Temperature and Entropy Profiles to the Virial Radius of Abell 1246 Cluster Observed with Suzaku

TL;DR

This study measures the temperature, density, and entropy profiles of the intracluster medium in Abell 1246 up to the virial radius using Suzaku, revealing insights into cluster mass, baryon fraction, and the ICM's outer boundary.

Contribution

First detailed measurement of ICM properties up to the virial radius of Abell 1246 with Suzaku, including mass and entropy profiles, and constraints on ICM emission beyond the virial radius.

Findings

Temperature decreases from 7 keV to 2.5 keV at r200.

Gas mass fraction at r200 is about 17%, consistent with cosmic baryon fraction.

No significant ICM emission detected outside r200, with upper limits on OVII and OVIII lines.

Abstract

We report properties of the intracluster medium (ICM) in Abell~1246 to the virial radius ($r_{200}$) and further outside as observed with Suzaku. The ICM emission is clearly detected to $r_{200}$, and we derive profiles of electron temperature, density, entropy, and cluster mass based on the spectral analysis. The temperature shows variation from $\sim 7$ keV at the central region to $\sim 2.5$ keV around $r_{200}$. The total mass in $r_{500}$ is $(4.3 \pm 0.4) \times 10^{14}~M_{\odot}$, assuming hydrostatic equilibrium. At $r>r_{500}$, the hydrostatic mass starts to decline and we, therefore, employ the total mass within $r_{200}$ based on weak-lens mass profile obtained from a sample of lower mass clusters. This yields the gas mass fraction at $r_{200}$ consistent with the cosmic baryon fraction, i.e. $\sim 17$%. The entropy profile indicates a flatter slope than that of the numerical simulation, particularly in $r>r_{500}$. These tendencies are similar to those of other clusters observed with Suzaku. We detect no significant ICM emission outside of $r_{200}$, and $2\sigma$ upper limits of redshifted OVII and OVIII line intensities are constrained to be less than 2.9 and $5.6\times 10^{-7}$ photons cm$^{-2}$ s$^{-1}$ arcmin$^{-2}$, respectively. The OVII line upper limit indicates $n_{\rm H}< 4.7\times 10^{-5}$ cm$^{-3}$ ($Z/0.2~Z_{\odot}$)$^{-1/2}$ ($L/20~{\rm Mpc}$)$^{-1/2}$, which corresponds to an overdensity, $\delta<160$ ($Z/0.2~Z_{\odot}$)$^{-1/2}$ ($L/20~{\rm Mpc}$)$^{-1/2}$.