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Table 2

Analytical fits and physical structure.

B1b-S B1b-N

Sizea (′′) 0.45 × 0.43 ± 0.05 0.42 ± 0.4
PAa (°) 25 ± 10 170 ± 10

F0, F1b (mJy/beam) 66 ± 2 1.1 ± 0.4 15.3 ± 0.6 0.8 ± 0.1
r0, r1b (′′) 0.34 ± 0.005 1.06 ± 0.22 0.21 ± 0.005 2.3 ± 0.5
α0, α1b 6 2 4 2

n0c (H2 cm-3) 0.9 × 1010 1.0 × 1010
ρgc (g cm-3) 3.9 × 10-14 4.3 × 10-14
Tcd (K) 56 41
T0 (K) 12 12
M(r < 0.3′′) (M) 0.093 0.11
M(r < 1.0′′) (M) 0.42 0.36
M(r < 2.0′′) (M) 0.67 0.72

Notes.

(a)

From Gaussian fitting of the ALMA images.

(b)

The fitting formula of the circularly averaged specific distribution for B1b-S and for B1b-N uses two modified power laws: . For isothermal optically thin dust emission, the slope of the density distribution is α + 1.

(c)

Assuming optically thin emission at 350 GHz.

(d)

Deduced from the specific intensity assuming optically thick emission.

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