Techniques d'observation spectroscopique d'astéroïdes
Techniques d'observation spectroscopique d'astéroïdes Techniques d'observation spectroscopique d'astéroïdes
118 M. Popescu, M. Birlan , R. M. Gherase , A. B. Sonka , M. Naiman , C. P. Cristescu tel-00785991, version 1 - 7 Feb 2013 from this meteorite contains SiO2 (50.1%), MgO(23.7%), FeO(15%), Al2O3(6.2%), CaO(3.8%) [26]. Laboratory spectra similar to the spectrum of (9147) Kourakuen are those of the meteorites Roda (Achondrite Diogenite), Le Teilleul (Achondrite, Howardite) and Kapoeta (Basaltic HED Howardite). The first fifty solutions that matched our spectrum are HED (Howardite Eucrite Diogenite) meteorites. These are basaltic meteorites believed to result from large asteroids that melted to form a metallic core and basaltic magmas after the formation. The absorption band parameters are diagnostic of the mineralogy present on the surface of the observed asteroids. The relationship between these spectral parameters and the mineralogy, particularly pyroxene and olivine, has been studied in various papers over the last years [28]. Most pyroxenes and the basaltic achondrites show a strong correlation between the position of band centers at 1 μm and 2 μm [28, 29, 30]. Thus, we computed the band minima and band centers (at 1 μm and 2 μm), defined as the wavelength position of the point of lowest reflectance before and after the removal of the continuum, respectively [28]. The computations were done using the standard procedures [31]. The results are given in Table 3. Table 3 Band centers and band separation as deduced from Cloutis model. BI center (μm) BII center (μm) Band separation [μm] 0.913 ±0.005 1.952 ±0.005 1.039±0.010 5. Discussions and conclusions We described here two types of spectra of celestial bodies – the emission spectrum of a very far away object, the quasar PG1634 +706 and the reflection spectrum of a remnant object from the solar system formation, (9147) Kourakuen. The techniques for acquiring the spectra and the models used for data analysis are presented. The two types of observations share common points in acquisition procedure, data reduction and data analysis methods. Conceptually the design of the acquisition system is the same: a telescope, a diffraction device (which could be a grating that works in transmission or reflection, or a prism) and the device to record the image of the spectrum – a charge coupled device (CCD). Also, extracting the spectrum from the image follows almost the same steps: the identification of the trace of the spectrum and getting pixel values, wavelength calibration, removing the Earth atmospheric influences in the spectrum. Data analysis includes the comparison between the spectra of celestial body with known spectra from the laboratory.
Applications of optical and infrared spectroscopy to astronomy 119 tel-00785991, version 1 - 7 Feb 2013 However the wide variety of results that can be obtained from analyzing the emission spectra and the reflection spectra from celestial bodies has lead to two separate domains of astronomy. Because PG1634 +706 is a bright quasar, it has been studied in some papers like [3, 4, 31, 32]. Our observation for this object was at the limited magnitude for the type of equipment used. With a robust method, we succeed to extract the signal from noise and compute the redshift. Our determination of redshift z = 1.340 ± 0.008, with a small telescope agrees with the value found after observation with large telescopes. The developed methods for observations and data reduction can be used as a starting point for spectroscopy of celestial bodies with small telescopes. We obtained an accurate near-infrared spectrum of the asteroid (9147) Kourakuen. Based on this spectrum, a description of the surface composition was made. The comparisons with meteorites spectra revealed a spectral matching with HED type meteorites and in particular with the spectrum of Pavlovka meteorite. Using the Bus-DeMeo taxonomy, we classified this object as a V-type (taxonomic class describing asteroids with similar spectra as Vesta), which agrees to the type identified using a relatively more noisy spectrum by [22]. R E F E R E N C E S [1] Anil K. Pradhan, Sultana N. Nahar; Atomic Astrophysics and Spectroscopy; Cambridge University Press 2011; [2] Bennoit Carry; Etudes des proprietes physiques des asteroides par imagerie a haute resolution angulaire, Ph. D. Thesis; UNIVERSITE PARIS.DIDEROT (Paris 7), 29/09/2009 [3] Schmidt, M.; Green, R. F.; Quasar evolution derived from the Palomar bright quasar survey and other complete quasar surveys; Astrophysical Journal, Part 1 (ISSN 0004-637X), vol. 269, June 15, 1983, p. 352-374.;06/1983 [4] Trevese, D.; et al.; Line and continuum variability of two intermediate-redshift, highluminosity quasars; Astronomy and Astrophysics, Vol. 470, Issue 2, August I 2007, pp.491- 496 [5] Schelte John Bus; Compositional structure in the asteroid belt: result of a spectroscopic survey; Ph. D. Thesis - MIT; 04/1999 [6] Francesca E. DeMeo; La variation compositionnelle des petits corps a travers le systeme solaire; Ph. D. Thesis - Observatoire de Paris 16/06/2010 [7] Star Analyser site: http://www.patonhawksley.co.uk/staranalyser.html [8] Rayner, J. T.; et al ; The Publications of the Astronomical Society of the Pacific, Vol. 115, Issue 805, pp. 362-382; 03/2003 [9] Birlan, M.; Barucci, A.; Thuillot, W.; Solar system observations by remote observing technique: useful experience for robotic telescope strategies; Astronomische Nachrichten, Vol.325, Issue 6, p.571-573; 10/2004 [10] Birlan, M.; et al.; Near infra-red spectroscopy of the asteroid 21 Lutetia. I. New results of long-term campaign; Astronomy and Astrophysics, Vol. 454, Issue 2, August I 2006, pp.677-681 [11] Dan Alin Nedelcu; Modelisation Dynamique et spectroscopique des asteroides; Ph. D. Thesis - Observatoire de Paris; 23 09/2010;
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118 M. Popescu, M. Birlan , R. M. Gherase , A. B. Sonka , M. Naiman , C. P. Cristescu<br />
tel-00785991, version 1 - 7 Feb 2013<br />
from this meteorite contains SiO2 (50.1%), MgO(23.7%), FeO(15%),<br />
Al2O3(6.2%), CaO(3.8%) [26].<br />
Laboratory spectra similar to the spectrum of (9147) Kourakuen are those<br />
of the meteorites Roda (Achondrite Diogenite), Le Teilleul (Achondrite,<br />
Howardite) and Kapoeta (Basaltic HED Howardite). The first fifty solutions that<br />
matched our spectrum are HED (Howardite Eucrite Diogenite) meteorites. These<br />
are basaltic meteorites believed to result from large asteroids that melted to form a<br />
metallic core and basaltic magmas after the formation.<br />
The absorption band parameters are diagnostic of the mineralogy present on the<br />
surface of the observed asteroids. The relationship between these spectral<br />
parameters and the mineralogy, particularly pyroxene and olivine, has been<br />
studied in various papers over the last years [28]. Most pyroxenes and the basaltic<br />
achondrites show a strong correlation between the position of band centers at 1<br />
μm and 2 μm [28, 29, 30]. Thus, we computed the band minima and band centers<br />
(at 1 μm and 2 μm), defined as the wavelength position of the point of lowest<br />
reflectance before and after the removal of the continuum, respectively [28]. The<br />
computations were done using the standard procedures [31]. The results are given<br />
in Table 3.<br />
Table 3<br />
Band centers and band separation as deduced from Cloutis model.<br />
BI center (μm) BII center (μm) Band separation [μm]<br />
0.913 ±0.005 1.952 ±0.005 1.039±0.010<br />
5. Discussions and conclusions<br />
We described here two types of spectra of celestial bodies – the emission<br />
spectrum of a very far away object, the quasar PG1634 +706 and the reflection<br />
spectrum of a remnant object from the solar system formation, (9147) Kourakuen.<br />
The techniques for acquiring the spectra and the models used for data analysis are<br />
presented.<br />
The two types of observations share common points in acquisition<br />
procedure, data reduction and data analysis methods. Conceptually the design of<br />
the acquisition system is the same: a telescope, a diffraction device (which could<br />
be a grating that works in transmission or reflection, or a prism) and the device to<br />
record the image of the spectrum – a charge coupled device (CCD). Also,<br />
extracting the spectrum from the image follows almost the same steps: the<br />
identification of the trace of the spectrum and getting pixel values, wavelength<br />
calibration, removing the Earth atmospheric influences in the spectrum. Data<br />
analysis includes the comparison between the spectra of celestial body with<br />
known spectra from the laboratory.