Wall emission in circumbinary disks: the case of CoKu Tau/4

TL;DR

This study models the mid-infrared emission of CoKu Tau/4 as originating from a circumbinary disk's inner wall, revealing insights into the disk structure, dust composition, and variability linked to the binary orbit.

Contribution

It provides the first detailed modeling of CoKu Tau/4's SED considering its binary nature, constraining the disk's inner wall location and dust properties.

Findings

Inner wall at 1.7 times the binary semi-major axis (~8 AU)

Minimal optically thin dust (<0.01 lunar masses) in the hole

Predicted mid-IR variability correlates with orbital period

Abstract

A few years ago, the mid-IR spectrum of a Weak Line T Tauri Star, CoKu Tau/4, was explained as emission from the inner wall of a circumstellar disk, with the inner disk truncated at ~10 AU. Based on the SED shape and the assumption that it was produced by a single star and its disk, CoKu Tau/4 was classified as a prototypical transitional disk, with a clean inner hole possibly carved out by a planet, some other orbiting body, or by photodissociation. However, recently it has been discovered that CoKu Tau/4 is a close binary system. This implies that the observed mid-IR SED is probably produced by the circumbinary disk. The aim of the present paper is to model the SED of CoKu Tau/4 as arising from the inner wall of a circumbinary disk, with parameters constrained by what is known about the central stars and by a dynamical model for the interaction between these stars and their surrounding disk. In order to fit the Spitzer IRS SED, the binary orbit should be almost circular, implying a small mid-IR variability (10%) related to the variable distances of the stars to the inner wall of the circumbinary disk. Our models suggest that the inner wall of CoKu Tau/4 is located at 1.7a, where a is the semi-major axis of the binary system (a~8AU). A small amount of optically thin dust in the hole (<0.01 lunar masses) helps to improve the fit to the 10microns silicate band. Also, we find that water ice should be absent or have a very small abundance (a dust to gas mass ratio <5.6X10^{-5}). In general, for a binary system with eccentricity e>0, the model predicts mid-IR variability with periods similar to orbital timescales, assuming that thermal equilibrium is reached instantaneously.