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The instrument

THE MARSEILLE OBSERVATORY Htex2html_wrap_inline140 SURVEY OF THE SOUTHERN GALACTIC PLANE AND MAGELLANIC CLOUDS

D. RUSSEIL, Y.M. GEORGELIN, P. AMRAM, Y.P. GEORGELIN, A. LAVAL, M. MARCELIN, PASA, 15 (1), 9
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The instrument

The instrument, located at the Southern European Observatory in La Silla, uses a 36 cm telescope equipped with a focal reducer (final F/D=3.3), a photon counting camera and a scanning Fabry-Perot interferometer, which provide the ideal characteristics for a systematic survey: large field (38'X38'), high luminosity, high spectral resolution and limited spectral range centered on the Htex2html_wrap_inline140 line. In practice we use two different Fabry-Perot interferometers depending on the expected velocity range of the object to observe. They offer free spectral ranges of 376 km tex2html_wrap_inline150 and 115 km tex2html_wrap_inline150 with respective spectrum samplings of 16 km tex2html_wrap_inline150 and 5 km tex2html_wrap_inline150. For these interferometers the finesse is about 12 or 10, explaining why we scan through 24 scanning steps according to common sampling criterion. The recent determination of the flux detection limit is about 0.2 Rayleigh (1 Rayleigh = 2.4 tex2html_wrap_inline158 erg tex2html_wrap_inline160tex2html_wrap_inline150tex2html_wrap_inline164 at Htex2html_wrap_inline140) for a typical observation time of two hours. This allows us to observe not only the individual HII regions but also the diffuse emission of the ionized gas.

The interpretation of the data requires splitting of the observed profiles into elementary components as is illustrated in Fig.1. The night-sky lines (geocoronal Htex2html_wrap_inline140 and OH lines) and the nebular ones are respectively modeled by a pure instrumental profile, and an instrumental profile convolved with a gaussian ( details are given in Georgelin et al., 1994).

á figure31
Figure 1: Htex2html_wrap_inline140 profiles resulting from the addition of several pixel profiles covering an "empty zone" (upper profile) and the HII region G296.593-0.975 (lower profile) in the direction l=298tex2html_wrap_inline172. The first profile is decomposed into two nightsky lines (components 2 and 3) and two nebular components ( components 0 and 1 ) associated to diffuse emissions. In the second profile, one more emission ( component 4) line appears at positive velocity, corresponding to the HII region.

á figure35
Figure: Htex2html_wrap_inline140 mosaic of the observed fields in the 305tex2html_wrap_inline172 area. This image is obtained by adding tex2html_wrap_inline146 maps over the whole free spectral range, flat fielding and then correcting for distortion. This is equivalent to a photograph obtained through a filter with a 2.4 ö…á bandwidth. The positions of radio sources and HII regions are shown with the corresponding Htex2html_wrap_inline140 velocity values, when observed.

á figure41
Figure 3: Spatial distribution of velocity components in the 305tex2html_wrap_inline172 area. Only the non-local components are indicated. Note that the velocities of the diffuse Htex2html_wrap_inline140 emission, as well as those of the discrete HII regions, are shown at the points of measurements. Bold letters correspond to Htex2html_wrap_inline140 emission patches in the mosaic. Very closely placed numbers represent multiple components at one point of measurements.


Next Section: The Survey of the
Title/Abstract Page: THE MARSEILLE OBSERVATORY H
Previous Section: Introduction
Contents Page: Volume 15, Number 1

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