Techniques d'observation spectroscopique d'astéroïdes
Techniques d'observation spectroscopique d'astéroïdes Techniques d'observation spectroscopique d'astéroïdes
114 M. Popescu, M. Birlan , R. M. Gherase , A. B. Sonka , M. Naiman , C. P. Cristescu their spectra of the emission lines (example: hydrogen Balmer lines - Hα, Hβ, Hγ) reveals that a large Doppler redshift exists for this type of objects. This redshift is defined as the ratio of the change in wavelength (Δλ = λ obs – λ 0 ) to the non-shifted wavelength from a stationary source: Δλ c + v z = = −1 (3) λ0 c − v where c is the speed of light and v is the recession speed of the object. tel-00785991, version 1 - 7 Feb 2013 Fig 6. Correlation coefficient between quasar spectrum and the template spectrum shifted with different z. The analysis of the obtained spectrum of the quasar PG1634+706 consists in redshift determination and application of Hubble law to determine the distance. The most common technique [14] to determine the redshift is the crosscorrelation of the observed spectrum with a template spectrum. The redshift is determined by the location of the largest peak in the cross-correlation functions. Several rest frame composite quasar spectra exists for the optical region like the one from article [15] obtained using data from Large Bright Quasar Survey (LBQS) and form article [16] based on Sloan Digital Sky Survey (SDSS). Thus for determining the redshift of our spectrum the following steps were taken: 1.) shift the template spectrum with a z varying from 0.4 to 1.8 using the step of 0.001. This is a reasonable assumption made after visual inspection of our data; 2.) at each step, the correlation coefficient between the quasar spectrum and the shifted template spectrum is computed (Fig. 6); 3.) choose the redshift corresponding to the best correlation coefficient found. In this way, we obtained z = 1.340 corresponding to the peak value of the correlation coefficient equal with 0.5416. Our determination is at ~ 3σ (where σ = 0.1987 is the standard deviation of the correlation coefficient values plotted in Fig. 6). Considering the value found for the redshift - z = 1.340, the emission lines of known chemical elements could be identified in the spectrum of PG1634+706
Applications of optical and infrared spectroscopy to astronomy 115 (Table 2). Based on the emission line identification the accuracy of z determination can be ascertained: z = 1.340 ± 0.008. Table 2 Emission line identification in spectrum of PG1634 +706 Line Rest-frame wavelength [nm] λ shifted with z=1.34 [nm] C III] 190.6 446.0 444 Fe III 207.7 485.8 488 Fe II + CII] 232.6 544.3 544 Mg II 280.0 655.2 655 λ observed in quasar spectrum [nm] tel-00785991, version 1 - 7 Feb 2013 Edwin Hubble showed that there is a pattern in the speeds with which the galaxies are receding form us which implies that the Universe is expanding [15]. Observations that followed confirmed Hubble law: v = H 0 ⋅d (4) where v is the radial velocity and d is the distance and H 0 is the Hubble constant. Recently, high-redshift measurements have been used to predict the value of H 0 [16, 17]: km H 0 = 70.3 ± 1. 3 (5) s ⋅ Mpc Applying the equation (3), (4), (5) the speed of this object and the distance to it can be computed (Eq. 6). 2 ( z + 1) −1 8 m v = c ⋅ = (2.073 ± 0.018) ⋅10 2 ( z + 1) + 1 s v 9 d = = (9.644 ± 0.16) ⋅10 light years H 0 These results are in agreement with the value found by other studies of this bright quasar [3, 4, 31]. (6) 4. Data reduction and data analysis of reflection spectra – application to 9147 Kourakuen The observation of reflection spectra from a celestial object implies additional steps in both observing method and data reduction procedure. This is due to the fact that the light reflected from the surface of the body must be divided by a spectrum of a solar-like star to determine the reflectance relative to that of the original light source, the Sun. Thus, the data reduction process for the reflection spectra consist in tree steps: 1) obtain the raw spectra for the object and the solar
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114 M. Popescu, M. Birlan , R. M. Gherase , A. B. Sonka , M. Naiman , C. P. Cristescu<br />
their spectra of the emission lines (example: hydrogen Balmer lines - Hα, Hβ, Hγ)<br />
reveals that a large Doppler redshift exists for this type of objects. This redshift is<br />
defined as the ratio of the change in wavelength (Δλ = λ obs – λ 0 ) to the non-shifted<br />
wavelength from a stationary source:<br />
Δλ<br />
c + v<br />
z = = −1<br />
(3)<br />
λ0<br />
c − v<br />
where c is the speed of light and v is the recession speed of the object.<br />
tel-00785991, version 1 - 7 Feb 2013<br />
Fig 6. Correlation coefficient between quasar spectrum and the template spectrum shifted with<br />
different z.<br />
The analysis of the obtained spectrum of the quasar PG1634+706 consists<br />
in redshift determination and application of Hubble law to determine the distance.<br />
The most common technique [14] to determine the redshift is the crosscorrelation<br />
of the observed spectrum with a template spectrum. The redshift is<br />
determined by the location of the largest peak in the cross-correlation functions.<br />
Several rest frame composite quasar spectra exists for the optical region like the<br />
one from article [15] obtained using data from Large Bright Quasar Survey<br />
(LBQS) and form article [16] based on Sloan Digital Sky Survey (SDSS). Thus<br />
for determining the redshift of our spectrum the following steps were taken: 1.)<br />
shift the template spectrum with a z varying from 0.4 to 1.8 using the step of<br />
0.001. This is a reasonable assumption made after visual inspection of our data;<br />
2.) at each step, the correlation coefficient between the quasar spectrum and the<br />
shifted template spectrum is computed (Fig. 6); 3.) choose the redshift<br />
corresponding to the best correlation coefficient found.<br />
In this way, we obtained z = 1.340 corresponding to the peak value of the<br />
correlation coefficient equal with 0.5416. Our determination is at ~ 3σ (where σ =<br />
0.1987 is the standard deviation of the correlation coefficient values plotted in<br />
Fig. 6).<br />
Considering the value found for the redshift - z = 1.340, the emission lines of<br />
known chemical elements could be identified in the spectrum of PG1634+706