# Separating extended disc features from the protoplanet in PDS 70 using   VLT/SINFONI

**Authors:** V. Christiaens, S. Casassus, O. Absil, F. Cantalloube, C. Gomez, Gonzalez, J. Girard, R. Ramirez, B. Pairet, V. Salinas, D. J. Price, C., Pinte, S. P. Quanz, A. Jordan, D. Mawet, Z. Wahhaj

arXiv: 1905.01860 · 2019-05-17

## TL;DR

This study uses advanced imaging techniques to analyze the PDS 70 transition disc, successfully redetecting the protoplanet and extended features, and comparing methods for optimal detection and characterization.

## Contribution

The paper introduces an optimized PCA-based PSF subtraction method for extended feature recovery and adapts the NEGFC technique for precise astrometry of the protoplanet.

## Key findings

- Redetection of PDS 70 b and disc features
- PCA-SADI better recovers extended features
- Derived astrometry and spectro-photometry of the protoplanet

## Abstract

Transition discs are prime targets to look for protoplanets and study planet-disc interactions. We present VLT/SINFONI observations of PDS~70, a transition disc with a recently claimed embedded protoplanet. We take advantage of the angular and spectral diversity present in our data for an optimal PSF modeling and subtraction using principal component analysis (PCA). We report the redetection of PDS 70 b, both the front and far side of the outer disc edge, and the detection of several extended features in the annular gap. We compare spectral differential imaging applied before (PCA-SADI), and after (PCA-ASDI) angular differential imaging. Our tests suggest that PCA-SADI better recovers extended features, while PCA-ASDI is more sensitive to point sources. We adapted the negative fake companion (NEGFC) technique to infer the astrometry of the companion, and derived $r = 193.5 \pm 4.9 \mathrm{mas}$ and PA = 158.7deg $\pm$ 3.0deg. We used both NEGFC and ANDROMEDA to infer the $K$-band spectro-photometry of the protoplanet, and found results consistent with recent VLT/SPHERE observations, except for their 2018/02 epoch measurement in the $K2$ filter. Finally, we derived an upper limit of $\dot{M_b} < 1.26 \times 10^{-7} \big[ \frac{5 M_{\rm Jup}}{M_b} \big] \big[ \frac{R_b}{R_{\rm Jup}}\big] M_{\rm Jup} $ yr$^{-1}$ for the accretion rate of the companion based on an adaptation of PCA-SADI/PCA-ASDI around the Br$\gamma$ line.

## Full text

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## Figures

12 figures with captions in the complete paper: https://tomesphere.com/paper/1905.01860/full.md

## References

82 references — full list in the complete paper: https://tomesphere.com/paper/1905.01860/full.md

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Source: https://tomesphere.com/paper/1905.01860