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Techniques d'observation spectroscopique d'astéroïdes

Techniques d'observation spectroscopique d'astéroïdes

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CHAPTER 2. WHY SPECTROSCOPY? 49<br />

0.6<br />

Flux [arbitrary units]<br />

(a)<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

400 450 500 550 600 650 700<br />

Wavelength [nm]<br />

Correlation coefficient<br />

(b)<br />

0.4<br />

0.2<br />

0<br />

−0.2<br />

−0.4<br />

0.4 0.6 0.8 1 1.2 1.4 1.6 1.8<br />

z<br />

Figure 2.4: a) PG1634 + 706 spectrum obtained after data reduction and continuum subtraction; b) the correlation<br />

coefficient between quasar spectrum and the template spectrum shifted with different z [Popescu et al., 2012a].<br />

tel-00785991, version 1 - 7 Feb 2013<br />

varying background to zero and essentially has the same effect as filtering out the long-period<br />

Fourier components of the spectra. Without continuum subtraction, the intensities of spectral<br />

lines are not clearly detectable. The continuum was removed by dividing the spectrum with<br />

a fifth order polynomial curve fitting. The obtained result after data reduction and continuum<br />

subtraction is given in Fig. 2.4.<br />

The redshift is defined as the ratio of the change in wavelength (∆λ = λ obs − λ 0 ) to the<br />

non-shifted wavelength (λ 0 ) from a stationary source:<br />

z= λ √<br />

obs− λ 0 c+v<br />

=<br />

λ 0 c−v − 1 (2.8)<br />

where c is the speed of light in free space and v is the recession speed of the object. The analysis<br />

of the obtained spectrum of PG1634+706 consists in redshift determination and application of<br />

Hubble law to determine its distance.<br />

The most common technique [Tonry & Davis, 1979] to determine the redshift is the crosscorrelation<br />

of the observed spectrum with a template spectrum. The redshift is determined by<br />

the location of the largest peak in the cross-correlation functions. Several rest frame composite<br />

quasar spectra exists for the optical region like the one from the article of [Francis et al.,<br />

1991] obtained using data from Large Bright Quasar Survey (LBQS). Thus for determining the<br />

redshift of our spectrum the following steps were taken:<br />

• Shift the template spectrum with a z varying from 0.4 to 1.8 using the step of 0.001. This<br />

is a reasonable assumption made after visual inspection of our data.<br />

• At each step, the correlation coefficient between the quasar spectrum and the shifted template<br />

spectrum is computed (Fig. 2.4).<br />

• Choose the redshift corresponding to the best correlation coefficient found.<br />

In this way, it was obtained z = 1.340 corresponding to the peak value of the correlation

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