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Jan 21, 2021 at 15:42 comment added Christian Remling Yes, actually an issue with the extension is that we must preserve $\Delta u=0$ (again, secretly we know that odd extension will work).
Jan 21, 2021 at 15:33 comment added Math604 Regarding your prior comment. I agree that making sense of (star) is a problem. Suppose we had limited $ \gamma$ to smooth compactly supported (instead of the slighty larger class) can we not view (star) as some distributional pairing (not claiming I can do anything with it)
Jan 21, 2021 at 15:31 comment added Math604 Is that the proper extension (or do we want the odd extension in $y$). In any case for the equation I have in mind it has some coefficients in $y$ and so it might be quite complicated to do a Fourier transform in $y$ also. So, if possible, I really preferred to keep it to a transform just in $x$
Jan 21, 2021 at 15:26 comment added Christian Remling Why don't you just take the FT in both variables (declaring $u=0$ for $y<0$) to conclude that $\widehat{u}$ is supported by $\{0\}$, so $u$ is a linear combination of derivatives of $\delta$, but then only $\widehat{u} = C \partial_y \delta$ is consistent with the imposed bound + boundary condition.
Jan 21, 2021 at 15:21 comment added Christian Remling On second thoughts, I think we are up against similar issues: since we only know that $x\mapsto u(x,y)$ is bounded, $\widehat{u}(\xi,y)$ is not guaranteed to be a function (and in fact we secretly know that it isn't, $\widehat{u}=Cy\delta$), and then it's not clear what (*) means.
Jan 21, 2021 at 15:01 comment added Math604 Thanks for the comment. Recall that we imposed $ u(x,y)$ is bounded for each $y$ (sorry, i know its kinda buried in the post).
Jan 21, 2021 at 9:45 history asked Math604 CC BY-SA 4.0