Table 2.
Results of the photometric parallax fit to the PWZ relation in different bands.
| Wesenheit | α | σαlow | σαhigh | β | σβlow | σβhigh | γ | σγlow | σγhigh | ϵ | σϵlow | σϵhigh | N | μLMC | σμLMC | AIC | BIC |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Gaia | –6.047 | 0.034 | 0.035 | –3.309 | 0.053 | 0.054 | –0.527 | 0.095 | 0.093 | –0.016 | 0.004 | 0.004 | 270 | 18.524 | 0.06 | 351 | 365 |
| VI_C89 | –6.075 | 0.035 | 0.035 | –3.264 | 0.057 | 0.058 | –0.632 | 0.099 | 0.097 | –0.011 | 0.004 | 0.004 | 267 | 18.418 | 0.064 | 298 | 312 |
| VI_F99 | –5.858 | 0.033 | 0.034 | –3.173 | 0.057 | 0.057 | –0.436 | 0.095 | 0.095 | –0.018 | 0.004 | 0.004 | 274 | 18.442 | 0.06 | 350 | 365 |
| cVI | –5.869 | 0.033 | 0.033 | –3.173 | 0.054 | 0.054 | –0.317 | 0.092 | 0.09 | –0.015 | 0.004 | 0.004 | 272 | 18.386 | 0.057 | 319 | 333 |
| cHVI | –6.011 | 0.032 | 0.033 | –3.214 | 0.05 | 0.051 | –0.509 | 0.088 | 0.086 | –0.01 | 0.004 | 0.004 | 270 | 18.417 | 0.055 | 327 | 341 |
| VKs | –6.073 | 0.032 | 0.033 | –3.289 | 0.05 | 0.051 | –0.47 | 0.088 | 0.084 | –0.008 | 0.004 | 0.004 | 271 | 18.457 | 0.056 | 350 | 365 |
| JKs_C89 | –6.101 | 0.032 | 0.033 | –3.347 | 0.052 | 0.053 | –0.387 | 0.089 | 0.09 | –0.007 | 0.004 | 0.004 | 271 | 18.439 | 0.057 | 331 | 346 |
| JKs_F99 | –6.145 | 0.033 | 0.034 | –3.366 | 0.052 | 0.054 | –0.397 | 0.091 | 0.089 | –0.006 | 0.004 | 0.004 | 271 | 18.446 | 0.058 | 336 | 350 |
Notes. C89 and F99 refer to the Cardelli et al. (1989) and Fitzpatrick (1999) extinction laws, respectively. The values of σlow and σhigh correspond to the 16th and 84th percentiles of the posterior probability, respectively (see text). The LMC distance modulus and its error were calculated in the manner described in the text. The units of α, β, γ, ϵ and of their uncertainties are mag, mag/dex, mag/dex, and mas, respectively.
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