Constrain the Scattering Geometry of the Cat’s Tail

Determine whether the β Pictoris Cat’s Tail lies behind the star relative to the observer, within the plane of the sky, or near the plane of the sky by applying more physically complete dust-scattering models to the combined scattered-light and thermal-emission observations.

Background

The authors use the ratio between the Cat’s Tail’s scattered-light flux measured with HST/STIS and its thermal-emission flux measured with JWST/MIRI to constrain the scattering phase function and therefore the three-dimensional location of the structure. Their Henyey–Greenstein model favors a location behind the star, but the available data do not uniquely determine the geometry.

The authors explicitly note that their model cannot exclude a Cat’s Tail located in or near the plane of the sky. They suggest that Mie-scattering or discrete-dipole-approximation calculations, together with additional near-infrared observations, could provide stronger constraints.

References

However from our analysis and modeling, we are unable to rule out the Cat's Tail being in or near the plane of the sky.

— Deep HST/STIS Coronagraphic Imaging of the $β$ Pictoris Debris Disk: On the Scattered Light Component of the Cat's Tail  (2609.30111 - Avsar et al., 24 Sep 2026) in Section 6.2, “Utility and Limitations of Scattered Light and Thermal Emission Observations to Constrain the Location of the Cat’s Tail”