Robust passivity analysis of mixed delayed neural networks with interval nondifferentiable time-varying delay based on multiple integral approach

1.   Framework and main results

We investigate equations of the form

where $f^T:\mathbb{R}\times\mathbb{R} \to \mathbb{R}$ is of the type

and $T$ is a positive parameter. We suppose that $g$ is a KPP (for Kolmogorov, Petrovsky and Piskunov) function of class $\mathcal{C}^1(\mathbb{R}^+)$ with $\mathbb{R}^+ = [0,+\infty)$. More precisely, we have

and

The previous hypotheses imply in particular that

and that

In Sections 2 and 4, the function $m^T$ is $T$-periodic, nonnegative and of class $\mathcal{C}^1(\mathbb{R})$. In this case, the function $f^T$ is a $T$-periodic in time function of class $\mathcal{C}^1(\mathbb{R}\times\mathbb{R}^+)$ such that $f^T(\cdot,0) = 0$ on $\mathbb{R}$. Furthermore, according to (6) and the nonnegativity of $m^T$, we have

In Section 3, the function $m^T$ is asymptotically periodic in time. We give more details about this notion later in this introduction.

1.1.   Biological interpretation

Equations of the type

are proposed to model the spatial evolution over time of a cancerous tumor in the presence of chemotherapy. The quantity $u(t,x)$ represents the density of cancer cells in the tumor at the position $x$ and at the time $t$. We begin by considering, for $T>1$, a particular case of periodic function $m^T:\mathbb{R}^+\to\mathbb{R}$ of class $\mathcal{C}^1(\mathbb{R}^+)$ for which there exists a nontrivial function $\varphi :[0,1]\to[0,+\infty)$ with $\varphi (0) = \varphi (1) = 0$ such that

In the absence of treatment, cancer cells reproduce and spread in space. This reproduction is modeled by the reaction term of KPP type $g(u)$, which takes into account the fact that the resources of the environment of the tumor are not infinite and so, that there is a maximal size beyond which the tumor cannot grow anymore. To treat the patient, cycles of chemotherapy are given. Every cycle lasts a lapse of time $T$ and is composed of two subcycles. The duration of the first one is equal to $1$. During this time, the drug acts on the tumor. At every moment of the first subcycle, the death rate of the cancer cells due to the drug is equal to $\varphi (t)$. In this case, the total reaction term is $g(u)-\varphi(t)u$. There is a competition between the reproduction term and the death term. The chemotherapy has a toxic effect on the body because it destroys white blood cells. It is thus essential to take a break in the administration of the treatment. This break is the second subcycle of the cycle of chemotherapy. It lasts during a time equal to $T-1$. In this case, the reaction term is just $g(u)$, and thus, the tumor starts to grow again. To summarize, the term $m^T(t)$ defined in (9) represents the concentration of drug in the body of the patient at time $t$, and the integral $\textstyle{\int_0^T m_T(s)ds = \int_0^1\varphi (t)dt}$ represents the total quantity of drug in the patient during a cycle of chemotherapy. Finally, we impose for this type of functions $m^T$ that

This inequality is not really restricting. Indeed, we shall see after that this hypothesis is in fact a condition so that the patient is cured in the case where there is no rest period in the cycles of chemotherapy (that is $T = 1)$.

We now refine the previous modelling. In fact, the concentration of drug in the patient's body is not a datum. We only know the concentration of drug injected to the patient. We denote $D^T(t)$ this concentration at time $t$, and we assume that the function $D^T:\mathbb{R}^+\to\mathbb{R}^+$ is $T$-periodic and satisfies

The concentration of drug $m$ is then the Lipschitz-continuous and piecewise $\mathcal{C}^1$ solution $m:\mathbb{R}^+\to\mathbb{R}$ of a Cauchy problem of the type

The real number $\tau>0$ is called clearance. It characterizes the ability of the patient's body to eliminate the drug. It is also possible to take into account that the patient does not necessarily take the treatment in an optimal way. It may happen to him$/$her, for example, to forget his$/$her medicine, or being forced to move a chemotherapy session if it is programmed on a holiday. So, we add to the nonlinearity a perturbative term of the type $\varepsilon p(t,u)$, where $\varepsilon \geq 0$ and $p:\mathbb{R}^+\times \mathbb{R} \to \mathbb{R}$. It corresponds to study equations of the type

where $m$ solves (12).

1.2.   Mathematical framework

The mathematical study of reaction-diffusion equations began in the 1930's. Fisher [12] and Kolmogorov, Petrovsky and Piskunov [17] were interested in wave propagation in population genetics modeled by the homogeneous equation

In the $1970$'s, their results were generalized by Aronson and Weinberger [1] and Fife and McLeod [11]. In particular, if $f$ is a KPP nonlinearity (that is, $f$ satisfies (3) and (5)), there exists a unique (up to translation) planar fronts $U_c$ of speed $c$, for any speed $\textstyle{c \geq c^*: = 2 \sqrt{f'(0)}}$, that is, for any $c\geq c^*$, there exists a function $u_c$ satisfying (13) and which can be written $u_c(t,x) = U_c(x-ct),~~\text{with}~0 <U_c<1,~U_c(-\infty) = 1~\text{and}~U_c(+\infty) = 0.$ Furthermore, if $c<c^*$, there is no such front connecting $0$ and $1$. Another property for this type of nonlinearities is that if we start from a nonnegative compactly supported initial datum $u_0$ such that $u_0\not\equiv 0$, then the solution $u$ of (13) satisfies $u(t,x)\to 1$ as $t\to+\infty$. Aronson and Weinberger name this phenomenon the "hair trigger effect". Moreover the set where $u(t,x)$ is close to $1$ expands at the speed $c^*$.

Freidlin and Gärtner in [13] were the first to study heterogeneous equations. More precisely, they generalized spreading properties for KPP type equations with periodic in space coefficients. Since this work, numerous papers have been devoted to the study of heterogeneous equations with KPP or other reaction terms. We can cite e.g. [2,3,4,5,6,8,10,16,19,27,28,29] in the case of periodic in space environment, [14,18,19,24,25] in the case of periodic in time environment and [21,22,23] in the case of periodic in time and in space environment. The works of Nadin [21,22] and Liang and Zhao [19] are the closest of our paper. We will compare later the contributions of our work with these references. We now give the main results of the paper.

When the nonlinearity is not homogeneous, there are no planar front solutions of (8) anymore. For equations with coefficients depending periodically on the space variable, Shigesada, Kawasaki and Teramoto [26] defined in 1986 a notion more general than the planar fronts, namely the pulsating fronts. This notion can be extended for time dependent periodic equations as follows.

Definition 1.1. For equation (1), assume that $f^T$ is $T$-periodic and that (1) has a $T$-periodic solution $\theta:\mathbb{R}\to(0,+\infty),~t\mapsto\theta(t)$. A pulsating front connecting $0$ and $\theta(t)$ for equation (1) is a solution $u:\mathbb{R}\times \mathbb{R} \to \mathbb{R}^+$ such that there exists a real number $c$ and a function $U:\mathbb{R} \times \mathbb{R} \to \mathbb{R}^+$ verifying

So, a pulsating front connecting $0$ and $\theta$ for equation (1) is a couple $(c,U(t,\xi))$ solving the problem

In this definition, by standard parabolic estimates, the limiting state $\theta = U(\cdot,-\infty)$ solves the system

whose solutions are called equilibrium states of the equation (1).

If $\theta:\mathbb{R}\to\mathbb{R}$ is a solution of (14), let us now define $\lambda_{\theta,f^T}$ and $\Phi_{\theta,f^T}:\mathbb{R}\to\mathbb{R}$ as the unique real number and the unique function (up to multiplication by a constant) which satisfy

These quantities are called respectively principal eigenvalue and principal eigenfunction associated with $f^T$ and the equilibrium state $\theta$. Furthermore, if we divide the previous equation by $\Phi_{\theta,f^T}$, and if we integrate over $(0,T)$, we obtain an explicit formulation of the principal eigenvalue, namely

We now recall the definition of the Poincaré map $P^T$ associated with $f^T$. For any $\alpha\geq0$, let $y_\alpha:\mathbb{R}^+\to \mathbb{R}^+$ be the solution of the Cauchy problem

Definition 1.2. The $\text{Poincaré}$ map associated with $f^T$ is the function $P^T:\mathbb{R}^+ \to \mathbb{R}^+$ defined by

We conclude, with the fact that each nonnegative solution of (14) is associated with a fixed point of $P^T$, and conversely. Furthermore, if $\alpha^T\geq0$ is a fixed point of $P_T$ we have the following equality

We can find these results concerning the notions of principal eigenvalue and Poincaré map in [7], [9], [15] and [20].

1.3.   Nonlinearities periodic in time

Let $T>0$. In Section 2, we study (1) and (2) with functions $m^T$ which are $T$-periodic in time. For these functions we assume there exists $T^*>0$ such that

This is indeed the case if $m^T$ is of the type (9) because

Furthermore, for this type of functions, hypothesis (10) implies that $\lambda_{0,f^{T = 1}}>0$. Hence, in this case $T^*>1$. The existence and uniqueness of positive solutions of (14) is summarized in the following result.

Proposition 1. We consider the real number $T^*$ defined in (18).

(Ⅰ) If $T\leq T^*$, there is no positive solution of (14).

(Ⅱ) If $T>T^*$, there is a unique positive solution $w^T$ of (14). Furthermore,

(i) For any $t\in\mathbb{R}$ we have $w^T(t)\in(0,1]$, and

(ii) If $T\mapsto m^T$ is continuous in $L^\infty_{\text{loc}}(\mathbb{R})$, then the function $T\in(T^*,+\infty) \mapsto w^T(0)$ is continuous and, if $m^T$ is of type (9) with assumption (10), it is increasing.

(iii) If $T\mapsto m^T$ is continuous in $L^\infty_{\text{loc}}(\mathbb{R})$, then the function $w^T$ converges uniformly to $0$ on $\mathbb{R}$ as $T\to (T^*)^+$.

(iv) If $m^T$ is of type (9) with assumption (10), then $w^T$ converges on average to $1$ as $T$ tends to $+\infty$:

The same result of existence and uniqueness (result of the type $(II)$) was proved for KPP nonlinearities depending periodically on space by Berestycki, Hamel and Roques in [5] and for KPP nonlinearities depending periodically on space and time by Nadin in [22]. We give here a proof using the Poincaré map associated with $f^T$. The last two points of the proposition are quite intuitive. Indeed, the limit as $T\to(T^*)^+$ is explained by the fact that for $T\leq T^*$, the only nonnegative equilibrium state is zero. The limit as $T\to+\infty$ is explained by the fact that in this case, the nonlinearity $f^T$ is "almost" the KPP function $g$ since the function $m^T$ has an average close to $0$ when $T$ is large.

Let us now summarize a result in [22], which deals with the evolution of $u(t,x)$ as $t\to+\infty$.

Proposition 2. [22] Let $u_0:\mathbb{R} \to \mathbb{R}$ be a bounded and continuous function on $\mathbb{R}$ such that $u_0\geq0$ and $u_0\not\equiv0$. Under assumption (18), we consider the function $u:\mathbb{R}^+\times \mathbb{R} \to \mathbb{R}$ satisfying

If $T <T^*$, then there exists $M>0$ depending only on $u_0$ and $\Phi_{0,f^T}$ such that

If $T = T^*$, then

If $T>T^*$, then for every compact set $K\subset\mathbb{R}$, we have

A similar result was proved for KPP nonlinearities depending periodically on space by Berestycki, Hamel and Roques in [5].

In the biological context with $m^T$ satisfying (9), the treatment is effective (in the sense that $u(t,x)\to0$ uniformly on $\mathbb{R}$ as $t\to+\infty$) if and only if the duration of cycles of chemotherapy is equal or less than $T^*$. In particular, since hypothesis (10) implies that $T^*>1$, the treatment is effective if there is no rest period between two injections of drug, that is as $T = 1$. The result is interesting because it implies that $T^*-1$ is the longest rest period for which the patient recovers. Inequality (20) refines the criterion of cure of the patient because according to the fact that the function $T\mapsto \lambda_{0,f^T}$ is decreasing and positive on $(0,T^*)$, the convergence rate of the density $u(t,x)$ to $0$ as $t\to+\infty$ is all the faster as $T$ is small. In other words, in the case of effective treatment, shorter the period between two injections, more quickly the patient will be cured. If the treatment is not effective, the equilibrium state $w^T$ invades the whole space as $t\to+\infty$. In particular, the tumor can not grow indefinitely. Finally, Proposition 2 also allows to clarify the result $(ii)$ of Proposition 1. The fact that $T\mapsto w^T(0)$ is increasing on $(T^*,+\infty)$ implies that in the case where the treatment is not effective (that is $w^T>0$ invades the whole space as $t\to+\infty$), the longer the rest period between two injections, the denser the equilibrium state of the tumor.

We now study in more detail the case where the treatment is not effective, that is, the case where $T>T^*$. We know that then, the equilibrium state $w^T$ invades the whole space as $t\to+\infty$. The purpose of this part is to give the invasion rate of the zero state by $w^T$. To answer this question, we quote two results. The first one is about the existence of pulsating fronts connecting $0$ and $w^T$, in the sense of Definition 1.1, and the second one concerns spreading properties. They are proved in [18] and in [21].

Theorem 1.3. [18], [21] Let $T>T^*$, where $T^*$ is given in (18). (Ⅰ) There exists a positive real number $c_T^*$ such that pulsating fronts with speed $c$ connecting $0$ and $w^T$ exist if and only if $c\geq c_T^*$.

(Ⅱ) We denote $u:\mathbb{R}^+\times \mathbb{R} \to \mathbb{R}$ the solution of the Cauchy problem

If $u_0$ is a bounded continuous function such that $u_0\geq0$ and $u_0\not\equiv0$, then

If $u_0$ is a continuous compactly supported function such that $u_0\geq0$, then

In his paper [21], Nadin considers in the first assertion of the spreading properties in Theorem 1.3 initial conditions which are more general. He assumes that $u_0$ is not necessarily compactly supported but that $u_0$ is of the form $O(e^{-\beta |x|})$ as $|x|\to +\infty$, where $\beta>0$. The previous theorem completes Proposition 2. Indeed, we know that in the case where the treatment is not effective, the equilibrium state $w^T$ invades the whole space as $t\to+\infty$. Theorem 1.3 states that this invasion takes place at the speed $c_T^*$.

We can now characterize the critical speed $c_T^*$ with the principal eigenvalue $\lambda_{0,f^T}$. More precisely:

Proposition 3. For every $T>T^*$, the critical speed $c_T^*$ is given by

Hence, if $T\mapsto\int_0^T m^T(s)ds$ is continuous, then the function $T\in(T^*,+\infty) \mapsto c^*_T$ is continuous and, if $\int_0^T m^T(s)ds$ does not depend on $T$, it is increasing. Furthermore, we have the two following limit cases:

and, if $\frac{1}{T}\int_0^T m^T(s)ds\xrightarrow{T\to+\infty}0$, then

In the case where the treatment is not effective, the invasion of space by the equilibrium state $w^T$ is all the faster as the rest time between injections is long. The two limits cases $T\to(T^*)^+$ and $T\to +\infty$ are explained in the same manner as in Proposition 1. Let us note that in the case where $m^T$ is of the type (9), then the previous properties concerning $\textstyle{\int_0^T m^T(s)ds}$ are satisfied.

We end this section by stating the existence of pulsating fronts in the case of nonlinearities which are not of KPP type (that is hypotheses (4) and (5) are not necessarily verified, but we still assume (3), (6) and (18)). For these nonlinearities, there is still a positive solution to problem (14), but it may not be unique. According to Cauchy-Lipschitz theorem, solutions of (14) are ordered on $[0,T]$. For $T>T^*$, we can thus define $y^T:\mathbb{R}\to\mathbb{R}$ as the infimum of all positive solutions of (14). After showing that $y^T>0$, we will prove there exists a critical speed $c_T^{**}>0$ such that there is a pulsating front connecting $0$ and $y^T$ for speed $c\geq c_T^{**}$ and there is no pulsating front connecting $0$ and $y^T$ for $c<c_T^{**}$. In this case, $c_T^{**}$ is not necessarily equal to $2\sqrt{-\lambda_{0,f^T}}$. For this type of nonlinearity, Nadin shows in [21] that there exist two critical speeds $c_*$ and $c^*$ for which there is a pulsating front for $c\geq c^*$ and there is no pulsating front for $c\leq c_*$. Nevertheless the case $c\in (c_*,c^*)$ is not treated in [21]. In [18], Liang and Zhao prove the result using a semiflow method. We give here an alternative proof. We begin by proving the existence of pulsating front $U(t,\xi)$ for domains of the type $\mathbb{R}\times[-a,a]$ which are bounded in $\xi$, then we pass in the limit as $a\to+\infty$. We state the result.

Proposition 4. Let $f^T$ satisfy assumptions (2), (3), (6) and (18), and $T>T^*$. There exists a positive real number $c_T^{**}$ such that pulsating fronts $U(t,\xi)$ monotone in $\xi$ connecting $0$ and $y^T$ exist if and only if $c\geq c_T^{**}$.

1.4.   Nonlinearities asymptotically periodic in time with perturbation

We are interested in the case of nonlinearities which are no more periodic in time, but which are the sum of a function which converges as $t\to+\infty$ to a time periodic nonlinearity and of a small perturbation. More precisely, for $\varepsilon \geq0$, we consider equations of the type

where $m$ solves (12) with $T>1$ and $D^T$ defined in (11). We assume that $p:\mathbb{R}^+\times \mathbb{R} \to \mathbb{R}$ is a function of class $\mathcal{C}^1$ for which there exists $C>0$ such that

The function $m$ is not periodic, but it is asymptotically $T$-periodic in time. More precisely, there exists a $T$-periodic positive function $m_\infty^T:\mathbb{R}\to(0,+\infty)$ such that

Indeed, an elementary calculation implies that for any $n\in \mathbb{N}$, we have

Consequently, if we define the positive $T$-periodic function $m_\infty^T:\mathbb{R}\to(0,+\infty)$ by

then the convergence result (24) holds. Furthermore, we have $\textstyle{\int_0^T m_\infty^T(t)dt = \tau.}$ Consequently the function $f^T:\mathbb{R}^+\times \mathbb{R}^+\to \mathbb{R}$ defined by $f^T(t,u) = g(u)-m_\infty^T(t)u$ satisfies (18) because $\lambda_{0,f^T} = -g'(0)+\tau / T$. We assume that $\tau>g'(0)$. We notice that $m_\infty^T$ is independent of $m_0$. It was predictable because $m_\infty^T$ is the unique positive $T$-periodic solution of $m' = D^T-m / \tau$ on $\mathbb{R}$. We define the nonlinearities $f:\mathbb{R}^+\times \mathbb{R}^+\to \mathbb{R}$ and $f_\varepsilon :\mathbb{R}^+\times \mathbb{R}^+\to \mathbb{R}$ by

According to (24), we have

The function $f^T$ is $T$-periodic and satisfies the general assumptions given in Section 1.3. We still denote $T^*$ the critical time (notice that $T^*>1$ because $\tau>g'(0)$), $w^T$ the unique positive equilibrium state for $T>T^*$ and $c_T^*$ the critical speed associated with $f^T$ for $T>T^*$.

The aim of this section is to show that Proposition 2 and the spreading results of Theorem 1.3 hold true when we replace $f^T$ by $f_\varepsilon$ in the statements, for $\varepsilon$ small enough. It is reasonable to hope so. Indeed, on the one hand, if $\varepsilon$ is small, then the term $\varepsilon p$ is negligible compared to $f$, and on the other hand, these results deal with the large time behavior of the solutions, and precisely, hypothesis (25) implies that $f$ "looks like" $f^T$ as $t\to+\infty$. The first result is the generalization of Proposition 2.

Theorem 1.4. Let $u_0:\mathbb{R} \to \mathbb{R}$ be a bounded and continuous function such that $u_0\geq0$ and $u_0\not\equiv0$. For all $\varepsilon \geq 0$, we consider the function $u_\varepsilon :\mathbb{R}^+\times \mathbb{R} \to \mathbb{R}$ satisfying

If $T <T^*$, there exists $\varepsilon _T>0$ such that for all $\varepsilon \in(0,\varepsilon _T)$ we have

If $T>T^*$ and if $\lambda_{w^T,f^T}>0$, then there exist $\tilde \varepsilon _T>0$ and $M_T>0$ such that for all $\varepsilon \in (0,\tilde \varepsilon _T)$ and for all compact $K\subset \mathbb{R}$, we have

We saw in Proposition 1 that $\lambda_{w^T,f^T}\geq0$. In the previous theorem, in case $T>T^*$, we impose that $\lambda_{w^T,f^T}>0$. This property is not necessarily satisfied. Indeed, if we consider the function $h:\mathbb{R}^+\to\mathbb{R}$ defined by $h(u) = u(1-u)^3$, then we have $h(0) = h(1) = 0$, $h>0$ on $(0,1)$, $h<0$ sur $(1,+\infty)$, $h(u) / u$ decreasing on $(0,+\infty)$ and $h'(1) = 0$. In the case where the function $f^T(t,\cdot)$ is concave for all $t\in\mathbb{R}^+$, the property $\lambda_{w^T,f^T}>0$ is verified for any $T>T^*$. Indeed, if we define $F:[0,1] \to \mathbb{R}$ by

then we have $F(0) = F(1) = 0$ and $F$ is convex on $[0,1]$. Consequently, if $F'(1) = 0$, that is, if $\lambda_{w^T,f^T} = 0$, then we have $F' = 0$ on $[0,1]$. It is a contradiction because $F'(0) = \lambda_{0,f^T} <0$.

Let us give a sketch of the proof. For $T>0$ and $\varepsilon >0$, we will frame $f_\varepsilon$ by two $T$-periodic functions $f_\varepsilon ^T$ and $f_{-\varepsilon }^T$ for which the results of Proposition 2 will apply. In the case where $T <T^*$, if $f^T_\varepsilon$ is the upper bound function, we will show that for $\varepsilon >0$ small enough, we have $\lambda_{0,f^T_\varepsilon }>0$. Hence, the solution of (26) with $f^T_\varepsilon$ as nonlinearity is a supersolution of problem (26) and, according to Proposition 2, it converges to $0$ as $t\to+\infty$. In the case where $T>T^*$, we will prove that for $\varepsilon >0$ small enough, we have $\lambda_{0,f^T_\varepsilon } <0$ and $\lambda_{0,f^T_{-\varepsilon }} <0$. Consequently, there is a unique positive solution $w^T_\varepsilon$ (resp. $w^T_{-\varepsilon }$) of system (14) with $f^T_\varepsilon$ (resp. $f^T_{-\varepsilon }$) as nonlinearity (owing to Proposition 1). The solution of (26) with $f^T_\varepsilon$ as nonlinearity is a supersolution of (26) and, according to Proposition 2, it converges to $w^T_\varepsilon$ as $t\to+\infty$. In the same way, the solution of (26) with $f^T_{-\varepsilon }$ as nonlinearity is a subsolution of (26), and it converges to $w^T_{-\varepsilon }$ as $t\to+\infty$. We will conclude using the fact that $w^T_\varepsilon$ and $w^T_{-\varepsilon }$ are close to $w^T$ as $\varepsilon$ is small enough.

Note that the case $T = T^*$ is not treated in Theorem 1.4. If $\varepsilon = 0$, the solution of the Cauchy problem (26) converges uniformly to $0$ as $t\to+\infty$, whereas if $\varepsilon >0$, the convergence to $0$ may not hold. We summarize these results in the following proposition.

Proposition 5. Let $T = T^*$ and $\varepsilon \geq0$. We consider the function $u_\varepsilon :\mathbb{R}^+\times \mathbb{R} \to \mathbb{R}$ satisfying the Cauchy problem (26).

(Ⅰ) If $\varepsilon = 0$, then $u_\varepsilon$ converges uniformly to $0$ as $t\to+\infty$.

(Ⅱ) If $\varepsilon >0$, we can conclude in two cases.

(i) If $f(t,u) = f^{T^*}(t,u)$ and $p(t,u) = u$, then, for $\varepsilon$ small enough, $u_\varepsilon$ converges to a positive solution of (14) with $f_\varepsilon$ as nonlinearity as $t\to+\infty$.

(ii) If $p(t,u)\leq0$, then, $u_\varepsilon$ converges uniformly to $0$ as $t\to+\infty$.

Concerning the spreading results of Theorem 1.3, they remain true if we replace $f^T$ by $f_\varepsilon$ in the statement.

Theorem 1.5. Let $T>T^*$. For any $\varepsilon \geq0$, we consider $u_\varepsilon :\mathbb{R}^+\times \mathbb{R} \to \mathbb{R}$ satisfying

If $u_0$ is a continuous bounded function such that $u_0\geq 0$ and $u_0\not\equiv0$, and if $\lambda_{w^T,f^T}>0$, then for all $c\in(0,c_T^*)$, there exists $\hat \varepsilon _{c,T}>0$ such that for all $\varepsilon \in(0,\hat \varepsilon _{c,T})$ we have

where $M_T$ is defined in Theorem 1.4.

If $u_0$ is a continuous compactly supported function such that $u_0\geq 0$, then, for all $c>c_T^*$, there exists $\bar \varepsilon _{c,T}>0$ such that for all $\varepsilon \in(0,\bar \varepsilon _{c,T})$ we have

The proof of this theorem uses the same ideas as the proof of Theorem 1.4. For $T>T^*$ and $\varepsilon >0$, we will frame $f_\varepsilon$ by two $T$-periodic functions $f_\varepsilon ^T$ and $f_{-\varepsilon }^T$ for which the results of Theorem 1.3 will apply. An important point of the demonstration will be to notice that for $\varepsilon$ small enough, the critical speeds $c^*_{T,\varepsilon }$ and $c^*_{T,-\varepsilon }$ associated respectively with $f_\varepsilon ^T$ and $f_{-\varepsilon }^T$ are close to the critical speed $c^*_T$ associated with $f^T$.

1.5.   Influence of the protocol of the treatment

As in Section 1.1, we consider a $\mathcal{C}^1$ and $T$-periodic function $m^T$ (with $T\geq1$) of the type

where $\varphi :[0,1]\to[0,+\infty)$ satisfies $\varphi (0) = \varphi (1) = 0$. In this part, we are interested in equations of the type

where $0 <\tau \leq T$. The function $g$ satisfies hypotheses (3), (4) and (6). The function $m^T_\tau :\mathbb{R}^+\to\mathbb{R}^+$ is $T$-periodic and defined by

where the function $\varphi$ is the same as in $m^T$. In these equations, the duration of the treatment is equal to $\tau$. Furthermore, we have

So, it is clear that the quantity of drug administered during a cycle of chemotherapy is independent of the treatment duration $\tau$. We will study the influence of the parameter $\tau$ with respect to the results of previous sections. We define the functions $f^T_\tau :\mathbb{R}^+\times\mathbb{R}^+\to\mathbb{R}$ and $f^T_\tau :\mathbb{R}^+\times\mathbb{R}^+\to\mathbb{R}$ by

The first proposition deals with the principal eigenvalue associated with $f^T_\tau$ and the equilibrium state $0$.

Proposition 6. Let $T>0$ and $\tau \in (0,T]$. The real number $\lambda_{0,f^T_\tau }$ is independent of $\tau$. Actually, we have

Consequently, if $T^*>0$ denotes the critical time for the function $f^T$, then, for any $\tau\in(0,T^*)$, $f^T_\tau$ satisfies (18) for $T\in[\tau,+\infty)$, and the critical time $T^*$ associated with $f^T_\tau$ is the same as the one associated with $f^T$. We are interested here in the solutions of the system

The same proof as in Proposition 1 implies that for any $\tau\in(0,T^*)$ and $T\in[\tau,T^*]$, there is no positive solution of (29), while for any $T>T^*$ and $\tau\in(0,T]$, there is a unique positive solution $w^T_\tau:\mathbb{R}\to(0,1]$ of (29). Furthermore, the same proof as in Proposition 2 implies that if $\tau\in(0,T^*)$ and $T\in[\tau,T^*]$, then the treatment is efficient, and if $T>T^*$ and $\tau\in(0,T]$, then the equilibrium state $w^T_\tau$ invades the whole space as $t\to+\infty$. More precisely, Proposition 2 remains true by replacing $f^T$ by $f^T_\tau$ and $w^T$ by $w^T_\tau$. To summarize, the optimal duration of a chemotherapy cycle for which the treatment is efficient does not depend on how the drug is injected.

Let us now study the case where the treatment is not efficient, that is, $T>T^*$ and $\tau\in(0,T]$. Theorem 1.3 remains valid if we replace $f^T$ by $f^T_\tau$ and $w^T$ by $w^T_\tau$, but with a critical speed $c_{T,\tau}^*$ depending a priori on $\tau$. Nevertheless Propositions 3 and 6 imply that $\textstyle{c_{T,\tau}^* = 2\sqrt{-\lambda_{0,f^T_\tau}} = 2\sqrt{-\lambda_{0,f^T}} = c_T^*}$, where $c^*_T$ is the critical speed associated with $f^T$. Consequently, the invasion rate does not depend on how the drug is administered.

Finally, we are interested in the influence of the parameter $\tau$ on the equilibrium state $w^T_\tau$.

Proposition 7. Let $T>T^*$. The function

is continuous and decreasing.

Consequently, in the case where the treatment is not efficient, the shorter the duration of the chemotherapy cycle, the larger the value of the equilibrium state $w^T_\tau (0)$. This means that it is better to administer the treatment over long periods.

Outline. Section 2 is devoted to the proof of Propositions 1, 3 and 4. Section 3 gathers the proof of Theorem 1.4, Proposition 5 and Theorem 1.5. Finally, we prove in Section 4 Propositions 6 and 7.

2.   Nonlinearities periodic in time

2.1.   Proof of Proposition 1

We first investigate solutions of (14), showing Proposition 1. We begin with the case where $T\leq T^*$. We argue by way of contradiction, supposing there is a positive solution $w^*$ of (14). Then

We integrate this equation between $0$ and $T$. We obtain

Yet, as $w^*>0$ on $[0,T]$ and according to (4) and (18), we have

which contradicts (30).

We now consider the case where $T>T^*$. To prove the existence of a positive solution of (14), we give two lemmas demonstrating the existence of a positive fixed point of the Poincaré map $P^T$ defined in Definition 1.2.

Lemma 2.1. There exists $\alpha_0>0$ such that for all $\alpha \in (0,\alpha_0]$ we have $P^T(\alpha)>\alpha$.

Proof. Indeed, according to the fact that $f^T(\cdot,0) = 0$, we have $P^T(0) = 0$, and owing to (17) and the fact that $\lambda_{0,f^T} <0$ we have $(P^T)'(0)>1$.

Lemma 2.2. For all $\alpha>1$, we have $P^T(\alpha) <\alpha$.

Proof. Let $\alpha>1$. We consider $y_\alpha$ solution of (16). Two cases can occur.

$1^{st}$ case. If $y_\alpha(t)>1$ for all $t\geq 0$, then, according to (7), we have $y_\alpha'(t)=f^T(t,y_\alpha(t))<0$ for all $t\geq 0$. Consequently $y_\alpha(T)<y_\alpha(0)$, that is $P^T(\alpha)<\alpha$.

$2^{nd}$ case. If there exists $t_0\geq0$ such that $y_\alpha(t_0)\leq1$, then, owing to (7), we have $y_\alpha(t)\leq1$ for all $t\geq t_0$. In particular, for $n_0\in \mathbb{N}$ such that $n_0T\geq t_0$, we have $y_\alpha(n_0T)\leq1<y_\alpha(0)$. Yet, the sequence $(y_\alpha(nT))_n$ is constant or strictly monotone. So it is decreasing. Consequently we have $y_\alpha(T)<y_\alpha(0)$, that is $P^T(\alpha) <\alpha$.

Lemma 2.1 and Lemma 2.2 imply that there exists $\alpha^* \in(\alpha_0,1]$ such that $P^T(\alpha^*) = \alpha^*$. Consequently, the solution of (16) with $\alpha = \alpha^*$ is a positive solution of (14). We prove now the uniqueness of such a solution. Let $w_1:\mathbb{R} \to \mathbb{R}$ and $w_2:\mathbb{R} \to \mathbb{R}$ two positive solutions of (14). There exists $\rho >1$ such that $w_1\leq \rho w_2$ on $[0,T]$. We can define

We have

Moreover there exists $t^* \in [0,T]$ such that

We are going to show that $\rho^* = 1$. We argue by way of contradiction supposing that $\rho^*>1$. So

Furthermore

Indeed, for all $t\in[0,T]$,

According to (31), (32), (33), (34) and the $T$-periodicity of $w_1$ and $w_2$, we have

It is a contradiction because $w_1$ is a solution of $y' = f^T(t,y)$ whereas $\rho^*w_2$ is a strict supersolution. So $\rho^* = 1$. Consequently, by the symmetry of the roles played by $w_1$ and $w_2$, we have $w_1\equiv w_2$ on $[0,T]$, and then on $\mathbb{R}$ by periodicity.

We denote $w^T$ the positive solution of (14). We now show the properties of $w^T$. The previous proof implies that $(P^T)'(w^T(0))\leq1$. Hence, according to (17), it follows that $\lambda_{w^T,f^T}\geq0$. We also saw that $w^T(0)\in(0,1]$. Consequently, owing to (7) and the fact that $f^T(\cdot,0) = 0$ on $\mathbb{R}$, we have $w^T(t)\in(0,1]$ for any $t\in\mathbb{R}$.

We now study the function $T\in(T^*,+\infty) \mapsto w^T(0)$. We show the monotonicity of $T\mapsto w^T(0)$ if $m^T$ is of type (9), with assumption (10) (in this case $T^*>1$). We consider two real numbers $T_1$ and $T_2$ such that $T^*<T_1<T_2$. For $i\in\{1,2\}$, the Poincaré map $P^{T_i}$ associated with $f^{T_i}$ is defined on $\mathbb{R}^+$ by

where $y^{T_i}_\alpha$ is the solution of the Cauchy problem

We saw in (Ⅱ) that the function $P^{T_i}$ has a unique positive fixed point $\alpha^{T_i}$. Furthermore $\alpha^{T_i} \in(0,1]$. The unique equilibrium state $w^{T_i}:\mathbb{R}\to(0,1]$ associated with $f^{T_i}$ is the solution of the Cauchy problem (35) with $\alpha = \alpha^{T_i}$. Consequently, if we prove that $P^{T_1} <P^{T_2}$ on $(0,1]$, then we will deduce that $\alpha^{T_1}<\alpha^{T_2}$, that is $w^{T_1}(0)<w^{T_2}(0)$. Let $\alpha\in(0,1]$. The functions $y^{T_1}_\alpha$ and $y^{T_2}_\alpha$ are solutions on $[0,T_1]$ of the equation

Consequently, since $y^{T_1}_\alpha(0) = y^{T_2}_\alpha(0) = \alpha$, we have

Furthermore, from (3), (7) and the fact that $\varphi$ in (9) is nonnegative and nontrivial, there holds

On $[T_1,T_2]$, $y^{T_2}_\alpha$ is a solution of $y' = g(y)$. Consequently, according to (3), we have $y^{T_2}_\alpha(T_1)< y^{T_2}_\alpha(T_2)$. Finally, it follows that

In other terms

Finally, we have necessarily $\alpha^{T_1}<\alpha^{T_2}$, that is $w^{T_1}(0)<w^{T_2}(0)$.

We show now the continuity property. Let $\tilde{T} \in (T^*,+\infty)$ and $(T_n)_n$ be a sequence of $(T^*,+\infty)$ such that $T_n \xrightarrow{n\to+\infty} \tilde{T}$. We fixe $T^-\in(T^*,\tilde{T})$. There exists $n^-\in\mathbb{N}$ and $T^+>T^*$ such that

We will demonstrate that $w^{T_n}(0) \xrightarrow{n\to+\infty} w^{\tilde{T}}(0)$. Since $0<w^{T_n}\leq1$ and $T\mapsto m^T$ is continuous in $L^\infty_{loc}(\mathbb{R})$, the sequence $(w^{T_n})_n$ converges up to extraction of a subsequence to a function $\tilde{w}$ in $\mathcal{C}^{0,\delta}([0,T^+])$ for any $\delta \in (0,1)$. The equilibrium state $w^{T_n}$ satisfies

Passing to the limit as $n\to+\infty$, we obtain

The function $t \mapsto \int_0^t f^{\tilde{T}}(s,\tilde{w}(s))ds$ is of class $\mathcal{C}^1([0,\tilde{T}])$. Consequently $\tilde{w}$ is of class $\mathcal{C}^1([0,\tilde{T}])$ and it satisfies

and $0\leq\tilde{w}\leq1$ in $[0,\tilde{T}]$. Owing to $(II)$, it follows that $\tilde{w}\equiv0$, or $\tilde{w}\equiv w^{\tilde{T}}$. If $\tilde{w} = 0$, then $w^{T_n}\to0$ as $n\to+\infty$ uniformly on $[0,T^+]$. For any $n\in\mathbb{N}$, we have

We integrate the previous equation over $[0,T_n]$, then we pass to the limit as $n\to+\infty$. We obtain $-\tilde{T}\lambda_{0,f^{\tilde{T}}} = 0$. It is a contradiction because $\lambda_{0,f^{\tilde{T}}}<0$, as $\tilde{T}>T^*$. Hence, we have necessarily $\tilde{w} \equiv w^{\tilde{T}}$. The uniqueness of the accumulation point of $(w^{T_n})_n$ implies that the convergence holds for the whole sequence. In particular, $w^{T_n}(0)\xrightarrow{n\to+\infty}w^{\tilde{T}}(0)$, and consequently, the function $T \mapsto w^T(0)$ is continuous on $(T^*,+\infty)$.

We study now the behavior of the equilibrium state $w^T$ for the limit cases where $T\to (T^*)^+$ and $T\to+\infty$. We begin by showing that the function $w^T$ converges uniformly to $0$ on $\mathbb{R}$ as $T\to (T^*)^+$. Let $(T_n)_n$ be a sequence such that $T_n\xrightarrow{n\to+\infty}T^*$ and $T_n>T^*$ for any $n\in \mathbb{N}$. Since $(T_n)_n$ is bounded, there exists $T^+>T^*$ such that for any $n\in \mathbb{N}$ we have $T_n\in(T^*,T^+)$. Up to extraction of a subsequence, $(w^{T_n})_n$ converges to a function $w^*$ in $\mathcal{C}^{0,\delta}([0,T^+])$ for any $\delta \in (0,1)$. The equilibrium state $w^{T_n}$ satisfies

Passing to the limit as $n\to+\infty$, we obtain

The function $t \mapsto \int_0^t f^{T^*}(s,w^*(s))ds$ is of class $\mathcal{C}^1([0,T^*])$. Consequently $w^*$ is of class $\mathcal{C}^1([0,T^*])$ and it satisfies

and $0\leq w^* \leq 1$ on $[0,T^*]$. According to $(II)$, $w^*\equiv0$. The uniqueness of accumulation point of $(w^{T_n})_n$ implies that the convergence holds for the whole sequence. Furthermore since $[0,T_n]\subset[0,T^+]$ for any $n\in\mathbb{N}$, by $T_n$-periodicity of $w^{T_n}$, it occurs that

which completes the proof of this point.

We study now the case where $T\to+\infty$ under assumptions (9) and (10). The function $w^T$ converges on average to $1$ as $T$ tends to $+\infty$. We give a technical lemma.

Lemma 2.3. Under assumptions (9) and (10), the real number $\delta$ defined by

is positive. Furthermore, $\delta<1$.

Proof. We argue by way of contradiction. Let us suppose there exists a sequence $(T_n)_n$ such that $T_n \xrightarrow{n\to+\infty}+\infty$ and $w^{T_n}(1)\xrightarrow{n\to+\infty}0$. We fix $T^+>T^*$. There exists $n^+\in\mathbb{N}$ such that for any $n\geq n^+$, we have $T_n \in [T^+,+\infty)$. According to the monotonicity of $T \mapsto w^T(0)$, it follows that

Up to extraction of a subsequence, $(w^{T_n})_n$ converges to a function $w^*$ in $\mathcal{C}^{0,\beta}([0,1])$ for any $\beta \in (0,1)$. Passing to the limit as $n\to+\infty$ in the previous inequalities implies that

The same reasoning as previously implies that the function $w^*$ is of class $\mathcal{C}^1([0,1])$ and satisfies the Cauchy problem

By uniqueness, we have necessarily $w^*\equiv0$, that is, $w^{T_n}$ converges uniformly to $0$ on $[0,1]$, which contradicts (37). Lastly, each function $w^T$ ranges in $(0,1]$, and due to (7) and the nontriviality of $\varphi$ in (9), one has $w^T<1$ on $\mathbb{R}$. Hence, we have $\delta<1$.

We return to the proof of the last point of Proposition 1. We consider $y_\delta$ the solution of the Cauchy problem

where $\delta \in(0,1)$ is defined in Lemma 2.3. Let $\varepsilon >0$ be such that $\delta<1-\varepsilon <1$. Since $y_\delta (t) \xrightarrow{t\to+\infty}1$, there exists $l_\varepsilon >1$ such that $y_\delta (l_\varepsilon ) = 1-\varepsilon / 2$. We define $T_\varepsilon = 4l_\varepsilon /\varepsilon$ ($>l_\varepsilon$), and we consider $T\geq T_\varepsilon$. The function $w^T$ is a solution of

Since $w^T(1)\geq\delta$, we have $w^T\geq y_\delta$ on $[1,T)$. In particular $w^T(l_\varepsilon )\geq1-\varepsilon / 2$, and since $w^T$ is increasing on $(l_\varepsilon ,T)$, we have

Furthermore

Yet,

and

So $|\frac{1}{T}\int_0^Tw^T(t)dt-1|\leq \varepsilon$, and the proof of Proposition 1 is complete.

2.2.   Proof of Proposition 3

We begin by showing the characterization of $c_T^*$ with the principal eigenvalue $\lambda_{0,f^T}$. Let $\mu\in \mathbb{R}$. We denote $\lambda_\mu$ the principal eigenvalue and $\Phi_\mu$ the principal eigenfunction associated with the operator $L_\mu:\mathcal{C}^1(\mathbb{R})\to\mathcal{C}^0(\mathbb{R})$ defined by $L_\mu\Psi = \Psi_t-\big(\mu^2+f_u^T(t,0)\big)\Psi.$ Consequently, we have

We divide the previous equation by $\Phi_\mu$, then we integrate between $0$ and $T$. According to the fact that $\Phi_\mu$ is $T$-periodic, we obtain $\lambda_\mu = -\mu^2+\lambda_{0,f^T}$. In [21], Nadin gives the following characterization of the critical speed $c_T^*$:

Consequently, we have

We thus look for the smallest real number $c$ for which the equation $\mu^2-\mu c-\lambda_{0,f^T} = 0$ of the variable $\mu$ admits a positive solution. An elementary calculation leads to $c^*_T = 2\sqrt{-\lambda_{0,f^T}}.$ Consequently, we have

Hence the function $T\in(T^*,+\infty)\mapsto c^*_T$ is continuous, increasing if $\int_0^T m^T(t)dt$ does not depend on $T$, and we have the two limits cases

which concludes the proof of Proposition 3.

2.3.   Proof of Proposition 4

Let $\alpha\in[0,1]$. We recall that if $y_\alpha:\mathbb{R}\to\mathbb{R}$ is the solution of the Cauchy problem

then we denote $P^T:\alpha\in [0,1]\mapsto P^T(\alpha) = y_\alpha(T)$ the Poincaré map associated to the function $f^T$. According to the proof of Proposition 1, there exists a fixed point of $P^T$ in $(0,1]$. Nevertheless, since hypothesis (4) is not satisfied here, this fixed point is not necessarily unique. We define

To simplify the notations, we denote $y^T:\mathbb{R}\to\mathbb{R}$ the function $y^T = y_{\alpha_0}$. We begin by proving that this infimum is not equal to zero.

Lemma 2.4. We have $\alpha_0>0.$

Proof. We assume that $\alpha_0 = 0.$ So, there exists a sequence $(\alpha_n)_n \subset (0,1]^N$ such that $P^T(\alpha_n) = \alpha_n$ and $\alpha_n \xrightarrow{n\to+\infty} 0$. We divide the equation $y'_{\alpha_n} = f^T(t,y_{\alpha_n})$ by $y_{\alpha_n}$, then we intregrate between $0$ and $T$. We obtain

Passing to the limit as $n \to +\infty$, since $y_{\alpha_n}\to0$ uniformly on $[0,T]$ as $n\to+\infty$ by Cauchy-Lipschitz theorem, we have

which contradicts the fact that $\lambda_{0,f^T}<0$. Consequently $\alpha_0>0$. Notice also that, by continuity of $P^T$, there holds $P^T(\alpha_0) = \alpha_0$, and $y^T = y_{\alpha_0}$ solves (14). Furthermore $0<y^T\leq1$ on $\mathbb{R}$.

Since $f^T$ is of class $\mathcal{C}^1(\mathbb{R} \times [0,1],\mathbb{R})$ and $T$-periodic, there exists $\varepsilon _0\in(0,1)$ such that for all $\varepsilon \in (0,\varepsilon _0]$ and for all $t\in \mathbb{R}$ we have

where $\Phi_{0,f^T}$ is the principal eigenfunction associated with $f^T$ and $0$. Since $\lambda_{0,f^T}<0$ and $y^T$ is the smallest positive solution of system (14), we can apply Theorem $2.3$ of the Nadin's paper [21]. Consequently, there exists a couple $(c_0,U_0)$, where $U_0:\mathbb{R}\times\mathbb{R} \to [0,1],~(t,\xi)\mapsto U_0(t,\xi)$ is of class $\mathcal{C}^{1,2}(\mathbb{R}^2)$ and solves

Necessarily $c_0>0$ because Nadin shows in [21] that for $\textstyle{c<2\sqrt{-\lambda_{0,f^T}}}$, which is a positive real number, there is no pulsating front of sped $c$ connecting $0$ and $y^T$. Furthermore, we have

Let $c_1>0$ be a real number such that there exists a pulsating front $U_1$ with speed $c_1$ such that $\partial_\xi U_1<0$ on $\mathbb{R}\times\mathbb{R}$, and let $c_2>c_1$. We are going to prove the existence of a pulsating front $U_2$ such that $(c_2,U_2)$ solves (39) and $\partial_\xi U_2<0$ on $\mathbb{R}^2$. Yet, by [21], the set

is closed and included in $[2\sqrt{-\lambda_{0,f^T}},+\infty)$. This will conclude the proof of Proposition 4 by denoting $c_T^{**} = \inf\mathcal{C}$.

Given $c_1<c_2$ as above, let $a>0$ and $r\in\mathbb{R}$. We define

We consider the problem

We begin by showing that the previous problem has a solution.

Proposition 8. There exists a solution to problem (40).

Proof. We consider the problem

where $\psi \in \mathcal{C}^0([-a,a],[0,1])$. This Cauchy problem admits a solution $U_\psi$ defined on $\mathbb{R}^+\times [-a,a]$. Furthermore, $0\leq U_\psi\leq 1$ in $\mathbb{R}^+\times [-a,a]$ from the maximum principle and the definition of $\varepsilon _{a,r}$. We define the closed convex set

Note that this set is not empty since $\Phi_{0,f^T}>0$, $U_1\leq1$ and $\varepsilon _{a,r}\Phi_{0,f^T}(0)\leq U_1(0,\cdot+r)$ on $[-a,a]$ according to the definition of $\varepsilon _{a,r}$. We start by proving that if $\psi \in C$, then $U_\psi(T,\cdot) \in C$ using a comparison lemma.

Lemma 2.5. Let $\psi \in C$. Then we have

Proof. Since $\partial_\xi U_1<0$ on $\mathbb{R}\times\mathbb{R}$ and $c_1<c_2$, the function $U_1(\cdot,\cdot+r)$ satisfies on $[0,+\infty) \times (-a,a),$

Moreover, since $\psi\in C$, we have $U_1(0,\cdot+r) \geq \psi$ on $[-a,a]$ and, according to the definition of $\varepsilon _{a,r}$ and the $T$-periodicity of $U_1$ and $\Phi_{0,f^T}$, we have $U_1(\cdot,a+r) \geq \varepsilon _{a,r}\Phi_{0,f^T}$ on $[0,+\infty)$. Consequently, we can apply a comparison principle, and we obtain

In the same way, since $\varepsilon _{a,r}\leq\varepsilon _0$, and according (38) and the negativity of $\lambda_{0,f^T}$, we have on $[0,+\infty) \times (-a,a)$

Furthermore since $\psi\in C$, we have $\varepsilon _{a,r}\Phi_{0,f^T}(0) \leq \psi$ on $[-a,a]$ and, according to the definition of $\varepsilon _{a,r}$ and the $T$-periodicity of $U_1$ and $\Phi_{0,f^T}$, we have $\varepsilon _{a,r}\Phi_{0,f^T} \leq U_1(\cdot,-a+r)$ on $[0,+\infty)$. Consequently, we can apply a comparison principle and we conclude that

The fact that the inequalities in (41) are strict is a consequence of the strong maximum principle.

We return to the proof of Proposition 8. We consider

Owing to (41) and the $T$-periodicity of $\Phi_{0,f^T}$ and $U_1$, $\mathcal{T}$ is well defined. We are going to demonstrate using the Schauder's fixed point theorem that the function $\mathcal{T}$ has a fixed point in the closed convex set $C$. We show now that $\mathcal{T}$ is continuous. In fact we show that $\mathcal{T}$ is a Lipschitz-continuous function. Let $\psi$ and $\varphi$ in $C$. We have on $(0,T]\times [-a,a]$

where $\beta:(0,T]\times[-a,a]\to \mathbb{R}$ is defined by

Since $|\beta| \leq \|f_u^T\|_{L^\infty([0,T]\times[0,1])}$ on $(0,T]\times[-a,a]$, and $U_\psi-U_\varphi = 0$ on $[0,T]\times\{-a,a\}$, the maximum principle yields for any $(t,\xi)\in [0,T] \times [-a,a]$

If we take $t = T$, we obtain

So $\mathcal{T}$ is a Lipschitz-continuous function.

We prove now that $\mathcal{T}({C})$ is compact. Let $(\psi_n)_n$ be a sequence of $C$. By standard parabolic estimates, the sequence $(U_{\psi_n}(T,\cdot))_n$ is bounded in $\mathcal{C}^{2,\alpha}([-a,a],[0,1])$ for any $\alpha \in (0,1)$. Since $\mathcal{C}^{2,\alpha}([-a,a],[0,1])$ embeds compactly into $\mathcal{C}^0([-a,a],[0,1])$, $(U_{\psi_n}(T,\cdot))_n$ converges up to extraction of a subsequence in $C$.

So, according to Shauder's fixed point theorem, there exists $\psi_{a,r} \in \mathcal{C}([-a,a],[0,1])$ such that $\mathcal{T}(\psi_{a,r}) = \psi_{a,r}$, that is $U_{\psi_{a,r}}(T,\cdot) = U_{\psi_{a,r}}(0,\cdot)$. Actually, the function $U_{\psi_{a,r}}$ is solution of (40). By uniqueness and $T$-periodicity of $f^T$, $U_{\psi_{a,r}}$ can be extended as a $T$-periodic solution of (40) in $\mathbb{R}\times[-a,a]$.

To simplify the notations, we denote now $U_{a,r}$ instead of $U_{\psi_{a,r}}$. Owing to Lemma 2.5 and the $T$-periodicity of $U_{a,r}$, we have the following inequalities

We are now going to use a sliding method and we first give a comparison lemma.

Lemma 2.6. Let $U$ and $V$ be two $T$-periodic functions solving problem (40). Let $h \in [0,2a]$. We define $V_h(t,\xi) = V(t,\xi+h)$ for any $(t,\xi)\in [0,T]\times [-a,a-h]$. Then, we have

Proof. We denote $I_h = [-a,a-h]$. For $h = 2a$, we have $I_h = \{-a\}$. Since $U(\cdot,-a) = U_1(\cdot,-a+r)$, $V_{2a}(\cdot,-a) = V(\cdot,a) = \varepsilon _{a,r}\Phi_{0,f^T}$ and

it occurs that $V_{2a}< U~\text{on}~[0,T]\times I_{2a}$. Furthermore, $V_h\leq U$ on $[0,T]\times I_h$ for all $h\in[0,2a]$ sufficiently close to $2a$, by continuity of $U$ and $V$. Consequently, we can define

We have $0\leq h^*<2a$. We are going to show by way of contradiction that $h^* = 0$. Thus let us suppose that $h^*>0$. By continuity and $T$-periodicity of $U$ and $V_h^*$, the definition of $h^*$ implies that

Furthermore, if we define the bounded function $\eta:\mathbb{R} \times I_{h^*} \to\mathbb{R}$ by

then, we have on $\mathbb{R} \times I_{h^*}$

Consequently, according to (43) and (44), if there exists $(t^*,\xi^*)\in \mathbb{R}\times(-a,a-h^*)$ such that $U(t^*,\xi^*) = V_{h^*}(t^*,\xi^*)$, then, by the strong maximum principle, the continuity and the $T$-periodicity of $U$ and $V_{h^*}$, we have

Yet, according to (42) (which is automatically fulfilled from the arguments used in Lemma 2.5), and since $\partial_\xi U_1<0$ on $\mathbb{R}\times\mathbb{R}$, we have for any $t\in\mathbb{R}$,

Consequently, $V_{h^*}< U~\text{on}~ \mathbb{R} \times [-a,a-h^*)$. Furthermore, according to (42), for any $t\in\mathbb{R}$, we also have

So, it occurs that

Since $[0,T] \times I_{h^*}$ is a compact set, and both $U$ and $V$ are continuous on $[0,T]\times[-a,a]$, there exists $h_0\in(0,h^*)$ such that for any $\eta \in(0,h_0)$, we have $V_{h^*-\eta}<U$ on $[0,T]\times I_{h^*-\eta}$. This contradicts the definition of $h^*$. Consequently we have $h^* = 0$ and the proof of Lemma 2.6 is complete.

Corollary 1. There exists a unique function $U_{a,r}$ solving (40).

Proof. We apply the conclusion of Lemma 2.6 with $h = 0$ and reverse the roles of $U$ and $V$.

Corollary 2. The function $r\in\mathbb{R} \mapsto U_{a,r}\in \mathcal{C}^0\big([0,T]\times[-a,a],[0,1]\big)$ is continuous.

Proof. Let $r^*\in\mathbb{R}$ and $(r_n)_n$ be a sequence of real numbers such that $r_n \xrightarrow{n \to \infty}r^*$. According to standard parabolic estimates and the $T$-periodicity of each function $U_{a,r_n}$, there exists $U^*$ such that, up to extraction of a subsequence, $U_{a,r_n} \xrightarrow{n \to \infty} U^*$ in $\mathcal{C}^{1,\frac{\alpha}{2}}$ in $t$ and in $\mathcal{C}^{2,\alpha}$ in $\xi$, for any $\alpha \in(0,1)$. Consequently,

The uniqueness of the solution of the previous problem (Corollary 1) implies that we have $U^* = U_{a,r^*}$, and that the whole sequence $(U_{a,r_n})$ converges to $U^*$.

Corollary 3. For any $t\in[0,T]$ and $\xi\in(-a,a)$, we have

Proof. We apply Lemma 2.6 with $U = V = U_{a,r}$. The strict inequality is a consequence of the maximum principle applied to $\partial_\xi U_{a,r}$.

Proposition 9. There exist $\varepsilon _a\in(0,\varepsilon _0]$ and $r_a\in\mathbb{R}$ such that $U_{a,r_a}(0,0) = \frac{\varepsilon _a\Phi_{0,f^T}(0)}{2}$.

Proof. There exists $(t_{a,r},\xi_{a,r})\in[0,T]\times[-a,a]$ such that

Let $(r_n)_n$ be a sequence of real numbers such that $r_n \xrightarrow{n\to+\infty}-\infty$. There exists a function $U_{a,-\infty}$ such that up to extraction of a subsequence, $U_{a,r_n}\xrightarrow{n\to+\infty}U_{a,-\infty}$ in $\mathcal{C}^{0,\alpha}\big([0,T]\times[-a,a]\big)$ for any $\alpha\in(0,1)$. Since $(t_{a,r_n})_n$ is bounded, there exists $t_a\in[0,T]$ such that up to extraction of a subsequence, we have $t_{a,r_n}\xrightarrow{n\to+\infty}t_a$. So, according to the fact that $(\xi_{a,r_n})$ is also bounded (because $a$ is fixed here), it follows that

We thus have $U_{a,-\infty}(\cdot,a) = \varepsilon _a\Phi_{0,f^T}$ on $[0,T]$. Consequently, since $\partial_\xi U_{a,-\infty}\leq0$ on $[0,T]\times[-a,a]$, it occurs that $U_{a,-\infty}(0,0) \geq \varepsilon _a\Phi_{0,f^T}(0)$. So there exists $n_0\in\mathbb{N}$ such that $r_{n_0}<0$ and

Let now $(\tilde{r}_n)_n$ be a sequence of real numbers such that $\tilde{r}_n \xrightarrow{n\to+\infty}+\infty$.There exists a function $U_{a,+\infty}$ such that up to extraction of a subsequence $U_{a,{\tilde{r}_n}}\xrightarrow{n\to+\infty}U_{a,+\infty}$ in $\mathcal{C}^{0,\alpha}([0,T]\times[-a,a])$ for any $\alpha\in(0,1)$. Furthermore, for any $t\in[0,T]$, we have $U_{a,\tilde{r}_n}(t,-a) = U_1(t,-a+\tilde{r}_n)\xrightarrow{n\to+\infty}0$. Consequently, since $\partial_\xi U_{a,+\infty}\leq0$ and $U_{a,+\infty}\geq0$ on $[0,T]\times[-a,a]$, it occurs that $U_{a,+\infty}\equiv0$. So, there exists $n_1\in \mathbb{N}$ such that $\tilde{r}_{n_1}>0$ and

According to Corollary 2, there exists $r_a \in (r_{n_0},\tilde{r}_{n_1})$ such that

which completes the proof.

Proposition 10. There exists a sequence $a_n\xrightarrow{n\to+\infty}+\infty$ such that $U_{a_n,r_{a_n}}$ converges on any compact set in $\mathcal{C}^{1,\frac{\alpha}{2}}$ in $t$ and in $\mathcal{C}^{2,\alpha}$ in $\xi$, for any $\alpha \in(0,1)$, to a function $U_2$ solving (39) with $c = c_2$, and such that $(U_2)_\xi <0$ on $\mathbb{R}^2$.

Proof. Since $t_a$ is bounded, there exist $t^*\in[0,T]$ and a sequence $a_n\xrightarrow{n\to+\infty}+\infty$ such that $t_{a_n}\xrightarrow{n\to+\infty}t^*$. Consequently,

According the standard parabolic estimates, up to extraction of a subsequence, $U_{a_n,r_{a_n}}$ converges on any compact set to a function $U_2$ in $\mathcal{C}^{1,\frac{\alpha}{2}}$ in $t$ and in $\mathcal{C}^{2,\alpha}$ in $\xi$, for any $\alpha \in(0,1)$. The function $U_2$ satisfies

Since $(\varepsilon ^*\Phi_{0,f^T})' \leq f^T(t,\varepsilon ^*\Phi_{0,f^T})$ and $(y^T)' = f^T(t,y^T)$ on $[0,T]$ and since we have $\varepsilon ^*\Phi_{0,f^T}(0)\leq y^T(0)$, it occurs that $\varepsilon ^*\Phi_{0,f^T} \leq y^T$ on $[0,T]$. Consequently

The functions $U_2(\cdot,-\infty)$ and $U_2(\cdot,+\infty)$ solve the equation $y' = f(t,y)$ on $[0,T]$. Furthermore, $U_2(t,\xi)\leq y^T(t)$ for all $t\in[0,T]$ and all $\xi\in\mathbb{R}$, since this inequality holds for $U_1$ and since each function $U_{a,r}$ satisfies (42). Consequently, since $(U_2)_\xi\ \leq 0$ on $[0,T]\times\mathbb{R}$, we have necessarily $U_2(\cdot,-\infty) = y^T$ and $U_2(\cdot,+\infty) = 0$. Finally we apply the strong maximum principle to the equation satisfied by $(U_2)_\xi$ and obtain $(U_2)_\xi< 0$ on $\mathbb{R}^2$ (otherwise $(U_2)_\xi$ would be identically equal to zero, which is impossible since $U_2(\cdot,-\infty) = y^T$ and $U_2(\cdot,+\infty) = 0$).

3.   Nonlinearities asymptotically periodic in time with perturbation

3.1.   Proof of Theorem 1.4

Let $T>0$ with $T\neq T^*$ (that is $\lambda_{0,f^T}\neq0$). We define

where $C$ is defined in (23). Let $\varepsilon \in(0,\varepsilon _T)$. According to (23) and (25), there exists $n_\varepsilon \in\mathbb{N}^*$ such that for all $t\geq n_\varepsilon T$ and for all $u\geq0$ we have

We define the $T-$periodic functions $f_{-\varepsilon }^T:\mathbb{R}\times \mathbb{R}^+ \to \mathbb{R}$ and $f_e^T:\mathbb{R}\times \mathbb{R}^+ \to \mathbb{R}$ by

According to (7), it occurs that

Furthermore, according to (4) and (6), for any $u\in [2,+\infty)$, we have $g(u) / u \leq g(2) / 2<0$. Consequently, since $\textstyle{\varepsilon \in (0,-\frac{1}{C+1}\frac{g(2)}{2})}$, the following inequality is true

Concerning the principal eigenvalues associated with the equilibrium $0$ and functions $f^T$, $f^T_{-\varepsilon }$ and $f^T_e$, the following relations hold

We begin by handling the case where $T<T^*$. Owing to (50), the fact that $\lambda_{0,f^T}>0$ and since $\textstyle{\varepsilon \in (0,\frac{\lambda_{0,f^T}}{C+1})}$, we have

We consider $v_\varepsilon :\mathbb{R}^+\times\mathbb{R} \to\mathbb{R}$ the solution of the Cauchy problem

Owing to (46) and the $T-$periodicity of $f^T_\varepsilon$, the function $u_\varepsilon (\cdot+n_\varepsilon T,\cdot)$ satisfies on $(0,+\infty)\times \mathbb{R}$

So, applying a comparison principle, we obtain

According to (51), Proposition 2 applied with the $T$-periodic nonlinearity $f^T_\varepsilon$ implies that

Hence, owing to (52),

which concludes the proof of the first part of Theorem 1.4.

We now consider the case where $T>T^*$. Since $\lambda_{w^T,f^T}>0$, there exists $\mu_T>0$ such that for all $\mu\in(0,\mu_T)$ and for all $(t,u,v)\in\mathbb{R}\times [0,2]^2$, we have

We define the two positive real numbers $\tilde{M}_T$ and $\tilde \varepsilon _T$ by

and

where $\Phi_{w^T,f^T}$ is the principal eigenfunction associated with $f^T$ and the equilibrium state $w^T$. Let $\varepsilon \in(0,\tilde \varepsilon _T)$. According to (50), the fact that $\lambda_{0,f^T} <0$ and since $\textstyle{\varepsilon \in (0,-\frac{\lambda_{0,f^T}}{C+1})}$, we have

Owing to (48), (49) and (55), the same proof as in Proposition 1 implies that there exists a unique $T$-periodic positive equilibrium state $w^T_\varepsilon$ (resp. $w^T_{-\varepsilon }$) associated with $f^T_\varepsilon$ (resp. $f^T_{-\varepsilon })$. Furthermore, for any $t\in\mathbb{R}$, we have $w^T_\varepsilon (t)\in(0,2]$ (resp. $w^T_{-\varepsilon }(t)\in(0,2]$).

Lemma 3.1. There exists $M_T>0$ independent of $\varepsilon$ such that

Proof. We begin by proving the first inequality. We define the function $\bar v_\varepsilon :\mathbb{R}\to\mathbb{R}$ by

We are interested in the problem

We will show that $\bar v_\varepsilon$ is a strict supersolution and $w^T$ is a strict subsolution of (57). Let $t\in\mathbb{R}$. We have

Since $\textstyle{\varepsilon \in(0,\frac{\mu_T}{\tilde{M}_T\sup\limits_{[0,T]}\Phi_{w^T,f^T}}})$, we have $|\bar v_\varepsilon (t)-w^T(t)|\leq\mu_T$. Furthermore, $w^T(t)\in[0,1]$, and since $\textstyle{\varepsilon \in(0,\frac{1}{\tilde{M}_T\sup\limits_{[0,T]}\Phi_{w^T,f^T}}})$, the definition of $\bar v_\varepsilon$ implies that $\bar v_\varepsilon (t)\in[0,2]$. Consequently, it follows from (53) that

Consequently,

Yet $\textstyle{\varepsilon \in (0,\frac{\lambda_{w^T,f^T}}{4(C+1)})}$. So

Hence

Consequently, according to the definition of $\tilde{M}_T$, it follows that

Finally, $\bar v_\varepsilon$ is a strict supersolution of (57).

We now show that $w^T$ is a strict subsolution of this problem. Let $t\in\mathbb{R}$. We have

According to Lemma $3.1$ of [22], there exists a solution $\tilde{w}_\varepsilon$ of (57), and one has

In particular, $\tilde{w}_\varepsilon$ is a positive solution of (57). So, by uniqueness, we have $\tilde{w}_\varepsilon = w^T_\varepsilon$. Finally, inequalities (58) rewrite

where $M_T$ is defined by $\textstyle{M_T = \tilde{M}_T\sup_{[0,T]}\Phi_{w^T,f^T}}$.

We now give a sketch of the proof of the second inequality of Lemma 3.1. We define the function $\underline v _\varepsilon :\mathbb{R}\to\mathbb{R}$ by

We are interested in the problem

We can show in the same way as previously that $\underline v _\varepsilon$ is a strict subsolution and that $w^T$ is a strict supersolution of (59). According to Lemma $3.1$ of [22], there exists a solution $\hat{w}_\varepsilon$ of (59), and one has

Yet $\textstyle{\varepsilon \in(0,\frac{\inf\limits_{[0,T]}w^T}{2\tilde{M}_T\sup\limits_{[0,T]}\Phi_{w^T,f^T}})}$. So for any $t\in\mathbb{R}$

Consequently $\hat{w}_\varepsilon$ is a positive solution of (59). So, by uniqueness, we have $\hat{w}_\varepsilon = w^T_{-\varepsilon }$. Finally, inequalities (60) rewrite

which completes the proof of Lemma 3.1.

Let us now complete the proof of Theorem Theorem 1.4. We recall that $\varepsilon \in(0,\tilde \varepsilon _T)$, where $\tilde \varepsilon _T$ is defined in (54). Let $K \subset \mathbb{R}$ be a compact set and let $\eta>0$. We consider $\tilde{u}_\varepsilon :\mathbb{R}^+\times\mathbb{R}\to\mathbb{R}$ and $\tilde{u}_{-\varepsilon }:\mathbb{R}^+\times\mathbb{R}\to\mathbb{R}$ solving respectively

and

where $n_\varepsilon \in \mathbb{N}$ is such that (46) holds for all $(t,u)\in [n_\varepsilon T,+\infty)\times \mathbb{R}^+$, and $u_\varepsilon$ solves (26). The function $v_\varepsilon :\mathbb{R}^+\times \mathbb{R} \to \mathbb{R}, (t,x) \mapsto u_\varepsilon (t+n_\varepsilon T,x)$ satisfies

Owing to (46) and the $T$-periodicity of $f^T_\varepsilon$, it occurs that on $\mathbb{R}^+ \times \mathbb{R}$

Consequently, since $v_\varepsilon (0,\cdot) = u_\varepsilon (n_\varepsilon T, \cdot) = \tilde{u}_\varepsilon (0,\cdot)$ on $\mathbb{R}$, applying a comparison principle, we obtain

In other words

Actually, we can show in the same way that

According to the $T$-periodicity of $w^T$, we have $w^T = w^T(\cdot+n_\varepsilon T)$ on $\mathbb{R}$. Hence, for any $(t,x)\in \mathbb{R}^+ \times \mathbb{R}$

Therefore, for any $(t,x)\in \mathbb{R}^+ \times K$,

On the other hand, owing to Proposition 2, there exists $t_{\varepsilon ,K,\eta}>0$ such that for any $t\geq t_{\varepsilon ,K,\eta}$

According to Lemma 3.1, (61) and (62), we thus have, for any $(t,x)\in[ t_{\varepsilon ,K,\eta},+\infty)\times K$

In other words, for any $t\geq t_{\varepsilon ,K,\eta}+n_eT$ we obtain

That is

which completes the proof of Theorem 1.4.

3.2.   Proof of Proposition 5

We begin by proving $(I)$. According to (25), there exists $t_0\geq0$ such that

where we recall that $g(2)<0$. According to (4) and (6), for any $u\in [2,+\infty)$, we have $g(u) / u \leq g(2) / 2<0$. Consequently, (63) implies that

We define

The real number $M$ is a supersolution of (26). Furthermore, $0$ is solution of (26) and $0 \leq u(0,\cdot) \leq M$ on $\mathbb{R}$. Consequently, according to the maximum principle we have

We denote $v:\mathbb{R}^+\to\mathbb{R}$ the function satisfying

Owing to (65), we have $0\leq u(t_0,\cdot)\leq M$ on $\mathbb{R}$. It follows from the comparison principle that

Furthemore, since $2\leq M$, it follows from (64) that

To summarize

We will show that $\textstyle{v(t)\xrightarrow{t\to+\infty}0}$. We argue by way of contradiction assuming there exists a real number $\delta_0>0$ and a sequence $\textstyle{t_n\xrightarrow{n\to+\infty}+\infty}$ such that

For any $n\in \mathbb{N}$, we write $t_n = \tilde{t}_n+k_n T^*$, where $\tilde{t}_n\in[0,T^*)$ and $k_n\in\mathbb{N}$, and we define the function $v_n:[-k_nT^*,+\infty)\to\mathbb{R}$ by $v_n(t) = v(t+k_nT^*)$. The function $v_n$ satisfies

Up to extraction of a subsequence, $\textstyle{\tilde{t}_n\xrightarrow{n\to+\infty}t^*\in[0,T^*]}$. Consequently, according to (25) and the Arzela-Ascoli theorem, there exists $v^*:\mathbb{R}\to\mathbb{R}$ such that $v_n\xrightarrow{n\to+\infty} v^*$ locally uniformly on $\mathbb{R}$ and which satisfies

Furthermore, owing to (66), we have

We consider $\sigma:\mathbb{R}^+\to\mathbb{R}$ such that

Owing to (7) and the fact that $M\geq1$, we have $\sigma(0)\geq\sigma(T^*)$. Consequently, the sequence $(\sigma(nT^*))_n$ is nonincreasing. Furthermore, it is bounded below by $0$. Hence, it converges up to extraction of a subsequence to a real number $l\geq0$. For any $n\in\mathbb{N}$, we define the function $\sigma_n:\mathbb{R}^+\to\mathbb{R}$ by $\sigma_n(t) = \sigma(t+nT^*)$. The sequence $(\sigma_n)_n$ converges up to extraction of a subsequence in $\mathcal{C}^1([0,T^*])$ to a function $\sigma^*$ satisfying

According to Proposition 1, we have necessarily $\sigma^* = 0$, and thus, the convergence holds for all the sequence. Owing to (68), for any $n\in\mathbb{N}$, we have $v^*(-nT^*)\leq M$. Consequently, since $f^{T^*}$ is $T^*-$periodic, we can apply a comparison principle and we obtain

In particular

Passing to the limit as $n\to+\infty$, we obtain

which is a contradiction with (67). Consequently $v(t)\xrightarrow{t\to+\infty}0$ and thus, we conclude the proof of (Ⅰ) using (66).

We now prove (Ⅱ). We begin by considering the case where $f(t,u) = f^{T^*}(t,u)$ and $p(t,u) = u$ for any $(t,u)\in\mathbb{R}^+\times\mathbb{R}^+$. In this case, we have

Let $\varepsilon \in(0,-g(2) / 2)$. The function $f_\varepsilon$ is $T^*$-periodic, and we have

Furthermore $\lambda_{0,f_\varepsilon } = \lambda_{0,f^{T^*}}-\varepsilon = -\varepsilon <0.$ Consequently, owing to Theorem 1, there exists $w^T_\varepsilon :\mathbb{R}\to(0,+\infty)$ solving (14) with $f_\varepsilon$ as nonlinearity. According to Proposition 2, for all compact set $K\subset\mathbb{R}$, we have

We now consider the case where $p(t,u)\leq0$ for any $(t,u)\in\mathbb{R}\times\mathbb{R}^+$. In this case

We denote $u$ the solution of the Cauchy problem

From the comparison principle, it occurs that

According to (Ⅰ), we have $\sup\limits_{x\in\mathbb{R}}u(t,x) = 0.$ Consequently $\sup\limits_{x\in\mathbb{R}}u_\varepsilon (t,x) = 0,$ which concludes the proof.

3.3.   Proof of Theorem 1.5

Proof. Let $T>T^*$ and $c \in (0,c_T^*)$, where $c_T^*$ is the critical speed associated with $f^T$ defined in Proposition 1.3. We recall that for $\varepsilon \in(0,\tilde \varepsilon _T)$, where $\tilde \varepsilon _T$ is defined in (54), inequalities (46), (48), (49) and (55) are satisfied. Furthermore, the critical speeds associated with nonlinearities $f^T_\varepsilon$ and $f^T_{-\varepsilon }$ are respectively defined by

and

In particular, since $c_T^* = 2\sqrt{|\lambda_{0,f^T}|} = 2\sqrt{-\lambda_{0,f^T}}$, there exists $\varepsilon _{c,T}>0$ such that for all $\varepsilon \in(0,\varepsilon _{c,T})$ we have

We define

We consider $\varepsilon \in(0,\hat \varepsilon _{c,T})$. According to the strong maximum principle, we have $u_\varepsilon (n_\varepsilon T,\cdot)>0$ on $\mathbb{R}$, where $n_\varepsilon \in \mathbb{N}$ is such that (46) holds for all $(t,u)\in [n_\varepsilon T,+\infty)\times \mathbb{R}^+$. Consequently, there exists a nonnegative and nontrivial compactly supported function $\tilde{u}_{\varepsilon ,0}:\mathbb{R} \to \mathbb{R}$ such that

Let $\tilde{u}_\varepsilon :\mathbb{R}^+ \times \mathbb{R} \to \mathbb{R}$ be the solution of the Cauchy problem

Owing to (46), (72) and the fact that $f^T_{-\varepsilon }$ is $T$-periodic, we can apply a comparison principle and get that

According to (49), we have $f_\varepsilon \leq0$ on $\mathbb{R}^+\times[2,+\infty)$. Hence, since $u_0$ is bounded, if we define

then according to the maximum principle, we have $u_\varepsilon \leq \tilde{C}$ on $\mathbb{R}^+\times \mathbb{R}$. In particular

Let $v_\varepsilon :\mathbb{R}^+\to \mathbb{R}$ be the solution of

Owing to (46) and (74), we can still apply a comparison principle to get that

According to (49) and the fact that $\tilde{C} \geq 2$, it occurs that $v_\varepsilon (T)\leq v_\varepsilon (0)$. So the sequence $(v_\varepsilon (nT))_n$ is nonincreasing. Furthermore, this sequence is bounded below by $0$. Consequently, it converges to a real number $l\geq0$. For any $n\in \mathbb{N}$, we define $v_{\varepsilon ,n}:\mathbb{R}^+\to \mathbb{R}$ by $v_{\varepsilon ,n}(t) = v_\varepsilon (t+nT).$ The sequence $(v_{\varepsilon ,n})_n$ converges up to extraction of a subsequence to $v^*_\varepsilon \geq0$ in $\mathcal{C}^1([0,T])$ satisfying

So $v^*_\varepsilon$ is equal to $0$ or $w^T_\varepsilon$. Yet, there exists $\kappa_\varepsilon >0$ such that $0 <\kappa_\varepsilon \Phi_{0,f^T_\varepsilon }(0) \leq \tilde{C}$ and

Consequently, we have on $\mathbb{R}^+$

Hence, the function $\kappa_\varepsilon \Phi_{0,f^T_\varepsilon }$ is a subsolution of the problem (75) on $\mathbb{R}^+$. Therefore

Using the $T$-periodicity of $\Phi_{0,f^T_\varepsilon }$ and passing to the limit as $n\to +\infty$, we obtain

Consequently, we have necessarily $v^*_\varepsilon \equiv w^T_\varepsilon$ on $[0,T]$. In particular, the uniqueness of accumulation point of the sequence $(v_{\varepsilon ,n})_n$ implies that the convergence to $w^T_\varepsilon$ holds for the whole sequence. Let $\eta>0$. There exists $n_{\eta,\varepsilon }\in \mathbb{N}$ such that

On the other hand, according to (70), the spreading properties in periodic case (Proposition 1.3) give the existence of $t_{c,\eta,\varepsilon }\geq0$ such that

Let $(t,x)\in \mathbb{R}^+\times \mathbb{R}$ such that $t\geq \max\{t_{c,\eta,\varepsilon },n_{\eta,\varepsilon }T\}$ and $|x|<ct$. According to (73) and (76), it occurs that

The fact that $t\geq n_{\eta,\varepsilon } T$ implies that we can write $t = n_t T +\tilde{t}$, where $\tilde{t}\in [0,T)$ and $n_t \in \mathbb{N}$ such that $n_t\geq n_{\eta,\varepsilon }$. Consequently, as the function $w^T$ is $T$-periodic, we have

Hence, according to (77) and Lemma 3.1

and on the other hand, owing to (78) and Lemma 3.1, it occurs that

To conclude, for any $t\geq \max\{t_{c,\eta,\varepsilon },n_{\eta,\varepsilon } T\}+n_\varepsilon T$, we have

which concludes the proof of the first assertion of Theorem 1.5.

We now show the second part of the theorem. We consider $c>c_T^*$ and $c'$ such that $c_T^* <c' <c$. There exists $\varepsilon '_{c,T}>0$ such that for all $\varepsilon \in(0,\varepsilon '_{c,T})$ we have

Furthermore, according to (4), (23) and (25), there exists $D>0$ such that for all $\varepsilon \in [0,1)$, we have

We define $\bar \varepsilon _{c,T} = \min\{1,\hat \varepsilon _{c,T},\varepsilon '_{c,T}\}>0$, where $\hat \varepsilon _{c,T}$ is defined in (71). Let $\varepsilon \in (0,\bar \varepsilon _{c,T})$. We consider $H:\mathbb{R}^+\times\mathbb{R}\to\mathbb{R}$ solving the heat equation

The function $H$ is given by

where $\text{Supp}(u_0)$ is the support of $u_0$, which is here assumed to be compact. We define the function $H_D:\mathbb{R}^+\times\mathbb{R}\to\mathbb{R}$ by $H_D(t,x) = H(t,x)e^{Dt}$. We have $(H_D)_t-(H_D)_{xx} = DH_D$ on $(0,+\infty)\times\mathbb{R}$. Furthermore, owing to (80), we have $(u_e)_t-(u_e)_{xx} = f_\varepsilon (t,u_e)\leq Du_\varepsilon$ on $(0,+\infty)\times\mathbb{R}$. Consequently, since $H_D(0,\cdot) = u_\varepsilon (0,\cdot) = u_0$ on $\mathbb{R}$, the comparison principle yields

In particular, owing to (81), it occurs that

We define the real number

Let us note that $(c')^2+4\lambda_{0,f^T_\varepsilon }>0~\text{because}~c'>c_{T,\varepsilon }^* = 2\sqrt{-\lambda_{0,f^T_\varepsilon }}$. According to (82), $u_\varepsilon (n_\varepsilon T,\cdot)$ has a Gaussian decay as $|x|\to+\infty$ and in particular, there exists a real number $M_{c',\varepsilon }>0$ such that

We also define the function $v_{c',\varepsilon } :\mathbb{R}^+ \times \mathbb{R} \to \mathbb{R}$ by

We have on $\mathbb{R}^+ \times \mathbb{R}$

Hence according to (5) and the fact that $-\gamma_{c',\varepsilon }^2+\gamma_{c',\varepsilon }c'+\lambda_{0,f^T_e} = 0$, we obtain on $\mathbb{R}^+\times \mathbb{R}$

Furthermore, owing to (46), (47) and the $T$-periodicity of $f^T_\varepsilon$, it occurs that on $\mathbb{R}^+ \times \mathbb{R}$

Consequently, since (83) implies that $u_\varepsilon (n_\varepsilon T,\cdot)\leq v_{c',\varepsilon }(0,\cdot)$ on $\mathbb{R}$, the comparison principle implies that

For all $t\geq0$, since $v_{c',\varepsilon }(t,\cdot)$ is decreasing on $\mathbb{R}$, we have

In the same way, we can show that

To summarize

which concludes the proof of the second assertion of Theorem 1.5.

4.   Influence of the protocol of the treatment

We begin by proving Proposition 6.

Proof. Owing to (28), the principal eigenvalue associated with $0$ and $f^T_\tau$ is given by

We now demonstrate Proposition 7.

Proof. Let $T>T^*$. We denote $P_T^T$ the Poincaré map associated with $f^T_T$. We recall that $P_T^T$ is defined on $\mathbb{R}^+$ by

where $y_{\tau ,\alpha}$ is the solution of the Cauchy problem

In the same way as in the proof of Proposition 1, we show that the function $P^T_\tau$ has a unique positive fixed point $\alpha_\tau ^T$. Furthermore $\alpha_\tau ^T \in(0,1]$. Consequently there is a unique equilibrium state $w^T_\tau :\mathbb{R}\to(0,1]$ associated with $f^T_\tau$. It is the solution of the Cauchy problem (84) with $\alpha = \alpha_\tau ^T$.

We begin by showing the continuity property. Let $\tau^* \in (0,T)$ and $(\tau_n)_n$ be a sequence of $(0,T)$ such that $\tau_n \xrightarrow{n\to+\infty} \tau^*$. We will demonstrate that $w_{\tau_n}^T(0) \xrightarrow{n\to+\infty} w_{\tau^*}^T(0)$. The sequence $(w_{\tau _n}^T)_n$ converges up to extraction of a subsequence to a function $w^*$ in $\mathcal{C}^{0,\delta}([0,T])$ for any $\delta \in (0,1)$. The equilibrium state $w_{\tau _n}^T$ satisfies

Passing to the limit as $n\to+\infty$, we obtain

The function $t \mapsto \int_0^t f_{\tau ^*}^T(s,w^*(s))ds$ is of class $\mathcal{C}^1([0,T])$. Consequently $w^*$ is of class $\mathcal{C}^1([0,T])$ and it satisfies

Owing to Proposition 1, it follows that $w^*\equiv0$, or $w^*\equiv w^T_{\tau ^*}$. If $w^* = 0$, then $w^T_{\tau_n}\to0$ as $n\to+\infty$ uniformly on $[0,T]$. For any $n\in\mathbb{N}$, we have

We integrate the previous equation over $[0,T]$, then we pass to the limit as $n\to+\infty$. We obtain $-T\lambda_{0,f^T_{\tau^*}} = 0$. It is a contradiction because since $T>T^*$, we have $\lambda_{0,f^T_{\tau^*}} = \lambda_{0,f^T}<0$. Hence, we have necessarily $w^*\equiv w_{\tau ^*}^T$. So the function $\tau \mapsto w^T_\tau (0)$ is continuous on $(0,T)$.

We now study the monotonicity of this function. We consider two real numbers $\tau _1$ and $\tau _2$ such that $0<\tau _1<\tau _2< T$. The Poincaré map $P^T_{\tau _i}$ associated with $f^T_{\tau _i}$ is defined on $\mathbb{R}^+$ by

where $y_{\tau _i,\alpha}$ is the solution of (84), with $\tau = \tau_i$. We recall that the equilibrium state $w^T_{\tau _i}$ is the solution on $\mathbb{R}^+$ of (84) with $\alpha = \alpha^T_{\tau _i}$. Consequently, if we prove that $P^T_{\tau_1}>P^T_{\tau_2}$ on $(0,+\infty)$, then we will deduce that $\alpha^T_{\tau _1}>\alpha^T_{\tau _2}$, that is, $w_{\tau _1}^T(0)>w_{\tau _2}^T(0)$. Fix $\alpha>0$. We define the function $z_{\tau _i,\alpha}:\mathbb{R}^+ \to \mathbb{R}$ by

This function solves on $\mathbb{R}^+$ the equation

For any $t\in[0,T]$, we have

According to (4) and the fact that $z_{\tau _1,\alpha}>0$, it follows that for any $t\in[0,T]$

In other terms, $z_{\tau_1,\alpha}$ is a subsolution of the equation satisfied by $z_{\tau _2,\alpha}$. Since $z_{\tau _1,\alpha}(0) = z_{\tau _2,\alpha}(0) = \alpha$, we can apply a comparison principle and we obtain

Actually, the previous inequality is strict with $t = T$ because (86) and (87) are strict on $(0,\tau _2)$. Owing to (85), we have

According to (28), it occurs that

Consequently

In other words, $P_{\tau _1}^T(\alpha) > P_{\tau _2}^T(\alpha)$, which concludes the proof.