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Table 6

Positional offsets between column density and velocity peaks.

λ HGBS 054203.2-02035 HGBS 054157.3-020101 HGBS 054153.4-020016 HGBS 054149.5-015941
Herschel column density peak z = 0.48 pc z = 0.81 pc z = 0.96 pc z = 1.10 pc

peak(obs./fit) z = 0.59 pc/0.61 pc z = 0.81 pc/0.81 pc z = 1.02 pc/1.02 pc
Nobeyama H13CO+ 0.21 pc offset(obs./fit) in pc −0.11 pc/−0.13 pc 0 pc/0 pc −0.062 pc/−0.062 pc
offset(obs./fit) in λ −0.54±0.12λ/−0.62±0.12λ 0.00±0.12λ/0.00±0.12λ −0.30±0.12λ/−0.30±0.12λ
offset(obs./fit) in λ (†) +0.06±0.12λ/−0.005±0.12λ

peak(obs./fit) z = 0.61 pc/0.59 pc z = 0.83 pc/0.85 pc z = 1.13 pc/1.11 pc
Nobeyama C18O 0.26 pc offset(obs./fit) in pc −0.13 pc/−0.11 pc −0.020 pc/−0.040 pc −0.029 pc/−0.038 pc
offset(obs./fit) in λ −0.50±0.09λ/−0.42±0.09λ −0.07±0.09λ/−0.15±0.09λ −0.11±0.09λ/−0.16±0.09λ
offset(obs./fit) in λ (†) +0.05±0.09λ/−0.10±0.09λ

Notes. z measures position along the filament crest shown in Fig. 1. The uncertainties of the positional offsets in units of λ were estimated assuming that the peaks in column density have an uncertainty corresponding to half a beam. (†): Given the additional errors arising from the definition of the curved filament crest around HGBS 054203.2-02035, we also provide offsets estimated assuming a straight filament crest toward this core (see text in Sect. 4.2.1).

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