The Advanced X-ray Astrophysics Facility by Fred Seward AXAF, the Advanced X-ray Astrophysics Facility, is the U.S. follow-on to the Einstein Observatory. Originally three instruments and a high-resolution mirror carried in one spacecraft, the project was reworked in 1992 and 1993. The AXAF spacecraft will carry a high resolution mirror, two imaging detectors, and two sets of transmission gratings. In addition, a cryogenic spectrometer is being developed to fly on the Japanese Astro-E mission. AXAF AXAF will be placed in an elliptical high-earth orbit allowing uninterrupted observing intervals up to 24 hours in length. The AXAF telescope has been designed to have three times the area of the Einstein mirror at low energies and to have considerable collecting area between 6 and 7 keV, the energy of the iron lines strongly emitted by many astrophysical sources. Capability of the observatory goes far beyond that of Einstein. There is an order of magnitude better angular resolution and imaging sensitivity is two orders of magnitude higher. Relative increase in spectroscopy capability is even greater. The mirror consists of four pairs of nested reflecting surfaces, arranged in the usual Wolter type 1 geometry. The high energy response is achieved by use of relatively small reflection angles and by coating the mirrors with iridium. Improvements in mirror technology since Einstein include significant advances in grinding, polishing, alignment, and testing. Mirrors with a resolution of 0.3 arcseconds have been achieved. The combination of high resolution, large collecting area, and sensitivity to higher energy X-rays will make it possible for AXAF to study extremely faint sources, sometimes strongly absorbed, in crowded fields. There are two focal plane instruments. One is a high resolution camera (HRC). Smaller pore size, larger microchannel plate (MCP) dimensions, lower background, charged particle anticoincidence, and possible energy resolution are all advances over ROSAT. It will be used for high resolution imaging, fast timing measurements, and for observations requiring a combination of both. The second instrument, the AXAF CCD imaging spectrometer (ACIS), is an array of charged coupled devices. A two-dimensional array of these small detectors will do simultaneous imaging and spectroscopy. Pictures of extended objects can be obtained along with spectral information from each element of the picture. This was done with the Einstein IPC but in a primitive way compared with this AXAF instrument. The new device combines the spatial resolution of the Einstein HRI with the spectral resolution of the Einstein SSS, an order of magnitude improvement over the IPC in both respects. ASCA (ASTRO-D) carries a similar CCD array but the mirror limits the spatial resolution to ~2 arcminutes. Two transmission grating spectrometers, formed by sets of gold gratings placed just behind the mirrors, are being built for AXAF-I. One set is optimized for low energies (LETG) and the other for high energies (HETG). Spectral resolving powers (E/deltaE) in the range 100-2000 can be achieved with good efficiency. These produce spectra dispersed in space at the focal plane. Either the CCD array or the HRC can be used to record data. XRS The X-ray spectrometer, the XRS, is a quantum calorimeter, a brand new development never used in space, currently being designed and tested at the Goddard Space Flight Center. The instrument will accurately measure the temperature rise due to energy deposited by a single X-ray photon in a small crystal of silicon. An energy resolution of 10 eV, some 10 times better than that of the Einstein SSS, is anticipated. The mirrors are being designed to concentrate radiation from moderately bright, isolated sources. Spatial resolution will probably be about one arcminute. Science AXAF will be capable of very sensitive observations. AXAF will be able to detect most of the ~300 stars in the Pleiades cluster. Individual O stars and RS CVn stars in the Magellanic Clouds can be detected. High resolution grating spectra can be obtained for hundreds of stars. The goal is to determine the temperature, extent, and density of the coronae, and the dependence of physical parameters on stellar type. More detailed structure of coronae might be derived from spectral observations of eclipsing binary systems. Maps can be made of emission from SNR in our galaxy and spectral information will be obtained for all features. Tycho's remnant, for example, can be mapped in the light of X-rays from Si ions, from S ions, and even from Fe ions. Thus, the distribution of different elements within the remnant can be measured. AXAF will be capable of detecting SNR in M31 and extended remnants such as the Cygnus Loop, which, in M31, would be approximately 10" in diameter, will be mapped. In M31 ~200 SNR should be accessible to AXAF. Since higher energy X-rays are capable of penetrating gas and dust, emission from the center of our Galaxy will be clearly seen. Sources in spiral arms on the other side of the center can also be measured and some of their properties determined. The bright bulge sources in M31 are strong enough so that light curves can be measured and a search for the eclipses which identify binary systems will be possible. AXAF in one pointing will be able to monitor the emission of approximately 50 bulge sources in M31. Brighter binary sources in galaxies within the Virgo cluster can also be resolved and detected individually, as obviously can sources in intermediate galaxies. Thus, the population of bright X-ray sources in hundreds of galaxies can be determined. Since high-energy X-rays are unaffected by obscuring material, luminosities of sources can be accurately measured and the hypothesis that these sources, or a subset of them, are "standard candles" can be accurately tested. If such "standard candles" are found, distances to nearby galaxies can be accurately determined. These distances are a crucial step in the derivation of the Hubble Constant and the potential of these measurements is truly exciting. X-rays from distant clusters of galaxies (which are faint and small) can be imaged and spectra measured as a function of position within the cluster. Since the emitting gas is quite hot (10**8 K), the high energy capability of AXAF gives a great sensitivity gain over that of Einstein and ROSAT. Furthermore, since clusters emit the characteristic iron line, the redshift can be measured directly. The spectral and spatial data combined delineate the gravitational potential. The distribution of all matter, including dark matter, within distant clusters can be determined. Data on the evolution of cluster structure with time will be collected. AXAF is expected to detect quasars and active galaxies 100 times fainter than Einstein and can thus look to significantly greater distances. This is unknown territory, except that the integrated emission from many unresolved faint sources probably contributes most of the X-ray background. Deep AXAF observations will come close to imaging this background and will provide a sample of distant objects which record the state of the universe at early times. Once launched, AXAF should enjoy a 5-10 year lifetime. The lifetime of the XRS instrument will be limited to 3-5 years due to the finite amount of cryogen, necessary to cool the detector. AXAF will operate as a true observatory, available through proposal, as is observing time at ground-based facilities. rsimon@matisse.harvard.edu