[evlatests] Aliasing
Claire Chandler
cchandle at nrao.edu
Thu Mar 27 17:10:36 EDT 2008
Hi Barry,
Gustaaf has reported that the "up" or "down"-ness of the shape of the
bandpasses is a function of IF (not just antenna). How does this fit in
with your analysis below, which has only one delay per antenna?
Claire
On Thu, 27 Mar 2008, Barry Clark wrote:
> Finally the penny dropped.
>
> The aliased power adds to the straight through power as
> 1 + v(f)exp(4*pi*f*Del)
> where f is the frequency in the bandpass, and v(f) the aliasing
> function of the digital filter, as provided by Mike, and Del is the
> differential delay to the two antennas involved introduced by the
> delay lines in the correlator.
>
> I have been assuming that the delay Del was just the adjustable part
> of the delay due to geometry, the w of (u,v,w). It is not. It also
> contains the compensation for the different fiber delays to the two
> antennas involved.
>
> The current fiber delays are given below
> ea01 W10 5214
> ea04 W18 12633
> ea11 E10 7129
> ea13 N16 12290
> ea14 E16 12004
> ea16 W6 3120
> ea17 W14 9144
> ea18 N12 9288
> ea19 W4 3943
> ea21 E2 5661
> ea23 E18 13493
> ea24 W12 6613
> ea25 N2 4941
> ea26 N6 6203
>
> So, in the observation Gustaaf recently took with w near zero, baselines
> in which these fiber delays are nearly the same will have the classic,
> rising to low frequency, profile - baseline 17-18 in particular, but also
> 1-25 and 13-14. Baselines where the difference is near a microsecond will
> still be plunging down to low frequency, with a turnaround below the usable
> bandpass - 21-24, 11-26, 19-25 for instance. Baselines where the difference
> is large will look all squiggly - (4, 13, 14)-(16, 19 25).
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