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Could this be similar to the problem produced in optical astronomy with diffraction spikes? A cross hair feature seems to be prevalent in some of the optical images/fourier plane (though that may just be due to the cross hair on the instrument); my interpretation of the loop used to produce the above images is that as we are getting closer to the dirty image we are making the model's fourier plane closer to the visibilities in the data (which would be similar to adding more points of the aperture), which is why we get more lines on the edges- these would be comparable to the diffraction spikes in optical astronomy; some features I see in the LFA figure as I go through the iterations are apparent in this paper for processing diffraction dominated images, namely figures 6 and 12- though it may be coincidental because I think one of the images is in the image plane. The figures contain a pattern of blobs surrounding the central feature, similarly to what I'm seeing in LFA figures: |
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It's interesting that you are seeing this cross-hair response in the Fourier plane. The crosshair locations correspond to the u=0 and v=0 locations. Your comment about these corresponding to dominant features of the image is correct. What that means is that the image that corresponds to this LFA (nice acronym :) has more power at spatial frequencies (u=0, for all vs) and (all us, for v=0). I don't know if there are any good physical reasons to expect this behavior for a "natural" image, though. For analytic image/Fourier transform pairs, (e.g, a Gaussian ring and its FT), we wouldn't expect to see such features, so this makes me think it's an artifact of the optimization process. As an example of how this comes about for an "unnatural" image, check out the FFT of the mock ALMA logo here. The sharp features in the Fourier plane are from the strong features from the text and border outlines, many of which are preferentially in the x and y directions. As a thought experiment, what would an image look like that only had power at (u=0, for all vs) and (all us, for v=0)? There is definitely a connection between diffraction spikes and the Fourier plane. For example, search on the term Fourier Optics. I haven't yet wrapped my head around whether these specific features have a direct analogy to the diffraction spikes seen by optical telescopes, though, which are usually caused by occulting from support structures holding up the secondary mirrors. But at the end of the day, it all comes back to Fourier transforms so I'm sure any intuition gained there will be helpful in some respect. |
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During last Thursday's discussion, we saw lines surrounding the outer edges of the log of the Fourier Amplitude (LFA) figure in the process of running an optimization loop. This occurred before reaching convergence.
I'm now producing both the image plane figure and the LFA figure when running the loop to initialize the model with the dirty image. In the current version of the pull request for the HD143006 P2 tutorial, we go through 400 iterations during this process. Out of curiosity, I increased the number of iterations in the initialization of the model with the dirty image and am now producing the same lines that we saw in the optimization process (that included hyperparameters and a different loss function) even though the loss function is converged. Below includes: the model initialized with the dirty image in the image plane (at 950 iterations), the corresponding LFA (at 950 iterations), and the loss function vs iterations (note only every 50 iterations were logged).
Why are we seeing different results with different loss functions even though they are both converging? Is it due to what data each loss function prefers?
Another thing to note, no matter how many iterations I use during this process, starting from step 0 to step 950, there is a resemblance of a cross hair dividing the LFA into four quadrants. Is that a property of the data?
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