2020
DOI: 10.1137/19m1256865
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Phase Retrieval: Uniqueness and Stability

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Cited by 75 publications
(54 citation statements)
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“…we have either g = f or g = − f , thus the only ambiguity is the (global) sign of f . Our proof yields a reconstruction procedure (see Section 2), but it is well-known that the phase-retrieval problem in infinite dimensions is necessarily ill-posed [4,6,13].…”
Section: Theorem 1 Says That For Realmentioning
confidence: 99%
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“…we have either g = f or g = − f , thus the only ambiguity is the (global) sign of f . Our proof yields a reconstruction procedure (see Section 2), but it is well-known that the phase-retrieval problem in infinite dimensions is necessarily ill-posed [4,6,13].…”
Section: Theorem 1 Says That For Realmentioning
confidence: 99%
“…Particular problems concern the recovery of a function f from its phaseless Fourier measurements |f (ξ )| or the recovery of a function f from its phaseless (or unsigned) samples | f (λ)|. For general information about the phase-retrieval problem we refer to the surveys [13,18].…”
mentioning
confidence: 99%
“…Furthermore, if F and G are rational functions, then they have same zeros and poles in C \ {0}, thus there exists c ∈ T and m ∈ Z such that G = cz m F . But then (7) implies that -on one hand |F (ρe it )| = |c|ρ m |F (ρe it )| for all t thus |c|ρ m = 1.…”
Section: Proof Of Theorem 21mentioning
confidence: 98%
“…Then F and G have the same zeros and poles in C \ {0}, with the same multiplicities. In particular, if F and G are rational functions that satisfy (7), then G = cF outside the poles with c ∈ T.…”
Section: Proof Of Theorem 21mentioning
confidence: 99%
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