Operator Theory and Integral Equations 802660S Lecture Notes

Total Page:16

File Type:pdf, Size:1020Kb

Operator Theory and Integral Equations 802660S Lecture Notes Operator theory and integral equations 802660S Lecture Notes Second printing Valery Serov University of Oulu 2012 Edited by Markus Harju Contents 1 Inner product spaces and Hilbert spaces 1 2 Symmetric operators in the Hilbert space 12 3 J. von Neumann’s spectral theorem 25 4 Spectrum of self-adjoint operators 38 5 Quadratic forms. Friedrichs extension. 54 6 Elliptic differential operators 58 7 Spectral function 67 8 Integral operators with weak singularities. Integral equations of the first and second kind. 71 9 Volterra and singular integral equations 81 10 Approximate methods 88 Index 98 i 1 Inner product spaces and Hilbert spaces A collection of elements is called a complex (real) vector space (linear space) H if the following axioms are satisfied: 1) To every pair x,y H there corresponds a vector x + y, called the sum, with the properties: ∈ a) x + y = y + x b) x +(y + z)=(x + y)+ z x + y + z ≡ c) there exists unique 0 H such that x +0= x ∈ d) for every x H there exists unique y1 H such that x+y1 = 0. We denote y := x. ∈ ∈ 1 − 2) For every x H and every λ,µ C there corresponds a vector λ x such that ∈ ∈ · a) λ(µx)=(λµ)x λµx ≡ b) (λ + µ)x = λx + µx c) λ(x + y)= λx + λy d) 1 x = x. · Definition. For a linear space H a mapping ( , ) : H H C is called an inner product or a scalar product if · · × → 1) (x,x) 0 and (x,x)=0 if and only if x =0 ≥ 2) (x,y + z)=(x,y)+(x,z) 3) (λx,y)= λ(x,y) 4) (x,y)= (y,x) for every x,y,z H and λ C. A linear space equipped with an inner product is called an inner product∈ space∈. An immediate consequence of this definition is that (λx + µy,z) = λ(x,z)+ µ(y,z), (x,λy) = λ(x,y) for every x,y,z H and λ,µ C. ∈ ∈ Example 1.1. On the complex Euclidean space H = Cn the standard inner product is n (x,y)= xjyj, j=1 X where x =(x ,...,x ) Cn and y =(y ,...,y ) Cn. 1 n ∈ 1 n ∈ 1 Example 1.2. On the linear space C[a,b] of continuous complex-valued functions, the formula b (f,g)= f(x)g(x)dx Za defines an inner product. Definition. Suppose H is an inner product space. We say that 1) x H orthogonal to y H if (x,y)=0. ∈ ∈ 1, α = β 2) a system xα α∈A H orthonormal if (xα,xβ) = δα,β = , where { } ⊂ 0, α = β A ( 6 is some index set. 3) x := (x,x) is called the length of x H. k k ∈ k Exercise 1. pProve the Theorem of Pythagoras: If xj j=1, k N is an orthonormal system in an inner product space H, then { } ∈ k k 2 2 2 x = (x,xj) + x (x,xj)xj k k | | − j=1 j=1 X X for every x H. ∈ k Exercise 2. Prove Bessel’s inequality: If xj j=1, k is an orthonormal system then { } ≤ ∞ k (x,x ) 2 x 2 , | j | ≤ k k j=1 X for every x H. ∈ Exercise 3. Prove the Cauchy-Schwarz-Bunjakovskii inequality: (x,y) x y , x,y H. | | ≤ k k k k ∈ Prove also that ( , ) is continuous as a map from H H to C. · · × If H is an inner product space, then x := (x,x) k k has the following properties: p 1) x 0 for every x H and x = 0 if and only if x = 0. k k≥ ∈ k k 2) λx = λ x for every x H and λ C. k k | | k k ∈ ∈ 3) x + y x + y for every x,y H. This is the triangle inequality. k k ≤ k k k k ∈ 2 The function = ( , ) is thus a norm on H. It is called the norm induced by the inner product.k·k · · p Every inner product space H is a normed space under the induced norm. The neighborhood of x H is the open ball Br(x) = y H : x y < r . This system of neighborhoods defines∈ the norm topology on H{such∈ that:k − k } 1) The addition x + y is a continuous map H H H. × → 2) The scalar multiplication λ x is a continuous map C H H. · × → 3) The inner product (x,y): H H C is continuous. × → ∞ Definition. 1) A sequence xj j=1 H is called a Cauchy sequence if for every ε> 0 there exists n N {such} that⊂ x x <ε for k, j n . 0 ∈ k k − jk ≥ 0 ∞ 2) A sequence xj j=1 H is said to be convergent if there exists x H such that for every ε>{ 0} there⊂ exists n N such that x x <ε whenever∈ j n . 0 ∈ k − jk ≥ 0 3) The inner product space H is complete space if every Cauchy sequence in H converges. Corollary. 1) Every convergent sequence is a Cauchy sequence. 2) If x ∞ converges to x H then { j}j=1 ∈ lim xj = x . j→∞ k k k k Definition (J. von Neumann, 1925). A Hilbert space is an inner product space which is complete (with respect to its norm topology). Exercise 4. Prove that in an inner product space the norm induced by this inner product satisfies the parallelogram law x + y 2 + x y 2 =2 x 2 +2 y 2 . k k k − k k k k k Exercise 5. Prove that if in a normed space H the parallelogram law holds, then there is an inner product on H such that x 2 =(x,x) and that this inner product is defined by the polarization identity k k 1 (x,y) := x + y 2 x y 2 + i x + iy 2 i x iy 2 . 4 k k − k − k k k − k − k Exercise 6. Prove that on C[a,b] the norm f = max f(x) k k x∈[a,b] | | is not induced by an inner product. 3 Exercise 7. Give an example of an inner product space which is not complete. Next we list some examples of Hilbert spaces. 1) The Euclidean spaces Rn and Cn. 2) The matrix space Mn(C) consisting of n n -matrices whose elements are complex numbers. For A, B M (C) the inner product× is given by ∈ n n ∗ (A, B)= akjbkj = Tr(AB ), k,jX=1 T where B∗ = B . 3) The sequence space l2(C) defined by ∞ l2(C) := x ∞ ,x C : x 2 < . { j}j=1 j ∈ | j| ∞ ( j=1 ) X The estimates x + y 2 2 x 2 + y 2 , λx 2 = λ 2 x 2 | j j| ≤ | j| | j| | j| | | | j| and 1 x y x 2 + y 2 | j j|≤ 2 | j| | j| imply that l2(C) is a linear space. Let us define the inner product by ∞ (x,y) := xjyj j=1 X 2 (k) ∞ 2 and prove that l (C) is complete. Suppose that x k=1 l (C) is a Cauchy sequence. Then for every ε> 0 there exists n N{ such} that∈ 0 ∈ ∞ 2 x(k) x(m) = x(k) x(m) 2 <ε2 − | j − j | j=1 X for k,m n . It implies that ≥ 0 x(k) x(m) < ε, j =1, 2,... | j − j | or that x(k) ∞ is a Cauchy sequence in C for every j = 1, 2,.... Since C is { j }k=1 a complete space then x(k) ∞ converges for every fixed j = 1, 2,... i.e. there { j }k=1 exists xj C such that ∈ (k) xj = lim xj . k→∞ 4 This fact and l x(k) x(m) 2 <ε2, l N | j − j | ∈ j=1 X imply that l l (k) (m) 2 (k) 2 2 lim xj xj = xj xj ε m→∞ | − | | − | ≤ j=1 j=1 X X for all k n and l N. Therefore the sequence ≥ 0 ∈ l s := x(k) x 2, k n l | j − j| ≥ 0 j=1 X is a monotone increasing sequence which is bounded from above by ε2. Hence this sequence has a limit with the same upper bound i.e. ∞ l (k) 2 (k) 2 2 xj xj = lim xj xj ε . | − | l→∞ | − | ≤ j=1 j=1 X X That’s why we may conclude that x x(k) + x(k) x x(k) + ε k k≤ − ≤ and x l2(C). ∈ 4) The Lebesgue space L2(Ω), where Ω Rn is an open set. The space L2(Ω) consists of all Lebesgue measurable functions⊂ f which are square integrable i.e. f(x) 2dx < . | | ∞ ZΩ It is a linear space with the inner product (f,g)= f(x)g(x)dx ZΩ and the Riesz-Fisher theorem reads as: L2(Ω) is a Hilbert space. k 2 5) The Sobolev spaces W2 (Ω) consisting of functions f L (Ω) whose weak or distributional derivatives Dαf also belong to L2(Ω) up∈ to order α k, k = k | | ≤ 1, 2,.... On the space W2 (Ω) the natural inner product is (f,g)= Dαf(x)Dαg(x)dx. Ω |Xα|≤k Z 5 Definition. Let H be an inner product space. For any subspace M H the orthogonal complement of M is defined as ⊂ M ⊥ := y H :(y,x)=0, for all x M . { ∈ ∈ } Remark. It is clear that M ⊥ is a linear subspace of H. Moreover, M M ⊥ = 0 since 0 M always. ∩ { } ∈ Definition.
Recommended publications
  • Some Schemata for Applications of the Integral Transforms of Mathematical Physics
    mathematics Review Some Schemata for Applications of the Integral Transforms of Mathematical Physics Yuri Luchko Department of Mathematics, Physics, and Chemistry, Beuth University of Applied Sciences Berlin, Luxemburger Str. 10, 13353 Berlin, Germany; [email protected] Received: 18 January 2019; Accepted: 5 March 2019; Published: 12 March 2019 Abstract: In this survey article, some schemata for applications of the integral transforms of mathematical physics are presented. First, integral transforms of mathematical physics are defined by using the notions of the inverse transforms and generating operators. The convolutions and generating operators of the integral transforms of mathematical physics are closely connected with the integral, differential, and integro-differential equations that can be solved by means of the corresponding integral transforms. Another important technique for applications of the integral transforms is the Mikusinski-type operational calculi that are also discussed in the article. The general schemata for applications of the integral transforms of mathematical physics are illustrated on an example of the Laplace integral transform. Finally, the Mellin integral transform and its basic properties and applications are briefly discussed. Keywords: integral transforms; Laplace integral transform; transmutation operator; generating operator; integral equations; differential equations; operational calculus of Mikusinski type; Mellin integral transform MSC: 45-02; 33C60; 44A10; 44A15; 44A20; 44A45; 45A05; 45E10; 45J05 1. Introduction In this survey article, we discuss some schemata for applications of the integral transforms of mathematical physics to differential, integral, and integro-differential equations, and in the theory of special functions. The literature devoted to this subject is huge and includes many books and reams of papers.
    [Show full text]
  • Integral Equation for the Number of Integer Points in a Circle
    ITALIAN JOURNAL OF PURE AND APPLIED MATHEMATICS { N. 41{2019 (522{525) 522 INTEGRAL EQUATION FOR THE NUMBER OF INTEGER POINTS IN A CIRCLE Magomed A. Chakhkiev Gagik S. Sulyan Manya A. Ziroyan Department of Applied Mathematics Social State University of Russia Wilhelm Pieck St. 4, Moscow Russian Federation Nikolay P. Tretyakov Department of Applied Mathematics Social State University of Russia Wilhelm Pieck St. 4, Moscow Russian Federation and School of Public Policy The Russian Presidential Academy of National Economy and Public Administration Prospect Vernadskogo, 84, Moscow 119571 Russian Federation Saif A. Mouhammad∗ Department of Physics Faculty of Science Taif University Taif, AL-Haweiah Kingdom of Saudi Arabia [email protected] Abstract. The problem is to obtain the most accurate upper estimate for the absolute value of the difference between the number of integer points in a circle and its area (when the radius tends to infinity). In this paper we obtain an integral equation for the function expressing the dependence of the number of integer points in a circle on its radius. The kernel of the equation contains the Bessel functions of the first kind, and the equation itself is a kind of the Hankel transform. Keywords: Gauss circle problem, integral equation, Hankel transform. 1. The problem and calculations The Gauss circle problem is the problem of determining how many integer lattice points there are in a circle centered at the origin andp with given radius. Let us consider the circle K(R): x2 + y2 ≤ R and let A( R) be the number of ∗. Corresponding author INTEGRAL EQUATION FOR THE NUMBER OF INTEGER POINTS IN A CIRCLE 523 p points with integer coordinates within this circle.
    [Show full text]
  • 18.102 Introduction to Functional Analysis Spring 2009
    MIT OpenCourseWare http://ocw.mit.edu 18.102 Introduction to Functional Analysis Spring 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 108 LECTURE NOTES FOR 18.102, SPRING 2009 Lecture 19. Thursday, April 16 I am heading towards the spectral theory of self-adjoint compact operators. This is rather similar to the spectral theory of self-adjoint matrices and has many useful applications. There is a very effective spectral theory of general bounded but self- adjoint operators but I do not expect to have time to do this. There is also a pretty satisfactory spectral theory of non-selfadjoint compact operators, which it is more likely I will get to. There is no satisfactory spectral theory for general non-compact and non-self-adjoint operators as you can easily see from examples (such as the shift operator). In some sense compact operators are ‘small’ and rather like finite rank operators. If you accept this, then you will want to say that an operator such as (19.1) Id −K; K 2 K(H) is ‘big’. We are quite interested in this operator because of spectral theory. To say that λ 2 C is an eigenvalue of K is to say that there is a non-trivial solution of (19.2) Ku − λu = 0 where non-trivial means other than than the solution u = 0 which always exists. If λ =6 0 we can divide by λ and we are looking for solutions of −1 (19.3) (Id −λ K)u = 0 −1 which is just (19.1) for another compact operator, namely λ K: What are properties of Id −K which migh show it to be ‘big? Here are three: Proposition 26.
    [Show full text]
  • Curl, Divergence and Laplacian
    Curl, Divergence and Laplacian What to know: 1. The definition of curl and it two properties, that is, theorem 1, and be able to predict qualitatively how the curl of a vector field behaves from a picture. 2. The definition of divergence and it two properties, that is, if div F~ 6= 0 then F~ can't be written as the curl of another field, and be able to tell a vector field of clearly nonzero,positive or negative divergence from the picture. 3. Know the definition of the Laplace operator 4. Know what kind of objects those operator take as input and what they give as output. The curl operator Let's look at two plots of vector fields: Figure 1: The vector field Figure 2: The vector field h−y; x; 0i: h1; 1; 0i We can observe that the second one looks like it is rotating around the z axis. We'd like to be able to predict this kind of behavior without having to look at a picture. We also promised to find a criterion that checks whether a vector field is conservative in R3. Both of those goals are accomplished using a tool called the curl operator, even though neither of those two properties is exactly obvious from the definition we'll give. Definition 1. Let F~ = hP; Q; Ri be a vector field in R3, where P , Q and R are continuously differentiable. We define the curl operator: @R @Q @P @R @Q @P curl F~ = − ~i + − ~j + − ~k: (1) @y @z @z @x @x @y Remarks: 1.
    [Show full text]
  • Laplace Transforms: Theory, Problems, and Solutions
    Laplace Transforms: Theory, Problems, and Solutions Marcel B. Finan Arkansas Tech University c All Rights Reserved 1 Contents 43 The Laplace Transform: Basic Definitions and Results 3 44 Further Studies of Laplace Transform 15 45 The Laplace Transform and the Method of Partial Fractions 28 46 Laplace Transforms of Periodic Functions 35 47 Convolution Integrals 45 48 The Dirac Delta Function and Impulse Response 53 49 Solving Systems of Differential Equations Using Laplace Trans- form 61 50 Solutions to Problems 68 2 43 The Laplace Transform: Basic Definitions and Results Laplace transform is yet another operational tool for solving constant coeffi- cients linear differential equations. The process of solution consists of three main steps: • The given \hard" problem is transformed into a \simple" equation. • This simple equation is solved by purely algebraic manipulations. • The solution of the simple equation is transformed back to obtain the so- lution of the given problem. In this way the Laplace transformation reduces the problem of solving a dif- ferential equation to an algebraic problem. The third step is made easier by tables, whose role is similar to that of integral tables in integration. The above procedure can be summarized by Figure 43.1 Figure 43.1 In this section we introduce the concept of Laplace transform and discuss some of its properties. The Laplace transform is defined in the following way. Let f(t) be defined for t ≥ 0: Then the Laplace transform of f; which is denoted by L[f(t)] or by F (s), is defined by the following equation Z T Z 1 L[f(t)] = F (s) = lim f(t)e−stdt = f(t)e−stdt T !1 0 0 The integral which defined a Laplace transform is an improper integral.
    [Show full text]
  • Numerical Operator Calculus in Higher Dimensions
    Numerical operator calculus in higher dimensions Gregory Beylkin* and Martin J. Mohlenkamp Applied Mathematics, University of Colorado, Boulder, CO 80309 Communicated by Ronald R. Coifman, Yale University, New Haven, CT, May 31, 2002 (received for review July 31, 2001) When an algorithm in dimension one is extended to dimension d, equation using only one-dimensional operations and thus avoid- in nearly every case its computational cost is taken to the power d. ing the exponential dependence on d. However, if the best This fundamental difficulty is the single greatest impediment to approximate solution of the form (Eq. 1) is not good enough, solving many important problems and has been dubbed the curse there is no way to improve the accuracy. of dimensionality. For numerical analysis in dimension d,we The natural extension of Eq. 1 is the form propose to use a representation for vectors and matrices that generalizes separation of variables while allowing controlled ac- r ͑ ͒ ϭ ͸ ␾l ͑ ͒ ␾l ͑ ͒ curacy. Basic linear algebra operations can be performed in this f x1,...,xd sl 1 x1 ··· d xd . [2] representation using one-dimensional operations, thus bypassing lϭ1 the exponential scaling with respect to the dimension. Although not all operators and algorithms may be compatible with this The key quantity in Eq. 2 is r, which we call the separation rank. representation, we believe that many of the most important ones By increasing r, the approximate solution can be made as are. We prove that the multiparticle Schro¨dinger operator, as well accurate as desired.
    [Show full text]
  • Solution to Volterra Singular Integral Equations and Non Homogenous Time Fractional Pdes
    Gen. Math. Notes, Vol. 14, No. 1, January 2013, pp. 6-20 ISSN 2219-7184; Copyright © ICSRS Publication, 2013 www.i-csrs.org Available free online at http://www.geman.in Solution to Volterra Singular Integral Equations and Non Homogenous Time Fractional PDEs A. Aghili 1 and H. Zeinali 2 1,2 Department of Applied Mathematics Faculty of Mathematical Sciences, University of Guilan, P.O. Box- 1841, Rasht – Iran 1E-mail: [email protected] 2E-mail: [email protected] (Received: 8-10-12 / Accepted: 19-11-12) Abstract In this work, the authors implemented Laplace transform method for solving certain partial fractional differential equations and Volterra singular integral equations. Constructive examples are also provided to illustrate the ideas. The result reveals that the transform method is very convenient and effective. Keywords : Non-homogeneous time fractional heat equations; Laplace transform; Volterra singular integral equations. 1 Introduction In this work, the authors used Laplace transform for solving Volterra singular integral equations and PFDEs. Solution to Volterra Singular Integral… 7 The Laplace transform is an alternative method for solving different types of PDEs. Also it is commonly used to solve electrical circuit and systems problems. In this work, the authors implemented transform method for solving the partial fractional heat equation which arise in applications. Several methods have been introduced to solve fractional differential equations, the popular Laplace transform method, [ 1 ] , [ 2 ] , [ 3 ], [ 4 ] , and operational method [ 10]. However, most of these methods are suitable for special types of fractional differential equations, mainly the linear with constant coefficients. More detailed information about some of these results can be found in a survey paper by Kilbas and Trujillo [10].
    [Show full text]
  • 23. Kernel, Rank, Range
    23. Kernel, Rank, Range We now study linear transformations in more detail. First, we establish some important vocabulary. The range of a linear transformation f : V ! W is the set of vectors the linear transformation maps to. This set is also often called the image of f, written ran(f) = Im(f) = L(V ) = fL(v)jv 2 V g ⊂ W: The domain of a linear transformation is often called the pre-image of f. We can also talk about the pre-image of any subset of vectors U 2 W : L−1(U) = fv 2 V jL(v) 2 Ug ⊂ V: A linear transformation f is one-to-one if for any x 6= y 2 V , f(x) 6= f(y). In other words, different vector in V always map to different vectors in W . One-to-one transformations are also known as injective transformations. Notice that injectivity is a condition on the pre-image of f. A linear transformation f is onto if for every w 2 W , there exists an x 2 V such that f(x) = w. In other words, every vector in W is the image of some vector in V . An onto transformation is also known as an surjective transformation. Notice that surjectivity is a condition on the image of f. 1 Suppose L : V ! W is not injective. Then we can find v1 6= v2 such that Lv1 = Lv2. Then v1 − v2 6= 0, but L(v1 − v2) = 0: Definition Let L : V ! W be a linear transformation. The set of all vectors v such that Lv = 0W is called the kernel of L: ker L = fv 2 V jLv = 0g: 1 The notions of one-to-one and onto can be generalized to arbitrary functions on sets.
    [Show full text]
  • Math 551 Lecture Notes Fredholm Integral Equations (A Brief Introduction)
    MATH 551 LECTURE NOTES FREDHOLM INTEGRAL EQUATIONS (A BRIEF INTRODUCTION) Topics covered • Fredholm integral operators ◦ Integral equations (Volterra vs. Fredholm) ◦ Eigenfunctions for separable kernels ◦ Adjoint operator, symmetric kernels • Solution procedure (separable) ◦ Solution via eigenfunctions (first and second kind) ◦ Shortcuts: undetermined coefficients ◦ An example (separable kernel, n = 2) • Non-separable kernels (briefly) ◦ Hilbert-Schmidt theory Preface Read the Fredholm alternative notes before proceeding. This is covered in the book (Section 9.4), but the material on integral equations is not. For references on integral equa- tions (and other topics covered in the book too!), see: • Riley and Hobson, Mathematical methods for physics and engineering (this is an extensive reference, also for other topics in the course) • Guenther and Lee, Partial differential equations of mathematical physics and integral equations (more technical; not the best first reference) • J.D. Logan, Applied mathematics (more generally about applied mathematics tech- niques, with a good section on integral equations) 1. Fredholm integral equations: introduction Differential equations Lu = f are a subset of more general equations involving linear op- erators L. Here, we give a brief treatment of a generalization to integral equations. To motivate this, every ODE IVP can be written as an `integral equation' by integrating. For instance, consider the first order IVP du = f(x; u(x)); u(a) = u : (1.1) dx 0 Integrate both sides from a to x to get the integral equation Z x u(x) = u0 + f(s; u(s)) ds: (1.2) a If u solves (1.2) then it also solves (1.1); they are `equivalent' in this sense.
    [Show full text]
  • October 7, 2015 1 Adjoint of a Linear Transformation
    Mathematical Toolkit Autumn 2015 Lecture 4: October 7, 2015 Lecturer: Madhur Tulsiani The following is an extremely useful inequality. Prove it for a general inner product space (not neccessarily finite dimensional). Exercise 0.1 (Cauchy-Schwarz-Bunyakowsky inequality) Let u; v be any two vectors in an inner product space V . Then jhu; vij2 ≤ hu; ui · hv; vi Let V be a finite dimensional inner product space and let fw1; : : : ; wng be an orthonormal basis for P V . Then for any v 2 V , there exist c1; : : : ; cn 2 F such that v = i ci · wi. The coefficients ci are often called Fourier coefficients. Using the orthonormality and the properties of the inner product, we get ci = hv; wii. This can be used to prove the following Proposition 0.2 (Parseval's identity) Let V be a finite dimensional inner product space and let fw1; : : : ; wng be an orthonormal basis for V . Then, for any u; v 2 V n X hu; vi = hu; wii · hv; wii : i=1 1 Adjoint of a linear transformation Definition 1.1 Let V; W be inner product spaces over the same field F and let ' : V ! W be a linear transformation. A transformation '∗ : W ! V is called an adjoint of ' if h'(v); wi = hv; '∗(w)i 8v 2 V; w 2 W: n Pn Example 1.2 Let V = W = C with the inner product hu; vi = i=1 ui · vi. Let ' : V ! V be represented by the matrix A. Then '∗ is represented by the matrix AT . Exercise 1.3 Let 'left : Fib ! Fib be the left shift operator as before, and let hf; gi for f; g 2 Fib P1 f(n)g(n) ∗ be defined as hf; gi = n=0 Cn for C > 4.
    [Show full text]
  • Chapter 1 Introduction to the Integral Equation(IE) and Construction Of
    Chapter 1 Introduction to the Integral Equation(IE) and Construction of the IE. 1.1. Introduction: Integral Equation began to appear since the mid-seventeenth century , when some scientists were not able to solve the differential equation . The integral equation developed with appear Abel kernel after that Volterra integral equation lastly Fredholm integral equation. In this time we find numerical method played a great role to solve integral equation. Therefore of great progressing in basic science whether physical or engineering has played essential role. Topics on integral equations has grown and evolved to its direct association lists the large branches of mathematics, such as account differential and integrative and questions of boundary conditions. During the twenty-five last year, there is a marked increase in the use of integral equations and formulations for finding scientific solutions to engineering problems and solving differential equations that are difficult to solve by normal methods. In the recent period found that the integral equations give a better solution than give differential equations. The explosive growth in industry and technology requires constructive adjustments in mathematics text researches. The integral equation it equation that appear in the unknown function under signal or more, from the signals of integrity. There more types of integral equation from it linear and nonlinear integral equation. The general formula linear integral equation it is: ١ () = () + (, )() (1 − 1) Where () unknown function, () known function and (, )known function are called kernel integral equation. We say that integral equation it is linear if that which operations on unknown function in equation it linear operations. And the general formula nonlinear integral equation it is : () = () + (, )(()) (1 − 2) Where unknown function it is nonlinear .
    [Show full text]
  • Operator Calculus
    Pacific Journal of Mathematics OPERATOR CALCULUS PHILIP JOEL FEINSILVER Vol. 78, No. 1 March 1978 PACIFIC JOURNAL OF MATHEMATICS Vol. 78, No. 1, 1978 OPERATOR CALCULUS PHILIP FEINSILVER To an analytic function L(z) we associate the differential operator L(D), D denoting differentiation with respect to a real variable x. We interpret L as the generator of a pro- cess with independent increments having exponential mar- tingale m(x(t), t)= exp (zx(t) — tL{z)). Observing that m(x, —t)—ezCl where C—etLxe~tL, we study the operator calculus for C and an associated generalization of the operator xD, A—CD. We find what functions / have the property n that un~C f satisfy the evolution equation ut~Lu and the eigenvalue equations Aun—nun, thus generalizing the powers xn. We consider processes on RN as well as R1 and discuss various examples and extensions of the theory. In the case that L generates a Markov semigroup, we have transparent probabilistic interpretations. In case L may not gene- rate a probability semigroup, the general theory gives some insight into what properties any associated "processes with independent increments" should have. That is, the purpose is to elucidate the Markov case but in such a way that hopefully will lead to practi- cable definitions and will present useful ideas for defining more general processes—involving, say, signed and/or singular measures. IL Probabilistic basis. Let pt(%} be the transition kernel for a process p(t) with stationary independent increments. That is, ί pί(a?) = The Levy-Khinchine formula says that, generally: tξ tL{ίξ) e 'pt(x) = e R where L(ίξ) = aiξ - σψ/2 + [ eiξu - 1 - iζη(u)-M(du) with jΛ-fO} u% η(u) = u(\u\ ^ 1) + sgn^(M ^ 1) and ί 2M(du)< <*> .
    [Show full text]