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System temperature

The system temperature is a summary of the noise added by the system. This noise comes from 1) the receiver and the optics, 2) the emission of the sky, and 3) the emission picked up by the secondary side lobes of the telescope. It is usual to approximate it (in the \ensuremath{T_\ensuremath{\mathrm{a}}^\star} scale) with

\begin{displaymath}
\ensuremath{T_\ensuremath{\mathrm{sys}}}= \frac{\ensuremath...
...hrm{cab}}}+\ensuremath{T_\ensuremath{\mathrm{rec}}} \right] },
\end{displaymath} (1)

where \ensuremath{G_\ensuremath{\mathrm{im}}} is the receiver image gain, \ensuremath{F_\ensuremath{\mathrm{eff}}} the telescope forward efficiency, $\ensuremath{A}= 1/\sin(\ensuremath{\mathrm{elevation}})$ the airmass, \ensuremath{\tau_\ensuremath{\mathrm{s}}} the atmospheric opacity in the signal band, \ensuremath{T_\ensuremath{\mathrm{atm}}} the mean physical atmospheric temperature, \ensuremath{T_\ensuremath{\mathrm{cab}}} the ambient temperature in the receiver cabine and \ensuremath{T_\ensuremath{\mathrm{rec}}} the noise equivalent temperature of the receiver and the optics. All those parameters are easily measured, except \ensuremath{\tau_\ensuremath{\mathrm{s}}}, which depends on the amount of water vapor in the atmosphere and which is estimated by complex atmospheric models.

The \ensuremath{T_\ensuremath{\mathrm{sys}}} value is expressed so that all these terms are corrected for the attenuation by the atmosphere, the coupling of the antenna to the sky, and the side-band rejection. In other words, the system temperature is given in units that assume a perfect antenna (coupling equal to 1) located outside the atmosphere for a single-sideband signal.


next up previous contents
Next: Power and sensitivity measured Up: The interferometric point source Previous: The interferometric point source   Contents
Gildas manager 2023-06-01