Abstract
We prove the existence of a curve (with respect to the scalar delay) of periodic positive solutions for a smooth model of Cooke-Kaplan’s integral equation by using the implicit function theorem under suitable conditions. We also show a situation in which any bounded solution with a sufficiently small delay is isolated, clearing an asymptotic stability result of Cooke and Kaplan.
Dedicated to Professor Giovanni Vidossich
1. Introduction
By modelling some infectious diseases with periodic contact rate that varies seasonally, Cooke and Kaplan [1] came up with the nonlinear integral equation where represents the proportion of infections in the population at time , ; is a (nonnegative) continuous function which is -periodic in the variable ; and is a positive real number corresponding to the length of time an individual remains infectious.
This has attracted many mathematicians such as Leggett and Williams [2], Nussbaum [3], and Agarwal and O’Regan [4] who have considered many variants of this model and used cone theoretic arguments to establish their existence results.
In this paper, we consider as a positive real parameter and prove under suitable conditions (5) the existence of a unique curve of periodic positive solutions when is of separable variables; say with continuous and -periodic, and is of class . Furthermore we show a uniqueness result for bounded solutions of (1) when , is continuous and continuously differentiable with respect to its second variable , and is sufficiently small.
2. The Results
In the sequel denotes a positive constant real number, denotes the real Banach space of -periodic continuous functions from to equipped with the supremum norm denotes the space of -periodic continuously differentiable functions from to , and denotes the real Banach space of bounded continuous functions from to equipped with the supremum norm Given a function of two variables , we shall set
Theorem 1.  Let  be a (nonnegative) continuous -periodic function that is not identically equal to zero and  be a nonnegative continuous function of class .
Suppose, moreover, that there exists a real number  such that where  (the mean value of ).
Then there exists  and a unique curve of nontrivial nonnegative -periodic solutions ; ;  such that by setting  we have and for each ,that is,  solves (1) with .
Remarks 2. (i) For  sufficiently closed but not equal to , the solution  provided by Theorem 1 is not constant (since it can be seen in the proof that ).
(ii) The assumptions of this theorem are satisfied (due to the intermediate value theorem) when  is a nonnegative continuous -periodic function that is not identically equal to zero and  is a nonnegative continuous function of class  such that (iii) The conclusion of Theorem 1 still holds, according to its proof, when  is a nonnegative continuous -periodic function that is not identically equal to zero, for some real number ,  is continuously differentiable from  into , and there exists a real number  that satisfies the conditions (5).
(iv) Note that if  is a nonnegative continuous -periodic function that is not identically equal to zero and  is a nonnegative continuous function of class  which is superlinear or for which there exists a positive number  such that then (1) with  has a positive constant solution but we cannot say more because .
Proposition 3. Let be a nonnegative bounded continuous function, -periodic with respect to , not identically equal to zero and having a continuous partial derivative . Suppose, moreover, that Then, (i)for every , any solution of (1) is a priori bounded,(ii)given , any solution of (1), such that is isolated,(iii)in particular, for any such that the zero function is an isolated solution of (1).
Example 4. The assumptions of this theorem are satisfied in each of the next two cases followed by an illustration of part (iii) of Remarks 2:(i)Let for every and for all and . Clearly is a -periodic nonnegative function with . Moreover is a nonnegative function of class on and so One can even realize that the positive solution of the equation belongs to the interval .(ii)Let for every and for all and . Clearly is a -periodic nonnegative function with Moreover is a nonnegative function of class on and for , Then we can conclude according to part (ii) of Remarks 2.(iii)Let for every , for all , and . It follows that is a -periodic nonnegative function with , and is a nonnegative function of class on with for . Moreover satisfies The result follows from part (iii) of Remarks 2.
Proof of Theorem 1. Suppose that the assumptions of Theorem 1 are satisfied.
Step  1. Let  be a real-valued -extension of  to ; for instance,  which may change sign; in other words  is defined from  into .
Although  we shall need just a positive real number  such that  for the sake of generality (see Remarks 2(iii)). Hence Now setClearly  is open in  and contains the constant function . Moreover consider the mapping  defined by Then  is well-defined by the -periodicity of  and the continuity of both  and . Also for every  fixed, we have Thus for ,  if and only if  is a positive solution of (1) with . 
Step  2. Now one can see that  is of class  by the properties of the parameter dependent integrals and those of Nemytskii operators [5].
It is not hard to check that, for every  and every , we have for all ,  In particular  is the function  since  is -periodic, while  is the endomorphism of ; , such that Step  3. We have .
Moreover showing that  is an isomorphism of , Cf [5, page 212] or [6, page 31].
Therefore by the implicit function theorem [5–7], there is an open neighbourhood  of  in , a positive real number , and an open neighbourhood  and a unique continuously differentiable map  from  to  such that  and for any ,  In addition  and so The result follows.
Proof of Proposition 3. (1) Let us fix  and suppose that  is any solution of (1) with  satisfying the hypotheses of Proposition 3. Then we have showing that  is bounded by the boundedness of .
(2) Let us fix  and suppose  is a solution of (1) such that  Consider the nonlinear map  defined by  Indeed if  is a bounded continuous function from  into , then  is also continuous by the continuity of  and is moreover bounded by the previous result.
Again it is not hard to see that , as a map from  into , is continuously differentiable and given , we have for every  So that  by assumption. This implies that  is an automorphism. And since , we conclude that  is an isolated zero of ; that is,  is an isolated solution of (1).
(3) follows immediately from (2).
Competing Interests
The author declares that there are no competing interests regarding the publication of this paper.
Acknowledgments
The author is very grateful to the Abdus Salam International Centre for Theoretical Physics (ICTP, Trieste, Italy) for its hospitality and financial support during his 2016 visit as a Regular Associate.