Nearby Supernova Factory: Étalonnage des données de SNIFS et ...
Nearby Supernova Factory: Étalonnage des données de SNIFS et ...
Nearby Supernova Factory: Étalonnage des données de SNIFS et ...
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tel-00372504, version 1 - 1 Apr 2009<br />
CHAPTER 2. OBSERVATIONAL COSMOLOGY<br />
Scaled f λ + Constant<br />
4<br />
3<br />
2<br />
1<br />
0<br />
Ca II<br />
Ca II<br />
Si II<br />
Fe II<br />
Co II<br />
Cr II<br />
Fe II<br />
Fe II<br />
Si II<br />
Fe III<br />
Fe II<br />
Cr II<br />
Co II<br />
S II<br />
Cr II<br />
Si II<br />
Si II<br />
Na I Si II Fe II<br />
SN 2001V<br />
day +20<br />
4000 5000 6000 7000<br />
Rest Wavelength (Å)<br />
(a)<br />
FLUX<br />
100<br />
10<br />
1<br />
98aq<br />
96X<br />
90N<br />
94ae<br />
98bu<br />
01el<br />
94D<br />
4000 5000 6000 7000 8000<br />
WAVELENGTH<br />
Figure 2.8: (a) Spectrum and characteristic lines at maximum (up) and 20 days later (bottom) for a<br />
typical SN Ia (SN1998aq). From Matheson <strong>et</strong> al. (2008). (b) Spectra at maximum luminosity for several<br />
“Branch-normal” SNe Ia. From Branch <strong>et</strong> al. (2006).<br />
The analysis of SNe Ia spectral evolution divi<strong><strong>de</strong>s</strong> their lif<strong>et</strong>ime into two phases: the early<br />
photospheric phase, where the outer layers are opaque to radiation and we observe their constitution<br />
in the form of absorption lines, that change as the layers expand and become transparent;<br />
and the nebular phase, several weeks after maximum, when the environment has become transparent<br />
and we observe the emission lines of the inner layers, that can be attributed to Co and<br />
Fe transitions. The nebular phase is dominated by the changing strength of these individual<br />
lines multipl<strong>et</strong>s. Despite the overall uniformity, subtle differences exist in lines strengths and<br />
velocities b<strong>et</strong>ween different SNe Ia (Hachinger <strong>et</strong> al. 2006).<br />
Deserving to be placed in a category apart, are a lot of peculiar SNe Ia presenting very<br />
different light curves and spectra from the “typical” ones. These will be presented in § 2.3.3.<br />
While this photom<strong>et</strong>ric/spectroscopic division was ma<strong>de</strong> for easier presentation, they are<br />
obviously intrinsically connected: a light curve point is nothing more than the integration of<br />
a supernova spectrum by a bandpass filter. It is then clear that we could easily study the<br />
homogeneity and standardization of the SNe Ia class by simply using absolutely flux calibrated<br />
spectra. We will see in § 3 how the SNfactory project intends to do this.<br />
2.3.3 SNe Ia h<strong>et</strong>erogeneity - peculiar objects<br />
Not all supernovæ fall into the “Branch-normal” category, as the ones already introduced.<br />
Some are substantially different, enough to place them into two distinct categories: un<strong>de</strong>rluminous<br />
and overluminous. They are connected to two objects observed in 1991 and used as<br />
the “reference” for each subclass: SN1991bg (un<strong>de</strong>r-) and SN1991T (overluminous) respectively.<br />
Typical light curves and spectra for these supernovæ are presented in Fig. 2.9.<br />
30<br />
(b)