Spectral Energy Distributions of Young Stars in IC 348: The Role of Disks in Angular Momentum Evolution of Young, Low-Mass Stars

TL;DR

This study models the spectral energy distributions of young stars in IC 348 to investigate the role of circumstellar disks in their angular momentum evolution, testing the disk-locking theory's predictions.

Contribution

It provides the first detailed modeling of disk inner edges in IC 348 stars, challenging the expected correlation between disk properties and stellar rotation.

Findings

No clear difference in inner disk radii between slow and rapid rotators.

Disk-locking may not be the dominant mechanism influencing stellar rotation in IC 348.

Both slow and rapid rotators may experience similar disk interactions.

Abstract

Theoretical work suggests that a young star's angular momentum and rotation rate may be strongly influenced by magnetic interactions with its circumstellar disk. A generic prediction of these 'disk-locking' (DL) theories is that a disk-locked star will be forced to co-rotate with the Keplerian angular velocity of the inner edge of the disk. These theories have also been interpreted to suggest a correlation between young stars' rotation periods and the structural properties of their disks, such that slowly rotating stars possess close-in disks that enforce the star's slow rotation, whereas rapidly rotating stars possess anemic or evacuated inner disks that are unable to brake the stars and they spin up as they contract. To test these expectations, we model the SEDs of 33 young stars in IC 348 with known rotation periods and infrared excesses indicating the presence of disks. For each star, we match the observed spectral energy distribution, typically sampling 0.6-8.0 \mum, to a grid of 200,000 pre-computed star+disk radiative transfer models, from which we infer the disk's inner-truncation radius (R_trunc). We then compare this R_trunc to the disk's co-rotation radius (R_co), calculated from the star's rotation period. We do not find obvious differences in the disk R_trunc of slow vs. rapid rotators. This holds true both at the level of whether close-in disk material is present at all, and in analyzing the precise location of the inner disk edge relative to the R_co amongst the subset of stars with close-in disk material. One interpretation is that DL is unimportant for the IC 348 stars in our sample. Alternatively, if DL does operate, then it must operate on both the slow and rapid rotators, potentially producing both spin-up and spin-down torques, and the transition from the disk-locked state to the disk-released state must occur more rapidly than the stellar contraction timescale.