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Table 1:

Summary of the mid-IR photometric measurements1 performed on the Spitzer IRAC, IRS PUI $16~\mu$m, and MIPS 24, and $70~\mu$m images (Fig. 1).

Target region
$3.6~\mu$m $4.5~\mu$m $5.8~\mu$m $8~\mu$m5 $16~\mu$m6 $24~\mu$m $70~\mu$m

SQ ridge2
$ 23.7\pm0.9$ $ 11.9\pm0.2$ $ 7.3\pm0.2$ $4.2\pm0.1$ $1.25\pm 0.05$ $2.25\pm0.12$ <6.43
SQ ridge (partial)3 $ 19.4\pm1.7$ $9.9\pm1.8$ $ 6.0\pm0.1$ $ 3.35\pm0.11$ $1.00\pm 0.06$ $0.89\pm0.15$ <5.04
17'' beam4 $ 17.6\pm0.9$ $9.15\pm0.12$ $ 5.29\pm 0.15$ $3.07\pm0.11$ $0.88\pm0.03$ $0.79\pm0.15$ <3.91

Notes. The background-subtracted surface brightnesses are indicated for three different apertures. The last row (17'' circular aperture ) shows the values we adopt throughout this paper, and in particular for the SED presented in Fig. 2.
(1) Fluxes are in units of $\times 10^{-8}$ W m-2 sr-1.
(2) Mid-IR signal integrated over the shock structure, defined by the 4$\sigma$ S(3) H2 rotational line contours (black line in Fig. 1). We exclude the SQ-A star-forming region.
(3) Mid-IR signal integrated over the S(3) H2 rotational line contours by excluding overlaps with the ( $\mathcal{F}_{24~\mu\rm m} > 0.25$ MJy sr-1) $24~\mu$m magenta contours (see Fig. 1). This allows us to partially remove the contribution from star-forming regions to the dust emission.
(4) Mid-IR signal integrated over the 17'' beam in the center of the SQ shock structure (yellow circle in Fig. 1).
(5) The contribution of the $8~\mu$m S(4) H2 line emission to the $8~\mu$m in-band flux is subtracted.
(6) The contribution of the $17~\mu$m S(1) H2 line emission to the $16~\mu$m in-band flux is subtracted.


Source LaTeX | All tables | In the text

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