 77
A20(*) 225 6.1(+24) 0.7

Notes. Exponents are given in parentheses, e.g., 1.4(16) = 1.4 × 1016. The errors of the continuum parameters are indicated by subscript (left) and superscript (right) values, e.g., is the lower limit of 1.0 × 10+25 − 4.7 × 10+00 and 1.0 × 10+25 + 3.0 × 10+00 is the upper limit of the corresponding hydrogen column density of 1.0 × 10+25. For sources marked with an asterisk (*), we could not derive a self-consistent description of the continuum of the corresponding core spectrum. Here Tdust indicates the dust temperature in K, NH,dust the hydrogen column density in cm−2, and βdust the power-law index of the dust emissivity. We use temperature units for the fitting. Therefore, the spectral indices for flux units α is given by α = β + 2. Additionally, γdust describes the contribution of dust to the total continuum of the corresponding core spectrum in %, Te the electron temperature in K, EM the emission measure in pc cm−6, and γff the free-free contribution to the total continuum in %.

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