EDP Sciences
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Volume 578, June 2015
Article Number L8
Number of page(s) 6
Section Letters
DOI http://dx.doi.org/10.1051/0004-6361/201526041
Published online 11 June 2015

Online material

Appendix A: Supplementary figure

thumbnail Fig. A.1

Spitzer IRS spectrum of GoHam (continuous black line) and fit (diamonds) using the PAHTAT model. The mid-IR optical depth derived with the model is shown in red. The positions and bandwidths of the VISIR PAH1 and PAH2 filters are indicated. This spectrum includes GoHam a and b, the absorption is dominated by the disk mid-plane.

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Appendix B: Model

Appendix B.1: Model description

We modeled GoHam b as a spherical clump of constant density nb and radius rb. The presence of this clump results in a localized excess of column density with a profile along the cut as a function of position p (Fig. 3) of parabolic form: (B.1)where pb is the position of GoHam b in the cross cut, that is, 4.25′′. The resulting mid-IR optical depth τb due to GoHam b is then (B.2)where Cext is the dust cross-section per unit of H atom. The mid-IR emission along the cut, corrected for the extinction by GoHam b, can then be recovered by (B.3)where IIR(p) is the observed mid-IR emission profile shown in Fig. 3. In addition, we computed the emission in the 13CO(21) line as a function of p: (B.4)where Δv is the width of the line measured to be 1.7 km s-1, Ωff is the beam-filling factor equal to , where a and b are the minor and major axis of the beam, that is, a = 1.14′′ and b = 1.52′′. K is a Gaussian kernel of width equal to b, which is the angular resolution along the cut shown in Fig. 3 (since the major axis of the beam is almost aligned north-south, see Bujarrabal et al. 2009, as is our cross cut). is the brightness temperature of the 13CO(21) line that is equal to zero for p<pbrb and p>pb + rb. For the other values of p, the brightness is equal to (optically thick line) (B.5)where Tex is the excitation temperature, which we fixed at 16 K, that is, the temperature of the disk midplane derived by Bujarrabal et al. (2009). Tex could be higher than this value in the internal parts of the clump, but this is not critical in the estimation of rb , which is a function of the square root of Tex. Overall, the parameters of the model are the density of GoHam b nb, the radius of GoHam b rb, and the dust cross-section Cext. For interstellar dust, the cross section is typically Cext = 2.5 × 10-23 cm2 per H atom at 8.6 and 11.2 μm (Weingartner & Draine 2001). In disks, however, this value is expected to decrease significantly due to grain growth, typically by a factor of 10 in the mid-IR (Andrews et al. 2009; D’Alessio et al. 2001). We therefore considered these two extreme cases and their effects on the parameters derived by the model.

Appendix B.2: Adjustment of the parameters nb and rb

First, rb was adjusted so as to reproduce the observed emission profile of ICO as shown in Fig. 3. Once the value of rb is adjusted, the following step consists of adjusting the parameter nb so as to obtain a symmetric profile, which is what is expected in a disk without any clump. The result of this procedure is shown in Fig. 3. From the adjusted values of nb and rb, we can derive the clump mass, (B.6)where μ is the mean molecular weight and mH the proton mass. The parameters used in the model and those derived from the fit for the two values of Cext are summarized in Table B.2.

Table B.1

Main physical parameters of the GoHam disk.

Table B.2

Main physical parameters of the GoHam b candidate protoplanet in the model.

© ESO, 2015