... MS2137-23[*]
Appendices A and B are only available in electronic form at http://www.edpsciences.org
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... photometric[*]
Using hyperz facilities (Bolzonella et al. 2000), see also G03.
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... library[*]
http://cernlib.web.cern.ch/cernlib/
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... elliptical[*]
Which are not approximated by elliptical lens potentials (numerically faster but leading to unphysical surface mass density at large radius).
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... modeled[*]
If we have used the former positional uncertainties of G03, the best fit model would not have been changed but we would have found a minimum $\chi^2_{\rm src}/{\rm d.o.f.}=1.64$ which is also acceptable fit.
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... satisfying[*]
It would have increased to $\chi^2_{\rm src}/{\rm d.o.f.}=1.39$ using the G03uncertainties.
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...$r\sim 0.1\hbox {$^{\prime \prime }$ }$)[*]
Which makes the issue of the fifth image worth addressing observationally.
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... model[*]
We find $\chi^2_{\rm kin}/N_{\rm bins}\sim8$ if we change $\sigma _{\rm h_4}$ by $\sigma _{\rm los}$ in Eq. (8), i.e. if we neglect the velocity bias due to non-Gaussian LOSVD. Consequently, the correction has a weak effect on the modelling.
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...$\vec{R}_i \rightarrow \vec{R}_i + \vec{\delta
R}_i$[*]
Where $\vec{\delta R}$ may follow a 2D Gaussian distribution with standard deviation $\sigma_{\rm
seeing}={\it FWHM}/2.35$.
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Copyright ESO 2005