Table 1.
Observed XRISM/Resolve calibration and GO pointings, their basic information (see also Table A.1), and best-fit single-temperature ICM properties including 1σ statistical uncertainties.
| Name | texp (ks)a | R (kpc)b | ℓeff (kpc)c | kBT (keV)d | ZFee | z (×10−2)f | ulos (km s−1)g | σlos (km s−1)h | fnth (×10−2)i |
|---|---|---|---|---|---|---|---|---|---|
| E | 45 | 328 | 250 − 470 | ![]() |
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| NE | 43 | 399 | 280 − 530 | ![]() |
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| E+NEj | 88 | 347 | 250 − 530 | ![]() |
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| N | 50 | 243 | 190 − 400 | ![]() |
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| M3 | 122 | 112 | 70 − 260 | ![]() |
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| O3 | 92 | 180 | 140 − 330 | ![]() |
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Notes. aNet exposure. bProjected radius of the pointing center. The E+NE region uses the geometric midpoint of the E and NE pointings as its center. cRange of effective length scale, including the uncertainties characterized by the emissivity fraction range of 40 − 60% (see Sect. 4.3 and Appendix A.3). dICM temperature. eFe abundance relative to the lpgs proto-solar abundances (Lodders et al. 2009), see Fig. A.1. fICM redshift. gBulk velocity of the ICM in the rest frame of the central ICM (zicm = 0.017628) with heliocentric correction. hICM velocity dispersion. For reference, the sound speed of 5 − 6 keV gas is ≃1100 − 1250 km s−1. iNonthermal pressure fraction (see Sect. 4.1). jCombined fit of the E and NE pointings.
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