Table 1.
Best-fit and derived hot halo parameters.
| Parameter | Units | Value |
|---|---|---|
| kT | [keV] | ![]() |
| norm | [10−4 cm−5] | ![]() |
| Z† | [Z⊙] | ![]() |
| β | ![]() |
|
| rcore | [kpc] | ![]() |
| normpow | [10−5] | ![]() |
| Γ | ![]() |
|
| T | [107 K] | ![]() |
| ne, 0 | [cm−3] | ![]() |
| Mhot gas(<38 kpc) | [1012 M⊙] | ![]() |
| Mvir | [1013 M⊙] | 3 ± 1 |
| Rvir | [kpc] | ![]() |
| Mhot gas(Rvir) | [1012 M⊙] | ![]() |
| Mhot/Mvir | ![]() |
|
| fhot | ![]() |
|
Notes. Values correspond to the median and the 16th and 84th percentiles of the posterior distributions from the MCMC analysis. The upper block lists parameters directly constrained by the X-ray data, while the lower block reports derived quantities. These derived quantities depend on assumptions that the observed emission traces a virialized halo extending to Rvir, that the gas temperature equals the virial temperature (T = Tvir), and that the β model profile can be extrapolated to the virial radius. †Metallicity was treated as a marginalization parameter and is not directly constrained by the data.
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