Thermal Sunyaev-Zel'dovich Effect in the circumgalactic medium -- II: dependence on star formation

TL;DR

This study measures the thermal Sunyaev-Zel'dovich effect in the circumgalactic medium of millions of galaxies up to redshift 1.2, revealing how star formation influences the thermal pressure and energy distribution in galaxy halos.

Contribution

It introduces a novel probabilistic cross-correlation method to analyze the tSZ effect, and provides the first detailed comparison of CGM thermal pressure between star-forming and quiescent galaxies across a wide mass range.

Findings

Detection of CGM signal down to M200=10^12.3 M_sun.

CGM pressure profile fits standard GNFW model without requiring modifications.

Star-forming galaxies show deviation from self-similar thermal energy relations.

Abstract

We measure thermal Sunyaev-Zel'dovich (tSZ) Effect in the circumgalactic medium (CGM) of $\approx$2.5 million $\rm M_{200}$=$\rm 10^{12-14}\,M_\odot$ WISE$\times$DESI galaxies out to $z$=1.2. We split the sample into quiescent (0.7 million) and star-forming (1.8 million) galaxies, exploring the relation between the thermal pressure of the CGM and star formation for the first time. We develop and implement a novel probabilistic approach to cross-correlate the galaxy catalog with the Atacama Cosmology Telescope+Planck data by taking into account the uncertainties in redshift, mass, and star formation rate. The S/N of the stacked Compton-$y$ value in the CGM varies from 4.9 to 18.5, depending on the sample size and the CGM signal strength within the relevant mass bin. We detect the CGM signal down to $\rm M_{200}=10^{12.3}\,M_\odot$, and provide stringent upper limit at $\rm M_{200}<10^{12.3}\,M_\odot$. The data fit well with the standard GNFW profile of thermal pressure and do not require a flatter or steeper profile. This suggests a significant impact of cooling and the absence of dominant feedback. In galaxies with $\rm M_{200}\approx10^{12.3-12.8}\,M_\odot$ halos, the volume filling CGM is likely the largest contributor to the $galactic$ baryons at their virial temperatures of $\sim$10$^{6-6.4}\rm\,K$. For $\rm M_{200}>10^{12.8}\,M_\odot$ halos, the most massive phase of the CGM is likely at a sub-virial temperature of $\rm\gtrsim 10^6\,K$. The thermal energy of the CGM of quiescent galaxies follows the self-similar relation with mass, but the star-forming galaxies deviate from this relation. This indicates that the impact of non-gravitational factors varies among halos of different degrees of star-forming activity.