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Nov 16, 2017 at 15:10 comment added Willie Wong why do you think the expression you wrote decay to 0 "infinite times when $t\to \infty$"? (In fact, by the Fourier inversion formula + Riemann-Lebesgue, if you have an integrable function whose Fourier transform decays "infinite times when $t\to\infty$", then the original function must be $C^\infty$.)
Nov 16, 2017 at 15:03 history edited Willie Wong
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Nov 16, 2017 at 12:11 comment added CC95 Thank you for your comments. Suppose $g(x) = |x|^p, x \in [-1,1]$ and is smooth and compactly supported otherwise. Since $\int_{-1}^{1}|x|^p cos(tx)dx =2*( \frac{sin(t)}{t} - \frac{\int_{0}^{t}px^{p-1}sin(x)dx}{t^{p+1}})$ and it will decay to $0$ infinite times when $t \rightarrow \infty$, the tail is still not as slow as $O(x^{-\beta})$. So it confuses me wether we can find a $\phi_{f}(x)$ that has a polynomial tail.
Nov 15, 2017 at 20:47 comment added Willie Wong The condition $|f'| < \epsilon |f|$ is not that restrictive. Let $g$ be any compactly supported $C^1$ function. Then for $\delta$ sufficiently small the function $$ f = \exp (- \frac12 \epsilon \sqrt{1 + x^2}) + \delta g(x) $$ would satisfy your constraint. The part of the Fourier transform coming from the $\exp$ would decay exponentially fast. You just need to make $g$ very poorly differentiable at some points (say something like $|x-a|^p$ where $p > 1$ is very close to 1) to guarantee a slow decay of the Fourier transform.
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