1994
DOI: 10.1109/5.284731
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Ground antennas in NASA's deep space telecommunications

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Cited by 7 publications
(4 citation statements)
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“…As N increases from one to a large number, the excess noise temperature given by Equation (2) increases to a maximum, and then goes to zero as N continues to become very large. This is not obvious from a cursory examina tion of Equation …”
Section: Excess Noise Temperature and Added-gain Lossmentioning
confidence: 94%
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“…As N increases from one to a large number, the excess noise temperature given by Equation (2) increases to a maximum, and then goes to zero as N continues to become very large. This is not obvious from a cursory examina tion of Equation …”
Section: Excess Noise Temperature and Added-gain Lossmentioning
confidence: 94%
“…Additionally, in the receive mode the antenna systems arc designed to have vety low system noise temperatures. Increasing the gain and lowering the system noise temperatures translate into maximizing the ground-received signal-to-noise ratio [2]. Over the years, a great deal of attention has been paid to low ering system noise temperatures, through the use of low-loss front end microwave waveguide components, ami cryog enically cooled low-noise amplifiers (masers and high-electron-mobility transis tors).…”
Section: Background On Dsn Antennasmentioning
confidence: 99%
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“…The G/TOp parameter is defined by 4 x A e k-z GffoP = __;. ;__ ;..._-- (1) where A e is the effective antenna area, X is the received wavelength, TOP = (T a + T e ) is the system operating noise temperature ( Ref 3,4), Ta is the antenna noise temperature with contributions from the 2.73 K cosmic background, the earth's atmosphere (Tatm) and the antenna transmission line (TI) and T e is the effective Page 2 Printed (1 1/15/93) noise temperature of the receiving system with contributions from the low noise amplifier (Tlna), and the follow-up amplifier (Tf).…”
Section: Calibrating Large Microwave Antennasmentioning
confidence: 99%