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In article , Charles Francis
writes: There seems to be some issue with SN1997ff anyway, because correction for gravitational lensing may not be accurate (see abstract below - any comment, Philip? this is your field isn't it). astro-ph/0105355, Gravitational Lensing of the Farthest Known Supernova SN 1997ff, Mörtsell, E.; Gunnarsson, C.; Goobar, A. ApJ 561, Issue 1, pp. 106-110. Abstract We investigate the effects of gravitational lensing due to intervening galaxies on the recently discovered Type Ia supernova at z~1.7, SN 1997ff, in the Hubble Deep Field North. We find that it is possible to obtain a wide range of magnifications by varying the mass and/or the velocity dispersion normalization of the lensing galaxies. In order to be able to use SN 1997ff to constrain the redshift-distance relation, very detailed modeling of the galaxies to control the systematic effects from lensing is necessary. Thus, we argue that, based on our current limited knowledge of the lensing galaxies, it is difficult to use SN 1997ff to constrain the values of OM and OLAMBDA, or even to place severe limits on gray dust obscuration or luminosity evolution of Type Ia supernovae. This is of course a real concern, more important for higher-redshift supernovae (because it is more likely that it is lensed, and, if so, less likely that the lensing galaxy or galaxies would be detected). However, the "interesting" result with the m-z relation for supernovae is the fact that the best fit has a positive cosmological constant, the universe is accelerating etc. This is due to the fact that supernovae are FAINTER than they would be in either the Einstein-de Sitter universe or a low-density universe without a cosmological constant. Thus, "hidden" gravitational lens effects leading to amplification of a supernovae would tend to bias the results AGAINST the current best-fit model. If the matter along the line of sight to the supernovae is less dense than average, then this will also make the objects fainter than expected, so in some sense this could make a lambda-dominated universe look more plausible than it should be. However, it's not just a question of fainter/less faint but rather the detailed shape of the m-z curve. In particular, if the current best-fit model is correct, then at higher redshift supernovae will become BRIGHTER than in competing models. This is a testable prediction and difficult to mimic with other effects (less-than-average density, absorption by grey dust etc) which make things fainter at low redshift, since for these the effect will tend to increase with redshift. In principle, one could introduce the inhomogeneity parameter as a separate free parameter and simultaneously fit for it. In practice, one would require many more data points. Also, it's not really a fixed parameter, or even a parameter with a fixed dependence on redshift, but more like an additional source of error for each data point. It is important to realise, though, that the current best-fit model can be obtained from a combination of other cosmological tests. In other words, take away ALL the supernova results and one would still be left with a lambda-dominated low-density universe. Thus, any theory which indicates that the supernova results should result in different cosmological parameters would have to explain why combinations of other data sets lead to the result they do. I think the situation is quite similar to that of 100 years ago when the question was "what is Avogadro's number?", coupled with the question "are atoms real?". The issue was decided not by any one decisive test, but rather the convergence of many different methods on the same result. Even though objections could be raised to any one method, any explanation as to how several different methods could conspire to give the same wrong result would have to be very ad-hoc. |
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