Integrated Radio Continuum Spectra of Galaxies

TL;DR

This study analyzes the radio continuum spectra of 250 bright galaxies across a wide frequency range, revealing spectral curvature and challenging simple thermal/non-thermal emission models.

Contribution

It provides the first detailed measurement of spectral curvature in galaxy radio spectra and compares two methods for estimating thermal emission fractions.

Findings

Detected spectral curvature with a change of about -0.2 per decade in frequency.

Found no correlation between spectral flattening and galaxy inclination.

Identified inconsistencies in thermal fraction estimates from different methods.

Abstract

We investigate the spectral shape of the total continuum radiation, between 74 MHz and 5 GHz (400 to 6 cm in wavelength), for a large sample of bright galaxies. We take advantage of the overlapping survey coverage of the VLA Low-Frequency Sky Survey, the Westerbork Northern Sky Survey, the NRAO VLA Sky Survey, and the Green Bank 6 cm survey to achieve significantly better resolution, sensitivity, and sample size compared to prior efforts of this nature. For our sample of 250 bright galaxies we measure a mean spectral index, ${\alpha}$, of -0.69 between 1.4 and 4.85 GHz, -0.55 between 325 MHz and 1.4 GHz, and -0.45 between 74 and 325 MHz, which amounts to a detection of curvature in the mean spectrum. The magnitude of this curvature is approximately ${\Delta \alpha}$ = -0.2 per logarithmic frequency decade when fit with a generalized function having constant curvature. No trend in low frequency spectral flattening versus galaxy inclination is evident in our data, suggesting that free-free absorption is not a satisfying explanation for the observed curvature. The ratio of thermal to non-thermal emission is estimated by two independent methods, (1) using the IRAS far-IR fluxes, and (2) with the value of the total spectral index. Method (1) results in a distribution of 1.4 GHz thermal fractions of 9% ${\pm}$ 3%, which is consistent with previous studies, while method (2) produces a mean 1.4 GHz thermal fraction of 51% with dispersion 26%. The highly implausible values produced by method (2) indicate that the sum of typical power-law thermal and non-thermal components is not a viable model for the total spectral index between 325 and 1.4 GHz.