By Robert M. Young
The idea of nonharmonic Fourier sequence is worried with the completeness and enlargement houses of units of complicated exponential services. this article for graduate scholars and mathematicians offers an creation to a few of the classical and smooth theories inside of this vast box. younger (mathematics, Oberlin university) discusses such subject matters because the balance of bases in Banach areas, estimates for canonical items, and second sequences in Hilbert house.
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Extra info for An Introduction to Non-Harmonic Fourier Series, Revised Edition
28) ,(Ωf )(t) ≤ −1/σ ct f q , t ∈ (0, ∞). , Lσ -weak). 29). 14 Consider the initial value problem (IVP) associated to the wave equation: ⎧ 2 ⎪ ⎨∂t w − Δw = 0, w(x, 0) = f (x), ⎪ ⎩ ∂t w(x, 0) = g(x), x ∈ Rn , t ∈ R, prove that (i) If n = 1, then f (x + t) + f (x − t) 1 + w(x, t) = 2 2 x+t g(s) ds. 18(i) or the change of variables ζ = x + t, η = x − t. 5 Exercises 43 (ii) If n = 3, f = 0 and g is a radial function (g( x )), then 1 w(x, t) = w( x , t) = 2 x x +t ρg(ρ) dρ. | x −t| Hint: Deduce the formula for the Laplacian of radial functions, use the change of variables v(ρ, t) = ρ w(ρ, t) = x w( x , t) and part (i) of this exercise.
3 (Hausdorff–Young’s inequality). Let f ∈ Lp (Rn ), 1 ≤ p ≤ 2. 4) p. Proof. 11) it follows that the Fourier transform is of type (1, ∞) and (2, 2) with norm 1. 1 tells us that it is also of type (p, q) with 1 (1 − θ ) θ θ 1 θ 1 1 = + =1− and =0+ =1− = p 1 2 2 q 2 p p with norm M ≤ 1(1−θ ) 1θ = 1. ✷ This estimate is the best possible when p = 1 or 2. This is not the case for 1 < p < 2. Beckner [B] found the best constant for the Hausdorff–Young inequality. 2 p ≤ (Ap )n f p , where Ap = p1/p p 1/p 1/2 .
3) 45 46 3 An Introduction to Sobolev Spaces and Pseudo-Differential Operators Using polar coordinates, it is easy to see that h ∈ H s (Rn ) if s < n/2 + 1. Notice that in this case s depends on the dimension. 4 Let n ≥ 1 and f (x) = δ0 (x). 9, we have δ0 (ξ ) = 1. Thus, δ0 ∈ H s (Rn ) if s < −n/2. From the definition of Sobolev spaces, we deduce the following properties. 1. s 1. If s < s , then H s (Rn )⊆H (Rn ). / s n 2. H (R ) is a Hilbert space with respect to the inner product follows: If f, g ∈ H s (Rn ), then f, g s = ·, · s defined as Λs f (ξ ) Λs g(ξ ) dξ.