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This article has an erratum: [https://doi.org/10.1051/0004-6361/202039465e]


Fig. 2

image

Spatial distributions of different molecular species, labeled in the lower right of each panel, over the Serpens filament. Panel a: Herschel H2 column density image. The contours are H2 column densities of 4 × 1021 cm−2 and 6 × 1021 cm−2. This region is divided by the two white dashed lines into three individual regions which are labeled NW (northwest), SE (southeast), and EX (extended). Panel b: C18 O (1–0) intensity map integrated from 7.4 to 8.7 km s−1. The contours start at 0.30 K km s−1 (5σ), and increase by 0.18 K km s−1 (3σ). Panel c: HCO+ (1–0) intensity map integrated from 6.5 to 9.5 km s−1. The contours start at 0.27 K km s−1, and increase by 0.27 K km s−1. Panel d: HNC (1–0) intensity map integrated from 7.0 to 9.0 km s−1. The contours start at 0.24 K km s−1, and increase by 0.24 K km s−1. Panel e: HCN (1–0) intensity map integrated from 0 to 1.6 km s−1, from 7.0 to 8.6 km s−1, and from 11.8 to 13.4 km s−1 relative to the frequency of the F = 2–1 hyperfine structure component. The contours start at 0.27 K km s−1, and increase by 0.27 K km s−1. Panel f: N2H+ (1–0) intensity map integrated from 6.5 to 9.5 km s−1. The contours start at 0.30 K km s−1, and increase by 0.30 K km s−1. Panel g: CS (2–1) intensity map integrated from 7.0 to 9.5 km s−1. The contours start at 0.18 K km s−1, and increase by 0.18 K km s−1. Panel h: CH3OH (20 –10) intensity map integrated from 7.5 to 8.8 km s−1. The contours start at 0.12 K km s−1, and increase by 0.12 K km s−1. In all panels, the (0, 0) offset corresponds to αJ2000 = 18h28m49.s642, δJ2000 = 00°50′01.′′08, and the three blue crosses give the positions of the three embedded YSOs (see also Fig. 1). The beam size is shown in the lower right of each panel.

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