Density and duality theorems for regular Gabor frames

By Mads Sielemann Jakobsen, Jakob Lemvig

http://www.sciencedirect.com/science/article/pii/S0022123615004152

We examine Gabor frames on in the community compact abelian teams with time–frequency shifts alongside non-separable, closed subgroups of the section house. Density theorems in Gabor research kingdom valuable stipulations for a Gabor approach to be a body or a Riesz foundation, formulated merely when it comes to the index subgroup. within the classical effects the subgroup is thought to be discrete. We end up density theorems for basic closed subgroups of the section house, the place the mandatory stipulations are given when it comes to the “size” of the subgroup. From those density effects we can expand the classical Wexler–Raz biorthogonal relatives and the duality precept in Gabor research to Gabor structures with time–frequency shifts alongside non-separable, closed subgroups of the part area. Even within the euclidean surroundings, our effects are new.

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Lemvig / magazine of practical research 270 (2016) 229–263 now have okay = N on account that okay is atomless. we will write ok = ∪i∈I Ki , the place Ki is of finite degree. Then, through a classical results of Sierpinski [37, Lemma fifty two. α], the degree μM takes a continuum of values [0, μM (Ki )] at the measurable subsets of Ki , which justifies the identify non-stop body. If F = {fk }k∈M is a easy body with bounds A and B and if CF has dense diversity, then CF |K is invertible on all of L2 (M, μM ), and we are saying that {fk }k∈M is a simple Riesz relations with bounds A and B. Equivalently, you may define simple Riesz households with bounds A and B as households of vectors F = {fk }k∈M for which DF defined on easy, integrable √ √ features is bounded lower than and above through A and B, respectively, i. e. , 2 A a 2 L2 (M ) ≤ a(k)fk dμM (k) ≤B a 2 L2 (M ) M for all easy features a on M with finite help. If M is countable and outfitted with the counting degree, a easy Riesz kinfolk is just a Riesz foundation for its closed linear span, also known as a Riesz series. Our inspiration of discrete frames may well look overly technical in comparison to the standard definition (i. e. , M countable and μM the counting measure). although, it permits us to categorise the next pathological “continuous” examples as discrete frames. instance 1. give some thought to the subsequent examples with a “continuous” index set M = R: (a) permit H = 2 (Z), allow {ek }k∈Z be its commonplace orthonormal foundation, and equip M = R with a only atomic degree, whose atoms are the periods [n, n + 1), n ∈ Z, every one with degree 1. Define {fk }k∈M ⊂ H by means of fk = e okay , ok ∈ R. (b) enable H = L2 ([0, 1]), and permit M = R. repair a ∈ R and define μM = n∈Z δn+a , the place δx denotes the Dirac degree at x ∈ R. Define {fk }k∈M ⊂ H via fk (x) = e2πikx . it isn't difficult to teach that either in case (a) and (b) the relatives {fk }k∈M is a Parseval body; it's even a Riesz kinfolk. because the degree in either instances is only atomic, the body {fk }k∈M is related to be discrete. There has lately been a few curiosity within the research of (continuous) Riesz households [2,36], also known as Riesz-type frames in [18]. instance 1 (b) is a concrete model of [2, Proposition three. 7]. the next outcome exhibits, despite the fact that, that this idea brings little new to the well-studied topic of (discrete) Riesz sequences. To be extra concise, Proposition three. three indicates that norm bounded, easy Riesz households inevitably are discrete. M. S. Jakobsen, J. Lemvig / magazine of useful research 270 (2016) 229–263 239 Proposition three. three. allow (M, Σ, μM ) be a degree area. consider that {fk }k∈M is a simple Riesz family members in H that's basically norm bounded, i. e. , C := supk∈M fk < ∞. Then {fk }k∈M is a discrete family members. in addition, it holds that the place Σ0 = {E ∈ Σ : μM (E) > zero} . inf μM (E) > zero, E∈Σ0 (3. four) evidence. allow a be an integrable uncomplicated functionality on M . From the computation a(k)fk dm(k) ≤ M |a(k)| fk dm(k) ≤ C M |a(k)| dm(k), M we see that the reduce Riesz certain implies √ A a L2 (M ) ≤C a L1 (M ) . For a = 1E with E ∈ Σ and nil < μM (E) < ∞, this in flip means that √ A μM (E) 0.5 ≤ CμM (E), and therefore μM (E) ≥ A/C 2 .

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