In this article we present a statistical version of the Candes-Tao restricted isometry property (SRIP for short) which holds in general for any incoherent dictionary which is a disjoint union of orthonormal bases. In addition, we show that, under appropriate normalization, the eigenvalues of the associated Gram matrix fluctuate around 1 according to the Wigner semicircle distribution. The result is then applied to various dictionaries that arise naturally in the setting of finite harmonic analysis, giving, in particular, a better understanding on a remark of Applebaum-Howard-Searle-Calderbank concerning RIP for the Heisenberg dictionary of chirp like functions.
Deep Dive into The statistical restricted isometry property and the Wigner semicircle distribution of incoherent dictionaries.
In this article we present a statistical version of the Candes-Tao restricted isometry property (SRIP for short) which holds in general for any incoherent dictionary which is a disjoint union of orthonormal bases. In addition, we show that, under appropriate normalization, the eigenvalues of the associated Gram matrix fluctuate around 1 according to the Wigner semicircle distribution. The result is then applied to various dictionaries that arise naturally in the setting of finite harmonic analysis, giving, in particular, a better understanding on a remark of Applebaum-Howard-Searle-Calderbank concerning RIP for the Heisenberg dictionary of chirp like functions.
Digital signals, or simply signals, can be thought of as complex valued functions on the finite field F p , where p is a prime number. The space of signals H = C (F p ) is a Hilbert space of dimension p, with the inner product given by the standard formula f, g = t∈Fp f (t) g (t).
A dictionary D is simply a set of vectors (also called atoms) in H. The number of vectors in D can exceed the dimension of the Hilbert space H, in fact, the most interesting situation is when |D| ≫ p = dim H. In this set-up we define a resolution of the Hilbert space H via D, which is the morphism of vector spaces
given by Θ (f ) = ϕ∈D f (ϕ) ϕ, for every f ∈ C (D). A more concrete way to think of the morphism Θ is as a p × |D| matrix with the columns being the atoms in D.
In the last two decades [11], and in particular in recent years [3,4,5,6,7,8], resolutions of Hilbert spaces became an important tool in signal processing, in particular in the emerging theories of sparsity and compressive sensing.
A useful property of a resolution is the restricted isometry property (RIP for short) defined by Candès-Tao in [7]. Fix a natural number n ∈ N and a pair of positive real numbers δ 1 , δ 2 ∈ R >0 . Definition 1.1. A dictionary D satisfies the restricted isometry property with coefficients (δ 1 , δ 2 , n) if for every subset S ⊂ D such that |S| ≤ n we have
for every function f ∈ C (D) which is supported on the set S.
Equivalently, RIP can be formulated in terms of the spectral radius of the corresponding Gram operator. Let G (S) denote the composition Θ * S • Θ S with Θ S denoting the restriction of Θ to the subspace C S (D) ⊂ C (D) of functions supported on the set S. The dictionary D satisfies (δ 1 , δ 2 , n)-RIP if for every subset S ⊂ D such that |S| ≤ n we have
where Id S is the identity operator on C S (D).
It is known [2,8] that the RIP holds for random dictionaries. However, one would like to address the following problem [1,10,9,20,21,22,23,25,24,26,27]: Problem 1.2. Find deterministic construction of a dictionary D with |D| ≫ p which satisfies RIP with coefficients in the critical regime
for some constant 0 < α < 1.
Fix a positive real number µ ∈ R >0 . The following notion was introduced in [9,12] and was used to study similar problems in [26,27]:
In this article we will explore a general relation between RIP and incoherence. Our motivation comes from three examples of incoherent dictionaries which arise naturally in the setting of finite harmonic analysis:
• The first example [18,19], referred to as the Heisenberg dictionary D H , is constructed using the Heisenberg representation of the finite Heisenberg group H (F p ). The Heisenberg dictionary is of size approximately p 2 and its coherence coefficient is µ = 1. • The second example [15,16,17], which is referred to as the oscillator dictionary D O , is constructed using the Weil representation of the finite symplectic group SL 2 (F p ). The oscillator dictionary is of size approximately p 3 and its coherence coefficient is µ = 4. • The third example [15,16,17], referred to as the extended oscillator dictionary D EO , is constructed using the Heisenberg-Weil representation [28,13] of the finite Jacobi group, i.e., the semi-direct product J (F p ) = SL 2 (F p ) ⋉ H (F p ). The extended oscillator dictionary is of size approximately p 5 and its coherence coefficient is µ = 4.
The three examples of dictionaries we just described constitute reasonable candidates for solving Problem 1.2: They are large in the sense that |D| ≫ p, and empirical evidences suggest (see [1] for the case of D H ) that they might satisfy RIP with coefficients in the critical regime (1.1). We summarize this as follows:
Question: Do the dictionaries D H , D O and D EO satisfy the RIP with coefficients δ 1 , δ 2 ≪ 1 and n = α • p, for some 0 < α < 1?
In this article we formulate a relaxed statistical version of RIP, called statistical isometry property (SRIP for short) which holds for any incoherent dictionary D which is, in addition, a disjoint union of orthonormal bases:
where
x is an orthonormal basis of H, for every x ∈ X.
The statistical isometry property. Let D be an incoherent dictionary of the form (3.1). Roughly, the statement is that for S ⊂ D, |S| = n with n = p 1-ε , for 0 < ε < 1, chosen uniformly at random, the operator norm G (S) -Id S is small with high probability. Precisely, we have Theorem 3.1 (SRIP property [14]). For every k ∈ N, there exists a constant C (k) such that the probability
above theorem, in particular, implies that probability P G (S) -Id S ≥ p -ε/2 → 0 as p → ∞ faster then p -l for any l ∈ N.
The statistics of the eigenvalues. A natural thing to know is how the eigenvalues of the Gram operator G (S) fluctuate around 1. In this regard, we study the spectral statistics of the normalized error term
Let ρ E(S) = n -1 n i=1 δ λ i denote the spectral distribution of E (S) where λ i , i = 1, .., n, are the real eigenvalues of the Hermitian operator E (S). Th
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