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Techniques d'observation spectroscopique d'astéroïdes

Techniques d'observation spectroscopique d'astéroïdes

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62 CHAPTER 3. OBSERVING TECHNIQUES<br />

1<br />

0.8<br />

Relative Flux<br />

0.6<br />

0.4<br />

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

0.2<br />

Asteroid<br />

Star<br />

0<br />

0.8 1 1.2 1.4 1.6 1.8 2 2.2 2.4<br />

Wavelength [um]<br />

Figure 3.3: The raw spectra of an asteroid and standard star. The twos spectra are modulated by the absorption<br />

bands of the Earth atmosphere (essentially telluric water bands).<br />

at two separate locations along the slit (close to top - "A" and close to bottom - "B"). This is<br />

call the nodding procedure [Nedelcu, 2010]. In the low resolution mode of SpeX, spectra are<br />

acquired only in a band of 512x100 pixels of the CCD.<br />

Flat field corrections.<br />

The flat field images are made using a lamp based on Quartz-<br />

Tungsten-Halogen (T=3200 K). This procedure is applied at the beginning and at the end of<br />

the observing session, by taking 10 images each time. If a pixel value is greater than 10%<br />

of the neighboring pixels, it is considered as a bad pixel. Such pixels are replaced in all images<br />

(object images, flat fields and arc images and standard star images) with a value obtained<br />

from interpolation of neighboring pixel values. A "master flat" is obtained by combining and<br />

averaging all flat field images. The master flat field is subtracted from all images.<br />

Removing the sky background. The consecutive images A and B are subtracted (A-B and<br />

B-A) resulting new images containing two spectra: one with positive pixel values and another<br />

with negative pixel values (Fig. 3.2.3).<br />

Wavelength calibration. The wavelength calibration is made by identifying the emission<br />

lines of an Argon lamp. Thus, it results a correspondence between the pixel position on the<br />

x-axis and the wavelength (Fig. 3.2.3).<br />

Combining the images. The two spectra (corresponding to both positive and negative pixel<br />

values ) are identified in each image. The images are cut, only the positive spectrum being kept.<br />

A final spectral image (Fig. 3.2.4) is obtained for each object by gathering all its corresponding<br />

images (before summing all images they are aligned by the brightest trace).<br />

Extraction of the raw spectrum. The final point of this stage consists in summing the value

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