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Future Instrumentation for Solar and Stellar Research at Radio ...

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By deploying N antennas over a two dimensional area, one<br />

can measure N(N-1)/2 Fourier components of the 2D radio<br />

brightness I instantaneously on a large number of angular<br />

scales <strong>and</strong> orient<strong>at</strong>ions.<br />

An inverse Fourier trans<strong>for</strong>m of the measured Fourier<br />

components yields I*B, the convolution of I with the<br />

instrumental response function B. Deconvolution<br />

techniques are used to recover I.<br />

The sensitivity of a radio telescope depends on the collecting<br />

area, the sensitivity of the receivers, <strong>and</strong> the signal<br />

b<strong>and</strong>width, <strong>and</strong> the integr<strong>at</strong>ion time.<br />

The imaging fidelity depends upon how well the Fourier<br />

trans<strong>for</strong>m of the sky is sampled, how well sources of<br />

system<strong>at</strong>ic error are elimin<strong>at</strong>ed, <strong>and</strong> how well<br />

deconvolution algorithms per<strong>for</strong>m.

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