Low frequency radio observations of SN 2011dh and the evolution of its post-shock plasma properties

TL;DR

This paper presents low-frequency radio observations of SN 2011dh over hundreds of days, modeling its post-shock plasma evolution and circumstellar environment, revealing a slowing shock expansion and consistent mass loss parameters.

Contribution

It provides the first detailed low-frequency radio analysis of SN 2011dh's late-time evolution, including modeling of shock properties and circumstellar medium characteristics.

Findings

Shock expansion slows over hundreds of days.

Mass loss parameter consistent across frequencies.

Radio emission evolution indicates interaction with circumstellar medium.

Abstract

We present late time, low frequency observations of SN 2011dh made using the Giant Metrewave Radio Telescope (GMRT). Our observations at $325\ \rm MHz$, $610\ \rm MHz$ and $1280\ \rm MHz$ conducted between $93-421\ \rm days$ after the explosion supplement the millimeter and centimeter wave observations conducted between $4-15 \ \rm days$ after explosion using the Combined Array for Research in Millimeter-wave Astronomy (CARMA) and extensive radio observations ($ 1.0-36.5\ \rm GHz$) conducted between $16-93\ \rm days$ after explosion using Jansky Very Large Array (JVLA). We fit a synchrotron self absorption model (SSA) to the $610\ \rm MHz$ and $1280\ \rm MHz$ radio light curves. We use it to determine the radius ($R_{\rm p}$) and magnetic field ($B_{\rm p}$) at $173$ \& $323$ days after the explosion. A comparison of the peak radio luminosity $L_{\rm op}$, with the product of the peak frequency $\nu_{\rm p}$ and time to peak $t_{\rm p}$ shows that the supernova evolves between the epochs of CARMA, JVLA and GMRT observations. It shows a general slowing down of the expansion speed of the radio emitting region on a timescale of several hundred days during which the shock is propagating through a circumstellar medium set up by a wind with a constant mass loss parameter, $\dot M/v_{\rm w}$. We derive the mass loss parameter ($A_{\star}$) based on $610\ \rm MHz$ and $1280\ \rm MHz$ radio light curves, which are found to be consistent with each other within error limits.