Oberwolfach Preprints

Size: px
Start display at page:

Download "Oberwolfach Preprints"

Transcription

1 Oberwolfach Preprints OWP ALEXANDER OLEVSKII AND ALEXANDER ULANOVSKII Interpolation in Bernstein and Paley-Wiener Spaces Mathematisches Forschungsinstitut Oberwolfach ggmbh Oberwolfach Preprints (OWP) ISSN

2 Oberwolfach Preprints (OWP) Starting in 007, the MFO publishes a preprint series which mainly contains research results related to a longer stay in Oberwolfach. In particular, this concerns the Research in Pairs- Programme (RiP) and the Oberwolfach-Leibniz-Fellows (OWLF), but this can also include an Oberwolfach Lecture, for example. A preprint can have a size from - 00 pages, and the MFO will publish it on its website as well as by hard copy. Every RiP group or Oberwolfach-Leibniz-Fellow may receive on request 30 free hard copies (DIN A4, black and white copy) by surface mail. Of course, the full copy right is left to the authors. The MFO only needs the right to publish it on its website as a documentation of the research work done at the MFO, which you are accepting by sending us your file. In case of interest, please send a pdf file of your preprint by to rip@mfo.de or owlf@mfo.de, respectively. The file should be sent to the MFO within months after your stay as RiP or OWLF at the MFO. There are no requirements for the format of the preprint, except that the introduction should contain a short appreciation and that the paper size (respectively format) should be DIN A4, "letter" or "article". On the front page of the hard copies, which contains the logo of the MFO, title and authors, we shall add a running number (0XX - XX). We cordially invite the researchers within the RiP or OWLF programme to make use of this offer and would like to thank you in advance for your cooperation. Imprint: Mathematisches Forschungsinstitut Oberwolfach ggmbh (MFO) Schwarzwaldstrasse Oberwolfach-Walke Germany Tel Fax admin@mfo.de URL The Oberwolfach Preprints (OWP, ISSN ) are published by the MFO. Copyright of the content is hold by the authors.

3 Interpolation in Bernstein and Paley Wiener spaces Alexander Olevskii and Alexander Ulanovskii A.O.: School of Mathematics, Tel Aviv University Ramat Aviv, Israel A.U.: Stavanger University, 4036 Stavanger, Norway Abstract We construct closed sets S of arbitrarily small measure with the property: given any discrete set Λ, every l function on Λ can be interpolated by an L function with spectrum on S. This should be contrasted against Beurling Landau type theorems for compact spectra. Introduction. Spaces. Let S be a closed set in R. We say that a function f defined on (another copy of) R belongs to Bernstein space B S if (i) f L (R); (ii) f is the Fourier transform of a Schwartz distribution F (notation: f = ˆF ), supported by S. The support of F is called the spectrum of f. In other words, a function f belongs to B S if and only if it is bounded and we have f(x) ˆϕ(x) dx = 0, R for every smooth function ϕ(x) whose support is compact and disjoint from S. Endowed with the L norm, B S is a Banach space.

4 We shall also consider the Paley Wiener spaces P W S := {f L (R); f = ˆF, F = 0 on R \ S}, where the spectrum S can be any measurable set. Classical Paley Wiener (Bernstein) spaces are defined when S is a bounded (compact) set. The elements of these spaces are entire functions of finite exponential type. We shall focus on the situation when S is an unbounded closed set, and so the elements of the corresponding spaces do not necessarily admit analytic continuation into the complex plain.. Interpolation. Let Λ = {λ j, j Z} R be a uniformly discrete (u.d.) set, that is inf j k λ j λ k > 0. Given a bounded data c = {c j, j Z}, one wishes to find a function f B S such that f(λ j ) = c j, j Z. () If this is possible for every c l (Z), one says that the interpolation problem is solvable, and Λ is called an interpolation set for B S. Similarly, if for arbitrary data c l (Z) there is a function f P W S satisfying (), one says that Λ is a set of interpolation for P W S. General principles of functional analysis imply that if Λ is a interpolation set for B S, then one can solve interpolation problem () with an additional estimate: f L C c l, () where the constant C does not depend on data c. A similar result is true for the Paley Wiener spaces (see [], p. 9). 3. Density. For every u.d. set Λ one can define its upper uniform density D + #(Λ (a, a + l)) (Λ) := lim max. l a R l A fundamental role of this quantity in the interpolation problem, in the case when S is a single interval, was found by A. Beurling and J-P. Kahane: Beurling proved ([]) that Λ is an interpolation set for B S if and only if D + (Λ) < mes S. π

5 Even earlier, Kahane proved in [5] that for Λ to be an interpolation set for P W S it is necessary that and it is sufficient that D + (Λ) π D + (Λ) < π mes S, (3) mes S. Both results are based on the theory of entire functions. 4. Disconnected spectra. The situation becomes much more delicate for disconnected spectra, in particular when S is a union of two intervals. For the sufficiency part, not only the size but also the arithmetics of Λ is important in that case. On the other hand, using a new approach Landau [6] succeeded to extend the necessity part to the general case: Theorem. [6] Let S be a bounded set. If a u.d. set Λ is an interpolation set for P W S then condition (3) is fulfilled. We shall prove some versions of this result for both Paley Wiener and Bernstein spaces. In fact, it already suffices to know that the delta-functions on Λ admit interpolation by B S or P W S functions (with not very fast growing norms) in order to obtain an estimate from below for the measure of S (see section below). However, for unbounded spectra the situation is completely different. The contrast is most striking for Bernstein spaces: Not only condition (3) is no longer necessary, but there exist universal spectra of arbitrary small measure which deliver positive solution to the interpolation problem for every u.d. Λ: Theorem. For every δ > 0 there is a closed (unbounded) set S, mes S < δ, such that every u.d. set Λ is an interpolation set for the space B S. This theorem will be proved in sec. 3. Such a result cannot hold for Paley Wiener spaces (see Propositions 4. and 4. in sec. 4). However, we show that for a generic Λ there are arbitrarily small spectra S such that Λ is almost a set of interpolation for P W S (Theorem 4.). Results of this paper concerning Paley Wiener spaces were announced in our note [8]. 3

6 Acknowledgment. Part of the present work was done at the Mathematisches Forschungsinstitut Oberwolfach during a stay within the Research in Pairs Programme from April to April 5, 007. The authors appreciate the hospitality of the institute. Compact spectra: Weak interpolation The aim of this section is to show that even a much weaker interpolation property of Λ ensures Beurling Landau type estimates on the measure of S. In what follows we shall denote by f and f the L and L norm of f, respectively... Concentration. Definition: Given a number c, 0 < c <, we say that a linear subspace W of P W S is c-concentrated on a set Q if f(x) dx c f, f W. Q Following Landau we estimate the dimension of a concentrated subspace. Lemma. Given sets S, Q R and a number 0 < c <, let W be a linear subspace of P W S which is c-concentrated on Q. Then dim W (mes Q) (mes S). πc Proof ([6], see (iii) and (iv) on p. 4). Let Q, S R be two sets of finite positive measure. Let A Q and B S denote the orthogonal projections of L (R) onto L (Q) and P W S, respectively: A Q f = Q f, B S f = F S F f, where Q denotes the characteristic function of Q, and Ff is the Fourier transform of f: Ff(x) = ˆf(x) := e itx f(t) dt. π R 4

7 The operator C := A Q B S A Q acts from L (R) into itself. Clearly, C is self-adjoint and positive. It can be written explicitly as Cf(y) = Q (x) Q (y)ˆ S (y x)f(x) dx. π R Since the kernel is square-integrable, C is a compact operator. Denote by l j its eigenvalues arranged in non-increasing order (counting multiplicities). The trace Tr C is equal to the integral of kernel along the diagonal : Tr C := j l j = (mes Q) (mes S). (4) π. One can easily show that the spectrum of operator D := B S A Q B S is identical to the spectrum of operator C. Let W be a linear subspace of P W S of dimension k. The quadratic form (Df, f) on W is given by (A Q f, f) = Q f. If W is c concentrated on Q, then inf (Df, f) c. f W, f = It is well-known that, among all subspaces of dimension k, the greatest value of inf(df, f) on the unit sphere is achieved on a subspace spanned by the first k eigenvectors of D. This means that c l k Tr D/k=Tr C/k. This and (4) prove the lemma. One can show that a similar result holds in several dimensions, too. Remark. The uncertainty principle in Fourier analysis is a statement that a function and its Fourier transform cannot both be concentrated on small sets. A simple corollary of Lemma. is the following variant of uncertainty principle due to Amrein and Berthier []: Let S and Q be any sets of finite measure. There exists C = C(S, Q) such that ( ) f(x) dx C f(x) dx + f(t) dt, f L (R). R R\S.. Interpolation of delta functions. We start with the following R\Q 5

8 Theorem. Let S be a compact set and Λ = {λ j, j Z} be a u.d. set. Suppose that for every j Z there is a function f j P W S such that {, k = j f j (λ k ) =, k Z; (5) 0, k j Then (3) holds. sup f j <. (6) j Z Proof.. Recall that if S is a compact set, then the corresponding Paley Wiener space consists of entire functions of exponential type. The following lemma is well known (see [], p. 8): Lemma. Suppose Λ = {λ j, j Z} is a u. d. set, and S R is a compact set. Then there exists C > 0 such that f C j Z f(λ j ), for every f P W S.. Fix a number δ > 0, and set S(δ) := S + [ δ, δ]. (7) Take functions f j P W S satisfying (5) and (6), and set ( ) sin δ(x λj ) g j (x) := f j (x), j Z. δ(x λ j ) Clearly, functions g j satisfy (5), (6) and belong to P W S(δ). 3. Fix any number R, and denote by #(Λ (R r, R + r)) the number of λ j Λ in the interval (R r, R + r). Since Λ is u.d. we have: # (Λ (R r, R + r)) Cr, for all r >, (8) where C > 0 is a constant which does not depend on R. Let us introduce a linear space of functions W r := g(x) = c k g k (x), c k C. k: λ k R <r Clearly, dim W r = #(Λ (R r, R + r)). 6

9 4. We would like to estimate the concentration of W r on the interval (R r rδ, R + r + rδ). Choose any function g = j c jg j W r. Then g(λ j ) = c j when λ j R < r, and g(λ j ) = 0 when λ j R r. By Lemma., there is a constant C = C(S, Λ) > 0 such that g C g(λ j ) = C c j. (9) λ j Λ λ j R <r On the other hand, by Parseval s identity and (6), we have ( ) f j (x) ˆf j (t) dt mes S π π ˆf j C, j Z, S for some C > 0. Observe that x λ j δr whenever λ j (R r, R + r) and x R r + δr. Hence, the last inequality and (8) give g(x) dx = Cr x R r+δr λ j R <r c j x R r+δr λ j R <r x >δr ( ) sin δ(x λj ) c j f j (x) dx δ(x λ j ) ( ) 4 dx C c δx δ 7 r j. λ j R <r This and (9) show that for every ɛ > 0 there exists r ɛ such that g is ( ɛ) concentrated on (R r δr, R + r + δr) for all r r ɛ. 4. It now follows from Lemma., that # (Λ (R r, R + r)) (mes S(δ))(mes (R r δr, R + r + δr)), π( ɛ) whenever r r ɛ. Since this is true for every R, we obtain: D + (Λ) + δ ɛ mes S(δ). π Letting δ 0 and ɛ 0, we conclude that D + (Λ) (π) mes S. Remark. The assumptions of Theorem. admit a geometric interpretation: Set E(Λ) := {e iλt, λ Λ}. 7

10 Conditions (5) and (6) are equivalent to the property that the exponential system E(Λ) is uniformly minimal in L (S), that is the L distance from any element of the system to the span of other elements is greater then some positive constant. Observe that assumptions (5) and (6) are less restrictive then the requirement for Λ to be an interpolation set for P W S. Indeed, consider a classical example: S = [ π, π] and Λ = {λ j, j Z}, λ j := j +, j =,, , j = 0 j, 4 j =,,... The corresponding exponential system E(Λ) is uniformly minimal in L ( π, π) (see [7], Theorem 5). However, Λ is not an interpolation set for L ( π, π) (see the remark following Theorem 5 in [7]). An analog of Theorem. for Bernstein spaces is also true: Theorem. Let S be a compact set, and Λ = {λ j } a u.d. set. Suppose that for every j Z there is a function f j B S satisfying (5) and sup f j <. (0) j Z Then (3) holds. Indeed, suppose functions f j B S satisfy assumptions of Theorem.. Take any positive number δ, and set g j (x) := f j (x) sin δ(x λ j). δ(x λ j ) Then the functions g j belong to P W S(δ), j Z, where S(δ) is defined in (7), and satisfy assumptions of Theorem.. Hence, D + (Λ) (π) mes S(δ). Letting δ 0, we obtain Theorem.. An immediate corollary of Theorem. is a variant of Landau s Theorem. for Bernstein spaces: Corollary Let S be a compact set. If a u.d. set Λ is an interpolation set for B S, then condition (3) is fulfilled..3. Growth of f j and upper density. An estimate similar to (3) holds even if the norms of functions satisfying (5) grow, but not very fast: f j Ce λ j α, j Z, () 8

11 where C > 0 and 0 < α <. We shall show that this and (5) imply estimate (3) in which D + is replaced by the upper density D. Definition: Let Λ be a u.d. set. The upper density of Λ is defined as follows: D #(Λ ( a, a)) (Λ) := lim sup. a a Clearly, we have D (Λ) D + (Λ). Observe that for regularly distributed Λ, for example if Λ = {j +O(), j Z}, these two densities are equal. Theorem.3 Let S R be a compact set, and Λ = {λ j, j Z} a u.d. set. Suppose there exist functions f j P W S, j Z, satisfying (5) and () with some C > 0 and 0 < α <. Then D (Λ) (π) mes S. Proof.. We shall need Lemma.3 Set ϕ(z) := sin(k β z), k β z k k 0 where k 0 N and 0 < β < are some numbers. Then ϕ P W [ σ,σ], where σ = k k 0 k β, and ( ϕ(x + iy) C exp ) C x +β, x R, y, () where C is a constant. Proof. For every a > 0, the function sin az/az is the Fourier transform of a positive constant function on [ a, a]. Hence, ϕ(z) is the Fourier transform of the convolution of such functions. This convolution is concentrated on [ σ, σ], σ = k k 0 k γ, and so ϕ P W [ σ,σ]. Let us denote by δ and δ positive constants such that e δ z sin z z e y δ δ x, z = x + iy C, z. (3) Since sin(a + ib) exp b, for a, b real, we have: sin(k β z) k β z sin(k β z) k 0 k< z +β k 0 k< z +β 9

12 exp y k +β k 0 k< z +β e C y, z = x + iy, where C is a constant. Now, using the right-hand inequality in (3), we get for every z C, z + k +β 0, that sin(k γ z) k β z C exp δ x k +β k z +β k z +β ( C exp ) C x +β, y, where C is a constant. This and the previous inequality give ().. Fix a small number δ > 0 and pick up k 0 in Lemma.3 so large that σ δ, i.e. the function ϕ P W [ δ,δ]. Also, assume that β < satisfies α < /( + β). The rest of the proof is pretty similar to the proof of Theorem.. Without loss of generality, we may assume that λ 0 = 0. Take functions f j P W S satisfying (5) and (), and set g j (x) := f j (x)ϕ(x λ j ), j Z, where ϕ is a function from Lemma.3. It is clear that g j P W S(δ), where S(δ) is defined in (7), and that (5) is true for every j Z. 3. Since Λ is u.d., we have # (Λ ( r, r)) Cr, (4) for some C > 0 and all r >. Set W r := g(x) = c k g k (x) : c k C. λ k <r Clearly, dim W r = #(Λ ( r, r)). 4. Let us estimate the concentration of W r on the interval ( r rδ, r + rδ). Take any function g W r. Since g(λ j ) = 0 when λ j r, by Lemma., we have: g C c j. (5) λ j <r 0

13 Further, by () and Parseval s identity, we have ( ) f j (x) ˆf j (t) dt mes S π π ˆf j Ce rα, S for some C > 0 and all j, λ j < r. Observe also that x λ j δr whenever λ j < r and x r+δr. This, (4) and the last inequality give g(x) dx = c j f j (x)ϕ(x λ j ) dx x r+δr x r+δr Cre rα c j λ j <r λ j <r x >δr ϕ(x) dx. Recall that α < /( + β), so that () gives: re rα ϕ(x) dx 0, r. x >δr Hence, by (5), we see that for every ɛ > 0 there exists r ɛ such that g is ( ɛ) concentrated on ( r δr, r + δr) for all r r ɛ. 4. It now follows from Lemma., that # (Λ ( r, r)) This gives: D (Λ) = lim sup r (mes S(δ))(mes ( r δr, r + δr)), r r ɛ. π( ɛ) # (Λ ( r, r)) r + δ mes S(δ). π( ɛ) Letting δ 0 and ɛ 0, we conclude that D (Λ) (π) mes S. By using the same argument which deduces Theorem. from Theorem., one can easily extend Theorem.3 to Bernstein spaces: Theorem.4 Let S R be a compact set, and Λ = {λ j, j Z} a u.d. set. Suppose that there exist functions f j B S, j Z, satisfying (5) and f j Ce λ j α, j Z, (6)

14 for some C > 0 and 0 < α <. Then D (Λ) (π) mes S. Remark. The growth restrictions () and (6) can be replaced by any non quasi-analytic growth. However, we do not know if they can be omitted at all..4. A counterexample. The results of last subsection are not true for the density D +. We shall show this only for the Paley Wiener case. Theorem.5 For every ρ > there exist a u.d. set Λ, D + (Λ) ρ, and functions f j P W [ π,π], j Z, which satisfy (5) and () with some C > 0, 0 < α <. Proof.. Fix any numbers k 0 N and 0 < β <, and let ϕ be the function in Lemma.3. Let us show that for every r 0 we have ( ϕ(x + ri) C exp ) C x +β log( + x ), x R, (7) where C > 0 depends only on r. For simplicity, we shall assume that r =. From the left-hand inequality of (3), we obtain: k x+i +β sin(k β (x + i)) k β (x + i) exp δ x + i ) exp ( C x + i +β, where C is a constant. Further, since we have k 0 k< x+i +β sin(a + ib) eb e b k 0 k< x+i +β b, a R, b > 0, sin(k β (x + i)) k β (x + i) exp ( k +β ) exp ( k +β ) x + i k β This and the previous estimate prove (7). k +β k x+i +β ( ) x+i /(+β). x + i

15 . Set k=0 ψ(z) := η(z)η( z), η(z) := k=0 j j= k=0 ( z ). 4 j + k Observe that j z ( ) j 4 j + k exp ( ) z j z exp < e j j, 4 j + k 4 j whenever j > z. This gives: η(z) e j j ( + z ) j log z C ( + z ) log Ce C log (+ z ), j > z j z from which is follows that ψ(z) Ce C log (+ z ), (8) where C is a constant. We also need to estimate from below the derivative ψ at the zero points ±(4 j + k) of ψ. Pick up numbers J N and K, 0 K < J. We have 0 k<j,k K Further, since 4J + K 4 J + k = 0 k<j,k K ( ) J K k 4 J + k e CJ. 4 J + J 4 J 4 j + k, j < J, 4 J + j, j > J, 0 k < j, 4 j we get: j 4J + K 4 j + k ( ) j 4J + J C. 4 j j>j j,j J k=0 This and the previous estimate show that η (4 J + K) Ce CJ, J N, 0 K < J, where C is a constant. Since η( x) for x 0, the same estimate holds for ψ (4 J + K). Since ψ is even, we obtain: ψ (λ) Ce C log λ, for all λ, ψ(λ) = 0. 3

16 Now, choose a number ρ > and set f(z) := ψ(ρz)ϕ( π (z + i)), σ where ϕ is a function from Lemma.3, and σ is its type. The last inequality and and (7) imply: f (λ) Ce C λ +β log(+ λ ), for all λ, ψ(ρλ) = 0. (9) Moreover, from (8) and (), we see the type of f is equal to π and that f L (R). Hence, f P W [ π,π], by the Paley Wiener theorem. Let Λ be the zero set of ψ(ρx) : Λ := Γ ( Γ), Γ := j= { 4j ρ,..., 4j + j }. ρ It is clear that D + (Λ) = ρ. Set λ 0 = 4, and numerate the elements of Λ = {λ j, j Z} in increasing order. Set f j (z) := f(z) f (λ j )(z λ j ), j Z. Then functions f j P W [ π,π] and satisfy (5). We have: f j f λj + f (λ j ) + f(x) f (λ j )(x λ j ) λ j dx. Using the Cauchy integral formula, one can estimate from above the integral in the right hand-side by ( f (λ j ) sup f(z) ). z λ j = We conclude that f j C f (λ j ), where C depends only on f. Now, by (9), we see that assumption () is also fulfilled for each α < satisfying α > /( + β). 4

17 3 Unbounded spectra: interpolation in Bernstein spaces The goal of this section is to construct universal interpolation spectra S of arbitrarily small measure: Theorem 3. For every δ > 0 there is a closed (unbounded) set S, mes S < δ, such that every set Λ which has no finite limit points is an interpolation set for the space B S. This result is a refinement of Theorem. in which we relax assumption of uniform discreteness of Λ. 3.. Lemmas. Lemmas 3. For every N there exists a set S(N) ( N, N), mes S(N) =, such that N N e itx sin Nx dt Nx C, x R, (0) N S(N) where C > 0 is an absolute constant independent on N. Proof.. Fix an integer N, and let M j, j =,..., N, be any even numbers satisfying Set M N 4, M j+ N M j, j =,..., N. () Ω(j, k) := j + k M j + M j (, ], Ω( j, k) := Ω(j, k), S(j, k) := j + k M j + N M j (, ], S( j, k) := S(j, k), where j =,..., N and k =,..., M j /. Set One can check that M j / k= S(N) := N j = M j / k= S(j, k). Ω(j, k) = (j, j], j =,..., N, 5

18 and that mes S(N) = N.. For simplicity, throughout the proof we denote by C different positive constants. Since sin Nx Nx = N e itx dt, N N to prove (0) it suffices to show that N e itx dt N e itx dt < C, x R. () N S(N) 3. Assume first that x M l, for some l N. Using (), we have for j l, j N, that e itx dt N e itx dt = sin(x/m j ) x This and () give: Ω(j,k) N sin(x/n M j ) x {l t N} e itx dt N N j =l M j / k= S(j,k) Cx M 3 j CM l M 3 j {l t N} S(N) CM l M 3 j Clearly, this proves () for x M., k =,..., M j. e itx dt C. (3) 4. Assume now that x > M l, for some l N. Then, clearly, we have e itx dt = sin(l )x x. (4) M l Also, { t l } N {l t l } S(N) 6 e itx dt

19 N mes ({l t l } S) =. (5) These estimates and (3) prove () for M < x M. Assume that x > M l, for some l 3. Since N e itx dt = N sin x/(n M j ) x N, x > M l, M l S(j,k) by (), we obtain: N { t l } S(N) l e itx dt From this, (4) and (5) we get e itx dt N { t l } j= { t l } S M j / k= N M l N M l M l C. e itx dt C, x > M l, l 3. Now, this and (3) imply () for x > M l, l 3, which completes the proof of Lemma 3.. Lemma 3. For every ɛ > 0 there is a compact S = S ɛ and a function g = g ɛ B S such that: (i) mes S ɛ; (ii) g = g(0) = ; (iii) g(x) < ɛ for x > ɛ. In addition, S can be chosen disjoint from any given segment. This follows from Lemma 3.. Indeed, fix an ɛ > 0, and choose N in Lemma 3. so large that mes S(N) < ɛ, sin Nx/Nx < ɛ/ when x > ɛ and C/N < ɛ/, where C is the constant in (0). Given a segment I, set S := R + S(N), where R is any number such that R + S(N) I =. Set g(x) := N e itx dt = N eirx e itx dt. S S(N) Conditions (ii) and (iii) follow immediately from Lemma Proof of Theorem 3.. Suppose 0 < δ <, and take any sequence ɛ(j) > 0, j Z, such that ɛ(j) < δ. (6) j Z 7

20 Fix a sequence of disjoint compacts S ɛ(j), mes S ɛ(j) < ɛ(j), tending to infinity and satisfying the conditions of Lemma 3., such that the set S := j Z S ɛ(j). is closed. Let Λ = {λ j, j Z} be a set without finite limit points. Taking if necessary a subsequence of ɛ(j), we may assume that d j := inf k:k j λ k λ j > ɛ(j), j Z. (7) Conditions (ii) and (iii) of Lemma 3. allow one to define a sequence of functions f j B S such that each function f j has a compact support, = f j = f j (l j ), and By (7), we see that f j (x) < ɛ(j), for x l j d j. (8) f j (λ k ) < ɛ(j), j k. (9) Consider a linear operator A : l l defined as { fj (λ A := (a(j, k)) j,k Z, a(j, k) = k ), j k f j (λ j ), j = k From (6) and (9) one can see that A = sup k a(j, k) = sup k f j (λ k ) <, j so that the operator A + I, I is the identity operator, is invertible in l. Take an arbitrary data c = {c j } l, and denote by b = {b j } l the solution of the equation (A + I)b = c. j k Set f(x) := j Z b j f j (x). 8

21 By (6), (7) and (8), we see that the series converges uniformly on every finite interval, and sup f(x) ( + δ) b l <. x R Also, it is clear that f satisfies the interpolation condition f(l j ) = c(j), j Z. Now let ϕ be any smooth test function supported by a segment disjoint from S. Let ɛ(r) 0 and N(R) as R, be some functions satisfying f(x) b j f j (x) < ɛ(r), x R. j N(R) Since each f j has a compact support which lies in S, then ( ˆϕ, f j ) = 0, j Z, and so we have ( ˆϕ, f) = ( ˆϕ, f b j f j ) ɛ(r) ϕ(x) dx+ x R ( + δ) b l j N(R) x >R ˆϕ(x) dx 0, R. Hence, ( ˆϕ, f) = 0, which shows that f B S Remark on sampling sets. We finish this section by the following remark. Definition. A set Λ is called a sampling set for B S if there is a constant C > 0 such that for every f B S. f C sup f(λ), λ Λ Similarly, one may define sampling set for P W S spaces. When S is a single interval, the sampling sets for B S were completely characterized by Beurling in terms of so-called lower uniform density D (L) (see [3]), by the following condition: D (L) > π 9 mes S.

22 For the disconnected compacts S no such metrical characterization may exist. However, one can construct a set of critical density which serves as B S sampling set for every compact of given measure. More precisely, the following is true: Theorem 3. There is a set Λ = {j + O(), j Z}, which is a sampling set for the Bernstein space B S, for every compact S of measure < π. This is a consequence of Theorem 3 in [9] (see details in [0]), where such a universal sampling set was constructed for Paley Wiener spaces. In order to deduce the proposition above from Theorem 3 in [9], one needs Lemma 3.3 Suppose there exists δ 0 > 0 such that a u.d. set Λ is a sampling set for P W S(δ), 0 < δ δ 0, where S(δ) is defined in (7). Then Λ is a sampling set for B S. Indeed, assume that the conclusion of Lemma 3.3 does not hold: for every ɛ > 0 there exists f B S such that sup x f(x) =, and f(λ) < ɛ for every λ Λ. Pick up a point x 0 such that f(x 0 ) /, and set g(x) := f(x) sin δ(x x 0) δ(x x 0 ) P W S(δ), where δ δ 0. Let σ > 0 be such that S(δ) [ σ, σ]. Since g(x) for all x, the Bernstein inequality says that sup f (x) σ. Using this and inequality g(x 0 ) /, one can easily deduce that g C, where C depends only on σ. On the other hand, since Λ is u.d., we have g(λ) ɛ sin δ(λ x 0 ) δ(λ x 0 ) Cɛ, λ Λ λ Λ where C depends only on the infimum of distances between elements of Λ. However, since this can be done for every ɛ > 0, we see that Λ is not a sampling set for P W S(δ), which is a contradiction. In a sharp contrast to Theorem 3., the following claim is true: Corollary 3. A sampling set for the closed (unbounded) spectrum S, constructed in the proof of Theorem 3., must be dense in R. 0

23 Indeed, suppose a set Λ satisfies Λ (a, b) =, for some a < b. By the construction in the proof of Theorem 3., for every ɛ > 0 and c R there exists f B S such that f(c) = and f(x) < ɛ for x c > ɛ. By choosing c = (a + b)/ and ɛ < (b a)/, we see that for every ɛ > 0 there exists a function f B S satisfying f > (/ɛ) f l (Λ), so that Λ is not a sampling set for B S. 4 Unbounded spectra: interpolation in Paley Wiener spaces In the previous section we have seen that there exist universal closed sets S of arbitrarily small measure such that for arbitrary Λ and c the interpolation problem () can be solved by functions f B S. In this section we obtain somewhat similar results for the Paley Wiener spaces. Observe, however, that the universality is not possible to achieve in this case: Proposition 4. No set of measure < π admits interpolation of any δ function on Z by f P W S. Proof. Given a set S R of finite measure, set ( [ π, S π := (S + πj)) π]. j Z Now, suppose there exists f P W S such that f(0) = and f(j) = 0, j Z \ {0}. Denote by F L (S) the inverse Fourier transform of f, and set F π (t) := j Z F (t + πj). Observe that π F π (t) dt = π R F (t) dt mes S F <, so that the function F π is a.e. finite. Also, we see that π {, j = 0 e ijt F π (t) dt = e ijt F (t) dt = f(j) = 0, j 0 π R

24 This implies F π (t) = π for a.e. t [ π, π], and so supp F π = [ π, π]. However, clearly, suppf π S π. We conclude that mes S π. Proposition 4. shows that some restrictions on Λ are necessary in order to get interpolation by P W functions with small spectra. We consider a generic situation: elements of Λ are supposed to be rationally-independent. In this case, we construct closed spectra which admit interpolation of any function on Λ with a certain weak decay condition. Theorem 4. Let a u.d. set Λ = {λ j, j Z} be linearly independent over rationales (mod π). Then for every δ > 0 there is is a set S, a union of some of intervals centered at integers, such that: (i) mes S < δ; (ii) for every sequence c = {c j } satisfying c j ( + j β ) < j Z with some β >, there is a function f P W S satisfying (). Remark. One can see from the proof below that the assumption (ii) can be relaxed by replacing it with j Z c j w j <, where the {w j } l (Z) is a fixed positive sequence. However, assumption (ii) cannot be replaced by c l. Indeed, consider a random sequence of interpolation knots: Λ := {n + ξ(n)}, (30) where ξ j, j Z, are independent random variables uniformly distributed on ( a, a), 0 < a < /. Clearly, Theorem 4. is applicable in this case: Almost surely, there is a closed set S of arbitrary small measure which admits interpolation in P W S of every sequence c satisfying (ii). On the other hand, we have Proposition 4. Let Λ be a random set in (30). With probability, there is no set S of measure < π such that Λ is an interpolation set for P W S.

25 Observe that we don t know if there exists Λ = {j + O(), j Z} which is a set of interpolation for P W S for some (unbounded) S, mes S < π. Proposition 4. shows that if such a set Λ does exist then it should be an exception. Proof of Proposition 4.. It is well-known that the interpolation property in a Hilbert space is equivalent to certain inequalities (see [], p.9). In our case, a set Λ = {λ j, j Z} is a set of interpolation for P W S if and only if there is a positive constant A such that c j e iλ jt dt A c j, (3) S j j for every finite sequence {c j }. Let ξ j be random sequence defined above. Fix an integer N. Clearly, we have with probability one that for every ɛ > 0 there exists k = k(ɛ, N) such that ξ k+j ξ k < ɛ, for all j, j N. Fix an element of the underlying probability space such that the latter is true, and assume that S R is such that the set Λ in (30) is a set of interpolation for P W S. By (3), we have for every c N,..., c N that N c S j e ijt N dt = lim c ɛ 0 S j e i(k+j+ξ k+j)t N dt A c j. j= N j= N j= N Since this is true for every N, we see that Z is also a set of interpolation for P W S. By Proposition, we conclude that mes S π. Proof of Theorem 4.. Throughout the proof we shall denote by C different positive constants.. Without loss of generality we may assume that β <. Set S := j Z S j, S j := ( M j 4β j, M j + 4β j ) (M j 4β j, M j + 4β j ), where β j := γ + j β, 3

26 the sequence M j will be specified in step 4, and γ is any small positive number such that mes S < δ. In what follows we also assume that γ is so small that S j S k =, for j k.. Set Λ k := (Λ λ k ) \ {0}, k Z. The independence condition on Λ implies, by Kronecker s theorem, that for every N > 0 the subgroup {mλ (mod π), λ Λ k [ N, N], m Z} is dense in the l dimensional torus, l being the number of elements in Λ k [ N, N]. Hence, the l numbers cos(mx), x Λ k [ N, N], can be made as small as we like by choosing appropriate M N. 3. Set g j (x) := cos (M j (x λ j )) ( ) 4 sin γj (x λ j ). γ j (x λ j ) Clearly, the spectrum of g j belongs to S j, and we have g j (λ j ) =, (3) and g j C γ j C ( + j β), j Z. (33) 4. Since Λ is uniformly discrete, there is a constant C > 0 such that ( sin γj (λ k λ j ) γ j (λ k λ j ) ) 4 γ 4 j C, k j, k, j Z. (k j)4 Take any small number ɛ > 0, and let N j be so large that we have ( ) 4 sin γj (λ k λ j ) γ j (λ k λ j ) ɛ ( + j )(k j), λ k λ j N j, k j. By Step, the first factor in the definition of g j can be made arbitrarily small for 0 λ k λ j < N j. We shall choose M j N such that ɛ cos M j (λ k λ j ) ( + j ) max{(k j), λ k λ j < N j }, 4

27 for all k j such that λ k λ j < N j. This and the previous estimate give ɛ g j (λ k ), k j, k, j Z. ( + j )(j k) One may check that this estimate implies j Z,j k 5. Given a sequence c = {c j, j Z}, set c β := g j (λ k ) Cɛ + k 3. (34) j= c j ( + j β). Let lβ denote the weighted space of all sequences c, c β <. Define a linear operator R : lβ l β as follows: Re j := k= g j (λ k )e k e j, j Z. Using (3), we have R c j e j β = ( ) c j g j (λ k ) e k β = j Z k Z j Z,j k c j g j (λ k ) ( + k β ) k Z j Z,j k ( ) c g j (λ k ) β ( + k β ). + j β k Z j Z,j k Since β <, we see from (34) that R j Z c j e j β Cɛ c β, for some constant C > 0. Choose ɛ so small that the norm of operator R in lβ is less than. It follows that the operator T := I+R is invertible in lγ, where I is the identity operator. We conclude that 5

28 for every c lβ the interpolation problem () has a solution f given by f(x) := b j g j (x), {b j } = T c lβ. j Z Recall, that the spectrum of g j belongs to the set S j defined in step. Since S j and S k are disjoint for j k, it follows that the functions g j and g k are orthogonal in L (R). Using this and (33), we see that f = j Z b j g j C b β <. Recall again that g j P W Sj P W S, j Z. We conclude that f P W S. References [] Amrein, W. O.; Berthier, A. M. On support properties of L p - functions and their Fourier transforms. J. Functional Analysis 4 (977), no. 3, [] Beurling, A. Interpolation for an interval in R. In: The collected Works of Arne Beurling, Vol., Harmonic Analysis. Birkhauser, Boston, 989. [3] Beurling, A. Balayage of Fouirer-Stiljetes trasnforms. In: The collected Works of Arne Beurling, Vol., Harmonic Analysis. Birkhauser, Boston, 989. [4] Beurling, A., Malliavin, P. On the closure of characters and the zeros of entire functions. Acta Math., 8 (967), [5] Kahane, J.-P. Sur les fonctions moyenne-périodiques bornées. Ann. Inst. Fourier, 7, 957, [6] Landau, H. J. Necessary density conditions for sampling and interpolation of certain entire functions. Acta Math. 7, 967, [7] Redheffer, R.M., Young, R.M. Completeness and basis properties of complex exponentials. Trans. Amer. Math. Soc. 77 (983), no., 93. 6

29 [8] Olevskii, A., Ulanovskii, A. Interpolation by functions with small spectra. C. R. Math. Acad. Sci. Paris 345 (007), no. 5, [9] Olevskii, A., Ulanovskii, A. Universal sampling of band-limited signals. C. R. Math. Acad. Sci. Paris 34 (006), no., [0] Olevskii, A., Ulanovskii, A. Universal sampling and interpolation of band-limited signals. To be published in GAFA. [] Young, R.M. An introduction to Nonharmonic Fourier Series. Academic Press

Oberwolfach Preprints

Oberwolfach Preprints Oberwolfach Preprints OWP 2009-17 ALEXANDER OLEVSKII AND ALEXANDER ULANOVSKII Approximation of Discrete Functions and Size of Spectrum Mathematisches Forschungsinstitut Oberwolfach ggmbh Oberwolfach Preprints

More information

arxiv: v1 [math.ca] 2 Apr 2013

arxiv: v1 [math.ca] 2 Apr 2013 arxiv:1304.0649v1 [math.ca] 2 Apr 2013 Approximation of discrete functions and size of spectrum Alexander Olevskii and Alexander Ulanovskii A.O.: School of Mathematics, Tel Aviv University Ramat Aviv,

More information

Oberwolfach Preprints

Oberwolfach Preprints Oberwolfach Preprints OWP 2018-11 HERY RANDRIAMARO A Deformed Quon Algebra Mathematisches Forschungsinstitut Oberwolfach ggmbh Oberwolfach Preprints (OWP ISSN 1864-7596 Oberwolfach Preprints (OWP Starting

More information

Oberwolfach Preprints

Oberwolfach Preprints Oberwolfach Preprints OWP 202-07 LÁSZLÓ GYÖFI, HAO WALK Strongly Consistent Density Estimation of egression esidual Mathematisches Forschungsinstitut Oberwolfach ggmbh Oberwolfach Preprints (OWP) ISSN

More information

Oberwolfach Preprints

Oberwolfach Preprints Oberwolfach Preprints OWP 2013-23 CLEONICE F. BRACCIALI AND JUAN JOSÉ MORENO- BALCÁZAR Mehler-Heine Asymptotics of a Class of Generalized Hypergeometric Polynomials Mathematisches Forschungsinstitut Oberwolfach

More information

Finite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product

Finite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product Chapter 4 Hilbert Spaces 4.1 Inner Product Spaces Inner Product Space. A complex vector space E is called an inner product space (or a pre-hilbert space, or a unitary space) if there is a mapping (, )

More information

1 Math 241A-B Homework Problem List for F2015 and W2016

1 Math 241A-B Homework Problem List for F2015 and W2016 1 Math 241A-B Homework Problem List for F2015 W2016 1.1 Homework 1. Due Wednesday, October 7, 2015 Notation 1.1 Let U be any set, g be a positive function on U, Y be a normed space. For any f : U Y let

More information

Frames of exponentials on small sets

Frames of exponentials on small sets Frames of exponentials on small sets J.-P. Gabardo McMaster University Department of Mathematics and Statistics gabardo@mcmaster.ca Joint work with Chun-Kit Lai (San Francisco State Univ.) Workshop on

More information

Decomposition of Riesz frames and wavelets into a finite union of linearly independent sets

Decomposition of Riesz frames and wavelets into a finite union of linearly independent sets Decomposition of Riesz frames and wavelets into a finite union of linearly independent sets Ole Christensen, Alexander M. Lindner Abstract We characterize Riesz frames and prove that every Riesz frame

More information

On Riesz-Fischer sequences and lower frame bounds

On Riesz-Fischer sequences and lower frame bounds On Riesz-Fischer sequences and lower frame bounds P. Casazza, O. Christensen, S. Li, A. Lindner Abstract We investigate the consequences of the lower frame condition and the lower Riesz basis condition

More information

Real Analysis Problems

Real Analysis Problems Real Analysis Problems Cristian E. Gutiérrez September 14, 29 1 1 CONTINUITY 1 Continuity Problem 1.1 Let r n be the sequence of rational numbers and Prove that f(x) = 1. f is continuous on the irrationals.

More information

Oberwolfach Preprints

Oberwolfach Preprints Oberwolfach Preprints OWP 2011-36 PAWEL GLADKI AND MURRAY MARSHALL Quotients of Index Two and General Quotients in a Space of Orderings Mathematisches Forschungsinstitut Oberwolfach ggmbh Oberwolfach Preprints

More information

Commutative Banach algebras 79

Commutative Banach algebras 79 8. Commutative Banach algebras In this chapter, we analyze commutative Banach algebras in greater detail. So we always assume that xy = yx for all x, y A here. Definition 8.1. Let A be a (commutative)

More information

REAL AND COMPLEX ANALYSIS

REAL AND COMPLEX ANALYSIS REAL AND COMPLE ANALYSIS Third Edition Walter Rudin Professor of Mathematics University of Wisconsin, Madison Version 1.1 No rights reserved. Any part of this work can be reproduced or transmitted in any

More information

MAT 570 REAL ANALYSIS LECTURE NOTES. Contents. 1. Sets Functions Countability Axiom of choice Equivalence relations 9

MAT 570 REAL ANALYSIS LECTURE NOTES. Contents. 1. Sets Functions Countability Axiom of choice Equivalence relations 9 MAT 570 REAL ANALYSIS LECTURE NOTES PROFESSOR: JOHN QUIGG SEMESTER: FALL 204 Contents. Sets 2 2. Functions 5 3. Countability 7 4. Axiom of choice 8 5. Equivalence relations 9 6. Real numbers 9 7. Extended

More information

SPECTRAL THEOREM FOR SYMMETRIC OPERATORS WITH COMPACT RESOLVENT

SPECTRAL THEOREM FOR SYMMETRIC OPERATORS WITH COMPACT RESOLVENT SPECTRAL THEOREM FOR SYMMETRIC OPERATORS WITH COMPACT RESOLVENT Abstract. These are the letcure notes prepared for the workshop on Functional Analysis and Operator Algebras to be held at NIT-Karnataka,

More information

Metric Spaces and Topology

Metric Spaces and Topology Chapter 2 Metric Spaces and Topology From an engineering perspective, the most important way to construct a topology on a set is to define the topology in terms of a metric on the set. This approach underlies

More information

d(x n, x) d(x n, x nk ) + d(x nk, x) where we chose any fixed k > N

d(x n, x) d(x n, x nk ) + d(x nk, x) where we chose any fixed k > N Problem 1. Let f : A R R have the property that for every x A, there exists ɛ > 0 such that f(t) > ɛ if t (x ɛ, x + ɛ) A. If the set A is compact, prove there exists c > 0 such that f(x) > c for all x

More information

Department of Mathematics, University of California, Berkeley. GRADUATE PRELIMINARY EXAMINATION, Part A Fall Semester 2016

Department of Mathematics, University of California, Berkeley. GRADUATE PRELIMINARY EXAMINATION, Part A Fall Semester 2016 Department of Mathematics, University of California, Berkeley YOUR 1 OR 2 DIGIT EXAM NUMBER GRADUATE PRELIMINARY EXAMINATION, Part A Fall Semester 2016 1. Please write your 1- or 2-digit exam number on

More information

MORE NOTES FOR MATH 823, FALL 2007

MORE NOTES FOR MATH 823, FALL 2007 MORE NOTES FOR MATH 83, FALL 007 Prop 1.1 Prop 1. Lemma 1.3 1. The Siegel upper half space 1.1. The Siegel upper half space and its Bergman kernel. The Siegel upper half space is the domain { U n+1 z C

More information

SHARP BOUNDARY TRACE INEQUALITIES. 1. Introduction

SHARP BOUNDARY TRACE INEQUALITIES. 1. Introduction SHARP BOUNDARY TRACE INEQUALITIES GILES AUCHMUTY Abstract. This paper describes sharp inequalities for the trace of Sobolev functions on the boundary of a bounded region R N. The inequalities bound (semi-)norms

More information

Linear independence of exponentials on the real line

Linear independence of exponentials on the real line Linear independence of exponentials on the real line Alexandre Eremenko August 25, 2013 The following question was asked on Math Overflow. Let (λ n ) be a sequence of complex numbers tending to infinity.

More information

Real Analysis Math 131AH Rudin, Chapter #1. Dominique Abdi

Real Analysis Math 131AH Rudin, Chapter #1. Dominique Abdi Real Analysis Math 3AH Rudin, Chapter # Dominique Abdi.. If r is rational (r 0) and x is irrational, prove that r + x and rx are irrational. Solution. Assume the contrary, that r+x and rx are rational.

More information

RUTGERS UNIVERSITY GRADUATE PROGRAM IN MATHEMATICS Written Qualifying Examination August, Session 1. Algebra

RUTGERS UNIVERSITY GRADUATE PROGRAM IN MATHEMATICS Written Qualifying Examination August, Session 1. Algebra RUTGERS UNIVERSITY GRADUATE PROGRAM IN MATHEMATICS Written Qualifying Examination August, 2014 Session 1. Algebra The Qualifying Examination consists of three two-hour sessions. This is the first session.

More information

Measurable functions are approximately nice, even if look terrible.

Measurable functions are approximately nice, even if look terrible. Tel Aviv University, 2015 Functions of real variables 74 7 Approximation 7a A terrible integrable function........... 74 7b Approximation of sets................ 76 7c Approximation of functions............

More information

Density results for frames of exponentials

Density results for frames of exponentials Density results for frames of exponentials P. G. Casazza 1, O. Christensen 2, S. Li 3, and A. Lindner 4 1 Department of Mathematics, University of Missouri Columbia, Mo 65211 USA pete@math.missouri.edu

More information

Your first day at work MATH 806 (Fall 2015)

Your first day at work MATH 806 (Fall 2015) Your first day at work MATH 806 (Fall 2015) 1. Let X be a set (with no particular algebraic structure). A function d : X X R is called a metric on X (and then X is called a metric space) when d satisfies

More information

3. 4. Uniformly normal families and generalisations

3. 4. Uniformly normal families and generalisations Summer School Normal Families in Complex Analysis Julius-Maximilians-Universität Würzburg May 22 29, 2015 3. 4. Uniformly normal families and generalisations Aimo Hinkkanen University of Illinois at Urbana

More information

POSITIVE DEFINITE FUNCTIONS AND MULTIDIMENSIONAL VERSIONS OF RANDOM VARIABLES

POSITIVE DEFINITE FUNCTIONS AND MULTIDIMENSIONAL VERSIONS OF RANDOM VARIABLES POSITIVE DEFINITE FUNCTIONS AND MULTIDIMENSIONAL VERSIONS OF RANDOM VARIABLES ALEXANDER KOLDOBSKY Abstract. We prove that if a function of the form f( K is positive definite on, where K is an origin symmetric

More information

(1) Consider the space S consisting of all continuous real-valued functions on the closed interval [0, 1]. For f, g S, define

(1) Consider the space S consisting of all continuous real-valued functions on the closed interval [0, 1]. For f, g S, define Homework, Real Analysis I, Fall, 2010. (1) Consider the space S consisting of all continuous real-valued functions on the closed interval [0, 1]. For f, g S, define ρ(f, g) = 1 0 f(x) g(x) dx. Show that

More information

MATH MEASURE THEORY AND FOURIER ANALYSIS. Contents

MATH MEASURE THEORY AND FOURIER ANALYSIS. Contents MATH 3969 - MEASURE THEORY AND FOURIER ANALYSIS ANDREW TULLOCH Contents 1. Measure Theory 2 1.1. Properties of Measures 3 1.2. Constructing σ-algebras and measures 3 1.3. Properties of the Lebesgue measure

More information

Exercise Solutions to Functional Analysis

Exercise Solutions to Functional Analysis Exercise Solutions to Functional Analysis Note: References refer to M. Schechter, Principles of Functional Analysis Exersize that. Let φ,..., φ n be an orthonormal set in a Hilbert space H. Show n f n

More information

TOOLS FROM HARMONIC ANALYSIS

TOOLS FROM HARMONIC ANALYSIS TOOLS FROM HARMONIC ANALYSIS BRADLY STADIE Abstract. The Fourier transform can be thought of as a map that decomposes a function into oscillatory functions. In this paper, we will apply this decomposition

More information

Real Analysis, 2nd Edition, G.B.Folland Elements of Functional Analysis

Real Analysis, 2nd Edition, G.B.Folland Elements of Functional Analysis Real Analysis, 2nd Edition, G.B.Folland Chapter 5 Elements of Functional Analysis Yung-Hsiang Huang 5.1 Normed Vector Spaces 1. Note for any x, y X and a, b K, x+y x + y and by ax b y x + b a x. 2. It

More information

Math The Laplacian. 1 Green s Identities, Fundamental Solution

Math The Laplacian. 1 Green s Identities, Fundamental Solution Math. 209 The Laplacian Green s Identities, Fundamental Solution Let be a bounded open set in R n, n 2, with smooth boundary. The fact that the boundary is smooth means that at each point x the external

More information

Outline of Fourier Series: Math 201B

Outline of Fourier Series: Math 201B Outline of Fourier Series: Math 201B February 24, 2011 1 Functions and convolutions 1.1 Periodic functions Periodic functions. Let = R/(2πZ) denote the circle, or onedimensional torus. A function f : C

More information

Analysis Finite and Infinite Sets The Real Numbers The Cantor Set

Analysis Finite and Infinite Sets The Real Numbers The Cantor Set Analysis Finite and Infinite Sets Definition. An initial segment is {n N n n 0 }. Definition. A finite set can be put into one-to-one correspondence with an initial segment. The empty set is also considered

More information

Fall TMA4145 Linear Methods. Solutions to exercise set 9. 1 Let X be a Hilbert space and T a bounded linear operator on X.

Fall TMA4145 Linear Methods. Solutions to exercise set 9. 1 Let X be a Hilbert space and T a bounded linear operator on X. TMA445 Linear Methods Fall 26 Norwegian University of Science and Technology Department of Mathematical Sciences Solutions to exercise set 9 Let X be a Hilbert space and T a bounded linear operator on

More information

CHARACTERISTIC POLYNOMIAL PATTERNS IN DIFFERENCE SETS OF MATRICES

CHARACTERISTIC POLYNOMIAL PATTERNS IN DIFFERENCE SETS OF MATRICES CHARACTERISTIC POLYNOMIAL PATTERNS IN DIFFERENCE SETS OF MATRICES MICHAEL BJÖRKLUND AND ALEXANDER FISH Abstract. We show that for every subset E of positive density in the set of integer squarematrices

More information

Real Analysis Notes. Thomas Goller

Real Analysis Notes. Thomas Goller Real Analysis Notes Thomas Goller September 4, 2011 Contents 1 Abstract Measure Spaces 2 1.1 Basic Definitions........................... 2 1.2 Measurable Functions........................ 2 1.3 Integration..............................

More information

Classification: Mathematics. Title: Oscillation of functions with a spectral gap. Authors and author affiliation: A. Eremenko ( ) and D.

Classification: Mathematics. Title: Oscillation of functions with a spectral gap. Authors and author affiliation: A. Eremenko ( ) and D. Classification: Mathematics. Title: Oscillation of functions with a spectral gap Authors and author affiliation: A. Eremenko ( ) and D. Novikov ( ) Department of Mathematics ( ) Purdue University West

More information

08a. Operators on Hilbert spaces. 1. Boundedness, continuity, operator norms

08a. Operators on Hilbert spaces. 1. Boundedness, continuity, operator norms (February 24, 2017) 08a. Operators on Hilbert spaces Paul Garrett garrett@math.umn.edu http://www.math.umn.edu/ garrett/ [This document is http://www.math.umn.edu/ garrett/m/real/notes 2016-17/08a-ops

More information

Some basic elements of Probability Theory

Some basic elements of Probability Theory Chapter I Some basic elements of Probability Theory 1 Terminology (and elementary observations Probability theory and the material covered in a basic Real Variables course have much in common. However

More information

Topological properties

Topological properties CHAPTER 4 Topological properties 1. Connectedness Definitions and examples Basic properties Connected components Connected versus path connected, again 2. Compactness Definition and first examples Topological

More information

MATH 722, COMPLEX ANALYSIS, SPRING 2009 PART 5

MATH 722, COMPLEX ANALYSIS, SPRING 2009 PART 5 MATH 722, COMPLEX ANALYSIS, SPRING 2009 PART 5.. The Arzela-Ascoli Theorem.. The Riemann mapping theorem Let X be a metric space, and let F be a family of continuous complex-valued functions on X. We have

More information

PROBLEMS. (b) (Polarization Identity) Show that in any inner product space

PROBLEMS. (b) (Polarization Identity) Show that in any inner product space 1 Professor Carl Cowen Math 54600 Fall 09 PROBLEMS 1. (Geometry in Inner Product Spaces) (a) (Parallelogram Law) Show that in any inner product space x + y 2 + x y 2 = 2( x 2 + y 2 ). (b) (Polarization

More information

Reminder Notes for the Course on Distribution Theory

Reminder Notes for the Course on Distribution Theory Reminder Notes for the Course on Distribution Theory T. C. Dorlas Dublin Institute for Advanced Studies School of Theoretical Physics 10 Burlington Road, Dublin 4, Ireland. Email: dorlas@stp.dias.ie March

More information

Trace Class Operators and Lidskii s Theorem

Trace Class Operators and Lidskii s Theorem Trace Class Operators and Lidskii s Theorem Tom Phelan Semester 2 2009 1 Introduction The purpose of this paper is to provide the reader with a self-contained derivation of the celebrated Lidskii Trace

More information

Homework If the inverse T 1 of a closed linear operator exists, show that T 1 is a closed linear operator.

Homework If the inverse T 1 of a closed linear operator exists, show that T 1 is a closed linear operator. Homework 3 1 If the inverse T 1 of a closed linear operator exists, show that T 1 is a closed linear operator Solution: Assuming that the inverse of T were defined, then we will have to have that D(T 1

More information

Problem Set 2: Solutions Math 201A: Fall 2016

Problem Set 2: Solutions Math 201A: Fall 2016 Problem Set 2: s Math 201A: Fall 2016 Problem 1. (a) Prove that a closed subset of a complete metric space is complete. (b) Prove that a closed subset of a compact metric space is compact. (c) Prove that

More information

MATH 8253 ALGEBRAIC GEOMETRY WEEK 12

MATH 8253 ALGEBRAIC GEOMETRY WEEK 12 MATH 8253 ALGEBRAIC GEOMETRY WEEK 2 CİHAN BAHRAN 3.2.. Let Y be a Noetherian scheme. Show that any Y -scheme X of finite type is Noetherian. Moreover, if Y is of finite dimension, then so is X. Write f

More information

ON PARABOLIC HARNACK INEQUALITY

ON PARABOLIC HARNACK INEQUALITY ON PARABOLIC HARNACK INEQUALITY JIAXIN HU Abstract. We show that the parabolic Harnack inequality is equivalent to the near-diagonal lower bound of the Dirichlet heat kernel on any ball in a metric measure-energy

More information

Recall that any inner product space V has an associated norm defined by

Recall that any inner product space V has an associated norm defined by Hilbert Spaces Recall that any inner product space V has an associated norm defined by v = v v. Thus an inner product space can be viewed as a special kind of normed vector space. In particular every inner

More information

Math 118B Solutions. Charles Martin. March 6, d i (x i, y i ) + d i (y i, z i ) = d(x, y) + d(y, z). i=1

Math 118B Solutions. Charles Martin. March 6, d i (x i, y i ) + d i (y i, z i ) = d(x, y) + d(y, z). i=1 Math 8B Solutions Charles Martin March 6, Homework Problems. Let (X i, d i ), i n, be finitely many metric spaces. Construct a metric on the product space X = X X n. Proof. Denote points in X as x = (x,

More information

are Banach algebras. f(x)g(x) max Example 7.4. Similarly, A = L and A = l with the pointwise multiplication

are Banach algebras. f(x)g(x) max Example 7.4. Similarly, A = L and A = l with the pointwise multiplication 7. Banach algebras Definition 7.1. A is called a Banach algebra (with unit) if: (1) A is a Banach space; (2) There is a multiplication A A A that has the following properties: (xy)z = x(yz), (x + y)z =

More information

An introduction to Birkhoff normal form

An introduction to Birkhoff normal form An introduction to Birkhoff normal form Dario Bambusi Dipartimento di Matematica, Universitá di Milano via Saldini 50, 0133 Milano (Italy) 19.11.14 1 Introduction The aim of this note is to present an

More information

2 Infinite products and existence of compactly supported φ

2 Infinite products and existence of compactly supported φ 415 Wavelets 1 Infinite products and existence of compactly supported φ Infinite products.1 Infinite products a n need to be defined via limits. But we do not simply say that a n = lim a n N whenever the

More information

Part V. 17 Introduction: What are measures and why measurable sets. Lebesgue Integration Theory

Part V. 17 Introduction: What are measures and why measurable sets. Lebesgue Integration Theory Part V 7 Introduction: What are measures and why measurable sets Lebesgue Integration Theory Definition 7. (Preliminary). A measure on a set is a function :2 [ ] such that. () = 2. If { } = is a finite

More information

Probability and Measure

Probability and Measure Part II Year 2018 2017 2016 2015 2014 2013 2012 2011 2010 2009 2008 2007 2006 2005 2018 84 Paper 4, Section II 26J Let (X, A) be a measurable space. Let T : X X be a measurable map, and µ a probability

More information

RIESZ BASES AND UNCONDITIONAL BASES

RIESZ BASES AND UNCONDITIONAL BASES In this paper we give a brief introduction to adjoint operators on Hilbert spaces and a characterization of the dual space of a Hilbert space. We then introduce the notion of a Riesz basis and give some

More information

SEMILINEAR ELLIPTIC EQUATIONS WITH DEPENDENCE ON THE GRADIENT

SEMILINEAR ELLIPTIC EQUATIONS WITH DEPENDENCE ON THE GRADIENT Electronic Journal of Differential Equations, Vol. 2012 (2012), No. 139, pp. 1 9. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu SEMILINEAR ELLIPTIC

More information

THE L 2 -HODGE THEORY AND REPRESENTATION ON R n

THE L 2 -HODGE THEORY AND REPRESENTATION ON R n THE L 2 -HODGE THEORY AND REPRESENTATION ON R n BAISHENG YAN Abstract. We present an elementary L 2 -Hodge theory on whole R n based on the minimization principle of the calculus of variations and some

More information

Math 209B Homework 2

Math 209B Homework 2 Math 29B Homework 2 Edward Burkard Note: All vector spaces are over the field F = R or C 4.6. Two Compactness Theorems. 4. Point Set Topology Exercise 6 The product of countably many sequentally compact

More information

Reducing subspaces. Rowan Killip 1 and Christian Remling 2 January 16, (to appear in J. Funct. Anal.)

Reducing subspaces. Rowan Killip 1 and Christian Remling 2 January 16, (to appear in J. Funct. Anal.) Reducing subspaces Rowan Killip 1 and Christian Remling 2 January 16, 2001 (to appear in J. Funct. Anal.) 1. University of Pennsylvania, 209 South 33rd Street, Philadelphia PA 19104-6395, USA. On leave

More information

Topics in Harmonic Analysis Lecture 1: The Fourier transform

Topics in Harmonic Analysis Lecture 1: The Fourier transform Topics in Harmonic Analysis Lecture 1: The Fourier transform Po-Lam Yung The Chinese University of Hong Kong Outline Fourier series on T: L 2 theory Convolutions The Dirichlet and Fejer kernels Pointwise

More information

NUMERICAL RADIUS OF A HOLOMORPHIC MAPPING

NUMERICAL RADIUS OF A HOLOMORPHIC MAPPING Geometric Complex Analysis edited by Junjiro Noguchi et al. World Scientific, Singapore, 1995 pp.1 7 NUMERICAL RADIUS OF A HOLOMORPHIC MAPPING YUN SUNG CHOI Department of Mathematics Pohang University

More information

The Hilbert Transform and Fine Continuity

The Hilbert Transform and Fine Continuity Irish Math. Soc. Bulletin 58 (2006), 8 9 8 The Hilbert Transform and Fine Continuity J. B. TWOMEY Abstract. It is shown that the Hilbert transform of a function having bounded variation in a finite interval

More information

From now on, we will represent a metric space with (X, d). Here are some examples: i=1 (x i y i ) p ) 1 p, p 1.

From now on, we will represent a metric space with (X, d). Here are some examples: i=1 (x i y i ) p ) 1 p, p 1. Chapter 1 Metric spaces 1.1 Metric and convergence We will begin with some basic concepts. Definition 1.1. (Metric space) Metric space is a set X, with a metric satisfying: 1. d(x, y) 0, d(x, y) = 0 x

More information

SYMPLECTIC GEOMETRY: LECTURE 5

SYMPLECTIC GEOMETRY: LECTURE 5 SYMPLECTIC GEOMETRY: LECTURE 5 LIAT KESSLER Let (M, ω) be a connected compact symplectic manifold, T a torus, T M M a Hamiltonian action of T on M, and Φ: M t the assoaciated moment map. Theorem 0.1 (The

More information

5 Compact linear operators

5 Compact linear operators 5 Compact linear operators One of the most important results of Linear Algebra is that for every selfadjoint linear map A on a finite-dimensional space, there exists a basis consisting of eigenvectors.

More information

A COUNTEREXAMPLE TO AN ENDPOINT BILINEAR STRICHARTZ INEQUALITY TERENCE TAO. t L x (R R2 ) f L 2 x (R2 )

A COUNTEREXAMPLE TO AN ENDPOINT BILINEAR STRICHARTZ INEQUALITY TERENCE TAO. t L x (R R2 ) f L 2 x (R2 ) Electronic Journal of Differential Equations, Vol. 2006(2006), No. 5, pp. 6. ISSN: 072-669. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) A COUNTEREXAMPLE

More information

CESARO OPERATORS ON THE HARDY SPACES OF THE HALF-PLANE

CESARO OPERATORS ON THE HARDY SPACES OF THE HALF-PLANE CESARO OPERATORS ON THE HARDY SPACES OF THE HALF-PLANE ATHANASIOS G. ARVANITIDIS AND ARISTOMENIS G. SISKAKIS Abstract. In this article we study the Cesàro operator C(f)() = d, and its companion operator

More information

THE KADISON-SINGER PROBLEM AND THE UNCERTAINTY PRINCIPLE

THE KADISON-SINGER PROBLEM AND THE UNCERTAINTY PRINCIPLE PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 00, Number 0, Pages 000 000 S 0002-9939(XX)0000-0 THE KADISON-SINGER PROBLEM AND THE UNCERTAINTY PRINCIPLE PETER G. CASAZZA AND ERIC WEBER Abstract.

More information

Applied Analysis (APPM 5440): Final exam 1:30pm 4:00pm, Dec. 14, Closed books.

Applied Analysis (APPM 5440): Final exam 1:30pm 4:00pm, Dec. 14, Closed books. Applied Analysis APPM 44: Final exam 1:3pm 4:pm, Dec. 14, 29. Closed books. Problem 1: 2p Set I = [, 1]. Prove that there is a continuous function u on I such that 1 ux 1 x sin ut 2 dt = cosx, x I. Define

More information

Problem Set 5: Solutions Math 201A: Fall 2016

Problem Set 5: Solutions Math 201A: Fall 2016 Problem Set 5: s Math 21A: Fall 216 Problem 1. Define f : [1, ) [1, ) by f(x) = x + 1/x. Show that f(x) f(y) < x y for all x, y [1, ) with x y, but f has no fixed point. Why doesn t this example contradict

More information

Tools from Lebesgue integration

Tools from Lebesgue integration Tools from Lebesgue integration E.P. van den Ban Fall 2005 Introduction In these notes we describe some of the basic tools from the theory of Lebesgue integration. Definitions and results will be given

More information

THEOREMS, ETC., FOR MATH 515

THEOREMS, ETC., FOR MATH 515 THEOREMS, ETC., FOR MATH 515 Proposition 1 (=comment on page 17). If A is an algebra, then any finite union or finite intersection of sets in A is also in A. Proposition 2 (=Proposition 1.1). For every

More information

PACKING-DIMENSION PROFILES AND FRACTIONAL BROWNIAN MOTION

PACKING-DIMENSION PROFILES AND FRACTIONAL BROWNIAN MOTION PACKING-DIMENSION PROFILES AND FRACTIONAL BROWNIAN MOTION DAVAR KHOSHNEVISAN AND YIMIN XIAO Abstract. In order to compute the packing dimension of orthogonal projections Falconer and Howroyd 997) introduced

More information

A NEW PROOF OF THE ATOMIC DECOMPOSITION OF HARDY SPACES

A NEW PROOF OF THE ATOMIC DECOMPOSITION OF HARDY SPACES A NEW PROOF OF THE ATOMIC DECOMPOSITION OF HARDY SPACES S. DEKEL, G. KERKYACHARIAN, G. KYRIAZIS, AND P. PETRUSHEV Abstract. A new proof is given of the atomic decomposition of Hardy spaces H p, 0 < p 1,

More information

Topics in Fourier analysis - Lecture 2.

Topics in Fourier analysis - Lecture 2. Topics in Fourier analysis - Lecture 2. Akos Magyar 1 Infinite Fourier series. In this section we develop the basic theory of Fourier series of periodic functions of one variable, but only to the extent

More information

Analysis in weighted spaces : preliminary version

Analysis in weighted spaces : preliminary version Analysis in weighted spaces : preliminary version Frank Pacard To cite this version: Frank Pacard. Analysis in weighted spaces : preliminary version. 3rd cycle. Téhéran (Iran, 2006, pp.75.

More information

MATH 205C: STATIONARY PHASE LEMMA

MATH 205C: STATIONARY PHASE LEMMA MATH 205C: STATIONARY PHASE LEMMA For ω, consider an integral of the form I(ω) = e iωf(x) u(x) dx, where u Cc (R n ) complex valued, with support in a compact set K, and f C (R n ) real valued. Thus, I(ω)

More information

NORM DEPENDENCE OF THE COEFFICIENT MAP ON THE WINDOW SIZE 1

NORM DEPENDENCE OF THE COEFFICIENT MAP ON THE WINDOW SIZE 1 NORM DEPENDENCE OF THE COEFFICIENT MAP ON THE WINDOW SIZE Thomas I. Seidman and M. Seetharama Gowda Department of Mathematics and Statistics University of Maryland Baltimore County Baltimore, MD 8, U.S.A

More information

HOMEWORK ASSIGNMENT 6

HOMEWORK ASSIGNMENT 6 HOMEWORK ASSIGNMENT 6 DUE 15 MARCH, 2016 1) Suppose f, g : A R are uniformly continuous on A. Show that f + g is uniformly continuous on A. Solution First we note: In order to show that f + g is uniformly

More information

Continuous functions that are nowhere differentiable

Continuous functions that are nowhere differentiable Continuous functions that are nowhere differentiable S. Kesavan The Institute of Mathematical Sciences, CIT Campus, Taramani, Chennai - 600113. e-mail: kesh @imsc.res.in Abstract It is shown that the existence

More information

The following definition is fundamental.

The following definition is fundamental. 1. Some Basics from Linear Algebra With these notes, I will try and clarify certain topics that I only quickly mention in class. First and foremost, I will assume that you are familiar with many basic

More information

Analysis Comprehensive Exam Questions Fall F(x) = 1 x. f(t)dt. t 1 2. tf 2 (t)dt. and g(t, x) = 2 t. 2 t

Analysis Comprehensive Exam Questions Fall F(x) = 1 x. f(t)dt. t 1 2. tf 2 (t)dt. and g(t, x) = 2 t. 2 t Analysis Comprehensive Exam Questions Fall 2. Let f L 2 (, ) be given. (a) Prove that ( x 2 f(t) dt) 2 x x t f(t) 2 dt. (b) Given part (a), prove that F L 2 (, ) 2 f L 2 (, ), where F(x) = x (a) Using

More information

Wavelets and modular inequalities in variable L p spaces

Wavelets and modular inequalities in variable L p spaces Wavelets and modular inequalities in variable L p spaces Mitsuo Izuki July 14, 2007 Abstract The aim of this paper is to characterize variable L p spaces L p( ) (R n ) using wavelets with proper smoothness

More information

THE INVERSE FUNCTION THEOREM

THE INVERSE FUNCTION THEOREM THE INVERSE FUNCTION THEOREM W. PATRICK HOOPER The implicit function theorem is the following result: Theorem 1. Let f be a C 1 function from a neighborhood of a point a R n into R n. Suppose A = Df(a)

More information

Computations of Critical Groups at a Degenerate Critical Point for Strongly Indefinite Functionals

Computations of Critical Groups at a Degenerate Critical Point for Strongly Indefinite Functionals Journal of Mathematical Analysis and Applications 256, 462 477 (2001) doi:10.1006/jmaa.2000.7292, available online at http://www.idealibrary.com on Computations of Critical Groups at a Degenerate Critical

More information

1.5 Approximate Identities

1.5 Approximate Identities 38 1 The Fourier Transform on L 1 (R) which are dense subspaces of L p (R). On these domains, P : D P L p (R) and M : D M L p (R). Show, however, that P and M are unbounded even when restricted to these

More information

1 Topology Definition of a topology Basis (Base) of a topology The subspace topology & the product topology on X Y 3

1 Topology Definition of a topology Basis (Base) of a topology The subspace topology & the product topology on X Y 3 Index Page 1 Topology 2 1.1 Definition of a topology 2 1.2 Basis (Base) of a topology 2 1.3 The subspace topology & the product topology on X Y 3 1.4 Basic topology concepts: limit points, closed sets,

More information

On an uniqueness theorem for characteristic functions

On an uniqueness theorem for characteristic functions ISSN 392-53 Nonlinear Analysis: Modelling and Control, 207, Vol. 22, No. 3, 42 420 https://doi.org/0.5388/na.207.3.9 On an uniqueness theorem for characteristic functions Saulius Norvidas Institute of

More information

Errata Applied Analysis

Errata Applied Analysis Errata Applied Analysis p. 9: line 2 from the bottom: 2 instead of 2. p. 10: Last sentence should read: The lim sup of a sequence whose terms are bounded from above is finite or, and the lim inf of a sequence

More information

A RECONSTRUCTION FORMULA FOR BAND LIMITED FUNCTIONS IN L 2 (R d )

A RECONSTRUCTION FORMULA FOR BAND LIMITED FUNCTIONS IN L 2 (R d ) PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 127, Number 12, Pages 3593 3600 S 0002-9939(99)04938-2 Article electronically published on May 6, 1999 A RECONSTRUCTION FORMULA FOR AND LIMITED FUNCTIONS

More information

Lecture 5 - Hausdorff and Gromov-Hausdorff Distance

Lecture 5 - Hausdorff and Gromov-Hausdorff Distance Lecture 5 - Hausdorff and Gromov-Hausdorff Distance August 1, 2011 1 Definition and Basic Properties Given a metric space X, the set of closed sets of X supports a metric, the Hausdorff metric. If A is

More information

A DECOMPOSITION THEOREM FOR FRAMES AND THE FEICHTINGER CONJECTURE

A DECOMPOSITION THEOREM FOR FRAMES AND THE FEICHTINGER CONJECTURE PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 00, Number 0, Pages 000 000 S 0002-9939(XX)0000-0 A DECOMPOSITION THEOREM FOR FRAMES AND THE FEICHTINGER CONJECTURE PETER G. CASAZZA, GITTA KUTYNIOK,

More information

ATOMIC DECOMPOSITIONS AND OPERATORS ON HARDY SPACES

ATOMIC DECOMPOSITIONS AND OPERATORS ON HARDY SPACES REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Volumen 50, Número 2, 2009, Páginas 15 22 ATOMIC DECOMPOSITIONS AND OPERATORS ON HARDY SPACES STEFANO MEDA, PETER SJÖGREN AND MARIA VALLARINO Abstract. This paper

More information

Harmonic Analysis on the Cube and Parseval s Identity

Harmonic Analysis on the Cube and Parseval s Identity Lecture 3 Harmonic Analysis on the Cube and Parseval s Identity Jan 28, 2005 Lecturer: Nati Linial Notes: Pete Couperus and Neva Cherniavsky 3. Where we can use this During the past weeks, we developed

More information

Introduction to Bases in Banach Spaces

Introduction to Bases in Banach Spaces Introduction to Bases in Banach Spaces Matt Daws June 5, 2005 Abstract We introduce the notion of Schauder bases in Banach spaces, aiming to be able to give a statement of, and make sense of, the Gowers

More information