CHARACTERIZATION OF THE FOURIER SERIES OF A DISTRIBUTION HAVING A VALUE AT A POINT

Size: px
Start display at page:

Download "CHARACTERIZATION OF THE FOURIER SERIES OF A DISTRIBUTION HAVING A VALUE AT A POINT"

Transcription

1 PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 124, Number 4, April 1996 CHARACTERIZATION OF THE FOURIER SERIES OF A DISTRIBUTION HAVING A VALUE AT A POINT RICARDO ESTRADA (Communicated by J. Marshall Ash) Abstract. Let f be a periodic distribution of period 2π. Let aneinθ be its Fourier series. We show that the distributional point value f(θ )exists and equals γ if and only if the partial sums x n ax aneinθ converge to γ in the Cesàro sense as x for each a>. 1. Introduction The study of the relationship between the local behavior of a periodic function at a point and the convergence and summability of the corresponding Fourier series has been one of the main concerns of classical harmonic analysis, a subject with many years of history. In particular, the characterization of the Fourier series having a value at a point is a very interesting problem, whose solution depends on the notion of value used. Among the various useful notions of value we could mention the value of a continuous function at a point, the measure-theoretical approximate value of an integrable function, or the distributional point value of a generalized function. In this article we shall be concerned with the characterization of the Fourier series of generalized functions having a distributional point value. The notion of distributional point value was introduced by Lojasiewicz [8] and corresponds, roughly, to the existence of value on the average. If f D (R) is a distribution and x R, we say that f has the distributional value γ at x = x,andwritef(x )=γin D if for each φ Dwehave lim ε f(x +εx),φ(x) =γ φ(x) dx (if f is given by an integral and φ(x) dx = 1 this means that the average f(x + εx)φ(x) dx tends to γ). It can be shown that f(x )=γin D if and only if there exists a primitive of order k of f, i.e., F (k) = f, which is continuous in a neighborhood of x = x and satisfies lim x x k!(x x ) k F(x)=γ. This corresponds to the notion of generalized derivatives (see [13] and the references therein) used in the theory of trigonometric series well before the definition of Lojasiewicz and even before the introduction of the notion of distributions by Schwartz [1]. It turns out that the existence of distributional point values is equivalent to the existence in the Cesàro sense of the limits of certain partial sums of the corresponding Fourier series. Convergence in the Cesàro sense is also a kind of convergence Received by the editors May 2, 1994 and, in revised form, October 18, Mathematics Subject Classification. Primary 46F1, 42A24. c 1996 American Mathematical Society 125

2 126 RICARDO ESTRADA on the average and is defined as follows [6]: if f is an integrable function defined for x wesaythatf(x) tends to L in the (C, 1) sense as x +, 1 x and write lim x + F (x) =L(C, 1) if lim x + x F (t) dt = L. Convergence in the (C, k) sense, k =2,3,..., is defined recursively by lim x F (x) =L(C, k) 1 x if lim x + x F (t) dt = L (C, k 1). We say that F (x) convergestolin the Cesàro sense and write lim x + F (x) =L(C) if lim x + F (x) =L(C, k) for some k. The Cesàro convergence of a sequence {x n } can be defined similarly and it is equivalent to the Cesàro convergence of the function F defined by F (t) =x [[t]].in particular a series n=1 a n is Cesàro summable to the sum S, written as n=1 a n = n S (C), if lim n j=1 a j = S (C). A series a n is (C) summable to S if both series n= a n and n=1 a n are (C) summable to S 1 and S 2, respectively, with S = S 1 + S 2. A series a n is principal value Cesàro summable to S, written as p. v. a n n = S (C), if lim n j= n a j = S (C). Now let f S be a periodic distribution of period 2π and let a ne inθ be the associated Fourier series. Let θ R. Then the following two results are known [3, 12]: (1) If a ne inθ = γ (C), i.e., if the partial sums M n= N a ne inθ tend to γ in the Cesàro sense as N and M tend to infinity independently, then f(θ )=γ in D. The converse does not hold (f(θ) = n=2 einθ (2) If f(θ )=γin D,thenp.v. a ne inθ lim N N n= N The converse does not hold (f(θ) = Here we prove the following a n e inθ = γ (C). n=1 n log n,atθ=,isanexample). = γ (C), i.e., n sin nθ, atθ=,isanexample). Theorem. Let f S be a periodic distribution of period 2π and let a ne inθ be its Fourier series. Let θ R. Then (1.1) f(θ )=γ, in D, if and only if there exists k such that (1.2) for each a>. lim x + x n ax a n e inθ = γ, (C, k) Our approach is based on the theory of distributional asymptotic expansions [4, 5, 11] and is inspired by the work of Ramanujan [9] who was one of the first to study a sequence {a n } by studying the asymptotic behavior of series of the type n=1 a nφ(nε), as ε +,forsmoothφ. See also [1, 2]. Here we study the Fourier series a ne inθ by analysing the behavior as ε oftheseries a ne inθ φ(nε) forφ S. Notice that we use the standard notation concerning spaces of distributions and test functions [7, 1].

3 THE FOURIER SERIES OF A DISTRIBUTION Asymptotically homogeneous functions In this section we define and give the basic properties of the asymptotically homogeneous functions of degree. These functions play a central role in our analysis. Lemma 1. Let τ be a real-valued continuous function defined in an interval of the form [A, ) for some A R. Suppose (2.1) τ(ax) =a µ τ(x)+o(1), as x +, for each a>.ifµ<,then (2.2) τ(x)=o(1), as x +. Proof. Let ε>. Let x > be such that τ(2x) 2 µ τ(x) ε for x>x. Let M =max{ τ(x) : x x 2x }. An inductive argument shows that if x [2 n x, 2 n+1 x ], n =,1,2,...,then τ(x) 2 nµ M + n 1 j=1 2jµ ε. Therefore, lim x + τ(x) 2µ 1 2 εand (2.2) follows. µ The lemma does not hold if µ =. Indeed, there are functions like ln(ln x), ln x α, α<1, or cos ln x that satisfy τ(ax) =τ(x)+o(1), as x +, foreach a>, but which do not tend to zero at infinity. Definition. Let τ be a continuous function defined in an interval of the form [A, ) for some A R. We say that τ is asymptotically homogeneous of degree if for each a>wehave (2.3) τ(ax) =τ(x)+o(1), as x +. The asymptotically homogeneous functions of degree are related to the slowly oscillating functions [5], also known as regularly varying functions of order. These are positive functions that satisfy ρ(ax) =ρ(x)+o(ρ(x)), as x,foreach a >. However, the two concepts are different: ln x is slowly oscillating but not asymptotically homogeneous of degree while cos ln x is asymptotically homogeneous of degree but not slowly oscillating. Observe that the argument of the proof of Lemma 1 shows that if τ is an asymptotically homogeneous function of order, then τ(x) =o(ln x), as x +. Notice also that we did not ask for any uniform behavior with respect to a in (2.3). The fact that (2.3) holds uniformly on a [A, B] if[a, B] (, ) follows from the definition, as we shall see. Lemma 2. Let τ be an asymptotically homogeneous function of degree, continuous in [, ). LetHbe the Heaviside function. Then (2.4) τ(λx)h(x) =τ(λ)h(x)+o(1), as λ, in S. If [A, B] (, ), then(2.3) holds uniformly for a [A, B]. Proof. Suppose first that τ is bounded in [, ). Then if φ S we can apply the Lebesgue dominated convergence theorem to obtain lim λ (τ(λx) τ(λ))φ(x) dx =. This is (2.4). The uniform convergence follows from the distributional formula (2.4). Indeed, weak convergence in S implies strong convergence [1]. Thus if K is a

4 128 RICARDO ESTRADA compact subset of S, then τ(λx)h(x) τ(λ)h(x),φ(x) = o(1) uniformly for φ K. Let φ S be a function that satisfies φ (x) dx = 1. Then if [A, B] (, ) thesetk={a 1 φ (a 1 x):a [A, B]} is a compact set of S. Then τ(λx)h(x),φ (x) =τ(λ)+o(1) as λ,andsoτ(λa) = τ(λax),φ (x) + o(1) = τ(λx),a 1 φ (a 1 x) +o(1) = τ(λ)+o(1) uniformly for a [A, B]. Let us now return to the general case when τ is not necessarily bounded. We shall first show that if [A, B] (, ), then τ(ax) =τ(x)+o(1), as x +, uniformly on a [A, B]. Observe first that the functions cos τ(x) andsinτ(x) are bounded asymptotically homogeneous functions. By what we have already proven it follows that if [A, B] (, ), then e iτ (ax) = e iτ (x) + o(1), as x, uniformly on a [A, B]. Let ε>. Suppose ε<πand A<1<B. There exists x > such that e iτ (ax) e iτ (x) 1 e iε for x x and a [A, B]. For each x x the set {τ(ax) :A a B}is a connected set contained in [τ(x) ε +2nπ, τ(x) +ε+2nπ] and it follows that it is contained in the component that contains τ(x); that is, τ(ax) τ(x) ε,fora [A, B]. To prove (2.4) it would be enough to prove that there are constants A,A 1 such that τ(λx) τ(λ) A ln x + A 1 for x>andλ>λ for then the dominated convergence theorem could be invoked again. Let λ > be such that τ(λx) τ(λ) 1ifλ λ and x [1/2, 2]. Then it follows by induction that τ(λx) τ(λ) n+1ifx [2 n, 2 n+1 ],λ λ, n = ln x,1,2... Therefore τ(λx) τ(λ) ln 2 +1 if x 1,λ λ. Proceeding similarly, ln x ln if x [ 2, 1 n+1 2 ],λ 2 n λ n, n=,1,2,...,then τ(λx) τ(λ) n+1 Recall now that τ(x) =o(ln x), as x. Then we can find constants M,M 1 such 1 that τ(x) M ln x + M 1,x>. Therefore, if x [ 2, 1 n+1 2 ] but λ<2 n λ n,then λ<λ /x and so τ(λx) τ(λ) 2(M ln λ +M 1 ) 2(M ln x +M ln λ +M 1 ). Summarizing, if A =max{2m,1/ln 2},A 1 =max{2(m ln λ + M 1 ), 1}, then τ(λx) τ(λ) A ln x + A 1 for x>andλ λ. The asymptotically homogeneous functions of degree do not have to be smooth, i.e., C. However, we have Lemma 3. Let τ be an asymptotically homogeneous function of degree, continuous in [, ). Then there exists a function σ, asymptotically homogeneous of degree, smoothin[, ), such that (2.5) τ(x) =σ(x)+o(1), as x. Proof. Define σ(λ) = τ(λx)φ (x) dx, λ 1, where φ Ssatisfies φ (x) dx = 1, and extend to [, + ) in any smooth way. Then (2.4) gives (2.5). 3. Primitives of a distributionally null sequence If {f n } is a sequence of continuous functions that converge uniformly to zero on an interval of the form [ A, A], then the sequence of primitives { x f n(t) dt} also converges uniformly to zero while, in general, the sequence of derivatives {f n}, even if defined, does not. On the other hand, the situation with the distributional convergence is the opposite: if f n ins,thenalsof n ins but the sequence of primitives { x f n(t) dt}, even if defined, might be divergent. We now turn our attention to the study of this last problem. Let F S. If F is integrable near x =, then we can define the primitive F (t) dt. If F is more singular near x =, then there is no canonical way to x

5 THE FOURIER SERIES OF A DISTRIBUTION 129 define x F (t) dt, that is, there is no canonical way to single out a primitive of F that vanishes at x =. However, if F is locally even near x =,ithasa unique locally odd primitive, which we denote as x F (t) dt. Observe that with this notation x δ(t) dt = 1 2 sgn x, wheresgnx=x/ x,x, is the sign function. We shall use the notation x F (t) dt so long as F = F + F 1,whereF is locally integrable near x =andwheref 1 is locally even. Let {F n } n=1 be a sequence of distributions of S. Suppose that lim n F n = in S. Then [1] there are primitives of the F n that also tend to zero. In particular, if x F n(t) dt is defined for each n, there are constants c n such that x F n(t) dt = c n + o(1), as n in S. The example F n (x) = 2nxe x2 (1 e x2 ) n 1, x F n(t) dt = 1 (1 e x2 ) n =1+o(1) shows that the c n s cannot be replaced by, in general. Observe also that if the F λ depend smoothly on the parameter λ and F λ = o(1), as λ,then x F λ(t)dt = σ(λ)+o(1), where σ is smooth. Lemma 4. Let F S be a Radon measure such that x F (t) dt is defined. Define the distributions F n, n 1, recursively by F n (x) = x F n 1(t)dt, n 1. Suppose (3.1) F (λx) =o(1/λ), as λ +, in S. Then there exists an asymptotically homogeneous function of degree,σ(λ),such that F n (λx) = λn 1 x n 1 σ(λ) (3.2) + o(λ n 1 ), as λ +, in S, (n 1)! for n 1. There exists n such that the convergence in (3.2) is uniform on compacts for n n. Conversely, if (3.2) holds for some n 1, thenf (λx) =o(1/λ) in S. Proof. Suppose F (λx) =o(1/λ) ins. Then there exists a smooth function σ(λ) such that F 1 (λx) =σ(λ)+o(1), as λ,ins. Replacing λx by λxa and grouping in two different ways, we obtain σ(aλ) =σ(λ)+o(1), as λ for each a>. Thus σ is asymptotically homogeneous of degree. Hence (3.2) holds for n = 1. Suppose now it holds for some n 1. Then integrating again we obtain F n+1 (λx) =λ n x n σ(λ)/n! +ρ(λ)+o(λ n ), as λ, for some function ρ. Evaluating at λax thus yields ρ(λa) =ρ(λ)+o(λ n ) and thus by Lemma 1, applied to λ n ρ(λ), it follows that ρ(λ) =o(λ n ) and (3.2) is obtained for n +1. That the convergence in (3.2) is uniform for x in compacts if n is large follows by the definition of the convergence of distributions. The converse is obtained by differentiating (3.2) n times with respect to x. Observe that if F is even, then F 1 is odd and thus σ(λ) =o(1), as λ,and (3.2) becomes F n (λx) =o(λ n 1 ), as λ. The same conclusion is obtained if supp F [, ). The sequence of functions {F n } n= is also related to Cesàro summability. The following lemma is an immediate corollary of the results proved in [6, p. 11]. Lemma 5. Let F be a function defined for x>that, suitably extended to R, defines an element of S for which x F (t) dt is defined. Then lim x + F (x) =γ (C, n) if and only if lim x n! x n F n (x) =γ. 4. The main result In this section we apply the results of the previous sections to characterize the Fourier series of the periodic distributions having a distributional point value.

6 121 RICARDO ESTRADA Lemma 6. Let f S be a periodic distribution of period 2π and let a ne inθ be its Fourier series. Let θ R. Then (4.1) if and only if f(θ )=γ, in D, (4.2) Proof. f(θ )=γ, in D a n e inθ δ(λx n) = γδ(x) λ + o(1/λ), as λ, in S. lim f(θ + εθ),φ(θ) = γ,φ(θ) φ D ε lim f(θ + εθ),φ(θ) = γ,φ(θ) φ S ε lim a n e inθ e inεθ,φ(θ) =γ φ(x) dx ε lim ε lim ε lim ε a n e inθ ˆφ(nε) =γˆφ() a n e inθ ψ(nε) =γψ() φ S ψ S a n e inθ δ(x nε) =γδ(x) in S a n e inθ δ(λx n) = γδ(x) λ φ S + o(1/λ), as λ in S. We are now ready to give our main result. Theorem. Let f S be a periodic distribution of period 2π and let a ne inθ be its Fourier series. Let θ R. Then (4.3) f(θ )=γ, in D, if and only if there exists k such that (4.4) lim a n e inθ = γ (C, k) x x n ax for each a>. Proof. Let F (x) = a ne inθ δ(x n) and define F 1,F 2,... recursively by F n+1 (x) = x F n(t)dt. Leta>, put G (x) =G (a, x) = x n ax a ne inθ and define G 1,G 2,... recursively by G n+1 (x) = x G n(t)dt. Observe that (4.4) means that lim x k! x k G k (x) =γ. Suppose first that f(θ )=γ.thenf (λx) =γδ(λx)+o(1/λ), as λ,ins. Using Lemma 4, there exists an asymptotically homogeneous function of degree such that if n 1, then F n (λx) = γsgn(λx)(λx)n 1 2(n 1)! + σ(λ)(λx)n 1 (n 1)! + o(λ n 1 ), as λ, in S

7 THE FOURIER SERIES OF A DISTRIBUTION 1211 and there exists n such that if n n this holds uniformly on x [ A, A] for A>. Thus, if n n, G n 1 (x) =a 1 n F n (ax) ( 1) 1 n F n ( x) = γxn 1 2(n 1)! + σ(x) (n 1)! + γ 2(n 1)! σ(x) (n 1)! + o(xn 1 ) = γxn 1 (n 1)! + o(xn 1 ) and (4.4) follows with k = n 1. Conversely, suppose (4.4) holds. Let n = k +1,sothat lim (n 1)! x x1 n G n 1 (x) =γ. Define τ(x) =(n 1)! x 1 n F n (x) γ/2. Then τ is asymptotically homogeneous of degree. Thus there exists a smooth asymptotically homogeneous function of degree such that τ(x) =σ(x)+o(1), as x. It follows that γsgn xxn 1 F n (x) = 2(n 1)! and therefore, by Lemma 2, + σ(x)xn 1 (n 1)! + o(x n 1 ), as x, F n (λx) = γsgn(λx)(λx)n 1 2(n 1)! + σ(λ)(λx)n 1 (n 1)! + o(λ n 1 ), as λ, in S. Differentiating n times we obtain F (λx) =γδ(λx)+o(1/λ), as λ, as required. It is interesting to observe that (4.4) holds uniformly on a [A, B] if[a, B] (, ) but that it is not necessary to assume such uniform behavior to obtain (4.3). Notice also that the theorem remains valid if (4.4) holds uniformly for a H where H is a set dense in some interval, H =[A, B], < A < B <. In particular, f(θ )=γif and only if (4.5) lim [[N/q]] N n= [[N/p]] a n e inθ = γ (C, k) for each p, q {1,2,3,...}, uniformly if A<p/q<Bfor [A, B] (, ). Observe that (4.5) considers the convergence, in the Cesàro sense, of sequences. The following consequences are worth recording. Corollary 1. If f is symmetric about θ = θ, i.e., f(θ θ )=f(θ θ),then f(θ )=γ in D if and only if a ne inθ = γ (C). Corollary 2. If f is antisymmetric about θ = θ, i.e., f(θ θ )= f(θ θ),then f(θ )=γin D if and only if there is a function σ, asymptotically homogeneous of degree, such that N n=1 a ne inθ = σ(n)+o(1) (C), asn. In this case γ =. Corollary 3. If the Fourier series of f is of the power series type, i.e., f(θ) = n= a ne inθ,thenf(θ )=γ in D if and only if n= a ne inθ = γ (C).

8 1212 RICARDO ESTRADA References 1. B. C. Berndt and R. J. Evans, Extensions of asymptotic expansions from Chapter 15 of Ramanujan s second notebook, J. Reine Angew. Math. 361 (1985), MR 87b: R. Estrada, The asymptotic expansion of certain series considered by Ramanujan, Appl. Anal. 43 (1992), MR 95i: , Valores puntuales distribucionales de series de Fourier, Memorias II Encuentro Centroamericano de Matemáticos, San Ramón, Costa Rica, R. Estrada and R. P. Kanwal, Asymptotic separation of variables, J. Math. Anal. Appl. 178 (1993), MR 94g: , Asymptotic analysi: A distributional approach, Birkhäuser, Boston, MR 95g: G. H. Hardy, Divergent series, Clarendon Press, Oxford, MR 11:25a 7. R. P. Kanwal, Generalized functions: Theory and technique, Academic Press, New York, MR 85f: S. Lojasiewicz, Sur la valeur et la limite d une distribution en un point, Studia Math. 16 (1957), MR 19:433d 9. S. Ramanujan, Notebooks, 2 vols., Bombay, MR 2: L. Schwartz, Théorie des distributions Hermann, Paris, MR 35: V. S. Vladimirov, Y. N. Drozhinov, and B. I. Zavyalov Multidimensional Tauberian theorems for generalized functions, Nauka, Moscow, MR 87m: G. Walter, Pointwise convergence of distributions, Studia Math. 26 (1966), MR 32: A. Zygmund, Trigonometric series, 2 vols., Cambridge Univ. Press, Cambridge and New York, MR 21:6498 Department of Mathematics, Texas A & M University, College Station, Texas Current address: P. O. Box 276, Tres Ríos, Costa Rica address: restrada@cariari.ucr.ac.cr

A DISTRIBUTIONAL VERSION OF THE FERENC LUKÁCS THEOREM

A DISTRIBUTIONAL VERSION OF THE FERENC LUKÁCS THEOREM SARAJEVO JOURNAL OF MATHEMATICS Vol.1 (13) (2005), 75 92 A DISTRIBUTIONAL VERSION OF THE FERENC LUKÁCS THEOREM RICARDO ESTRADA Abstract. The theorem of F. Lukács determines the generalized jumps of a periodic,

More information

In: Proceedings of the Edinburgh Mathematical Society (Series 2), 53 (1), , 2010

In: Proceedings of the Edinburgh Mathematical Society (Series 2), 53 (1), , 2010 biblio.ugent.be The UGent Institutional Repository is the electronic archiving and dissemination platform for all UGent research publications. Ghent University has implemented a mandate stipulating that

More information

R. Estrada and J. Vindas ON DISTRIBUTIONAL POINT VALUES AND BOUNDARY VALUES OF ANALYTIC FUNCTIONS

R. Estrada and J. Vindas ON DISTRIBUTIONAL POINT VALUES AND BOUNDARY VALUES OF ANALYTIC FUNCTIONS Rend. Sem. Mat. Univ. Politec. Torino Vol. 70, 2 (2012), 121 126 R. Estrada and J. Vindas ON DISTRIBUTIONAL POINT VALUES AND BOUNDARY VALUES OF ANALYTIC FUNCTIONS Abstract. We give the following version

More information

JASSON VINDAS AND RICARDO ESTRADA

JASSON VINDAS AND RICARDO ESTRADA A QUICK DISTRIBUTIONAL WAY TO THE PRIME NUMBER THEOREM JASSON VINDAS AND RICARDO ESTRADA Abstract. We use distribution theory (generalized functions) to show the prime number theorem. No tauberian results

More information

Characterization of Distributional Point Values of Tempered Distribution and Pointwise Fourier Inversion Formula

Characterization of Distributional Point Values of Tempered Distribution and Pointwise Fourier Inversion Formula Characterization of Distributional Point Values of Tempered Distribution and Pointwise Fourier Inversion Formula Jasson Vindas jvindas@math.lsu.edu Louisiana State University Seminar of Analysis and Fundations

More information

WAVELET EXPANSIONS OF DISTRIBUTIONS

WAVELET EXPANSIONS OF DISTRIBUTIONS WAVELET EXPANSIONS OF DISTRIBUTIONS JASSON VINDAS Abstract. These are lecture notes of a talk at the School of Mathematics of the National University of Costa Rica. The aim is to present a wavelet expansion

More information

Czechoslovak Mathematical Journal

Czechoslovak Mathematical Journal Czechoslovak Mathematical Journal Oktay Duman; Cihan Orhan µ-statistically convergent function sequences Czechoslovak Mathematical Journal, Vol. 54 (2004), No. 2, 413 422 Persistent URL: http://dml.cz/dmlcz/127899

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

APPLICATIONS OF THE THICK DISTRIBUTIONAL CALCULUS

APPLICATIONS OF THE THICK DISTRIBUTIONAL CALCULUS Novi Sad J. Math. Vol. 44, No. 2, 2014, 121-135 APPLICATIONS OF THE THICK DISTRIBUTIONAL CALCULUS Ricardo Estrada 1 and Yunyun Yang 2 Abstract. We give several applications of the thick distributional

More information

CALCULUS JIA-MING (FRANK) LIOU

CALCULUS JIA-MING (FRANK) LIOU CALCULUS JIA-MING (FRANK) LIOU Abstract. Contents. Power Series.. Polynomials and Formal Power Series.2. Radius of Convergence 2.3. Derivative and Antiderivative of Power Series 4.4. Power Series Expansion

More information

We denote the space of distributions on Ω by D ( Ω) 2.

We denote the space of distributions on Ω by D ( Ω) 2. Sep. 1 0, 008 Distributions Distributions are generalized functions. Some familiarity with the theory of distributions helps understanding of various function spaces which play important roles in the study

More information

LOCAL BEHAVIOR OF DISTRIBUTIONS AND APPLICATIONS

LOCAL BEHAVIOR OF DISTRIBUTIONS AND APPLICATIONS LOCAL BEHAVIOR OF DISTRIBUTIONS AND APPLICATIONS A Dissertation Submitted to the Graduate Faculty of the Louisiana State University and Agricultural and Mechanical College in partial fulfillment of the

More information

Riemann integral and volume are generalized to unbounded functions and sets. is an admissible set, and its volume is a Riemann integral, 1l E,

Riemann integral and volume are generalized to unbounded functions and sets. is an admissible set, and its volume is a Riemann integral, 1l E, Tel Aviv University, 26 Analysis-III 9 9 Improper integral 9a Introduction....................... 9 9b Positive integrands................... 9c Special functions gamma and beta......... 4 9d Change of

More information

Universally divergent Fourier series via Landau s extremal functions

Universally divergent Fourier series via Landau s extremal functions Comment.Math.Univ.Carolin. 56,2(2015) 159 168 159 Universally divergent Fourier series via Landau s extremal functions Gerd Herzog, Peer Chr. Kunstmann Abstract. We prove the existence of functions f A(D),

More information

A Result on the Neutrix Composition of the Delta Function

A Result on the Neutrix Composition of the Delta Function Advances in Dynamical Systems and Applications ISSN 973-5321, Volume 6, Number 1, pp. 49 56 (211) http://campus.mst.edu/adsa A Result on the Neutrix Composition of the Delta Function Brian Fisher Department

More information

BOUNDARY PROPERTIES OF FIRST-ORDER PARTIAL DERIVATIVES OF THE POISSON INTEGRAL FOR THE HALF-SPACE R + k+1. (k > 1)

BOUNDARY PROPERTIES OF FIRST-ORDER PARTIAL DERIVATIVES OF THE POISSON INTEGRAL FOR THE HALF-SPACE R + k+1. (k > 1) GEORGIAN MATHEMATICAL JOURNAL: Vol. 4, No. 6, 1997, 585-6 BOUNDARY PROPERTIES OF FIRST-ORDER PARTIAL DERIVATIVES OF THE POISSON INTEGRAL FOR THE HALF-SPACE R + k+1 (k > 1) S. TOPURIA Abstract. Boundary

More information

be the set of complex valued 2π-periodic functions f on R such that

be the set of complex valued 2π-periodic functions f on R such that . Fourier series. Definition.. Given a real number P, we say a complex valued function f on R is P -periodic if f(x + P ) f(x) for all x R. We let be the set of complex valued -periodic functions f on

More information

ASYMPTOTIC STRUCTURE FOR SOLUTIONS OF THE NAVIER STOKES EQUATIONS. Tian Ma. Shouhong Wang

ASYMPTOTIC STRUCTURE FOR SOLUTIONS OF THE NAVIER STOKES EQUATIONS. Tian Ma. Shouhong Wang DISCRETE AND CONTINUOUS Website: http://aimsciences.org DYNAMICAL SYSTEMS Volume 11, Number 1, July 004 pp. 189 04 ASYMPTOTIC STRUCTURE FOR SOLUTIONS OF THE NAVIER STOKES EQUATIONS Tian Ma Department of

More information

STRONG MOMENT PROBLEMS FOR RAPIDLY DECREASING SMOOTH FUNCTIONS

STRONG MOMENT PROBLEMS FOR RAPIDLY DECREASING SMOOTH FUNCTIONS proceedings of the american mathematical society Volume 120, Number 2, February 1994 STRONG MOMENT PROBLEMS FOR RAPIDLY DECREASING SMOOTH FUNCTIONS ANA LIA DURAN AND RICARDO ESTRADA (Communicated by J.

More information

An Abel-Tauber theorem for Fourier sine transforms

An Abel-Tauber theorem for Fourier sine transforms J. Math. Sci. Univ. Tokyo 2 (1995), 33 39. An Abel-Tauber theorem for Fourier sine transforms By Akihiko Inoue Abstract. We prove an Abel-Tauber theorem for Fourier sine transforms. It can be considered

More information

Distributional asymptotic expansions of spectral functions and of the associated Green kernels

Distributional asymptotic expansions of spectral functions and of the associated Green kernels Electronic Journal of Differential Equations, Vol. 1999(1999), No. 07, pp. 1 37. ISSN: 1072-6691. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu ftp ejde.math.unt.edu (login:

More information

A Note on the 2 F 1 Hypergeometric Function

A Note on the 2 F 1 Hypergeometric Function A Note on the F 1 Hypergeometric Function Armen Bagdasaryan Institution of the Russian Academy of Sciences, V.A. Trapeznikov Institute for Control Sciences 65 Profsoyuznaya, 117997, Moscow, Russia E-mail:

More information

ON THE CLASS OF SATURATION IN THE THEORY OF APPROXIMATION II" GEN-ICHIRO SUNOUCHI

ON THE CLASS OF SATURATION IN THE THEORY OF APPROXIMATION II GEN-ICHIRO SUNOUCHI ON THE CLASS OF SATURATION IN THE THEORY OF APPROXIMATION II" GEN-ICHIRO SUNOUCHI (Received July 20,1960) 1. Introduction. We have already determined the class of saturation for various methods of summation

More information

Journal of Inequalities in Pure and Applied Mathematics

Journal of Inequalities in Pure and Applied Mathematics Journal of Inequalities in Pure and Applied Mathematics NEWER APPLICATIONS OF GENERALIZED MONOTONE SEQUENCES L. LEINDLER Bolyai Institute, University of Szeged, Aradi vértanúk tere 1 H-6720 Szeged, Hungary

More information

Math 4263 Homework Set 1

Math 4263 Homework Set 1 Homework Set 1 1. Solve the following PDE/BVP 2. Solve the following PDE/BVP 2u t + 3u x = 0 u (x, 0) = sin (x) u x + e x u y = 0 u (0, y) = y 2 3. (a) Find the curves γ : t (x (t), y (t)) such that that

More information

MATH 220: INNER PRODUCT SPACES, SYMMETRIC OPERATORS, ORTHOGONALITY

MATH 220: INNER PRODUCT SPACES, SYMMETRIC OPERATORS, ORTHOGONALITY MATH 22: INNER PRODUCT SPACES, SYMMETRIC OPERATORS, ORTHOGONALITY When discussing separation of variables, we noted that at the last step we need to express the inhomogeneous initial or boundary data as

More information

FOURIER SERIES WITH THE CONTINUOUS PRIMITIVE INTEGRAL

FOURIER SERIES WITH THE CONTINUOUS PRIMITIVE INTEGRAL Real Analysis Exchange Summer Symposium XXXVI, 2012, pp. 30 35 Erik Talvila, Department of Mathematics and Statistics, University of the Fraser Valley, Chilliwack, BC V2R 0N3, Canada. email: Erik.Talvila@ufv.ca

More information

Remarks on various generalized derivatives

Remarks on various generalized derivatives Remarks on various generalized derivatives J. Marshall Ash Department of Mathematics, DePaul University Chicago, IL 60614, USA mash@math.depaul.edu Acknowledgement. This paper is dedicated to Calixto Calderón.

More information

ON THE GROWTH OF ENTIRE FUNCTIONS WITH ZERO SETS HAVING INFINITE EXPONENT OF CONVERGENCE

ON THE GROWTH OF ENTIRE FUNCTIONS WITH ZERO SETS HAVING INFINITE EXPONENT OF CONVERGENCE Annales Academiæ Scientiarum Fennicæ Mathematica Volumen 7, 00, 69 90 ON THE GROWTH OF ENTIRE FUNCTIONS WITH ZERO SETS HAVING INFINITE EXPONENT OF CONVERGENCE Joseph Miles University of Illinois, Department

More information

A CLASS OF M-DILATION SCALING FUNCTIONS WITH REGULARITY GROWING PROPORTIONALLY TO FILTER SUPPORT WIDTH

A CLASS OF M-DILATION SCALING FUNCTIONS WITH REGULARITY GROWING PROPORTIONALLY TO FILTER SUPPORT WIDTH PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 26, Number 2, December 998, Pages 350 3506 S 0002-9939(98)05070-9 A CLASS OF M-DILATION SCALING FUNCTIONS WITH REGULARITY GROWING PROPORTIONALLY

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

OSCILLATORY SINGULAR INTEGRALS ON L p AND HARDY SPACES

OSCILLATORY SINGULAR INTEGRALS ON L p AND HARDY SPACES POCEEDINGS OF THE AMEICAN MATHEMATICAL SOCIETY Volume 24, Number 9, September 996 OSCILLATOY SINGULA INTEGALS ON L p AND HADY SPACES YIBIAO PAN (Communicated by J. Marshall Ash) Abstract. We consider boundedness

More information

International Journal of Pure and Applied Mathematics Volume 60 No ,

International Journal of Pure and Applied Mathematics Volume 60 No , International Journal of Pure and Applied Mathematics Volume 60 No. 3 200, 259-267 ON CERTAIN CLASS OF SZÁSZ-MIRAKYAN OPERATORS IN EXPONENTIAL WEIGHT SPACES Lucyna Rempulska, Szymon Graczyk 2,2 Institute

More information

Multidimensional Riemann derivatives

Multidimensional Riemann derivatives STUDIA MATHEMATICA 235 (1) (2016) Multidimensional Riemann derivatives by J. Marshall Ash and Stefan Catoiu (Chicago, IL) Abstract. The well-known concepts of nth Peano, Lipschitz, Riemann, Riemann Lipschitz,

More information

Fourier Series. 1. Review of Linear Algebra

Fourier Series. 1. Review of Linear Algebra Fourier Series In this section we give a short introduction to Fourier Analysis. If you are interested in Fourier analysis and would like to know more detail, I highly recommend the following book: Fourier

More information

Fourier Series. ,..., e ixn ). Conversely, each 2π-periodic function φ : R n C induces a unique φ : T n C for which φ(e ix 1

Fourier Series. ,..., e ixn ). Conversely, each 2π-periodic function φ : R n C induces a unique φ : T n C for which φ(e ix 1 Fourier Series Let {e j : 1 j n} be the standard basis in R n. We say f : R n C is π-periodic in each variable if f(x + πe j ) = f(x) x R n, 1 j n. We can identify π-periodic functions with functions on

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

Hausdorff operators in H p spaces, 0 < p < 1

Hausdorff operators in H p spaces, 0 < p < 1 Hausdorff operators in H p spaces, 0 < p < 1 Elijah Liflyand joint work with Akihiko Miyachi Bar-Ilan University June, 2018 Elijah Liflyand joint work with Akihiko Miyachi (Bar-Ilan University) Hausdorff

More information

11.8 Power Series. Recall the geometric series. (1) x n = 1+x+x 2 + +x n +

11.8 Power Series. Recall the geometric series. (1) x n = 1+x+x 2 + +x n + 11.8 1 11.8 Power Series Recall the geometric series (1) x n 1+x+x 2 + +x n + n As we saw in section 11.2, the series (1) diverges if the common ratio x > 1 and converges if x < 1. In fact, for all x (

More information

A CENTURY OF TAUBERIAN THEORY. david borwein

A CENTURY OF TAUBERIAN THEORY. david borwein A CENTURY OF TAUBERIAN THEORY david borwein Abstract. A narrow path is cut through the jungle of results which started with Tauber s corrected converse of Abel s theorem that if a n = l, then a n x n l

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

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

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

2 (Bonus). Let A X consist of points (x, y) such that either x or y is a rational number. Is A measurable? What is its Lebesgue measure?

2 (Bonus). Let A X consist of points (x, y) such that either x or y is a rational number. Is A measurable? What is its Lebesgue measure? MA 645-4A (Real Analysis), Dr. Chernov Homework assignment 1 (Due 9/5). Prove that every countable set A is measurable and µ(a) = 0. 2 (Bonus). Let A consist of points (x, y) such that either x or y is

More information

Uniform convergence of N-dimensional Walsh Fourier series

Uniform convergence of N-dimensional Walsh Fourier series STUDIA MATHEMATICA 68 2005 Uniform convergence of N-dimensional Walsh Fourier series by U. Goginava Tbilisi Abstract. We establish conditions on the partial moduli of continuity which guarantee uniform

More information

MATH. 4548, Autumn 15, MWF 12:40 p.m. QUIZ 1 September 4, 2015 PRINT NAME A. Derdzinski Show all work. No calculators. The problem is worth 10 points.

MATH. 4548, Autumn 15, MWF 12:40 p.m. QUIZ 1 September 4, 2015 PRINT NAME A. Derdzinski Show all work. No calculators. The problem is worth 10 points. MATH. 4548, Autumn 15, MWF 12:40 p.m. QUIZ 1 September 4, 2015 PRINT NAME A. Derdzinski Show all work. No calculators. The problem is worth 10 points. 1. Let f : (, 0) IR be given by f(x) = 1/x 2. Prove

More information

Convergence of greedy approximation I. General systems

Convergence of greedy approximation I. General systems STUDIA MATHEMATICA 159 (1) (2003) Convergence of greedy approximation I. General systems by S. V. Konyagin (Moscow) and V. N. Temlyakov (Columbia, SC) Abstract. We consider convergence of thresholding

More information

On the distributional divergence of vector fields vanishing at infinity

On the distributional divergence of vector fields vanishing at infinity Proceedings of the Royal Society of Edinburgh, 141A, 65 76, 2011 On the distributional divergence of vector fields vanishing at infinity Thierry De Pauw Institut de Recherches en Mathématiques et Physique,

More information

1.1 Appearance of Fourier series

1.1 Appearance of Fourier series Chapter Fourier series. Appearance of Fourier series The birth of Fourier series can be traced back to the solutions of wave equation in the work of Bernoulli and the heat equation in the work of Fourier.

More information

NECESSARY CONDITIONS FOR WEIGHTED POINTWISE HARDY INEQUALITIES

NECESSARY CONDITIONS FOR WEIGHTED POINTWISE HARDY INEQUALITIES NECESSARY CONDITIONS FOR WEIGHTED POINTWISE HARDY INEQUALITIES JUHA LEHRBÄCK Abstract. We establish necessary conditions for domains Ω R n which admit the pointwise (p, β)-hardy inequality u(x) Cd Ω(x)

More information

PERIODIC HYPERFUNCTIONS AND FOURIER SERIES

PERIODIC HYPERFUNCTIONS AND FOURIER SERIES PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 128, Number 8, Pages 2421 2430 S 0002-9939(99)05281-8 Article electronically published on December 7, 1999 PERIODIC HYPERFUNCTIONS AND FOURIER SERIES

More information

Measure and Integration: Solutions of CW2

Measure and Integration: Solutions of CW2 Measure and Integration: s of CW2 Fall 206 [G. Holzegel] December 9, 206 Problem of Sheet 5 a) Left (f n ) and (g n ) be sequences of integrable functions with f n (x) f (x) and g n (x) g (x) for almost

More information

8.1 Sequences. Example: A sequence is a function f(n) whose domain is a subset of the integers. Notation: *Note: n = 0 vs. n = 1.

8.1 Sequences. Example: A sequence is a function f(n) whose domain is a subset of the integers. Notation: *Note: n = 0 vs. n = 1. 8. Sequences Example: A sequence is a function f(n) whose domain is a subset of the integers. Notation: *Note: n = 0 vs. n = Examples: 6. Find a formula for the general term a n of the sequence, assuming

More information

Stieltjes Transformation as the Iterated Laplace Transformation

Stieltjes Transformation as the Iterated Laplace Transformation International Journal of Mathematical Analysis Vol. 11, 2017, no. 17, 833-838 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ijma.2017.7796 Stieltjes Transformation as the Iterated Laplace Transformation

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

I and I convergent function sequences

I and I convergent function sequences Mathematical Communications 10(2005), 71-80 71 I and I convergent function sequences F. Gezer and S. Karakuş Abstract. In this paper, we introduce the concepts of I pointwise convergence, I uniform convergence,

More information

Math 321 Final Examination April 1995 Notation used in this exam: N. (1) S N (f,x) = f(t)e int dt e inx.

Math 321 Final Examination April 1995 Notation used in this exam: N. (1) S N (f,x) = f(t)e int dt e inx. Math 321 Final Examination April 1995 Notation used in this exam: N 1 π (1) S N (f,x) = f(t)e int dt e inx. 2π n= N π (2) C(X, R) is the space of bounded real-valued functions on the metric space X, equipped

More information

Power Series. Part 1. J. Gonzalez-Zugasti, University of Massachusetts - Lowell

Power Series. Part 1. J. Gonzalez-Zugasti, University of Massachusetts - Lowell Power Series Part 1 1 Power Series Suppose x is a variable and c k & a are constants. A power series about x = 0 is c k x k A power series about x = a is c k x a k a = center of the power series c k =

More information

GENERAL STIELTJES MOMENT PROBLEMS FOR RAPIDLY DECREASING SMOOTH FUNCTIONS

GENERAL STIELTJES MOMENT PROBLEMS FOR RAPIDLY DECREASING SMOOTH FUNCTIONS GENERAL STIELTJES MOMENT PROBLEMS FOR RAPIDLY DECREASING SMOOTH FUNCTIONS RICARDO ESTRADA AND JASSON VINDAS Abstract. We give (necessary and sufficient) conditions over a sequence {f n } n= of functions

More information

1 Continuity Classes C m (Ω)

1 Continuity Classes C m (Ω) 0.1 Norms 0.1 Norms A norm on a linear space X is a function : X R with the properties: Positive Definite: x 0 x X (nonnegative) x = 0 x = 0 (strictly positive) λx = λ x x X, λ C(homogeneous) x + y x +

More information

A NOTE ON WEAK CONVERGENCE OF SINGULAR INTEGRALS IN METRIC SPACES

A NOTE ON WEAK CONVERGENCE OF SINGULAR INTEGRALS IN METRIC SPACES A NOTE ON WEAK CONVERGENCE OF SINGULAR INTEGRALS IN METRIC SPACES VASILIS CHOUSIONIS AND MARIUSZ URBAŃSKI Abstract. We prove that in any metric space (X, d) the singular integral operators Tµ,ε(f)(x) k

More information

WEIGHTED REVERSE WEAK TYPE INEQUALITY FOR GENERAL MAXIMAL FUNCTIONS

WEIGHTED REVERSE WEAK TYPE INEQUALITY FOR GENERAL MAXIMAL FUNCTIONS GEORGIAN MATHEMATICAL JOURNAL: Vol. 2, No. 3, 995, 277-290 WEIGHTED REVERSE WEAK TYPE INEQUALITY FOR GENERAL MAXIMAL FUNCTIONS J. GENEBASHVILI Abstract. Necessary and sufficient conditions are found to

More information

CONVERGENCE OF THE STEEPEST DESCENT METHOD FOR ACCRETIVE OPERATORS

CONVERGENCE OF THE STEEPEST DESCENT METHOD FOR ACCRETIVE OPERATORS PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 127, Number 12, Pages 3677 3683 S 0002-9939(99)04975-8 Article electronically published on May 11, 1999 CONVERGENCE OF THE STEEPEST DESCENT METHOD

More information

Singular Integrals. 1 Calderon-Zygmund decomposition

Singular Integrals. 1 Calderon-Zygmund decomposition Singular Integrals Analysis III Calderon-Zygmund decomposition Let f be an integrable function f dx 0, f = g + b with g Cα almost everywhere, with b

More information

An introduction to Mathematical Theory of Control

An introduction to Mathematical Theory of Control An introduction to Mathematical Theory of Control Vasile Staicu University of Aveiro UNICA, May 2018 Vasile Staicu (University of Aveiro) An introduction to Mathematical Theory of Control UNICA, May 2018

More information

Average theorem, Restriction theorem and Strichartz estimates

Average theorem, Restriction theorem and Strichartz estimates Average theorem, Restriction theorem and trichartz estimates 2 August 27 Abstract We provide the details of the proof of the average theorem and the restriction theorem. Emphasis has been placed on the

More information

A global solution curve for a class of free boundary value problems arising in plasma physics

A global solution curve for a class of free boundary value problems arising in plasma physics A global solution curve for a class of free boundary value problems arising in plasma physics Philip Korman epartment of Mathematical Sciences University of Cincinnati Cincinnati Ohio 4522-0025 Abstract

More information

Fourier Sin and Cos Series and Least Squares Convergence

Fourier Sin and Cos Series and Least Squares Convergence Fourier and east Squares Convergence James K. Peterson Department of Biological Sciences and Department of Mathematical Sciences Clemson University May 7, 28 Outline et s look at the original Fourier sin

More information

arxiv: v1 [math.ca] 31 Dec 2018

arxiv: v1 [math.ca] 31 Dec 2018 arxiv:181.1173v1 [math.ca] 31 Dec 18 Some trigonometric integrals and the Fourier transform of a spherically symmetric exponential function Hideshi YAMANE Department of Mathematical Sciences, Kwansei Gakuin

More information

Stability of Adjointable Mappings in Hilbert

Stability of Adjointable Mappings in Hilbert Stability of Adjointable Mappings in Hilbert arxiv:math/0501139v2 [math.fa] 1 Aug 2005 C -Modules M. S. Moslehian Abstract The generalized Hyers Ulam Rassias stability of adjointable mappings on Hilbert

More information

Herz (cf. [H], and also [BS]) proved that the reverse inequality is also true, that is,

Herz (cf. [H], and also [BS]) proved that the reverse inequality is also true, that is, REARRANGEMENT OF HARDY-LITTLEWOOD MAXIMAL FUNCTIONS IN LORENTZ SPACES. Jesús Bastero*, Mario Milman and Francisco J. Ruiz** Abstract. For the classical Hardy-Littlewood maximal function M f, a well known

More information

A Riemann Lebesgue Lemma for Jacobi expansions

A Riemann Lebesgue Lemma for Jacobi expansions A Riemann Lebesgue Lemma for Jacobi expansions George Gasper 1 and Walter Trebels Dedicated to P. L. Butzer on the occasion of his 65-th birthday (To appear in Contemporary Mathematics) Abstract. A Lemma

More information

THE RADON NIKODYM PROPERTY AND LIPSCHITZ EMBEDDINGS

THE RADON NIKODYM PROPERTY AND LIPSCHITZ EMBEDDINGS THE RADON NIKODYM PROPERTY AND LIPSCHITZ EMBEDDINGS Motivation The idea here is simple. Suppose we have a Lipschitz homeomorphism f : X Y where X and Y are Banach spaces, namely c 1 x y f (x) f (y) c 2

More information

MATH 220: THE FOURIER TRANSFORM TEMPERED DISTRIBUTIONS. Beforehand we constructed distributions by taking the set Cc

MATH 220: THE FOURIER TRANSFORM TEMPERED DISTRIBUTIONS. Beforehand we constructed distributions by taking the set Cc MATH 220: THE FOURIER TRANSFORM TEMPERED DISTRIBUTIONS Beforehand we constructed distributions by taking the set Cc ( ) as the set of very nice functions, and defined distributions as continuous linear

More information

A review: The Laplacian and the d Alembertian. j=1

A review: The Laplacian and the d Alembertian. j=1 Chapter One A review: The Laplacian and the d Alembertian 1.1 THE LAPLACIAN One of the main goals of this course is to understand well the solution of wave equation both in Euclidean space and on manifolds

More information

On the stirling expansion into negative powers of a triangular number

On the stirling expansion into negative powers of a triangular number MATHEMATICAL COMMUNICATIONS 359 Math. Commun., Vol. 5, No. 2, pp. 359-364 200) On the stirling expansion into negative powers of a triangular number Cristinel Mortici, Department of Mathematics, Valahia

More information

JUHA KINNUNEN. Harmonic Analysis

JUHA KINNUNEN. Harmonic Analysis JUHA KINNUNEN Harmonic Analysis Department of Mathematics and Systems Analysis, Aalto University 27 Contents Calderón-Zygmund decomposition. Dyadic subcubes of a cube.........................2 Dyadic cubes

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

Velocity averaging a general framework

Velocity averaging a general framework Outline Velocity averaging a general framework Martin Lazar BCAM ERC-NUMERIWAVES Seminar May 15, 2013 Joint work with D. Mitrović, University of Montenegro, Montenegro Outline Outline 1 2 L p, p >= 2 setting

More information

Laplace s Equation. Chapter Mean Value Formulas

Laplace s Equation. Chapter Mean Value Formulas Chapter 1 Laplace s Equation Let be an open set in R n. A function u C 2 () is called harmonic in if it satisfies Laplace s equation n (1.1) u := D ii u = 0 in. i=1 A function u C 2 () is called subharmonic

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

Weakly Compact Composition Operators on Hardy Spaces of the Upper Half-Plane 1

Weakly Compact Composition Operators on Hardy Spaces of the Upper Half-Plane 1 Int. Journal of Math. Analysis, Vol. 4, 2010, no. 37, 1851-1856 Weakly Compact Composition Operators on Hardy Spaces of the Upper Half-Plane 1 Hong Bin Bai School of Science Sichuan University of Science

More information

First In-Class Exam Solutions Math 410, Professor David Levermore Monday, 1 October 2018

First In-Class Exam Solutions Math 410, Professor David Levermore Monday, 1 October 2018 First In-Class Exam Solutions Math 40, Professor David Levermore Monday, October 208. [0] Let {b k } k N be a sequence in R and let A be a subset of R. Write the negations of the following assertions.

More information

Uncertainty principles for far field patterns and applications to inverse source problems

Uncertainty principles for far field patterns and applications to inverse source problems for far field patterns and applications to inverse source problems roland.griesmaier@uni-wuerzburg.de (joint work with J. Sylvester) Paris, September 17 Outline Source problems and far field patterns AregularizedPicardcriterion

More information

New York Journal of Mathematics. A Refinement of Ball s Theorem on Young Measures

New York Journal of Mathematics. A Refinement of Ball s Theorem on Young Measures New York Journal of Mathematics New York J. Math. 3 (1997) 48 53. A Refinement of Ball s Theorem on Young Measures Norbert Hungerbühler Abstract. For a sequence u j : R n R m generating the Young measure

More information

Sequences. Chapter 3. n + 1 3n + 2 sin n n. 3. lim (ln(n + 1) ln n) 1. lim. 2. lim. 4. lim (1 + n)1/n. Answers: 1. 1/3; 2. 0; 3. 0; 4. 1.

Sequences. Chapter 3. n + 1 3n + 2 sin n n. 3. lim (ln(n + 1) ln n) 1. lim. 2. lim. 4. lim (1 + n)1/n. Answers: 1. 1/3; 2. 0; 3. 0; 4. 1. Chapter 3 Sequences Both the main elements of calculus (differentiation and integration) require the notion of a limit. Sequences will play a central role when we work with limits. Definition 3.. A Sequence

More information

Functions preserving slowly oscillating double sequences

Functions preserving slowly oscillating double sequences An Ştiinţ Univ Al I Cuza Iaşi Mat (NS) Tomul LXII, 2016, f 2, vol 2 Functions preserving slowly oscillating double sequences Huseyin Cakalli Richard F Patterson Received: 25IX2013 / Revised: 15IV2014 /

More information

MATH 104 : Final Exam

MATH 104 : Final Exam MATH 104 : Final Exam 10 May, 2017 Name: You have 3 hours to answer the questions. You are allowed one page (front and back) worth of notes. The page should not be larger than a standard US letter size.

More information

lim f f(kx)dp(x) = cmf

lim f f(kx)dp(x) = cmf proceedings of the american mathematical society Volume 107, Number 3, November 1989 MAGNIFIED CURVES ON A FLAT TORUS, DETERMINATION OF ALMOST PERIODIC FUNCTIONS, AND THE RIEMANN-LEBESGUE LEMMA ROBERT

More information

Final: Solutions Math 118A, Fall 2013

Final: Solutions Math 118A, Fall 2013 Final: Solutions Math 118A, Fall 2013 1. [20 pts] For each of the following PDEs for u(x, y), give their order and say if they are nonlinear or linear. If they are linear, say if they are homogeneous or

More information

RELATION BETWEEN SMALL FUNCTIONS WITH DIFFERENTIAL POLYNOMIALS GENERATED BY MEROMORPHIC SOLUTIONS OF HIGHER ORDER LINEAR DIFFERENTIAL EQUATIONS

RELATION BETWEEN SMALL FUNCTIONS WITH DIFFERENTIAL POLYNOMIALS GENERATED BY MEROMORPHIC SOLUTIONS OF HIGHER ORDER LINEAR DIFFERENTIAL EQUATIONS Kragujevac Journal of Mathematics Volume 38(1) (2014), Pages 147 161. RELATION BETWEEN SMALL FUNCTIONS WITH DIFFERENTIAL POLYNOMIALS GENERATED BY MEROMORPHIC SOLUTIONS OF HIGHER ORDER LINEAR DIFFERENTIAL

More information

Math 115 ( ) Yum-Tong Siu 1. Derivation of the Poisson Kernel by Fourier Series and Convolution

Math 115 ( ) Yum-Tong Siu 1. Derivation of the Poisson Kernel by Fourier Series and Convolution Math 5 (006-007 Yum-Tong Siu. Derivation of the Poisson Kernel by Fourier Series and Convolution We are going to give a second derivation of the Poisson kernel by using Fourier series and convolution.

More information

INTRODUCTION TO REAL ANALYSIS II MATH 4332 BLECHER NOTES

INTRODUCTION TO REAL ANALYSIS II MATH 4332 BLECHER NOTES INTRODUCTION TO REAL ANALYSIS II MATH 433 BLECHER NOTES. As in earlier classnotes. As in earlier classnotes (Fourier series) 3. Fourier series (continued) (NOTE: UNDERGRADS IN THE CLASS ARE NOT RESPONSIBLE

More information

= F (b) F (a) F (x i ) F (x i+1 ). a x 0 x 1 x n b i

= F (b) F (a) F (x i ) F (x i+1 ). a x 0 x 1 x n b i Real Analysis Problem 1. If F : R R is a monotone function, show that F T V ([a,b]) = F (b) F (a) for any interval [a, b], and that F has bounded variation on R if and only if it is bounded. Here F T V

More information

Power series solutions for 2nd order linear ODE s (not necessarily with constant coefficients) a n z n. n=0

Power series solutions for 2nd order linear ODE s (not necessarily with constant coefficients) a n z n. n=0 Lecture 22 Power series solutions for 2nd order linear ODE s (not necessarily with constant coefficients) Recall a few facts about power series: a n z n This series in z is centered at z 0. Here z can

More information

NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS

NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS Fixed Point Theory, Volume 9, No. 1, 28, 3-16 http://www.math.ubbcluj.ro/ nodeacj/sfptcj.html NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS GIOVANNI ANELLO Department of Mathematics University

More information

On stable inversion of the attenuated Radon transform with half data Jan Boman. We shall consider weighted Radon transforms of the form

On stable inversion of the attenuated Radon transform with half data Jan Boman. We shall consider weighted Radon transforms of the form On stable inversion of the attenuated Radon transform with half data Jan Boman We shall consider weighted Radon transforms of the form R ρ f(l) = f(x)ρ(x, L)ds, L where ρ is a given smooth, positive weight

More information

FIXED POINT ITERATION FOR PSEUDOCONTRACTIVE MAPS

FIXED POINT ITERATION FOR PSEUDOCONTRACTIVE MAPS PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 127, Number 4, April 1999, Pages 1163 1170 S 0002-9939(99)05050-9 FIXED POINT ITERATION FOR PSEUDOCONTRACTIVE MAPS C. E. CHIDUME AND CHIKA MOORE

More information

A Singular Integral Transform for the Gibbs-Wilbraham Effect in Inverse Fourier Transforms

A Singular Integral Transform for the Gibbs-Wilbraham Effect in Inverse Fourier Transforms Universal Journal of Integral Equations 4 (2016), 54-62 www.papersciences.com A Singular Integral Transform for the Gibbs-Wilbraham Effect in Inverse Fourier Transforms N. H. S. Haidar CRAMS: Center for

More information

INTRODUCTION TO REAL ANALYTIC GEOMETRY

INTRODUCTION TO REAL ANALYTIC GEOMETRY INTRODUCTION TO REAL ANALYTIC GEOMETRY KRZYSZTOF KURDYKA 1. Analytic functions in several variables 1.1. Summable families. Let (E, ) be a normed space over the field R or C, dim E

More information