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The cosmic microwave background (CMB) is the photon remnant from the Big Bang. By tracing fluctuations in the light intensity, the fluctuations in the matter density of the universe at roughly 100,000 years after the big bang can be inferred. Understanding these fluctuations may allow measurements of fundamental cosmological parameters that can enlighten the state of the universe in the past, present, and future. Because of the importance of the CMB, satellites are being designed to map it over the whole sky, but significant progress can be made before they are launched. The MAT proposal was to modify an existing high altitude balloon borne telescope for ground-based operations. Test measurements indicated the site in the Chilean Andes will allow such a high quality data that nearly 90% could be used in the final analysis, as compared to 20% at a similar ground-based instrument in Saskatchewan. This is due to the site's altitude and dry atmosphere, which reduce the total atmospheric emission by two-thirds. The called MAT (Mobile Anisotropy Telescope) was a modification of the QMAP experiment, which flew on high altitude balloons. The portable instrument allowed the most sensitive measurement then of the power spectrum of the CMB. We observed 3,400 deg2 in a ring of 10 degrees width around the entire sky at a declination of -15 degrees. The Science: The Technology: The Site: Detailed site measurements by NRAO for the Millimeter Array indicate that it is one of the best sites in the world for taking millimeter measurements. With two months of observations, same as at Saskatoon, the net sensitivity is expected to be 2.5-3 times better at the Chilean site. This is due to the fact that nearly every day the overall sky opacity and its stability at the Chilean site is better than during the best days in Saskatoon, making one observing season in Chile worth 6-9 in Saskatoon. The Instrument: The chopping flat is a 5' by 4' oval of 0.5" thick aluminum honeycomb panel. It resonantly chops the beam sinusoidally at 4.6 Hz with an amplitude of 3.25°. This leads to a peak-to-peak angle on the sky of 10° (2 x 2 x 3.25° x cos 42°). The flat is attached to the telescope by two bearings on its rotation axis and by two leaf springs. The spring constants are adjusted to give the desired resonant frequency. The Q of the system has been measured to be as high as 100 resulting in a minimum amount of power required to operate (an important consideration at a remote site). Operation at a remote location makes the use of liquid helium to keep the SIS detectors at 4.2 K impractical. In the past we have used a recycling Gifford-MacMahon refrigerator operating at 17 K. We have identified a new closed system which can maintain the cold plate at 4.2 K with 500 mW of cooling power. The secondary stage of the system is at 40 K and will act as a thermal shunt for the wires and waveguide going to the cold plate. Mechanical Design/Support Electronics: The telescope pointing will be determined by a 16 bit digital encoder on the axis of the main azimuthal bearing. The encoder calibration will be determined during each of the planetary observations. At night, a computer-controlled CCD camera will log the positions of the stars in the field of view and determine the encoder azimuth almost continuously for both east and west observations. The encoder position information is then used by the gear motor to point the telescope to the desired place on the sky. Pointing and data acquisition are controlled by two separate computers synchronized with a common clock. The pointing computer records the encoder position, runs the CCD and interprets commands from a remote station (located in the nearest town approximately 100 miles from the site). The data computer simply logs the detector outputs (both AC and DC components), chopper position, and housekeeping information. From the remote station we can monitor all signals and plot any channel to quickly assess and correct any problems. Logistics: |