L P and Sobolev Spaces

Total Page:16

File Type:pdf, Size:1020Kb

L P and Sobolev Spaces NOTES ON Lp AND SOBOLEV SPACES STEVE SHKOLLER 1. Lp spaces 1.1. Definitions and basic properties. Definition 1.1. Let 0 < p < 1 and let (X; M; µ) denote a measure space. If f : X ! R is a measurable function, then we define 1 Z p p kfkLp(X) := jfj dx and kfkL1(X) := ess supx2X jf(x)j : X Note that kfkLp(X) may take the value 1. Definition 1.2. The space Lp(X) is the set p L (X) = ff : X ! R j kfkLp(X) < 1g : The space Lp(X) satisfies the following vector space properties: (1) For each α 2 R, if f 2 Lp(X) then αf 2 Lp(X); (2) If f; g 2 Lp(X), then jf + gjp ≤ 2p−1(jfjp + jgjp) ; so that f + g 2 Lp(X). (3) The triangle inequality is valid if p ≥ 1. The most interesting cases are p = 1; 2; 1, while all of the Lp arise often in nonlinear estimates. Definition 1.3. The space lp, called \little Lp", will be useful when we introduce Sobolev spaces on the torus and the Fourier series. For 1 ≤ p < 1, we set ( 1 ) p 1 X p l = fxngn=1 j jxnj < 1 : n=1 1.2. Basic inequalities. Lemma 1.4. For λ 2 (0; 1), xλ ≤ (1 − λ) + λx. Proof. Set f(x) = (1 − λ) + λx − xλ; hence, f 0(x) = λ − λxλ−1 = 0 if and only if λ(1 − xλ−1) = 0 so that x = 1 is the critical point of f. In particular, the minimum occurs at x = 1 with value f(1) = 0 ≤ (1 − λ) + λx − xλ : Lemma 1.5. For a; b ≥ 0 and λ 2 (0; 1), aλb1−λ ≤ λa + (1 − λ)b with equality if a = b. Date: March 19, 2009. 1 2 STEVE SHKOLLER Proof. If either a = 0 or b = 0, then this is trivially true, so assume that a; b > 0. Set x = a=b, and apply Lemma 1 to obtain the desired inequality. Theorem 1.6 (H¨older'sinequality). Suppose that 1 ≤ p ≤ 1 and 1 < q < 1 with 1 1 p q 1 p + q = 1. If f 2 L and g 2 L , then fg 2 L . Moreover, kfgkL1 ≤ kfkLp kgkLq : Note that if p = q = 2, then this is the Cauchy-Schwarz inequality since kfgkL1 = j(f; g)L2 j. Proof. We use Lemma 1.5. Let λ = 1=p and set jfjp jgjq a = p ; and b = q kfkLp kgkLp for all x 2 X. Then aλb1−λ = a1=pb1−1=p = a1=pb1=q so that jfj · jgj 1 jfjp 1 jgjq ≤ p + q : kfkLp kgkLq p kfkLp q kgkLq Integrating this inequality yields Z jfj · jgj Z 1 jfjp 1 jgjq 1 1 dx ≤ p + q dx = + = 1 : X kfkLp kgkLq X p kfkLp q kgkLq p q p 1 1 Definition 1.7. q = p−1 or q = 1 − p is called the conjugate exponent of p. Theorem 1.8 (Minkowski's inequality). If 1 ≤ p ≤ 1 and f; g 2 Lp then kf + gkLp ≤ kfkLp + kgkLp : Proof. If f + g = 0 a.e., then the statement is trivial. Assume that f + g 6= 0 a.e. Consider the equality jf + gjp = jf + gj · jf + gjp−1 ≤ (jfj + jgj)jf + gjp−1 ; and integrate over X to find that Z Z jf + gjpdx ≤ (jfj + jgj)jf + gjp−1 dx X X H¨older's p−1 p p ≤ (kfkL + kgkL ) jf + gj Lq : p Since q = p−1 , 1 Z q p−1 p jf + gj Lq = jf + gj dx ; X from which it follows that 1− 1 Z q p jf + gj dx ≤ kfkLp + kgkLq ; X 1 1 which completes the proof, since p = 1 − q . Corollary 1.9. For 1 ≤ p ≤ 1, Lp(X) is a normed linear space. NOTES ON Lp AND SOBOLEV SPACES 3 Example 1.10. Let Ω denote a (Lebesgue) measure-1 subset of Rn. If f 2 L1(Ω) satisfies f(x) ≥ M > 0 for almost all x 2 Ω, then log(f) 2 L1(Ω) and satisfies Z Z log fdx ≤ log( fdx) : Ω Ω To see this, consider the function g(t) = t − 1 − log t for t > 0. Compute g0(t) = 1 00 1 − t = 0 so t = 1 is a minimum (since g (1) > 0). Thus, log t ≤ t − 1 and letting 1 t 7! t we see that 1 1 − ≤ log t ≤ t − 1 : (1.1) t Since log x is continuous and f is measurable, then log f is measurable for f > 0. Let t = f(x) in (1.1) to find that kfkL1 kfkL1 f(x) 1 − ≤ log f(x) − log kfkL1 ≤ − 1 : (1.2) f(x) kfkL1 Since g(x) ≤ log f(x) ≤ h(x) for two integrable functions g and h, it follows that log f(x) is integrable. Next, integrate (1.2) to finish the proof, as R f(x) − 1 dx = X kfkL1 0. p 1.3. The space (L (X); k·kLp (X) is complete. Recall the a normed linear space is a Banach space if every Cauchy sequence has a limit in that space; furthermore, recall that a sequence xn ! x in X if limn!1 kxn − xkX = 0. The proof of completeness makes use of the following two lemmas which are restatements of the Monotone Convergence Theorem and the Dominated Conver- gence Theorem, respectively. 1 Lemma 1.11 (MCT). If fn 2 L (X), 0 ≤ f1(x) ≤ f2(x) ≤ · · ·, and kfnkL1(X) ≤ 1 C < 1, then limn!1 fn(x) = f(x) with f 2 L (X) and kfn − fkL1 ! 0 as n ! 0. 1 Lemma 1.12 (DCT). If fn 2 L (X), limn!1 fn(x) = f(x) a.e., and if 9 g 2 1 1 L (X) such that jfn(x)j ≤ jg(x)j a.e. for all n, then f 2 L (X) and kfn−fkL1 ! 0. Proof. Apply the Dominated Convergene Theorem to the sequence hn = jfn −fj ! 0 a.e., and note that jhnj ≤ 2g. Theorem 1.13. If 1≤ p < 1 then Lp (X) is a Banach space. 1 Proof. Step 1. The Cauchy sequence. Let ffngn=1 denote a Cauchy sequence in Lp, and assume without loss of generality (by extracting a subsequence if neces- −n sary) that kfn+1 − fnkLp ≤ 2 . Step 2. Conversion to a convergent monotone sequence. Define the se- 1 quence fgngn=1 as g1 = 0; gn = jf1j + jf2 − f1j + ··· + jfn − fn−1j for n ≥ 2 : It follows that 0 ≤ g1 ≤ g2 ≤ · · · ≤ gn ≤ · · · so that gn is a monotonically increasing sequence. Furthermore, fgng is uniformly bounded in Lp as Z 1 !p p p X p gndx = kgnkLp ≤ kf1kLp + kfi − fi−1kLp ≤ (kfkLp + 1) ; X i=2 4 STEVE SHKOLLER p p p thus, by the Monotone Convergence Theorem, gn % g a.e., g 2 L , and gn ≤ g a.e. Step 3. Pointwise convergence of ffng. For all k ≥ 1, jfn+k − fnj = jfn+k − fn+k−1 + fn+k−1 + · · · − fn+1 + fn+1 − fnj k+1 X ≤ jfi − fi−1j = gn+k − gn −! 0 a.e. i=n+1 Therefore, fn ! f a.e. Since n X jfnj ≤ jf1j + jfi − fi−1j ≤ gn ≤ g for all n 2 N ; i=2 p p p p p p it follows that jfj ≤ g a.e. Hence, jfnj ≤ g , jfj ≤ g , and jf − fnj ≤ 2g , and by the Dominated Convergence Theorem, Z Z p p lim jf − fnj dx = lim jf − fnj dx = 0 : n!1 X X n!1 p p 1.4. Convergence criteria for L functions. If ffng is a sequence in L (X) p which converges to f in L (X), then there exists a subsequence ffnk g such that fnk (x) ! f(x) for almost every x 2 X (denoted by a.e.), but it is in general not true that the entire sequence itself will converge pointwise a.e. to the limit f, without some further conditions holding. Example 1.14. Let X = [0; 1], and consider the subintervals 1 1 1 1 2 2 1 1 2 2 3 3 1 0; ; ; 1 ; 0; ; ; ; ; 1 ; 0; ; ; ; ; ; ; 1 ; 0; ; ··· 2 2 3 3 3 3 4 4 4 4 4 4 5 th Let fn denote the indicator function of the n interval of the above sequence. Then kfnkLp ! 0, but fn(x) does not converge for any x 2 [0; 1]. Example 1.15. Set X = R, and for n 2 N, set fn = 1[n;n+1]. Then fn(x) ! 0 as p n ! 1, but kfnkLp = 1 for p 2 [1; 1); thus, fn ! 0 pointwise, but not in L . Example 1.16. Set X = [0; 1], and for n 2 , set fn = n1 1 . Then fn(x) ! 0 N [0; n ] p a.e. as n ! 1, but kfnkL1 = 1; thus, fn ! 0 pointwise, but not in L . p Theorem 1.17. For 1 ≤ p < 1, suppose that ffng ⊂ L (X) and that fn(x) ! p f(x) a.e. If limn!1 kfnkLp(X) = kfkLp(X), then fn ! f in L (X). a+b p 1 p p p Proof. Given a; b ≥ 0, convexity implies that 2 ≤ 2 (a +b ) so that (a+b) ≤ p−1 p p p p−1 p p 2 (a +b ), and hence ja−bj ≤ 2 (jaj +jbj ). Set a = fn and b = f to obtain the inequality p−1 p p p 0 ≤ 2 (jfnj + jfj ) − jfn − fj : Since fn(x) ! f(x) a.e., Z Z p p p−1 p p p 2 jfj dx = lim 2 (jfnj + jfj ) − jfn − fj dx : X X n!1 Thus, Fatou's lemma asserts that Z Z p p p−1 p p p 2 jfj dx ≤ lim inf 2 (jfnj + jfj ) − jfn − fj dx X n!1 X NOTES ON Lp AND SOBOLEV SPACES 5 Since kfnkLp(X) ! kfkLp(X), we see lim supn!1 kfn − fkLp(X) = 0.
Recommended publications
  • Sobolev Spaces, Theory and Applications
    Sobolev spaces, theory and applications Piotr Haj lasz1 Introduction These are the notes that I prepared for the participants of the Summer School in Mathematics in Jyv¨askyl¨a,August, 1998. I thank Pekka Koskela for his kind invitation. This is the second summer course that I delivere in Finland. Last August I delivered a similar course entitled Sobolev spaces and calculus of variations in Helsinki. The subject was similar, so it was not posible to avoid overlapping. However, the overlapping is little. I estimate it as 25%. While preparing the notes I used partially the notes that I prepared for the previous course. Moreover Lectures 9 and 10 are based on the text of my joint work with Pekka Koskela [33]. The notes probably will not cover all the material presented during the course and at the some time not all the material written here will be presented during the School. This is however, not so bad: if some of the results presented on lectures will go beyond the notes, then there will be some reasons to listen the course and at the same time if some of the results will be explained in more details in notes, then it might be worth to look at them. The notes were prepared in hurry and so there are many bugs and they are not complete. Some of the sections and theorems are unfinished. At the end of the notes I enclosed some references together with comments. This section was also prepared in hurry and so probably many of the authors who contributed to the subject were not mentioned.
    [Show full text]
  • Geometric Integration Theory Contents
    Steven G. Krantz Harold R. Parks Geometric Integration Theory Contents Preface v 1 Basics 1 1.1 Smooth Functions . 1 1.2Measures.............................. 6 1.2.1 Lebesgue Measure . 11 1.3Integration............................. 14 1.3.1 Measurable Functions . 14 1.3.2 The Integral . 17 1.3.3 Lebesgue Spaces . 23 1.3.4 Product Measures and the Fubini–Tonelli Theorem . 25 1.4 The Exterior Algebra . 27 1.5 The Hausdorff Distance and Steiner Symmetrization . 30 1.6 Borel and Suslin Sets . 41 2 Carath´eodory’s Construction and Lower-Dimensional Mea- sures 53 2.1 The Basic Definition . 53 2.1.1 Hausdorff Measure and Spherical Measure . 55 2.1.2 A Measure Based on Parallelepipeds . 57 2.1.3 Projections and Convexity . 57 2.1.4 Other Geometric Measures . 59 2.1.5 Summary . 61 2.2 The Densities of a Measure . 64 2.3 A One-Dimensional Example . 66 2.4 Carath´eodory’s Construction and Mappings . 67 2.5 The Concept of Hausdorff Dimension . 70 2.6 Some Cantor Set Examples . 73 i ii CONTENTS 2.6.1 Basic Examples . 73 2.6.2 Some Generalized Cantor Sets . 76 2.6.3 Cantor Sets in Higher Dimensions . 78 3 Invariant Measures and the Construction of Haar Measure 81 3.1 The Fundamental Theorem . 82 3.2 Haar Measure for the Orthogonal Group and the Grassmanian 90 3.2.1 Remarks on the Manifold Structure of G(N,M).... 94 4 Covering Theorems and the Differentiation of Integrals 97 4.1 Wiener’s Covering Lemma and its Variants .
    [Show full text]
  • Introduction to Sobolev Spaces
    Introduction to Sobolev Spaces Lecture Notes MM692 2018-2 Joa Weber UNICAMP December 23, 2018 Contents 1 Introduction1 1.1 Notation and conventions......................2 2 Lp-spaces5 2.1 Borel and Lebesgue measure space on Rn .............5 2.2 Definition...............................8 2.3 Basic properties............................ 11 3 Convolution 13 3.1 Convolution of functions....................... 13 3.2 Convolution of equivalence classes................. 15 3.3 Local Mollification.......................... 16 3.3.1 Locally integrable functions................. 16 3.3.2 Continuous functions..................... 17 3.4 Applications.............................. 18 4 Sobolev spaces 19 4.1 Weak derivatives of locally integrable functions.......... 19 1 4.1.1 The mother of all Sobolev spaces Lloc ........... 19 4.1.2 Examples........................... 20 4.1.3 ACL characterization.................... 21 4.1.4 Weak and partial derivatives................ 22 4.1.5 Approximation characterization............... 23 4.1.6 Bounded weakly differentiable means Lipschitz...... 24 4.1.7 Leibniz or product rule................... 24 4.1.8 Chain rule and change of coordinates............ 25 4.1.9 Equivalence classes of locally integrable functions..... 27 4.2 Definition and basic properties................... 27 4.2.1 The Sobolev spaces W k;p .................. 27 4.2.2 Difference quotient characterization of W 1;p ........ 29 k;p 4.2.3 The compact support Sobolev spaces W0 ........ 30 k;p 4.2.4 The local Sobolev spaces Wloc ............... 30 4.2.5 How the spaces relate.................... 31 4.2.6 Basic properties { products and coordinate change.... 31 i ii CONTENTS 5 Approximation and extension 33 5.1 Approximation............................ 33 5.1.1 Local approximation { any domain............. 33 5.1.2 Global approximation on bounded domains.......
    [Show full text]
  • Functional Analysis 1 Winter Semester 2013-14
    Functional analysis 1 Winter semester 2013-14 1. Topological vector spaces Basic notions. Notation. (a) The symbol F stands for the set of all reals or for the set of all complex numbers. (b) Let (X; τ) be a topological space and x 2 X. An open set G containing x is called neigh- borhood of x. We denote τ(x) = fG 2 τ; x 2 Gg. Definition. Suppose that τ is a topology on a vector space X over F such that • (X; τ) is T1, i.e., fxg is a closed set for every x 2 X, and • the vector space operations are continuous with respect to τ, i.e., +: X × X ! X and ·: F × X ! X are continuous. Under these conditions, τ is said to be a vector topology on X and (X; +; ·; τ) is a topological vector space (TVS). Remark. Let X be a TVS. (a) For every a 2 X the mapping x 7! x + a is a homeomorphism of X onto X. (b) For every λ 2 F n f0g the mapping x 7! λx is a homeomorphism of X onto X. Definition. Let X be a vector space over F. We say that A ⊂ X is • balanced if for every α 2 F, jαj ≤ 1, we have αA ⊂ A, • absorbing if for every x 2 X there exists t 2 R; t > 0; such that x 2 tA, • symmetric if A = −A. Definition. Let X be a TVS and A ⊂ X. We say that A is bounded if for every V 2 τ(0) there exists s > 0 such that for every t > s we have A ⊂ tV .
    [Show full text]
  • Proving the Regularity of the Reduced Boundary of Perimeter Minimizing Sets with the De Giorgi Lemma
    PROVING THE REGULARITY OF THE REDUCED BOUNDARY OF PERIMETER MINIMIZING SETS WITH THE DE GIORGI LEMMA Presented by Antonio Farah In partial fulfillment of the requirements for graduation with the Dean's Scholars Honors Degree in Mathematics Honors, Department of Mathematics Dr. Stefania Patrizi, Supervising Professor Dr. David Rusin, Honors Advisor, Department of Mathematics THE UNIVERSITY OF TEXAS AT AUSTIN May 2020 Acknowledgements I deeply appreciate the continued guidance and support of Dr. Stefania Patrizi, who supervised the research and preparation of this Honors Thesis. Dr. Patrizi kindly dedicated numerous sessions to this project, motivating and expanding my learning. I also greatly appreciate the support of Dr. Irene Gamba and of Dr. Francesco Maggi on the project, who generously helped with their reading and support. Further, I am grateful to Dr. David Rusin, who also provided valuable help on this project in his role of Honors Advisor in the Department of Mathematics. Moreover, I would like to express my gratitude to the Department of Mathematics' Faculty and Administration, to the College of Natural Sciences' Administration, and to the Dean's Scholars Honors Program of The University of Texas at Austin for my educational experience. 1 Abstract The Plateau problem consists of finding the set that minimizes its perimeter among all sets of a certain volume. Such set is known as a minimal set, or perimeter minimizing set. The problem was considered intractable until the 1960's, when the development of geometric measure theory by researchers such as Fleming, Federer, and De Giorgi provided the necessary tools to find minimal sets.
    [Show full text]
  • Five Lectures on Optimal Transportation: Geometry, Regularity and Applications
    FIVE LECTURES ON OPTIMAL TRANSPORTATION: GEOMETRY, REGULARITY AND APPLICATIONS ROBERT J. MCCANN∗ AND NESTOR GUILLEN Abstract. In this series of lectures we introduce the Monge-Kantorovich problem of optimally transporting one distribution of mass onto another, where optimality is measured against a cost function c(x, y). Connections to geometry, inequalities, and partial differential equations will be discussed, focusing in particular on recent developments in the regularity theory for Monge-Amp`ere type equations. An ap- plication to microeconomics will also be described, which amounts to finding the equilibrium price distribution for a monopolist marketing a multidimensional line of products to a population of anonymous agents whose preferences are known only statistically. c 2010 by Robert J. McCann. All rights reserved. Contents Preamble 2 1. An introduction to optimal transportation 2 1.1. Monge-Kantorovich problem: transporting ore from mines to factories 2 1.2. Wasserstein distance and geometric applications 3 1.3. Brenier’s theorem and convex gradients 4 1.4. Fully-nonlinear degenerate-elliptic Monge-Amp`eretype PDE 4 1.5. Applications 5 1.6. Euclidean isoperimetric inequality 5 1.7. Kantorovich’s reformulation of Monge’s problem 6 2. Existence, uniqueness, and characterization of optimal maps 6 2.1. Linear programming duality 8 2.2. Game theory 8 2.3. Relevance to optimal transport: Kantorovich-Koopmans duality 9 2.4. Characterizing optimality by duality 9 2.5. Existence of optimal maps and uniqueness of optimal measures 10 3. Methods for obtaining regularity of optimal mappings 11 3.1. Rectifiability: differentiability almost everywhere 12 3.2. From regularity a.e.
    [Show full text]
  • HYPERCYCLIC SUBSPACES in FRÉCHET SPACES 1. Introduction
    PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 134, Number 7, Pages 1955–1961 S 0002-9939(05)08242-0 Article electronically published on December 16, 2005 HYPERCYCLIC SUBSPACES IN FRECHET´ SPACES L. BERNAL-GONZALEZ´ (Communicated by N. Tomczak-Jaegermann) Dedicated to the memory of Professor Miguel de Guzm´an, who died in April 2004 Abstract. In this note, we show that every infinite-dimensional separable Fr´echet space admitting a continuous norm supports an operator for which there is an infinite-dimensional closed subspace consisting, except for zero, of hypercyclic vectors. The family of such operators is even dense in the space of bounded operators when endowed with the strong operator topology. This completes the earlier work of several authors. 1. Introduction and notation Throughout this paper, the following standard notation will be used: N is the set of positive integers, R is the real line, and C is the complex plane. The symbols (mk), (nk) will stand for strictly increasing sequences in N.IfX, Y are (Hausdorff) topological vector spaces (TVSs) over the same field K = R or C,thenL(X, Y ) will denote the space of continuous linear mappings from X into Y , while L(X)isthe class of operators on X,thatis,L(X)=L(X, X). The strong operator topology (SOT) in L(X) is the one where the convergence is defined as pointwise convergence at every x ∈ X. A sequence (Tn) ⊂ L(X, Y )issaidtobeuniversal or hypercyclic provided there exists some vector x0 ∈ X—called hypercyclic for the sequence (Tn)—such that its orbit {Tnx0 : n ∈ N} under (Tn)isdenseinY .
    [Show full text]
  • The Logarithmic Sobolev Inequality Along the Ricci Flow
    The Logarithmic Sobolev Inequality Along The Ricci Flow (revised version) Rugang Ye Department of Mathematics University of California, Santa Barbara July 20, 2007 1. Introduction 2. The Sobolev inequality 3. The logarithmic Sobolev inequality on a Riemannian manifold 4. The logarithmic Sobolev inequality along the Ricci flow 5. The Sobolev inequality along the Ricci flow 6. The κ-noncollapsing estimate Appendix A. The logarithmic Sobolev inequalities on the euclidean space Appendix B. The estimate of e−tH Appendix C. From the estimate for e−tH to the Sobolev inequality 1 Introduction Consider a compact manifold M of dimension n 3. Let g = g(t) be a smooth arXiv:0707.2424v4 [math.DG] 29 Aug 2007 solution of the Ricci flow ≥ ∂g = 2Ric (1.1) ∂t − on M [0, T ) for some (finite or infinite) T > 0 with a given initial metric g(0) = g . × 0 Theorem A For each σ > 0 and each t [0, T ) there holds ∈ R n σ u2 ln u2dvol σ ( u 2 + u2)dvol ln σ + A (t + )+ A (1.2) ≤ |∇ | 4 − 2 1 4 2 ZM ZM 1 for all u W 1,2(M) with u2dvol =1, where ∈ M R 4 A1 = 2 min Rg0 , ˜ 2 n − CS(M,g0) volg0 (M) n A = n ln C˜ (M,g )+ (ln n 1), 2 S 0 2 − and all geometric quantities are associated with the metric g(t) (e.g. the volume form dvol and the scalar curvature R), except the scalar curvature Rg0 , the modified Sobolev ˜ constant CS(M,g0) (see Section 2 for its definition) and the volume volg0 (M) which are those of the initial metric g0.
    [Show full text]
  • 27. Sobolev Inequalities 27.1
    ANALYSIS TOOLS WITH APPLICATIONS 493 27. Sobolev Inequalities 27.1. Morrey’s Inequality. d 1 d Notation 27.1. Let S − be the sphere of radius one centered at zero inside R . d 1 d For a set Γ S − ,x R , and r (0, ), let ⊂ ∈ ∈ ∞ Γx,r x + sω : ω Γ such that 0 s r . ≡ { ∈ ≤ ≤ } So Γx,r = x + Γ0,r where Γ0,r is a cone based on Γ, seeFigure49below. Γ Γ Figure 49. The cone Γ0,r. d 1 Notation 27.2. If Γ S − is a measurable set let Γ = σ(Γ) be the surface “area” of Γ. ⊂ | | Notation 27.3. If Ω Rd is a measurable set and f : Rd C is a measurable function let ⊂ → 1 fΩ := f(x)dx := f(x)dx. − m(Ω) Ω ZΩ Z By Theorem 8.35, r d 1 (27.1) f(y)dy = f(x + y)dy = dt t − f(x + tω) dσ(ω) Γx,r Γ0,r 0 Z Z Z ZΓ and letting f =1in this equation implies d (27.2) m(Γx,r)= Γ r /d. | | d 1 Lemma 27.4. Let Γ S − be a measurable set such that Γ > 0. For u 1 ⊂ | | ∈ C (Γx,r), 1 u(y) (27.3) u(y) u(x) dy |∇ d | 1 dy. − | − | ≤ Γ x y − ΓZx,r | |ΓZx,r | − | 494 BRUCE K. DRIVER† d 1 Proof. Write y = x + sω with ω S − , then by the fundamental theorem of calculus, ∈ s u(x + sω) u(x)= u(x + tω) ωdt − ∇ · Z0 and therefore, s u(x + sω) u(x) dσ(ω) u(x + tω) dσ(ω)dt | − | ≤ 0 Γ |∇ | ZΓ Z Z s d 1 u(x + tω) = t − dt |∇ d | 1 dσ(ω) 0 Γ x + tω x − Z Z | − | u(y) u(y) = |∇ d | 1 dy |∇ d | 1 dy, y x − ≤ x y − ΓZx,s | − | ΓZx,r | − | wherein the second equality we have used Eq.
    [Show full text]
  • Fact Sheet Functional Analysis
    Fact Sheet Functional Analysis Literature: Hackbusch, W.: Theorie und Numerik elliptischer Differentialgleichungen. Teubner, 1986. Knabner, P., Angermann, L.: Numerik partieller Differentialgleichungen. Springer, 2000. Triebel, H.: H¨ohere Analysis. Harri Deutsch, 1980. Dobrowolski, M.: Angewandte Funktionalanalysis, Springer, 2010. 1. Banach- and Hilbert spaces Let V be a real vector space. Normed space: A norm is a mapping k · k : V ! [0; 1), such that: kuk = 0 , u = 0; (definiteness) kαuk = jαj · kuk; α 2 R; u 2 V; (positive scalability) ku + vk ≤ kuk + kvk; u; v 2 V: (triangle inequality) The pairing (V; k · k) is called a normed space. Seminorm: In contrast to a norm there may be elements u 6= 0 such that kuk = 0. It still holds kuk = 0 if u = 0. Comparison of two norms: Two norms k · k1, k · k2 are called equivalent if there is a constant C such that: −1 C kuk1 ≤ kuk2 ≤ Ckuk1; u 2 V: If only one of these inequalities can be fulfilled, e.g. kuk2 ≤ Ckuk1; u 2 V; the norm k · k1 is called stronger than the norm k · k2. k · k2 is called weaker than k · k1. Topology: In every normed space a canonical topology can be defined. A subset U ⊂ V is called open if for every u 2 U there exists a " > 0 such that B"(u) = fv 2 V : ku − vk < "g ⊂ U: Convergence: A sequence vn converges to v w.r.t. the norm k · k if lim kvn − vk = 0: n!1 1 A sequence vn ⊂ V is called Cauchy sequence, if supfkvn − vmk : n; m ≥ kg ! 0 for k ! 1.
    [Show full text]
  • Basic Differentiable Calculus Review
    Basic Differentiable Calculus Review Jimmie Lawson Department of Mathematics Louisiana State University Spring, 2003 1 Introduction Basic facts about the multivariable differentiable calculus are needed as back- ground for differentiable geometry and its applications. The purpose of these notes is to recall some of these facts. We state the results in the general context of Banach spaces, although we are specifically concerned with the finite-dimensional setting, specifically that of Rn. Let U be an open set of Rn. A function f : U ! R is said to be a Cr map for 0 ≤ r ≤ 1 if all partial derivatives up through order r exist for all points of U and are continuous. In the extreme cases C0 means that f is continuous and C1 means that all partials of all orders exists and are continuous on m r r U. A function f : U ! R is a C map if fi := πif is C for i = 1; : : : ; m, m th where πi : R ! R is the i projection map defined by πi(x1; : : : ; xm) = xi. It is a standard result that mixed partials of degree less than or equal to r and of the same type up to interchanges of order are equal for a C r-function (sometimes called Clairaut's Theorem). We can consider a category with objects nonempty open subsets of Rn for various n and morphisms Cr-maps. This is indeed a category, since the composition of Cr maps is again a Cr map. 1 2 Normed Spaces and Bounded Linear Oper- ators At the heart of the differential calculus is the notion of a differentiable func- tion.
    [Show full text]
  • Optimal Filter and Mollifier for Piecewise Smooth Spectral Data
    MATHEMATICS OF COMPUTATION Volume 75, Number 254, Pages 767–790 S 0025-5718(06)01822-9 Article electronically published on January 23, 2006 OPTIMAL FILTER AND MOLLIFIER FOR PIECEWISE SMOOTH SPECTRAL DATA JARED TANNER This paper is dedicated to Eitan Tadmor for his direction Abstract. We discuss the reconstruction of piecewise smooth data from its (pseudo-) spectral information. Spectral projections enjoy superior resolution provided the function is globally smooth, while the presence of jump disconti- nuities is responsible for spurious O(1) Gibbs’ oscillations in the neighborhood of edges and an overall deterioration of the convergence rate to the unaccept- able first order. Classical filters and mollifiers are constructed to have compact support in the Fourier (frequency) and physical (time) spaces respectively, and are dilated by the projection order or the width of the smooth region to main- tain this compact support in the appropriate region. Here we construct a noncompactly supported filter and mollifier with optimal joint time-frequency localization for a given number of vanishing moments, resulting in a new fun- damental dilation relationship that adaptively links the time and frequency domains. Not giving preference to either space allows for a more balanced error decomposition, which when minimized yields an optimal filter and mol- lifier that retain the robustness of classical filters, yet obtain true exponential accuracy. 1. Introduction The Fourier projection of a 2π periodic function π ˆ ikx ˆ 1 −ikx (1.1) SN f(x):= fke , fk := f(x)e dx, 2π − |k|≤N π enjoys the well-known spectral convergence rate, that is, the convergence rate is as rapid as the global smoothness of f(·) permits.
    [Show full text]