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# On a fractional differential equation with infinitely many solutions

*Advances in Difference Equations*
**volume 2012**, Article number: 145 (2012)

## Abstract

We present a set of restrictions on the fractional differential equation {x}^{(\alpha )}(t)=g(x(t)), t\ge 0, where \alpha \in (0,1) and g(0)=0, that leads to the existence of an infinity of solutions (a continuum of solutions) starting from x(0)=0. The operator {x}^{(\alpha )} is the Caputo differential operator.

## 1 Introduction

The issue of multiplicity for solutions of an initial value problem that is associated to some nonlinear differential equation is essential in the modeling of complex phenomena.

Typically, when the nonlinearity of an equation is not of Lipschitz type [1], there are only a few techniques to help us decide whether an initial value problem has more than one solution. As an example, the equation {x}^{\mathrm{\prime}}=f(x)=\sqrt{x}\cdot {\chi}_{(0,+\mathrm{\infty})}(x) has an infinity of solutions (a continuum of solutions [8], p.15]) {x}_{T}(t)=\frac{{(t-T)}^{2}}{4}\cdot {\chi}_{(T,+\mathrm{\infty})}(t) defined on the nonnegative half-line which start from x(0)=0. Here, by *χ* we denote the characteristic function of a Lebesgue-measurable set.

An interesting classical result [1, 10], which generalizes the example, asserts that the initial value problem

where the continuous function g:\mathbb{R}\to \mathbb{R} has a zero at {x}_{0} and is positive everywhere else, possesses an infinity of solutions if and only if {\int}_{{x}_{0}+}\frac{du}{g(u)}<+\mathrm{\infty}.

Recently, variants of this result have been employed in establishing various facts regarding some mathematical models [13, 14]. In particular, if the function *g* is allowed to have two zeros {x}_{0}<{x}_{1} while remaining positive everywhere else and

then the problem (1) has an infinity of solutions {({x}_{T})}_{T>0} such that {lim}_{t\to +\mathrm{\infty}}{x}_{T}(t)={x}_{1}.

Our intention in the following is to discuss a particular case of the above non-uniqueness theorem in the framework of fractional differential equations. To the best of our knowledge, the result has not been established in its full generality yet for any generalized differential equation. We mention at this point the closely connected investigation [5].

In the last number of years, it became evident that differential equations of non-integer order, also called *fractionals* (FDE’s), can capture better in models many of the relevant features of complex phenomena from engineering, physics or chemistry, see the references in [2–4, 6, 7, 9, 11, 12, 16].

Let us consider a function h\in {C}^{1}(I,\mathbb{R})\cap C(\overline{I},\mathbb{R}) with {lim}_{t\searrow 0}[{t}^{1-\alpha}{h}^{\mathrm{\prime}}(t)]\in \mathbb{R} for some \alpha \in (0,1), where I=(0,1]. The *Caputo derivative* of order *α* of *h* is defined as

where Γ is Euler’s function Gamma, cf. [16], p.79]. To have an idea about the eventual smoothness of this quantity, we mention that by letting the function {h}^{\mathrm{\prime}} be at least absolutely continuous [17], Chapter 7] the (usual) derivative of {h}^{(\alpha )} will exist almost everywhere with respect to the Lebesgue measure *m* on \mathbb{R}, see [18], p.35, Lemma 2.2]. Further, we have that

provided that {h}^{(\alpha )} is in {L}^{\mathrm{\infty}}(m).

The initial value problem we investigate in this paper is

where the function g:\mathbb{R}\to \mathbb{R} is continuous, g(0)=0 and g(u)>0 when u\in (0,1]. Further restrictions will be imposed on *g* to ensure that {\int}_{0+}\frac{du}{g(u)}<+\mathrm{\infty}.

By means of (2), we deduce that

and so the problem (3) can be recast as

where y={x}^{(\alpha )}, \beta =1-\alpha and the (general) function *g* has absorbed the constant \frac{1}{\mathrm{\Gamma}(\alpha )}.

In the next section, we look for a family {({y}_{T})}_{T>0}, with {y}_{T}\in C([0,1],\mathbb{R}), of (non-trivial) solutions to (4).

## 2 Infinitely many solutions to (4)

We start by noticing that the function f:[0,1]\to (0,1) with the formula f(x)=\frac{1+x}{2+x-\beta}=1-\frac{1-\beta}{2+x-\beta} is increasing. Introduce now the numbers {\delta}_{1} and {\delta}_{2} such that

Obviously, {\delta}_{1},{\delta}_{2}\in (0,1).

Set {c}_{1}\le {c}_{2} in (0,+\mathrm{\infty}) and assume that

As a by-product, {\int}_{0+}^{1}\frac{dy}{g(y)}\le \frac{{c}_{1}^{-1}}{1-{\delta}_{1}}<+\mathrm{\infty}. Further, suppose that there exists c>0 such that

The latter condition has been inspired by the analysis in [15].

Introduce now the numbers {Y}_{1},{Y}_{2}\ge 1 and T\in (0,1) with

and

and

These will be used in the following for describing the solution {y}_{T}.

Several simple estimates, of much help in the proof of our result, are established next. Notice first that, *via* the change of variables s=T+u(t-T), we get

where \epsilon \in (0,1) and *B* represents Euler’s function Beta [16]. Also,

and

Now, returning to (5), there exist {\epsilon}_{1},{\epsilon}_{2}\in (0,1), with {\epsilon}_{1}\ge {\epsilon}_{2}, such that

In particular, 1-{\delta}_{1}=\frac{1-\beta}{2+{\epsilon}_{1}-\beta} and, by means of (13),

Taking into account (12) and (9), we deduce that

which leads to

and, *via* (13),

which implies that

Let the set \mathcal{Y}\subset C([T,1],\mathbb{R}) be given by the double inequality

Observe that, by means of (16), (11), (6),

and

Similarly, *via* (17),

and

In conclusion, the mapping t\mapsto g({\int}_{T}^{t}\frac{y(s)}{{(t-s)}^{\beta}}\phantom{\rule{0.2em}{0ex}}ds) is a member of \mathcal{Y} whenever y\in \mathcal{Y}. Also, taking into account (15), we deduce that the quantities y={Y}_{1}B(2+{\epsilon}_{1},1-\beta ){(t-T)}^{2+{\epsilon}_{1}-\beta} from (20) and y={Y}_{2}B(2+{\epsilon}_{2},1-\beta ){(t-T)}^{2+{\epsilon}_{2}-\beta} from (21) belong to [0,1] as imposed in (6).

We are now ready to state and prove our main result.

**Theorem 1** *Assume that the nonlinearity* *g* *of* (4) *satisfies the restrictions* (5), (6), (7). *Given the numbers* {Y}_{1}, {Y}_{2}, *T* *subject to* (8), (9), (10) *and the set* \mathcal{Y}=\mathcal{Y}({Y}_{1},{Y}_{2},T) *from* (18), *the problem* (4) *has a unique solution* {y}_{T} *in* \mathcal{Y}.

*Proof* The operator \mathcal{O}:\mathcal{Y}\to \mathcal{Y} with the formula

is well defined.

The typical sup-metric d({y}_{1},{y}_{2})={sup}_{t\in [T,1]}|{y}_{1}(t)-{y}_{2}(t)| provides the set \mathcal{Y} with the structure of a complete metric space.

Taking into account (7), (19) and (10), we get

The operator \mathcal{O} being thus a contraction, its fixed point {y}_{T} in \mathcal{Y} is the solution we are looking for. Notice that {y}_{T} is identically null in [0,T]. □

As an easily computed example, consider the initial value problem

where {c}_{1}>0 and \delta \in (\frac{2}{3},\frac{4}{5}). Then, introducing Y>0 such that {c}_{1}\cdot B{(\frac{1}{2},\frac{2-3\delta}{2-2\delta})}^{\delta}\cdot {Y}^{\delta -1}=1, the problem (22) has the solution y(t)=Y{(t-T)}^{\frac{\delta}{2(1-\delta )}} throughout [T,1] which can be extended as a {C}^{1}-function downward to 0.

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## Acknowledgements

The work of the second author has been supported by a grant of the Romanian National Authority for Scientific Research, CNCS-UEFISCDI, project number PN-II-ID-PCE-2011-3-0075. The authors would like to thank the referees for their comments and remarks in order to improve the manuscript.

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Băleanu, D., Mustafa, O.G. & O’Regan, D. On a fractional differential equation with infinitely many solutions.
*Adv Differ Equ* **2012**, 145 (2012). https://doi.org/10.1186/1687-1847-2012-145

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DOI: https://doi.org/10.1186/1687-1847-2012-145