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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)

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