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Here is a short simulation that I made to demonstrate a 2D PFB. I multiply a 96x96 grid (with a resolution of 1 deg, for example) with a 2D sinc filter. I then divide it into nine 32x32 grids (our allowed grid size) and accumulate them to perform FFT. This is essentially folding through the edges. The resulting PSF is compressed into a single pixel compared to the one generated using the 96x96 grid. But I'm a little confused about the resolution. Does the sky resolution remain the same between larger and smaller grid sizes? Or does the smaller grid have a 3x lower resolution than the full grid. Also, how do we ensure we conserve the flux after we down-weight the outlying antennas? |
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I've been thinking about how to fold in long baselines for better resolution (and not to waste information), especially for when we add a node to OVRO-LWA. We don't have the resources in the GPU to expand our image/aperture grids, but we could borrow a technique from software implementations of polyphase filter banks (PFBs). In 1D, PFBs apply a sync window function to a long array of data and then cut apart the long array into shorter segments, co-add/stack the segments, and FFT the short-length array. This improves the PSF compared to doing FFTs on individual unweighted short segments of data (at the expense of less sensitivity since some of the data is down weighted by the sync window function--that loss of sensitivity can be regained by sliding the PFB along the original array, although that won't apply here). I think we could do that spatially (in 2D) with our aperture planes, essentially weight and fold outlier antennas back into the central part of the aperture before we FFT. We can't do better than our maximum grid dimension for imaging resolution, but we can shrink the PSF closer to the size of a pixel in the image domain and reduce sidelobes. A simple test in simulation would be a good start and possible a nice quick paper.
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