SOLVABILITY OF A QUADRATIC INTEGRAL EQUATION OF FREDHOLM TYPE IN HÖLDER SPACES

Similar documents
ON QUADRATIC INTEGRAL EQUATIONS OF URYSOHN TYPE IN FRÉCHET SPACES. 1. Introduction

EXISTENCE OF POSITIVE SOLUTIONS OF A NONLINEAR SECOND-ORDER BOUNDARY-VALUE PROBLEM WITH INTEGRAL BOUNDARY CONDITIONS

Q-INTEGRAL EQUATIONS OF FRACTIONAL ORDERS. 1. Introduction In this paper, we are concerned with the following functional equation

Application of Measure of Noncompactness for the System of Functional Integral Equations

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR FOURTH-ORDER BOUNDARY-VALUE PROBLEMS IN BANACH SPACES

EXISTENCE OF SOLUTIONS TO A BOUNDARY-VALUE PROBLEM FOR AN INFINITE SYSTEM OF DIFFERENTIAL EQUATIONS

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR THE FRACTIONAL INTEGRO-DIFFERENTIAL EQUATIONS IN BANACH SPACES

FIXED POINT RESULTS FOR GENERALIZED APPLICATIONS

ULAM-HYERS-RASSIAS STABILITY OF SEMILINEAR DIFFERENTIAL EQUATIONS WITH IMPULSES

SOLUTION OF AN INITIAL-VALUE PROBLEM FOR PARABOLIC EQUATIONS VIA MONOTONE OPERATOR METHODS

EXISTENCE OF SOLUTIONS TO ASYMPTOTICALLY PERIODIC SCHRÖDINGER EQUATIONS

HOMOCLINIC SOLUTIONS FOR SECOND-ORDER NON-AUTONOMOUS HAMILTONIAN SYSTEMS WITHOUT GLOBAL AMBROSETTI-RABINOWITZ CONDITIONS

BOUNDARY-VALUE PROBLEMS FOR NONLINEAR THIRD-ORDER q-difference EQUATIONS

Approximating solutions of nonlinear second order ordinary differential equations via Dhage iteration principle

CONVERGENCE BEHAVIOUR OF SOLUTIONS TO DELAY CELLULAR NEURAL NETWORKS WITH NON-PERIODIC COEFFICIENTS

AN EXTENSION OF THE LAX-MILGRAM THEOREM AND ITS APPLICATION TO FRACTIONAL DIFFERENTIAL EQUATIONS

EXISTENCE AND APPROXIMATION OF SOLUTIONS OF SECOND ORDER NONLINEAR NEUMANN PROBLEMS

NONLINEAR FREDHOLM ALTERNATIVE FOR THE p-laplacian UNDER NONHOMOGENEOUS NEUMANN BOUNDARY CONDITION

Research Article Uniqueness of Positive Solutions for a Class of Fourth-Order Boundary Value Problems

SPACES ENDOWED WITH A GRAPH AND APPLICATIONS. Mina Dinarvand. 1. Introduction

EXISTENCE OF SOLUTIONS FOR CROSS CRITICAL EXPONENTIAL N-LAPLACIAN SYSTEMS

KRASNOSELSKII-TYPE FIXED POINT THEOREMS UNDER WEAK TOPOLOGY SETTINGS AND APPLICATIONS

Nonlocal Cauchy problems for first-order multivalued differential equations

ON PERIODIC BOUNDARY VALUE PROBLEMS OF FIRST-ORDER PERTURBED IMPULSIVE DIFFERENTIAL INCLUSIONS

ANALYSIS AND APPLICATION OF DIFFUSION EQUATIONS INVOLVING A NEW FRACTIONAL DERIVATIVE WITHOUT SINGULAR KERNEL

Research Article A Fixed Point Theorem for Mappings Satisfying a Contractive Condition of Rational Type on a Partially Ordered Metric Space

FUNCTIONAL COMPRESSION-EXPANSION FIXED POINT THEOREM

LIFE SPAN OF BLOW-UP SOLUTIONS FOR HIGHER-ORDER SEMILINEAR PARABOLIC EQUATIONS

POTENTIAL LANDESMAN-LAZER TYPE CONDITIONS AND. 1. Introduction We investigate the existence of solutions for the nonlinear boundary-value problem

Second order Volterra-Fredholm functional integrodifferential equations

TRIPLE POSITIVE SOLUTIONS FOR A CLASS OF TWO-POINT BOUNDARY-VALUE PROBLEMS

NONHOMOGENEOUS ELLIPTIC EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENT AND WEIGHT

Some generalizations of Darbo s theorem and applications to fractional integral equations

ELLIPTIC EQUATIONS WITH MEASURE DATA IN ORLICZ SPACES

EXISTENCE OF POSITIVE SOLUTIONS FOR KIRCHHOFF TYPE EQUATIONS

MULTIPLE SOLUTIONS FOR THE p-laplace EQUATION WITH NONLINEAR BOUNDARY CONDITIONS

STOKES PROBLEM WITH SEVERAL TYPES OF BOUNDARY CONDITIONS IN AN EXTERIOR DOMAIN

EXISTENCE OF NONTRIVIAL SOLUTIONS FOR A QUASILINEAR SCHRÖDINGER EQUATIONS WITH SIGN-CHANGING POTENTIAL

NON-EXTINCTION OF SOLUTIONS TO A FAST DIFFUSION SYSTEM WITH NONLOCAL SOURCES

EXISTENCE AND UNIQUENESS OF POSITIVE SOLUTIONS TO HIGHER-ORDER NONLINEAR FRACTIONAL DIFFERENTIAL EQUATION WITH INTEGRAL BOUNDARY CONDITIONS

POSITIVE SOLUTIONS OF A NONLINEAR THREE-POINT BOUNDARY-VALUE PROBLEM. Ruyun Ma

LIOUVILLE S THEOREM AND THE RESTRICTED MEAN PROPERTY FOR BIHARMONIC FUNCTIONS

Positive Solutions of a Third-Order Three-Point Boundary-Value Problem

SEMILINEAR ELLIPTIC EQUATIONS WITH DEPENDENCE ON THE GRADIENT

EXISTENCE AND UNIQUENESS OF SOLUTIONS TO FUNCTIONAL INTEGRO-DIFFERENTIAL FRACTIONAL EQUATIONS

A NONLINEAR NEUTRAL PERIODIC DIFFERENTIAL EQUATION

RESOLVENT OF LINEAR VOLTERRA EQUATIONS

TWO MAPPINGS RELATED TO SEMI-INNER PRODUCTS AND THEIR APPLICATIONS IN GEOMETRY OF NORMED LINEAR SPACES. S.S. Dragomir and J.J.

EXISTENCE OF CONJUGACIES AND STABLE MANIFOLDS VIA SUSPENSIONS

On Positive Solutions of Boundary Value Problems on the Half-Line

JUNXIA MENG. 2. Preliminaries. 1/k. x = max x(t), t [0,T ] x (t), x k = x(t) dt) k

On a perturbed functional integral equation of Urysohn type. Mohamed Abdalla Darwish

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

HAIYUN ZHOU, RAVI P. AGARWAL, YEOL JE CHO, AND YONG SOO KIM

EXISTENCE OF SOLUTIONS FOR A RESONANT PROBLEM UNDER LANDESMAN-LAZER CONDITIONS

A fixed point theorem for Meir-Keeler contractions in ordered metric spaces

The (CLR g )-property for coincidence point theorems and Fredholm integral equations in modular metric spaces

MEAN VALUE THEOREM FOR HOLOMORPHIC FUNCTIONS

Existence and Uniqueness Results for Nonlinear Implicit Fractional Differential Equations with Boundary Conditions

DISSIPATIVITY OF NEURAL NETWORKS WITH CONTINUOUSLY DISTRIBUTED DELAYS

Banach Algebras of Matrix Transformations Between Spaces of Strongly Bounded and Summable Sequences

CONVERGENCE OF HYBRID FIXED POINT FOR A PAIR OF NONLINEAR MAPPINGS IN BANACH SPACES

On boundary value problems for fractional integro-differential equations in Banach spaces

HYERS-ULAM STABILITY FOR SECOND-ORDER LINEAR DIFFERENTIAL EQUATIONS WITH BOUNDARY CONDITIONS

Differentiability with Respect to Lag Function for Nonlinear Pantograph Equations

GLOBAL ATTRACTIVITY IN A NONLINEAR DIFFERENCE EQUATION

A fixed point theorem for weakly Zamfirescu mappings

Convergence to Common Fixed Point for Two Asymptotically Quasi-nonexpansive Mappings in the Intermediate Sense in Banach Spaces

BLOW-UP OF SOLUTIONS FOR A NONLINEAR WAVE EQUATION WITH NONNEGATIVE INITIAL ENERGY

Bulletin of the. Iranian Mathematical Society

EXISTENCE OF SOLUTIONS FOR KIRCHHOFF TYPE EQUATIONS WITH UNBOUNDED POTENTIAL. 1. Introduction In this article, we consider the Kirchhoff type problem

ASYMPTOTIC PROPERTIES OF SOLUTIONS TO LINEAR NONAUTONOMOUS DELAY DIFFERENTIAL EQUATIONS THROUGH GENERALIZED CHARACTERISTIC EQUATIONS

Existence And Uniqueness Of Mild Solutions Of Second Order Volterra Integrodifferential Equations With Nonlocal Conditions

HYBRID DHAGE S FIXED POINT THEOREM FOR ABSTRACT MEASURE INTEGRO-DIFFERENTIAL EQUATIONS

MULTIPLE POSITIVE SOLUTIONS FOR FOURTH-ORDER THREE-POINT p-laplacian BOUNDARY-VALUE PROBLEMS

Xiyou Cheng Zhitao Zhang. 1. Introduction

ASYMPTOTIC THEORY FOR WEAKLY NON-LINEAR WAVE EQUATIONS IN SEMI-INFINITE DOMAINS

PERIODIC SOLUTIONS FOR NON-AUTONOMOUS SECOND-ORDER DIFFERENTIAL SYSTEMS WITH (q, p)-laplacian

BOUNDEDNESS AND EXPONENTIAL STABILITY OF SOLUTIONS TO DYNAMIC EQUATIONS ON TIME SCALES

EXISTENCE RESULTS FOR NONLINEAR FUNCTIONAL INTEGRAL EQUATIONS VIA NONLINEAR ALTERNATIVE OF LERAY-SCHAUDER TYPE

SYNCHRONIZATION OF NONAUTONOMOUS DYNAMICAL SYSTEMS

Existence, Uniqueness and Stability of Hilfer Type Neutral Pantograph Differential Equations with Nonlocal Conditions

DELAY INTEGRO DIFFERENTIAL EQUATIONS OF MIXED TYPE IN BANACH SPACES. Tadeusz Jankowski Technical University of Gdańsk, Poland

SIMULTANEOUS AND NON-SIMULTANEOUS BLOW-UP AND UNIFORM BLOW-UP PROFILES FOR REACTION-DIFFUSION SYSTEM

Remarks on Bronštein s root theorem

SOLUTIONS TO QUASI-LINEAR DIFFERENTIAL EQUATIONS WITH ITERATED DEVIATING ARGUMENTS

AN EXISTENCE-UNIQUENESS THEOREM FOR A CLASS OF BOUNDARY VALUE PROBLEMS

AW -Convergence and Well-Posedness of Non Convex Functions

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER NONLINEAR HYPERBOLIC SYSTEM

FORMAL AND ANALYTIC SOLUTIONS FOR A QUADRIC ITERATIVE FUNCTIONAL EQUATION

Abdulmalik Al Twaty and Paul W. Eloe

EXISTENCE OF WEAK SOLUTIONS FOR A NONUNIFORMLY ELLIPTIC NONLINEAR SYSTEM IN R N. 1. Introduction We study the nonuniformly elliptic, nonlinear system

Tomasz Człapiński. Communicated by Bolesław Kacewicz

Positive and monotone solutions of an m-point boundary-value problem

MULTIPLE POSITIVE SOLUTIONS FOR KIRCHHOFF PROBLEMS WITH SIGN-CHANGING POTENTIAL

Common fixed point of multivalued mappings in ordered generalized metric spaces

Nonlinear Control Systems

MULTIPLE SOLUTIONS FOR CRITICAL ELLIPTIC PROBLEMS WITH FRACTIONAL LAPLACIAN

ASYMPTOTICALLY I 2 -LACUNARY STATISTICAL EQUIVALENCE OF DOUBLE SEQUENCES OF SETS

THE ALTERNATIVE DUNFORD-PETTIS PROPERTY FOR SUBSPACES OF THE COMPACT OPERATORS

Transcription:

Electronic Journal of Differential Equations, Vol. 214 (214), No. 31, pp. 1 1. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu SOLVABILITY OF A QUADRATIC INTEGRAL EQUATION OF FREDHOLM TYPE IN HÖLDER SPACES JOSEFA CABALLERO, MOHAMED ABDALLA DARWISH, KISHIN SADARANGANI Abstract. In this article, we prove the existence of solutions of a quadratic integral equation of Fredholm type with a modified argument, in the space of functions satisfying a Hölder condition. Our main tool is the classical Schauder fixed point theorem. 1. Introduction Differential equations with a modified arguments arise in a wide variety of scientific and technical applications, including the modelling of problems from the natural and social sciences such as physics, biological and economics sciences. A special class of these differential equations have linear modifications of their arguments, and have been studied by several authors, see [1] [9] and their references. The aim of this article is to investigate the existence of solutions of the following integral equation of Fredholm type with a modified argument, x(t) = p(t) + x(t) k(t, τ) x(r(τ)) dτ, t [, 1]. (1.1) Our solutions are placed in the space of functions satisfying the Hölder condition. A sufficient condition for the relative compactness in these spaces and the classical Schauder fixed point theorem are the main tools in our study. 2. Preliminaries Our starting point in this section is to introduce the space of functions satisfying the Hölder condition and some properties in this space. These properties can be found in [2]. Let [a, b] be a closed interval in R, by C[a, b] we denote the space of continuous functions on [a, b] equipped with the supremum norm; i.e., x = sup{ x(t) : t [a, b]} for x C[a, b]. For < α 1 fixed, by H α [a, b] we will denote the space of the real functions x defined on [a, b] and satisfying the Hölder condition; that is, those functions x for which there exists a constant Hx α such that x(t) x(s) Hx α, (2.1) for all t, s [a, b]. It is easily proved that H α [a, b] is a linear subspace of C[a, b]. 2 Mathematics Subject Classification. 4G1, 4M99, 47H9. Key words and phrases. Fredholm; Hölder condition; Schauder fixed point theorem. c 214 Texas State University - San Marcos. Submitted October 31, 213. Published January 27, 214. 1

2 J. CABALLERO, M. A. DARWISH, K. SADARANGANI EJDE-214/31 In the sequel, for x H α [a, b], by Hx α we will denote the least possible constant for which inequality (2.1) is satisfied. More precisely, we put H α x = sup { x(t) x(s) : t [a, b], t s }. (2.2) The spaces H α [a, b] with < α 1 can be equipped with the norm x α = x(a) + sup { x(t) x(s) : t [a, b], t s }, for x H α [a, b]. In [2], the authors proved that (H α [a, b], α ) with < α 1 is a Banach space. The following lemmas appear in [2]. Lemma 2.1. For x H α [a, b] with < α 1, the following inequality is satisfied Lemma 2.2. For < α < γ 1, we have x max ( 1, (b a) α) x α. (2.3) H γ [a, b] H α [a, b] C[a, b]. (2.4) Moreover, for x H γ [a, b] the following inequality holds x α max ( 1, (b a) γ α) x γ. (2.) Now, we present the following sufficient condition for relative compactness in the spaces H α [a, b] with < α 1 which appears in Example 6 of [2] and it is an important result for our study. Theorem 2.3. Suppose that < α < β 1 and that A is a bounded subset in H β [a, b] (this means that x β M for certain constant M >, for any x A) then A is a relatively compact subset of H α [a, b]. 3. Main results In this section, we will study the solvability of (1.1) in the Hölder spaces. We will use the following assumptions: (i) p H β [, 1], < β 1. (ii) k : [, 1] [, 1] R is a continuous function such that it satisfies the Hölder condition with exponent β with respect to the first variable, that is, there exists a constant K β such that k(t, τ) k(s, τ) K β, for any t, s, τ [, 1]. (iii) r : [, 1] [, 1] is a measurable function. (iv) The following inequality is satisfied p β (2K + K β ) < 1 4, where the constant K is defined by which exists by (ii). K = sup { k(t, τ) dτ : t [, 1] },

EJDE-214/31 SOLVABILITY OF A QUADRATIC INTEGRAL EQUATION 3 Theorem 3.1. Under assumptions (i) (iv), Equation (1.1) has at least one solution belonging to the space H α [, 1], where α is arbitrarily fixed number satisfying < α < β. Proof. Consider the operator T defined on H β [, 1] by (T x)(t) = p(t) + x(t) k(t, τ) x(r(τ)) dτ, t [, 1]. In the sequel, we will prove that T transforms the space H β [, 1] into itself. In fact, we take x H β [, 1] and t, s [, 1] with t s. Then, by assumptions (i) and (ii), we obtain (T x)(t) (T x)(s) p(t) + x(t) = k(t, τ) x(r(τ)) dτ p(s) x(s) k(s, τ) x(r(τ)) dτ p(t) p(s) x(t) + k(t, τ) x(r(τ)) dτ x(s) k(t, τ) x(r(τ)) dτ 1 x(s) + k(t, τ) x(r(τ)) dτ x(s) k(s, τ) x(r(τ)) dτ p(t) p(s) x(t) x(s) + + x(s) k(t, τ) k(s, τ) x(r(τ)) dτ p(t) p(s) x(t) x(s) + x k(t, τ) x(r(τ)) dτ + x x k(t, τ) k(s, τ) dτ k(t, τ) dτ p(t) p(s) + K x x(t) x(s) + x 2 H β p + K x H β x + K β x 2. K β dτ By Lemma 2.1, since x x β and, as H β x x β, we infer that (T x)(t) (T x)(s) H β p + (K + K β ) x 2 β.

4 J. CABALLERO, M. A. DARWISH, K. SADARANGANI EJDE-214/31 Therefore, T x β = (T x)() + sup { (T x)(t) (T x)(s) : t, s [, 1], t s } (T x)() + H β p + (K + K β ) x 2 β p() + x() k(, τ) x(r(τ)) dτ + H β p + (K + K β ) x 2 β p β + x x k(, τ) dτ + (K + K β ) x 2 β (3.1) p β + K x 2 β + (K + K β ) x 2 β = p β + (2K + K β ) x 2 β <. This proves that the operator T maps H β [, 1] into itself. Taking into account that the inequality p β + (2K + K β )r 2 < r is satisfied for values between the numbers and r 1 = 1 1 4 p β (2K + K β ) 2(2K + K β ) r 2 = 1 1 + 4 p β (2K + K β ) 2(2K + K β ) which are positive by assumption (iv), consequently, from (3.1) it follows that T transforms the ball Br β = {x H β [, 1] : x β r } into itself, for any r [r 1, r 2 ]; i.e., T : Br β Br β, where r 1 r r 2. By Theorem 2.3, we have that the set Br β is relatively compact in H α [, 1] for any < α < β 1. Moreover, we can prove that Br β is a compact subset in H α [, 1] for any < α < β 1 (see Appendix). Next, we will prove that the operator T is continuous on Br β, where in Br β we consider the induced norm by α, where < α < β 1. To do this, we fix x Br β and ε >. Suppose that y Br β and x y α δ, where δ is a positive ε number such that δ < 2(2K+3K β )r. Then, for any t, s [, 1] with t s, we have [(T x)(t) (T y)(t)] [(T x)(s) (T y)(s)] [ x(t) = k(t, τ) x(r(τ)) dτ y(t) k(t, τ) y(r(τ)) dτ] [ x(s) k(s, τ) x(r(τ)) dτ y(s) k(s, τ) y(r(τ)) dτ] [ x(t) k(t, τ) x(r(τ)) dτ y(t) k(t, τ) x(r(τ)) dτ] [ y(t) + k(t, τ) x(r(τ)) dτ y(t) k(t, τ) y(r(τ)) dτ]

EJDE-214/31 SOLVABILITY OF A QUADRATIC INTEGRAL EQUATION [ x(s) k(s, τ) x(r(τ)) dτ y(s) k(s, τ) x(r(τ)) dτ] [ y(s) k(s, τ) x(r(τ)) dτ y(s) k(s, τ) y(r(τ)) dτ] 1 (x(t) = y(t)) (x(s) y(s)) k(t, τ) x(r(τ)) dτ + y(t) k(s, τ) x(r(τ)) dτ y(s) 1 { (x(t) y(t)) (x(s) y(s)) + x(s) y(s) + y(t) (k(t, τ) k(s, τ)) x(r(τ)) dτ k(t, τ)(x(r(τ) y(r(τ))) dτ y(s) (x(t) y(t)) (x(s) y(s)) x k(t, τ)(x(r(τ) y(r(τ))) dτ k(s, τ) (x(r(τ)) y(r(τ))) dτ k(t, τ) x(r(τ)) dτ k(t, τ) dτ + [ (x(s) y(s)) (x() y()) + x() y() ] x k(t, τ) k(s, τ) dτ + 1 y(t) k(t, τ)(x(r(τ) y(r(τ))) dτ y(s) 1 y(s) + y(s) K x y α x + k(t, τ)(x(r(τ) y(r(τ))) dτ k(s, τ)(x(r(τ) y(r(τ))) dτ sup p,q [,1] (x(p) y(p)) (x(q) y(q)) K β x dτ + x() y() x y(s) x(s) + + y(s) k(t, τ) x(r(τ) y(r(τ)) dτ } k(s, τ)(x(r(τ) y(r(τ))) dτ k(t, τ)(x(r(τ) y(r(τ))) dτ k(t, τ) k(s, τ) x(r(τ) y(r(τ)) dτ K x x y α + x K β α { (x(p) y(p)) (x(q) y(q)) sup p,q [,1], p q p q α p q α} + K β x β α x() y() + KH α y x y + y x y K β dτ K β dτ K x β x y α + 2K β x β x y α + K y α x y α + K β y α x y α

6 J. CABALLERO, M. A. DARWISH, K. SADARANGANI EJDE-214/31 ( K x β + 2K β x β + K y α + K β y α ) x y α. Since y α y β (see, Lemma 2.2) and x, y B β r, from the above inequality we infer that [(T x)(t) (T y)(t)] [(T x)(s) (T y)(s)] (2Kr + 3K β r ) x y α (2Kr + 3K β r )δ < ε 2. (3.2) On the other hand, (T x)() (T y)() = x() x() + x() x() + (x() y()) k(, τ) x(r(τ)) dτ y() k(, τ) x(r(τ)) dτ x() k(, τ) y(r(τ)) dτ y() k(, τ)y(r(τ)) dτ k(, τ)(x(r(τ)) y(r(τ))) dτ k(, τ) y(r(τ))) dτ K x x y + K y x y α K x β x y α + K y β x y α k(, τ) y(r(τ)) dτ k(, τ) y(r(τ)) dτ From (3.2) and (3.3), it follows that T x T y = (T x)() (T y)() 2Kr x y α < 2Kr δ < ε 2. (3.3) + sup { ((T x)(t) (T y)(t)) ((T x)(s) (T y)(s)) : t, s [, 1], t s } < ε 2 + ε 2 = ε. This proves that the operator T is continuous at the point x Br δ for the norm α. Since Br δ is compact in H α [, 1], applying the classical Schauder fixed point theorem we obtain the desired result. 4. Example To present an example illustrating our result we need some previous results. Definition 4.1. A function f : R + R + is said to be subadditive if f(x + y) f(x) + f(y) for any x, y R +. Lemma 4.2. Suppose that f : R + R + is subadditive and y x then f(x) f(y) f(x y). Proof. Since f(x) = f(x y + y) f(x y) + f(y) the result follows.

EJDE-214/31 SOLVABILITY OF A QUADRATIC INTEGRAL EQUATION 7 Remark 4.3. From Lemma 4.2, we infer that if f : R + R + is subadditive then f(x) f(y) f( x y ) for any x, y R +. Lemma 4.4. Let f : R + R + be a concave function with f() =. Then f is subadditive. Proof. For x, y R + and, since f is concave and f() =, we have ( x f(x) = f (x + y) + y ) x + y x + y x f(x + y) + y x + y x + y f() = x f(x + y) x + y and ( x f(y) = f x + y + x f()f(x + y) + y x + y = y f(x + y). x + y y ) (x + y) x + y f(x + y) x + y Adding these inequalities, we obtain f(x) + f(y) x f(x + y) + y f(x + y) = f(x + y). x + y x + y This completes the proof. Remark 4.. Let f : R + R + be the function defined by f(x) = p x, where p > 1. Since this function is concave (because f (x) for x > ) and f() =, Lemma 4.4 says us that f is subadditive. By Remark 4.3, we have for any x, y R +. f(x) f(y) = p x p y p x y Example 4.6. Let us consider the quadratic integral equation x(t) = arctan 4 q sin t + ˆq + x(t) mt2 + τ x ( τ ) dτ, τ + 1 t [, 1], (4.1) where, q, ˆq and m are nonnegative constants. Notice that (4.1) is a particular case of (1.1), where p(t) = arctan q sin t + ˆq, k(t, τ) = 4 mt 2 + τ and r(τ) = τ τ+1. In what follows, we will prove that assumptions (i)-(iv) of Theorem 3.1 are satisfied. Since the inverse tangent function is concave (because its second derivative is nonpositive) and its value at zero is zero, taking into account Remarks 4.3 and 4., we have p(t) p(s) = arctan q sin t + ˆq arctan q sin s + ˆq ( arctan q sin t + ˆq q sin s + ˆq ) q sin t + ˆq q sin s + ˆq q sin t sin s q t s 1/,

8 J. CABALLERO, M. A. DARWISH, K. SADARANGANI EJDE-214/31 where we have used that arctan x x for x and sin x sin y x y for any x, y R. This says that p H 1 [, 1] and, moreover, H1/ p = q. Therefore, assumptions (i) of Theorem 3.1 is satisfied. Note that p 1 = p() + sup { p(t) p(s) : t, s [, 1], t s } t s 1/ arctan ˆq + H 1/ p = arctan ˆq + q. Since for any t, s, τ [, 1], we have (see, Remark 4.) k(t, τ) k(s, τ) = 4 mt 2 + τ 4 ms 2 + τ 4 mt 2 ms 2 = 4 m 4 t 2 s 2 = 4 m 4 t + s 4 t s 4 m 4 2 t s 1/4 = 4 m 4 2 t s 1/2 t s 1/ 4 2m t s 1/, assumption (ii) of Theorem 3.1 is satisfied with K β = K 1 = 4 2m. It is clear that r(τ) = τ τ+1 satisfies assumption (iii). In our case, the constant K is given by K = sup { k(t, τ) dτ : t [, 1] } = sup { 4 mt2 + τ dτ : t [, 1] } = sup { 4 ( 4 (mt2 + 1) 4 ) } m t 1 = 4 ( 4 (m + 1) 4 ) m. Therefore, the inequality appearing in assumption (iv) takes the form ( p 1 (2K + K β) = arctan ˆq + )( 8 [ q 4 (m + 1) 4 m ] + 4 2m) < 1 4. It is easily seen that the above inequality is satisfied when, for example, ˆq =, q = 1 2 and m = 1. Therefore, using Theorem 3.1, we infer that (4.1) for ˆq =, 2 q = 1 2 and m = 1 has at least one solution in the space H 2 α [, 1] with < α < 1/. Note that in (4.1), we can take as r(τ) a particular functions such as r(τ) = {e τ }, where { } denotes the fractional part. Remark 4.7. Note that any solution x(t) of (1.1), i.e., x(t) = p(t) + x(t) k(t, τ) x(r(τ)) dτ, t [, 1],

EJDE-214/31 SOLVABILITY OF A QUADRATIC INTEGRAL EQUATION 9 satisfies that its zeroes are also zeroes of p(t). From this, we infer that if p(t) for any t [, 1] then x(t) for any t [, 1]. By Bolzano s theorem, this means that the solution x(t) of Eq(1.1) does not change of sign on [, 1] when p(t) for any t [, 1]. These questions seem to be interesting from a practical standpoint.. Appendix Suppose that < α < β 1 and by Br β we denote the ball centered at θ and radius r in the space H β [a, b]; i.e., Br β = {x H β [a, b] : x β r}. Then Br β is a compact subset in the space H α [a, b]. In fact, by Theorem 2.3, since Br β is a bounded subset in H β [a, b], Br β is a relatively compact subset of H α [a, b]. In the sequel, we will prove that Br β is a closed subset of H α [a, b]. Suppose that (x n ) Br β We have to prove that x Br β. α and x n x with x Hα [a, b]. α Since x n x, for ε > given we can find n N such that x x α ε for any n n, or, equivalently, x n (a) x(a) + sup { (x n (t) x(t)) (x n (s) x(s)) : t, s [a, b], t s } < ε, (.1) for any n n. Particularly, this implies that x n (a) x(a). Moreover, if in (.1) we put s = a then we get sup { (x n (t) x(t)) (x n (a) x(a)) t a α : t, s [a, b], t a } < ε, for any n n. This says that (x n (t) x(t)) (x n (a) x(a)) < ε t a α, for any n n and for any t [a, b]. (.2) Therefore, for any n n and any t [a, b] by (.1) and (.2), we have x n (t) x(t) (x n (t) x(t)) (x n (a) x(a)) + x n (a) x(a) From this, it follows that < ε(t a) α + ε = ε(1 + (b a) α ). x n x. (.3) Next, we will prove that x B β r. In fact, as (x n ) B β r H β [a, b], we have that x n (t) x n (s) r for any t, s [a, b] with t s. Consequently, x n (t) x n (s) r for any t, s [a, b]. Letting n and taking into account (.3), we obtain for any t, s [a, b]. Therefore, x(t) x(s) r x(t) x(s) r

1 J. CABALLERO, M. A. DARWISH, K. SADARANGANI EJDE-214/31 for any t, s [a, b] with t s, and this means that x B β r. This completes the proof. References [1] C. Bacoţiu; Volterra-Fredholm nonlinear systems with modified argument via weakly Picard operators theory, Carpath. J. Math. 24(2) (28), 1 19. [2] J. Banaś, R. Nalepa; On the space of functions with growths tempered by a modulus of continuity and its applications, J. Func. Spac. Appl., (213), Article ID 82437, 13 pages. [3] M. Benchohra, M.A. Darwish; On unique solvability of quadratic integral equations with linear modification of the argument, Miskolc Math. Notes 1(1) (29), 3 1. [4] J. Caballero, B. López, K. Sadarangani; Existence of nondecreasing and continuous solutions of an integral equation with linear modification of the argument, Acta Math. Sin. (English Series) 23 (27), 1719 1728. [] M. Dobriţoiu; Analysis of a nonlinear integral equation with modified argument from physics, Int. J. Math. Models and Meth. Appl. Sci. 3(2) (28), 43 412. [6] T. Kato, J.B. Mcleod; The functional-differential equation y (x) = ay(λx)+by(x), Bull. Amer. Math. Soc., 77 (1971), 891 937. [7] M. Lauran; Existence results for some differential equations with deviating argument, Filomat 2(2) (211), 21 31. [8] V. Mureşan; A functional-integral equation with linear modification of the argument, via weakly Picard operators, Fixed Point Theory, 9(1) (28), 189 197. [9] V. Mureşan; A Fredholm-Volterra integro-differential equation with linear modification of the argument, J. Appl. Math., 3(2) (21), 147 18. Josefa Caballero Departamento de Matemáticas, Universidad de Las Palmas de Gran Canaria, Campus de Tafira Baja, 317 Las Palmas de Gran Canaria, Spain E-mail address: fefi@dma.ulpgc.es Mohamed Abdalla Darwish Department of Mathematics, Sciences Faculty for Girls, King Abdulaziz University, Jeddah, Saudi Arabia. Department of Mathematics, Faculty of Science, Damanhour University, Damanhour, Egypt E-mail address: dr.madarwish@gmail.com Kishin Sadarangani Departamento de Matemáticas, Universidad de Las Palmas de Gran Canaria, Campus de Tafira Baja, 317 Las Palmas de Gran Canaria, Spain E-mail address: ksadaran@dma.ulpgc.es