Advances in Difference Equations
Volume 2009 (2009), Article ID 728484, 12 pages
doi:10.1155/2009/728484
Research Article

Existence and Uniqueness of Positive Solution for Singular BVPs on Time Scales

1Departamento de Matemática Aplicada, Facultade de Matemáticas, Universidade de Santiago de Compostela, 15782 Galicia, Spain
2Departamento de Análise Matemática, Facultade de Matemáticas, Universidade de Santiago de Compostela, 15782 Galicia, Spain

Received 27 March 2009; Accepted 12 May 2009

Academic Editor: Alberto Cabada

Copyright © 2009 Ana Gómez González and Victoria Otero-Espinar. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

This paper is devoted to derive some sufficient conditions for the existence and uniqueness of positive solutions to a singular second-order dynamic equation with Dirichlet boundary conditions.

1. Introduction

Hilger [1] introduced the notion of time scale in 1990 in order to unify the theory of continuous and discrete calculus. The field of dynamic equations on time scale contains, links, and extends the classical theory of differential and difference equations, besides many others. There are more time scales than just (corresponding to the continuous case) and (discrete case) and hence many more classes of dynamic equations.

By time scale we mean a closed subset of the real numbers. Let 𝕋 be an arbitrary time scale. We assume that 𝕋 has the topology that it inherits from the standard topology on . Assume that 𝑎 < 𝑏 are points in 𝕋 and define the time scale interval [ 𝑎 , 𝑏 ] 𝕋 = { 𝑡 𝕋 𝑎 𝑡 𝑏 } . For 𝑡 𝕋 , define the forward jump operator 𝜎 𝕋 𝕋 by 𝜎 ( 𝑡 ) = i n f { 𝑠 𝕋 𝑠 > 𝑡 } and the backward jump operator 𝜌 𝕋 𝕋 by 𝜌 ( 𝑡 ) = s u p { 𝑠 𝕋 𝑠 < 𝑡 } . In this definition we put 𝜎 ( 𝑡 ) = 𝑡 if 𝕋 attains a maximum 𝑡 and 𝜌 ( 𝑡 ) = 𝑡 if 𝕋 attains a minimum 𝑡 . If 𝜎 ( 𝑡 ) > 𝑡 , 𝑡 is said to be right-scattered and if 𝜎 ( 𝑡 ) = 𝑡 , 𝑡 is said to be right-dense. If 𝜌 ( 𝑡 ) < 𝑡 , 𝑡 is said to be left-scattered and if 𝜌 ( 𝑡 ) = 𝑡 , 𝑡 is said to be left-dense.

A function 𝑓 𝕋 is said to be rd-continuous provided it is continuous at all right-dense points of 𝕋 , and its left-sided limit exists at left-dense points of 𝕋 . For 𝑡 𝕋 , the delta derivative 𝑓 Δ ( 𝑡 ) of 𝑓 at 𝑡 is defined to be the number (if exists) such that for given 𝜖 > 0 , there exists a neighborhood 𝑈 of 𝑡 such that See [2] for general theory about time scales.

The problem we will consider in this work is of the type

Under this general form it included the Emden-Fowler equation, which arises in several fields, such as the following:

(i)Astrophysics: related to the stellar structure (gaseous dynamics). In this case the fundamental problem is to investigate the equilibrium configuration of the mass of spherical clouds of gas. (ii)Gas dynamics and fluid mechanics. The solutions of physical interest in this context are bounded nonoscillatory and possess a positive zero. (iii)Relativistic mechanics. (iv)Nuclear physics. (v)Chemically reacting systems: in the theory of diffusion and reaction this equation appears as governing the concentration 𝑢 of a substance which disappears by an isothermal reaction at each point of a slab of catalyst.

We refer to Wong [3], for a general historical overview about this equation.

Many works on this equation have been written in the continuous case, and we can cite among others, [4, 5] or [6].

On the discrete case we find the book [7] which studies the oscillation properties of the solutions of different difference equations. For the specific problem 𝑢 Δ Δ ( 𝑡 ) + 𝑝 ( 𝑡 ) 𝑢 𝛾 ( 𝜎 ( 𝑡 ) ) = 0 , where 𝑝 0 and 𝛾 quotient of odd positive numbers, also oscillation properties were studied in [8].

On time scales some results on existence and uniqueness of solutions in the sense of distribution for this equation can be found in the article [9]. Considering classical solutions, oscillation properties have also been studied, in works such as [10] (with delay) or [11].

In the present paper we present some results on time scales considering classical solutions which generalize the ones from the continuous case.

2. Lower and Upper Solutions Method

Let 𝑎 , 𝑏 𝕋 , such that 𝑎 < 𝜌 ( 𝑏 ) . Let us put 𝐽 = [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 , 𝐽 𝜅 = [ 𝑎 , 𝜎 ( 𝑏 ) ] 𝕋 , and ( 𝐽 𝜅 ) 𝑜 = [ 𝑎 , 𝜎 ( 𝑏 ) ) 𝕋 if 𝑎 𝜎 ( 𝑎 ) and 𝐽 = ( 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 , 𝐽 𝜅 = ( 𝑎 , 𝜎 ( 𝑏 ) ] 𝕋 , and ( 𝐽 𝜅 ) 𝑜 = ( 𝑎 , 𝜎 ( 𝑏 ) ) 𝕋 if 𝑎 = 𝜎 ( 𝑎 ) .

We consider the second-order dynamic equation with Dirichlet boundary conditions, where ( H 1 ) , satisfies the following condition.

𝑥 𝒜 (i) For every 𝑓 ( , 𝑥 ) 𝐶 r d ( ( 𝐽 𝜅 ) 𝑜 ) , , 𝑓 ( 𝑡 , ) (ii) 𝒜 is continuous on 𝑡 ( 𝐽 𝜅 ) 𝑜 uniformly in 𝐸 = 𝐶 r d ( 𝐽 𝜅 ) 𝑜 , + 𝑎 𝜎 ( 𝑏 ) 𝜎 ( 𝜎 ( 𝑠 ) 𝑎 ) 2 ( 𝑏 ) 𝑠 ( 𝑠 ) Δ 𝑠 < + . ( 2 . 1 ) .

For convenience, we denote We say that ( H 2 ) satisfies the condition ( 𝐽 𝜅 ) 𝑜 × 𝒜 on 𝐸 if there exists a function ( H 2 ) such that

| | | | 𝑓 ( 𝑡 , 𝑥 ) ( 𝑡 ) , ( 𝑡 , 𝑥 ) . ( 2 . 2 )

Definition 2.1. A solution of 𝑢 𝐶 2 r d ( ( 𝑎 , 𝑏 ) 𝕋 ) is a function 𝑢 ( 𝑡 ) 𝒜 such that 𝑡 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 , for all ( 𝑃 ) , which satisfies the equalities on 𝑡 ( 𝐽 𝜅 ) 𝑜 for each 𝐶 2 r d ( 𝑎 , 𝑏 ) 𝕋 = 𝑦 𝐶 𝑎 , 𝜎 2 ( 𝑏 ) 𝕋 , 𝑦 Δ Δ ( 𝐽 𝜅 ) 𝑜 , 𝑦 Δ Δ 𝐶 r d ( 𝑎 , 𝑏 ) 𝕋 . ( 2 . 3 ) , where

Definition 2.2. We say that ( 𝑃 ) is a lower solution of 𝛼 ( 𝑡 ) 𝒜 if 𝑡 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 , for all 𝛼 Δ Δ ( 𝑡 ) 𝑓 ( 𝑡 , 𝛼 𝜎 ( 𝑡 ) ) , 𝑡 ( 𝐽 𝜅 ) 𝑜 , 𝛼 𝜎 ( 𝑎 ) 𝐴 , 𝛼 2 ( 𝑏 ) 𝐵 . ( 2 . 4 ) and An upper solution ( 𝑃 ) of 𝛼 is defined similarly by reversing the previous inequalities.

We have the following result.

Theorem 2.3. Let 𝛽 and ( 𝑃 ) be, respectively, a lower and upper solution for problem 𝛼 𝛽 , such that [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 on 𝑓 . If ( H 1 ) satisfies ( H 2 ) and the conditions 𝒟 𝛽 𝛼 = ( 𝑡 , 𝑥 ) ( 𝐽 𝜅 ) 𝑜 × 𝛼 𝜎 ( 𝑡 ) 𝑥 𝛽 𝜎 ( 𝑡 ) , ( 2 . 5 ) on then problem ̃ 𝑢 has at least one solution 𝛼 ̃ 𝑢 𝛽 such that [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 on 𝑢 Δ Δ ( 𝑡 ) = 𝑓 ( 𝑡 , 𝑢 𝜎 ( 𝑡 ) ) , 𝑡 ( 𝐽 𝜅 ) 𝑜 , 𝑢 𝜎 ( 𝑎 ) = 𝐴 , 𝑢 2 ( 𝑏 ) = 𝐵 . ( ( 𝑃 𝑚 ) ) .

Proof. We consider the following modified problem: with Due to the hypothesis it can be easily checked that 𝑓 and 𝑢 are satisfied by the function ( 𝑃 𝑚 ) .
Note that, if 𝛼 𝑢 𝛽 is a solution of [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 such that 𝑢 on ( 𝑃 ) , then 𝛼 𝑢 𝛽 is a solution of [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 , also satisfying 𝑢 on ( 𝑃 𝑚 ) .
To show that any solution 𝛼 of 𝛽 is between 𝑣 ( 𝑡 ) = 𝛼 ( 𝑡 ) 𝑢 ( 𝑡 ) and 𝑡 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 , let 𝑣 ( 𝑡 ) > 0 , and suppose that there exists 𝑣 ( 𝑎 ) 0 such that 𝑣 ( 𝜎 2 ( 𝑏 ) ) 0 . As 𝑡 0 ( 𝑎 , 𝜎 2 ( 𝑏 ) ) 𝕋 and 𝑣 𝑡 0 = m a x 𝑣 ( 𝑡 ) , 𝑡 𝑎 , 𝜎 2 ( 𝑏 ) 𝕋 > 0 , ( 2 . 7 ) , then there exists 𝑣 ( 𝑡 ) < 𝑣 ( 𝑡 0 ) with and 𝑡 0 for ( 𝜎 𝜌 ) ( 𝑡 0 ) = 𝑡 0 . The point 𝑣 Δ Δ ( 𝜌 ( 𝑡 0 ) ) 0 is not simultaneously left-dense and right-scattered (see [12, Theorem  2.1]) (this implies that 𝑣 Δ Δ 𝜌 𝑡 0 = 𝑢 Δ Δ 𝑡 0 𝛼 Δ Δ 𝑡 0 𝑓 𝜌 𝑡 0 , 𝑢 𝜎 𝜌 𝑡 0 𝜌 𝑡 + 𝑓 0 , 𝛼 𝜎 𝜌 𝑡 0 𝛼 𝑡 = 0 𝑡 𝑢 0 𝛼 𝑡 1 + 0 𝑡 𝑢 0 < 0 . ( 2 . 8 ) ), and we have that 𝑣 Δ Δ ( 𝜌 ( 𝑡 0 ) ) > 0 (see [12]), so So 𝑢 ( 𝑡 ) 𝛽 ( 𝑡 ) , 𝑡 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 , that is a contradiction. And so we have proved that ( 𝑃 𝑚 ) .
Analogously it can be proved that 𝑁 𝐶 ( [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) 𝐶 ( [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) .
We only need to prove that problem 𝑁 𝑢 ( 𝑡 ) = 𝜙 ( 𝑡 ) + 𝑎 𝜎 ( 𝑏 ) 𝐺 ( 𝑡 , 𝑠 ) 𝑓 ( 𝑠 , 𝑢 𝜎 ( 𝑠 ) ) Δ 𝑠 , ( 2 . 9 ) has at least one solution.
Consider now the operator 𝑡 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 , defined by for each 𝑥 Δ Δ 𝑥 𝜎 = 0 , ( 𝑎 ) = 𝑥 2 ( 𝑏 ) = 0 , ( 2 . 1 1 ) , where (see [2]) is Green's function of the problem and for 𝑥 Δ Δ = 0 is the solution of 𝜙 ( 𝜎 2 ( 𝑏 ) ) = 𝐵 such that 𝐺 ( 𝑡 , 𝑠 ) > 0 and ( 𝑎 , 𝜎 2 ( 𝑏 ) ) 𝕋 × ( 𝑎 , 𝜎 2 ( 𝑏 ) ) 𝕋 , 𝐺 ( 𝑡 , ) .
Clearly, [ 𝑎 , 𝜎 ( 𝑏 ) ] 𝕋 on 𝐺 ( , 𝑠 ) is rd-continuous on [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 and 𝑁 𝑢 is continuous on 𝐶 ( [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) .
The function 𝑓 defined by (2.9) belongs to ( H 1 ) because ( H 2 ) checks the conditions ( 𝐽 𝜅 ) 𝑜 × and 𝐺 ( 𝑡 , 𝑠 ) 𝑠 ( 1 𝑠 ) on 𝑡 , 𝑠 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 and 𝑢 𝐶 ( [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) , for each ( 𝑃 𝑚 ) .
It is obvious that 𝑢 = 𝑁 𝑢 is a solution of 𝑁 if and only if 𝑁 . So the problem now is ensuring the existence of fixed-points of 𝑁 ( 𝐶 ( [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) ) .
First of all, 𝑁 is well defined, is continuous, and 𝑁 ( 𝐶 ( [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) ) is a bounded set. The existence of a fixed-point of 𝑁 ( 𝐶 ( [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) ) follows from the Schauder fixed-point theorem, once we have checked that 𝐸 is relatively compact, that using the Ascoli-Arzela theorem is equivalent to proving that 𝑓 is an equicontinuous family.
Let ( H 2 ) be the function related to 𝑁 𝑢 by condition | | ( 𝑁 𝑢 ) Δ | | = 1 ( 𝑡 ) 𝜎 2 | | | | ( 𝑏 ) 𝑎 ( 𝐵 𝐴 ) 𝑡 𝑎 ( 𝜎 ( 𝑠 ) 𝑎 ) 𝑓 ( 𝑠 , 𝑢 𝜎 + ( 𝑠 ) ) Δ 𝑠 𝑡 𝜎 ( 𝑏 ) 𝜎 2 ( 𝑓 𝑏 ) 𝜎 ( 𝑠 ) ( 𝑠 , 𝑢 𝜎 ( | | | | 1 𝑠 ) ) Δ 𝑠 𝜎 2 | | | | + ( 𝑏 ) 𝑎 𝐵 𝐴 𝑡 𝑎 ( 𝜎 ( 𝑠 ) 𝑎 ) ( 𝑠 ) Δ 𝑠 + 𝑡 𝜎 ( 𝑏 ) 𝜎 2 ( 𝑏 ) 𝜎 ( 𝑠 ) 1 ( 𝑠 ) Δ 𝑠 = 𝜎 2 | | | | . ( 𝑏 ) 𝑎 𝐵 𝐴 + 𝜆 ( 𝑡 ) ( 2 . 1 3 ) . We compute the first derivative of 𝜆 𝐿 1 ( ( 𝐽 𝜅 ) 𝑜 ) using [2, Theorem  1.117]
Finally it is enough to check that 𝐸 , using integration by parts we obtain due to 𝑔 ( 𝐽 𝜅 ) 𝑜 × ( 0 , + ) , and the fact And so the result is proved.

3. Existence and Uniqueness of Positive Solution

Let 𝒜 = ( 0 , + ) in the condition 𝑢 Δ Δ ( 𝑡 ) = 𝑔 ( 𝑡 , 𝑢 𝜎 ( 𝑡 ) ) , 𝑡 ( 𝐽 𝜅 ) 𝑜 , 𝑢 𝜎 ( 𝑎 ) = 𝑢 2 ( 𝑏 ) = 0 . ( ( 𝑄 ) ) , where ( 𝑄 ) , and consider the problem We will deduce the existence of solution to 𝐿 > 0 by supposing that the following hypothesis holds.

𝐷 ( 𝐽 𝜅 ) 𝑜 𝜀 = 𝜀 𝐷 > 0 There exists a constant ] 𝑔 ( 𝑡 , 𝑥 ) > 𝐿 , ( 𝑡 , 𝑥 ) 𝐷 × ( 0 , 𝜀 . ( 3 . 1 ) such that for any compact set ( H 1 ) , there is ( H 3 ) :

Theorem 3.1. Suppose that ( H 2 ) and ( 𝐽 𝜅 ) 𝑜 × [ 𝛿 , + ) hold. If, for any ( 𝑄 ) satisfies the condition { 𝑎 𝑛 } 𝑛 1 , { 𝑏 𝑛 } 𝑛 1 ( 𝐽 𝜅 ) 𝑜 on { 𝑎 𝑛 } 𝑛 1 ( 𝑎 , ( 𝑎 + 𝜎 ( 𝑏 ) ) / 2 ) 𝕋 , then problem 𝑎 has at least one solution.

Proof. Let's consider 𝑎 = 𝜎 ( 𝑎 ) as two sequences such that 𝑎 𝑛 = 𝑎 is strictly decreasing to 𝑛 1 if 𝑎 < 𝜎 ( 𝑎 ) , and { 𝑏 𝑛 } 𝑛 1 ( ( 𝑎 + 𝜎 ( 𝑏 ) ) / 2 , 𝜎 ( 𝑏 ) ) 𝕋 for all 𝜎 ( 𝑏 ) if 𝜌 ( 𝜎 ( 𝑏 ) ) = 𝜎 ( 𝑏 ) , 𝑏 𝑛 = 𝜌 ( 𝜎 ( 𝑏 ) ) , and 𝑛 1 is strictly increasing to 𝜌 ( 𝜎 ( 𝑏 ) ) < 𝜎 ( 𝑏 ) if 𝐷 𝑛 = [ 𝑎 𝑛 , 𝑏 𝑛 ] 𝕋 ( 𝐽 𝜅 ) 𝑜 , 𝑛 1 for all 𝜀 𝑛 > 0 if 𝑔 ( 𝑡 , 𝑥 ) > 𝐿 . We denote as ( 𝑡 , 𝑥 ) 𝐷 𝑛 × ( 0 , 𝜀 𝑛 ] .
Due to the first hypothesis, we can then ensure the existence of { 𝜀 𝑛 } such that l i m 𝑛 + 𝜀 𝑛 = 0 , for all 𝛾 [ 𝑎 , 𝑎 1 ] 𝕋 + . We can suppose, without restriction that 𝛾 ( 𝑎 ) = 0 is a decreasing sequence and 𝑎 𝑎 1 .
Consider the function 𝛾 ( 𝑡 ) = 𝜀 2 , such that 𝑡 [ 𝑎 2 , 𝑎 1 ] , 𝛾 ( 𝑡 ) = 𝜀 𝑛 , and if 𝑡 𝐷 𝑛 𝐷 𝑛 1 then 𝑛 3 for 𝛾 , for all 𝑡 [ 𝑎 , 𝑎 1 ] , with 𝛾 1 ( 1 𝑡 ) = 𝜎 2 ( 𝑏 ) 𝑎 𝑡 𝑎 𝛾 ( 𝑠 ) Δ 𝑠 𝛾 ( 𝑡 ) ( 3 . 2 ) . Since 𝑖 = 2 , 3 is nondecreasing, we obtain that for 𝛾 𝑖 ( 1 𝑡 ) = 𝜎 2 ( 𝑏 ) 𝑎 𝑡 𝑎 𝛾 𝑖 1 ( 𝑠 ) Δ 𝑠 𝛾 ( 𝑡 ) . ( 3 . 3 ) is continuous and increasing. Repeating this argument twice, for 𝛾 3 ( 𝑡 ) 𝜀 𝑛 , 𝑡 𝐷 𝑛 𝐷 𝑛 1 we define So ̃ 𝛾 [ 𝑏 1 , 𝜎 2 ( 𝑏 ) ] 𝕋 + is a convex function verifying ̃ 𝛾 ( 𝜎 2 ( 𝑏 ) ) = 0 , ̃ 𝛾 ( 𝜎 ( 𝑏 ) ) = 0 , ̃ 𝛾 ( 𝑡 ) = 𝜀 2 , 𝑡 [ 𝑏 1 , 𝑏 2 ] .
Analogously, we can consider ̃ 𝛾 ( 𝑡 ) = 𝜀 𝑛 , such that 𝑡 𝐷 𝑛 𝐷 𝑛 1 , for all 𝑛 3 and ̃ 𝛾 0 = ̃ 𝛾 , for all 𝑖 = 1 , 2 , 3 , with 𝑡 [ 𝑏 1 , 𝜎 2 ( 𝑏 ) ] . Taking ̃ 𝛾 𝑖 1 ( 𝑡 ) = 𝜎 2 ( 𝑏 ) 𝑎 𝜎 2 𝑡 ( 𝑏 ) ̃ 𝛾 𝑖 1 ( 𝑠 ) Δ 𝑠 ̃ 𝛾 ( 𝑡 ) ( 3 . 4 ) , we obtain, for ̃ 𝛾 3 𝐶 2 ( [ 𝑏 1 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) , that for ̃ 𝛾 3 ( 𝑡 ) 𝜀 𝑛 , 𝑡 𝐷 𝑛 𝐷 𝑛 1 , 𝑛 2 is continuous and decreasing, and 𝛼 ( 𝑡 ) a convex function such that 𝛼 𝐶 2 ( [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) .
We now define with 𝑡 [ 𝑎 1 , 𝑏 1 ] 𝕋 a convenient function, so that 𝛼 𝐶 2 ( [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 ) , and 𝛼 ( 𝑎 ) = 𝛼 ( 𝜎 2 ( 𝑏 ) ) = 0 , 𝛼 ( 𝑡 ) > 0 for all 𝑡 ( 𝑎 , 𝜎 ( 𝑏 ) ) 𝕋 , 𝛼 ( 𝑡 ) 𝜀 1 .
So 𝑡 𝐷 1 is a function such that 𝛼 ( 𝑡 ) 𝜀 𝑛 for 𝑡 𝐷 𝑛 𝐷 𝑛 1 , 𝑛 2 for 𝑔 ( 𝑡 , 𝑥 ) > 𝐿 , ( 𝑡 , 𝑥 ) ( 𝐽 𝜅 ) 𝑜 × { 𝑥 ( 0 , + ) 0 < 𝑥 𝛼 ( 𝑡 ) } . ( 3 . 6 ) , and 𝑚 0 = m i n { 1 , 𝐿 / ( 𝛼 Δ Δ + 1 ) } , for 𝐹 ( 𝑡 , 𝑥 ) 𝑔 ( 𝑡 , 𝑥 ) .
In this way, we note that
Let 𝐹 .
Let ( H 1 ) , for all 𝑣 𝐶 2 r d ( ( 𝑎 , 𝜎 2 ( 𝑏 ) ) 𝕋 ) , with 𝑣 Δ Δ = 𝐹 ( 𝑡 , 𝑣 𝜎 ( 𝑡 ) ) , ( 3 . 7 ) in the conditions 𝑣 ( 𝑎 ) 0 , 𝑣 ( 𝜎 2 ( 𝑏 ) ) 0 . We will prove that if 𝑣 ( 𝑡 ) > 0 is any solution of with 𝑣 ( 𝑡 ) 𝑚 0 𝛼 ( 𝑡 ) , 𝑡 𝑎 , 𝜎 2 ( 𝑏 ) 𝕋 . ( 3 . 8 ) and 𝑡 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 for all 𝑣 ( 𝑡 ) 𝑚 0 𝛼 ( 𝑡 ) < 0 , then, Suppose there exists 𝑣 Δ Δ 𝜌 𝑡 𝑚 0 𝛼 Δ Δ 𝜌 𝑡 , ( 3 . 9 ) , such that 𝜌 𝑡 𝐿 < 𝐹 , 𝑣 𝜎 𝜌 𝑡 = 𝑣 Δ Δ 𝜌 𝑡 𝑚 0 𝛼 Δ Δ 𝜌 𝑡 < 𝑚 0 𝛼 Δ Δ + 1 𝐿 , ( 3 . 1 0 ) . Then, we can assure, using arguments analogous to the ones in the proof of Theorem 2.3, that there exists 𝑛 verifying which implies that which is a contradiction.
We define now, for each 𝜏 𝑛 𝑎 ( 𝑡 ) = m a x 𝑛 , m i n 𝑡 , 𝑏 𝑛 . ( 3 . 1 2 ) where, for each ̃ 𝑔 𝑛 For each ( 𝐽 𝜅 ) 𝑜 × ( 0 , + ) we have that ̃ 𝑔 𝑛 ( 𝑡 , 𝑥 ) 𝑔 ( 𝑡 , 𝑥 ) is a function verifying ( 𝑡 , 𝑥 ) 𝐽 × ( 0 , + ) on ̃ 𝑔 𝑛 ( 𝑡 , 𝑥 ) = 𝑔 ( 𝑡 , 𝑥 ) , and 𝑡 𝐷 𝑛 , for all { ̃ 𝑔 𝑛 } 𝑛 and 𝑔 , for 𝐷 × ( 0 , + ) .
The sequence 𝐷 ( 𝐽 𝜅 ) 𝑜 converges to 𝑔 1 ( 𝑡 , 𝑥 ) = ̃ 𝑔 1 ( 𝑡 , 𝑥 ) uniformly in every set of the form 𝑛 > 1 , where 𝑔 𝑛 + 1 𝑔 ( 𝑡 , 𝑥 ) = m i n 𝑛 ( 𝑡 , 𝑥 ) , ̃ 𝑔 𝑛 + 1 ( 𝑡 , 𝑥 ) , ( 3 . 1 3 ) is a compact set.
Defining, by induction, 𝑛 and for 𝑔 𝑛 we have that, for each ( 𝐽 𝜅 ) 𝑜 × ( 0 , + ) , the function 𝑔 1 𝑔 2 𝑔 𝑛 𝑔 , satisfies the condition { 𝑔 𝑛 } 𝑛 on 𝑔 . As well 𝐷 × ( 0 , + ) and 𝐷 ( 𝐽 𝜅 ) 𝑜 converges to 𝑔 𝑛 ( 𝑡 , 𝑥 ) = 𝑔 ( 𝑡 , 𝑥 ) , 𝑡 [ 𝑎 𝑛 , 𝑏 𝑛 ] , 𝑥 ( 0 , + ) uniformly, in every set of the form 𝑢 Δ Δ ( 𝑡 ) + 𝑔 𝑛 ( 𝑡 , 𝑢 𝜎 ( 𝑡 ) ) = 0 , 𝑡 ( 𝐽 𝜅 ) 𝑜 , 𝑢 𝜎 ( 𝑎 ) = 𝑢 2 ( 𝑏 ) = 𝜀 𝑛 . ( ( ( 𝑄 ) 𝑛 ) ) , where 𝑐 ( 0 , 𝜀 𝑛 ] is a compact set.
It is also verified that 𝛼 𝑛 𝑐 .
Now we define the following problems: We will prove that for any 𝑐 = 𝛼 𝑛 ( 𝜎 2 ( 𝑏 ) ) 𝜀 𝑛 , the constant function 𝑔 𝑛 ( 𝑡 , 𝑐 ) > 0 , 𝑡 ( 𝐽 𝜅 ) 𝑜 , 𝑐 0 , 𝜀 𝑛 . ( 3 . 1 4 ) is a (strict) lower solution for 𝑛 = 1 .
It is obvious that 𝑐 ( 0 , 𝜀 1 ] , and 𝑔 1 ( 𝑡 , 𝑐 ) = ̃ 𝑔 1 𝑔 𝜏 ( 𝑡 , 𝑐 ) = m a x 1 𝜏 ( 𝑡 ) , 𝑐 , 𝑔 ( 𝑡 , 𝑐 ) 𝑔 1 ( 𝑡 ) , 𝑐 > 𝐿 . ( 3 . 1 5 ) . Now we have to prove that
For 𝑛 1 , let 𝑔 𝑛 + 1 ( 𝑡 , 𝑐 ) > 0 , 𝑡 ( 𝐽 𝜅 ) 𝑜 such that Suppose now that 𝑔 𝑛 + 1 𝑔 ( 𝑡 , 𝑐 ) = m i n 𝑛 ( 𝑡 , 𝑐 ) , ̃ 𝑔 𝑛 + 1 𝑔 ( 𝑡 , 𝑐 ) m i n 𝑛 𝜏 ( 𝑡 , 𝑐 ) , 𝑔 𝑛 + 1 ( 𝑡 ) , 𝑐 > 0 . ( 3 . 1 6 ) , for a given 𝑔 𝑛 𝑔 𝑛 + 1 , and we will check that ( 𝐽 𝜅 ) 𝑜 × ( 0 , + ) . Let 𝑢 𝑛 such that Thus the assertion is proved.
Moreover, as ( 𝑄 ) 𝑛 + 1 on ( 𝑄 ) 1 , it can be easily checked that any solution 𝑀 𝜀 1 of 𝑀 𝐶 r d ( ( 𝐽 𝜅 ) 𝑜 , + ) is an upper solution for | | | | 𝑔 ( 𝑡 , 𝑥 ) 𝑀 ( 𝑡 ) , 𝑡 ( 𝐽 𝜅 ) 𝑜 , 𝑥 𝑀 . ( 3 . 1 7 ) .
To show that problem | | 𝑔 𝜏 1 | | ( 𝑡 ) , 𝑥 𝑀 𝜏 1 ( 𝑡 ) 𝑅 , 𝑡 ( 𝐽 𝜅 ) 𝑜 , 𝑥 𝑀 , ( 3 . 1 8 ) has at least one solution. We fix a constant 𝑅 > 0 . From the assumption imposed, there exists a function 𝑞 ( 𝑡 ) = 𝑀 ( 𝑡 ) + 𝑅 such that Note that with 𝛽 𝐶 2 r d ( ( 𝑎 , 𝑏 ) 𝕋 ) is a suitable constant.
Set 𝑢 Δ Δ ( 𝑢 𝜎 𝑡 ) + 𝑞 ( 𝑡 ) = 0 , ( 𝑎 ) = 𝑢 2 ( 𝑏 ) = 𝑀 . ( 3 . 2 0 ) . We have that 𝛽 ( 𝑡 ) 𝑀 , and Let 𝛽 Δ Δ ( 𝑡 ) + 𝑔 1 ( 𝑡 , 𝛽 𝜎 ( 𝑡 ) ) = 𝑞 ( 𝑡 ) + 𝑔 1 ( 𝑡 , 𝛽 𝜎 ( 𝑡 ) ) 0 , ( 3 . 2 1 ) be a solution of the boundary value problem: It is easy to check that such a function exists and that ( 𝑄 ) 1 , for all 𝛼 1 𝜀 1 , and thus which implies that 𝛽 1 = 𝛽 is an upper solution of ( 𝑄 ) 1 .
Taking 𝛼 1 ( 𝑡 ) 𝛽 1 ( 𝑡 ) , we have that 𝑡 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 and 𝑢 1 are, respectively, a lower and upper solutions of ( 𝑄 ) 1 . Moreover 𝜀 1 = 𝛼 1 ( 𝑡 ) 𝑢 1 ( 𝑡 ) 𝛽 1 ( 𝑡 ) , 𝑡 𝑎 , 𝜎 2 ( 𝑏 ) 𝕋 . ( 3 . 2 2 ) , for all 𝛼 𝑛 𝜀 𝑛 , 𝛽 𝑛 𝑢 𝑛 1 . Then, by Theorem 2.3 there exists a solution ( 𝑄 ) 𝑛 , 𝑛 2 of { 𝑢 𝑛 } such that Proceeding by induction, using 𝜀 𝑛 𝑢 𝑛 ( 𝑡 ) 𝑢 𝑛 1 ( 𝑡 ) , lower and upper solution of 𝑡 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 , we obtain (via Theorem 2.3) a sequence 𝑢 𝑛 ( 𝑎 ) = 𝑢 𝑛 ( 𝜎 2 ( 𝑏 ) ) = 𝜀 𝑛 , 𝑛 2 of solutions of 𝑔 𝑛 𝑔 , such that ( 𝐽 𝜅 ) 𝑜 × ( 0 , + ) , for all 𝑢 𝑛 and ( 𝑄 ) 𝑛 .
Since 𝑢 𝑛 ( 𝑡 ) > 0 on 𝑡 ( 𝐽 𝜅 ) 𝑜 , and 𝑢 𝑛 ( 𝑡 ) 𝑚 0 𝛼 ( 𝑡 ) is a solution of 𝑡 [ 𝑎 , 𝜎 2 ( 𝑏 ) ] 𝕋 with ̃ 𝑢 ( 𝑡 ) = l i m 𝑛 + 𝑢 𝑛 ( 𝑡 ) ( 3 . 2 3 ) for all ( 𝑄 ) , then 𝑛 1 , for every 𝑚 0 𝛼 ( 𝑡 ) ̃ 𝑢 ( 𝑡 ) 𝑢 𝑛 ( 𝑡 ) , 𝑡 𝑎 , 𝜎 2 ( 𝑏 ) 𝕋 . ( 3 . 2 4 ) .
To end, we will prove that is a solution of problem 𝑛 = 𝑛 ( 𝐷 ) .
We have that, for any 𝐷 𝐷 𝑛 ,
Now let 𝑛 𝑛 be a compact interval. There exists an index 𝑡 𝐷 such that 0 = 𝑢 𝑛 Δ Δ ( 𝑡 ) + 𝑔 𝑛 𝑡 , 𝑢 𝜎 𝑛 ( 𝑡 ) = 𝑢 𝑛 Δ Δ ( 𝑡 ) + 𝑔 𝑡 , 𝑢 𝜎 𝑛 ( 𝑡 ) . ( 3 . 2 5 ) for all 𝑢 𝑛 . Let ( 𝑄 ) , if 𝑡 𝐷 , then Hence, | | 𝑔 | | s u p ( 𝑡 , 𝑥 ) , 𝑡 𝐷 , 𝑚 0 𝛼 ( 𝑡 ) 𝑥 𝑢 𝑛 ( 𝑡 ) < + . ( 3 . 2 6 ) verifies the first equality of problem ̃ 𝑢 for all ( 𝑄 ) , and for all 𝐷 . Moreover
Then by the Ascoli-Arzelá theorem, we can conclude that ̃ 𝑢 𝐶 ( ( 𝑎 , 𝜎 ( 𝑏 ) ) 𝕋 ) is a solution of ̃ 𝑢 Δ Δ + 𝑔 ( 𝑡 , ̃ 𝑢 𝜎 ( 𝑡 ) ) = 0 , 𝑡 ( 𝐽 𝜅 ) 𝑜 . ( 3 . 2 7 ) in ̃ 𝑢 ( 𝑎 ) = ̃ 𝑢 ( 𝜎 2 ( 𝑏 ) ) = l i m 𝑛 + 𝜀 𝑛 = 0 . Since the compact ̃ 𝑢 was arbitrary, we have that 𝑎 , and As 𝜀 > 0 , we just have to check the continuity of 𝑛 𝜀 in 𝑢 𝑛 𝜀 ( 𝑎 ) < 𝜀 and 𝑢 𝑛 𝜀 ( 𝑡 ) .
Let 𝑎 . Take 𝛿 = 𝛿 𝜀 > 0 in such a way that 0 < 𝑢 𝑛 𝜀 ( 𝑡 ) < 𝜀 , 𝑡 ( 𝑎 , 𝑎 + 𝛿 ) 𝕋 . ( 3 . 2 8 ) . From the continuity of 0 < 𝑚 0 𝛼 ( 𝑡 ) ̃ 𝑢 ( 𝑡 ) 𝑢 𝑛 𝜀 ( 𝑡 ) < 𝜀 , 𝑡 ( 𝑎 , 𝑎 + 𝛿 ) 𝕋 . ( 3 . 2 9 ) at 𝜎 2 ( 𝑏 ) , it follows that we can find a constant ( 𝑄 ) such that So Using the same argument the continuity at 𝑡 ( 𝐽 𝜅 ) 𝑜 is proved.

In order to prove the uniqueness of the solution to problem ( 𝑄 ) we have the following result.

Theorem 3.2. Under the hypotheses of Theorem 3.1, if ( 𝑄 ) is strictly decreasing in 𝑣 1 , for each 𝑣 2 , then problem ( 𝑄 ) has a unique solution.

Proof. By Theorem 3.1 the problem 𝑡 ( 𝐽 𝜅 ) 𝑜 has at least one solution.
Suppose that there exist 𝑣 1 ( 𝑡 ) > 𝑣 2 ( 𝑡 ) and 𝑧 ( 𝑡 ) = 𝑣 1 ( 𝑡 ) 𝑣 2 ( 𝑡 ) , solutions of 𝑡 0 ( 𝑎 , 𝜎 2 ( 𝑏 ) ) 𝕋 and 𝑧 ( 𝑡 0 ) > 0 such that 𝑧 Δ Δ ( 𝜌 ( 𝑡 0 ) ) 0 . If this occurs, setting 𝑔 ( 𝑡 , 𝑥 ) we can find 𝑥 such that 𝑧 Δ Δ 𝜌 𝑡 0 𝜌 𝑡 = 𝑔 0 , 𝑣 𝜎 1 𝜌 𝑡 0 𝜌 𝑡 𝑔 0 ,