Table 2
Best-fitting parameters for the LT relations modelled in this work taking the form L/L0 = E(z)γLTALT(T/T0)BLT, where L0 = 3 × 1043 erg s-1 and T0 = 3 keV.
| Relation | Fit | ALT | BLT | γLT | σLT | Ndet |
| (1) | (2) | (3) | (4) | (5) | (6) | (7) |
|
|
||||||
| LXXL-T | BCES | 0.90 ± 0.06 | 3.03 ± 0.28 | 1.0 (fixed) | 0.53 ± 0.07 | – |
| LP09-T | BCES | 1.54 ± 0.22 | 2.97 ± 0.34 | 1.0 (fixed) | 0.62 ± 0.07 | – |
| LC14-T | BCES | 1.26 ± 0.25 | 3.12 ± 0.43 | 1.0 (fixed) | 0.84 ± 0.15 | – |
| L XXL - T | XXL | 0.71 ± 0.11 | 2.63 ± 0.15 | 1.64 ± 0.77 | 0.47 ± 0.07 | 117 |
| Lbol-T | XXL | 1.21 ± 0.19 | 3.08 ± 0.15 | 1.64 ± 0.77 | 0.47 ± 0.07 | – |
| LXXL-T | M10 | 0.71 ± 0.10 | 2.70 ± 0.14 | 1.27 ± 0.49 | 0.50 ± 0.06 | 104 |
Notes. The fit highlighted in bold represents our main result obtained with the bias correction method described in Sect. 4.3. The bolometric relations are transformed from the soft-band relation via the method described in Sect. 4.7. (1) LT relation; (2) fit method; (3) normalisation; (4) slope; (5) evolution term (E(z)γLT); (6) intrinsic scatter; and (7) number of clusters predicted by the model.
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