Fourier phase (unwrapping problem)

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    Fourier Phase
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SUMMARY

The discussion centers on the Fourier phase unwrapping problem, specifically addressing the continuity of the phase function derived from the Fourier transform of an integrable function f(x). The phase function, defined as \mathrm{Ph}_f (\omega) = \mathrm{arg}(\mathcal{F}\{f\}(\omega)), experiences discontinuities due to the wrapping effect from -π to π. The participants seek to understand the conditions or theorems that ensure the phase remains continuous, referencing Steven W. Smith's "Scientist and Engineer's Guide to Digital Signal Processing" for further insights.

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  • Understanding of Fourier transforms and their properties
  • Familiarity with complex analysis, particularly the argument function
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  • Basic mathematical concepts related to integrable functions
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mnb96
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Hello,
given an integrable function f(x), and its Fourier transform

[tex]\mathcal{F}\{f\}(\omega)=\int_{\mathbb{R}}f(x)e^{-i\omega x}dx[/tex],

we consider the phase [tex]\mathrm{Ph}_f : \mathbb{R}\rightarrow [-\pi,\pi)[/tex] which is given by:

[tex]\mathrm{Ph}_f (\omega) = \mathrm{arg}(\mathcal{F}\{f\}(\omega))[/tex]

In general the phase function will have discontinuities (when it wraps from [itex]-\pi[/itex] to [itex]\pi[/itex], and there are algorithms that attempts to recover a continuous phase function.
My question is: why should the phase be a continuous function? What is the condition/theorem that guarantees that the phase is always continuous?
 
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I am afraid that chapter doesn't answer my question which was:

"...Is there a condition on f (or a theorem) that guarantees that the phase is certainly continuous? ..."
 

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