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The Chandra
X-ray Observatory (CXO) was launched on the Space Shuttle Columbia on
The Advanced CCD Imaging Spectrometer (ACIS), built by the Pennsylvania State University in collaboration with the Massachusetts Institute of Technology (MIT);
The High Resolution Camera (HRC) built by the Smithsonian Astrophysical Observatory (SAO);
The Low Energy Transmission Grating (LETG) built by the Scientific Research Organization of the Netherlands (SRON) in collaboration with the Max-Planck-Institüt für Extraterrestriche Physik (MPE); and
The High Energy Transmission Grating (HETG) built by MIT.
Chandra has as its primary mission the study of the structure and emission properties of astrophysical sources of high-energy radiation. The scientific objectives of the Chandra Mission are to utilize the Observatory to:
Determine the nature of celestial objects from normal stars to quasars;
Understand the nature of physical processes that take place in and between astronomical objects; and
Understand the history and evolution of the universe.
Chandra is comprised of the spacecraft, the X-ray telescope, and the Science Instrument Module (SIM). The spacecraft provides the power, attitude control, communications, etc. for the telescope and instruments. The X-ray telescope consists of an optical bench, the High Resolution Mirror Assembly (HRMA), an aspect camera system, and two objective transmission gratings: the High Energy Transmission Grating (HETG) and the Low Energy Transmission Grating (LETG). The HRMA is a Wolter Type I, 1.2-m diameter, 10-m focal length, iridium-coated X-ray telescope consisting of 4 nested pairs of cylindrical hyperboloid and paraboloid mirrors. At 1.5 keV, >85% of the on-axis, imaged and aspect-corrected X-rays are contained in a circle of diameter ~1.0 arc second.
Chandra carries two focal-plane scientific instruments mounted in the SIM: the ACIS, and the HRC. The SIM provides three functions: launch lock, translation (to interchange focal plane instruments), and focus. Only one of the two focal plane instruments can be placed at the telescope’s focus at any time; therefore, simultaneous observations with both focal-plane instruments cannot be accommodated.
The ACIS has two arrays of CCDs, one (ACIS-I) optimized for imaging wide fields (16x16 arc minutes) the other (ACIS-S) optimized as a readout for the HETG transmission grating. One chip of the ACIS-S (S3) can also be used for on-axis (8x8 arc minutes) imaging and offers the best energy resolution of the ACIS system.
The HRC is comprised of two micro-channel plate imaging detectors, and offers the highest spatial (<0.5 arc second) and temporal (16 msec) resolutions. The HRC-I is a single micro-channel plate and has a field-of-view of 31x31 arc minutes. The HRC-S consists of three contiguous segments, tilted slightly in order to conform to the Rowland circle of the LETG. The background rate is quite different in the two devices, being larger in the HRC-S.
The HETG is optimized for high-resolution spectroscopy over the energy band 0.4-10 keV. Two types of gratings are mounted in the HETG: medium-energy gratings (MEGs) covering the 0.4–5 keV band and high-energy gratings (HEGs) covering the 0.9–10 keV band. The MEGs are mounted behind the annular aperture of the outer two mirror pairs while the HEGs are mounted behind the apertures of the inner two mirror pairs. The two sets of gratings operate simultaneously so that the dispersed axes of the spectra cross at a shallow angle in the focal plane. The ACIS-S is the readout of choice for use with the HETG. The resolving power (E/DE) varies from ~800 at 1.5 keV to ~200 at 6 keV.
The LETG is optimized for high-resolution spectroscopy over the energy bandwidth ~0.09–4 keV. The LETG provides resolving power ~1000 at 0.1 keV and ~200 at 1.5 keV. The HRC-S is the only detector aboard the Observatory that can fully accommodate the LETG-dispersed spectrum.
Detailed descriptions of all of the instruments are contained in the Proposers’ Observatory Guide. Proposers should refer to that document for additional details before preparing a proposal.
The initial Chandra operational orbit was achieved by use of Boeing’s Inertial Upper Stage and Chandra’s own propulsion system. There are sufficient expendables (control gas for momentum unloading) for well over 10 years of operation. The orbital period of about 63.5 hours allows for reasonably long, uninterrupted observations of up to ~160 ksec before the instruments have to be powered down as the satellite dips into the radiation belts. Approved longer observations are split into several orbit-sized observations on ingestion into the observation catalog.
The Observatory’s solar panels can rotate about an axis perpendicular to the optical axis so that at any time the Observatory can be pointed to any position in the sky except for avoidance regions around the Sun (46 degrees), Moon (6 degrees), and Earth (10 degrees). Both the Moon and Earth may be viewed if specially requested and as long as an accurate aspect solution is not required. In order to avoid over-heating the EPHIN charged particle detector or excessive cooling of the propellant lines, the maximum length of an exposure is dependent on the pitch angle at which the target is observed. Some pitch angles are excluded. Observations with exposure times longer than the maximum allowed at a given pitch angle will be segmented. Current details of these restrictions are given in the Proposers’ Observatory Guide (http://cxc.harvard.edu/proposer/POG/index.html). However, pitch angle restrictions are evolving with time and proposers are urged to check the CXC website for current information.
The high elliptical orbit and the radiation belts that prevent the conduct of observations at low altitudes imply that most of observations are made nearer apogee, where the Earth, as seen from Chandra, appears to move only slowly through the sky. As a result, the Earth and its surrounding avoidance region constitute a portion of the sky that will be partially blocked from view, and long, continuous observations in this region (>30 ksec at the center of the region) will be difficult, although shorter observations are possible. The proposer is urged to read the appropriate chapter of the Proposers’ Observatory Guide (POG) to become familiar with all Chandra observing constraints and to make use of the Observation Visualizer (ObsVis) (http://obsvis.harvard.edu/) to see how these constraints might impact their observations.
The Chandra
X-ray Center (CXC), funded by NASA via a contract to the Smithsonian
Astrophysical Observatory (SAO) in
SAO, through its management of the CXC, is responsible for scientific research of the highest technical merit utilizing the Chandra X-ray Observatory. In order to carry out this responsibility, NASA has directed SAO to engage the participation of the broader science community and has determined that this function will be accomplished by SAO allotting observing time and research funding to users in accordance with the following process conducted at appropriate intervals:
SAO is not responsible for transferring funds to
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The Chandra X-Ray
Center (CXC) is operated for NASA by the Smithsonian Astrophysical Observatory. 60 Garden Street, Cambridge, MA 02138 USA. Email: cxcweb@head.cfa.harvard.edu Smithsonian Institution, Copyright © 1998-2004. All rights reserved. |