next up previous
Next: Calibration and corrections Up: Type Ia Supernovae Previous: Type Ia Supernovae

SNe Ia as standard candles

In the past, various types of galaxies were proposed as standard candle candidates, but it has been found that any cosmological dependences exhibited by these galaxies are dominated by the process of galactic evolution (see, e.g., Tinsley & Gunn 1976). In contrast, a supernova event contains additional information (e.g. light-curve decline rates, and variations of colour and spectral features with declining light) which can be scrutinised for evidence of evolution as a function of look-back time. Additionally, SNe Ia are theorised to result from the thermonuclear explosion of a carbon-oxygen white dwarf which has accreted material until it reaches the Chandrasekhar mass; if true, the uniformity of mass and similarity of chemical composition for SN Ia progenitors could explain why these supernovae are particularly good standard candles. As supernovae are rare, short-lived, and unpredictable, extensive searches have been mounted using large-aperture telescopes and search techniques that guarantee finding batches of high-redshift supernovae (see, e.g., Perlmutter et al. 1997B), allowing follow-up searches to be scheduled so that the SN Ia light curves and spectra can be monitored.

The basic approach to determining cosmological parameters from supernova observations is contained in the relation between the apparent magnitude m, the absolute magnitude M, and the intervening luminosity distance tex2html_wrap_inline770 :

equation73

This can be rewritten in terms of a tex2html_wrap_inline772 -free luminosity distance tex2html_wrap_inline774 :

  equation76

where defining tex2html_wrap_inline776 means that determining tex2html_wrap_inline778 removes all tex2html_wrap_inline772 dependence from the cosmological density parameters. At a given redshift z, this equation will constrain tex2html_wrap_inline604 and tex2html_wrap_inline700 to an elongated confidence region, the slope of which changes with redshift. Thus by making several measurements over a range of z, one can in principle isolate tex2html_wrap_inline604 and tex2html_wrap_inline700 separately. This is a point stressed by Perlmutter et al. (1997); unless tex2html_wrap_inline794 the luminosity distance tex2html_wrap_inline770 is not a function of merely the deceleration parameter tex2html_wrap_inline746 but of tex2html_wrap_inline604 and tex2html_wrap_inline700 independently:

  equation84

where tex2html_wrap_inline804 is defined as sinh(x), x, and sin(x) for tex2html_wrap_inline812 , tex2html_wrap_inline744 , and tex2html_wrap_inline638 , respectively.


next up previous
Next: Calibration and corrections Up: Type Ia Supernovae Previous: Type Ia Supernovae

Michael Dorris
Tue Jan 18 12:35:56 PST 2000