Abstract
In this article, we investigate Gevrey and summability properties of the formal power series solutions of the inhomogeneous generalized Boussinesq equations. Even if the case that really matters physically is an analytic inhomogeneity, we systematically examine here the cases where the inhomogeneity is s-Gevrey for any
Keywords
Introduction
Setting the problem
The nonlinear evolution equations are often used to represent the motion of the isolated waves, localized in a small part of space in many fields such as optical fibers, neural physics, solid state physics, hydrodynamics, diffusion process, plasma physics and nonlinear optics (nonlinear heat equation, nonlinear Klein–Gordon equation, nonlinear Euler–Lagrange equation, Burgers equation, Korteweg–de Vries equation, Boussinesq equation, etc.).
When studying such equations, one of the major challenges is the determination of exact solutions, if any exists, and the precise analysis of their properties (dynamic, asymptotic behavior, etc.) in order to have a better understanding of the mechanism of the underlying physical phenomena and dynamic processes.
Thus, for several decades, many analytical methods have been developed in this perspective. For example, in the case of real variables, that is when the variables
In the following, we will be more particularly interested in this theory which we shall apply to the generalized Boussinesq equation.
The generalized Boussinesq equation
The Boussinesq equation
In the case of real variables, Eq. (1.1) has already been the subject of many investigations and many results have already been established (see for instance [1,6,27] and the references therein). On the other hand, to our knowledge, it does not seem that there are known results when (at least) one of the coefficients a, b, or c is variable, or when the variables t and x are complex.
In the present paper, we are interested in the following inhomogeneous generalized Boussinesq equation
the inhomogeneity We denote
the initial conditions
The very general Eq. (1.2), and in particular the consideration of variable coefficients, allows to consider many very general physical problems: varying characteristic velocities of long waves, varying bathymetry, improved frequency dispersion, improved nonlinear behavior, inclusion of wave breaking, inclusion of surface tension, inclusion of internal waves on an interface between fluid domains of different mass density, etc.
Considering t as the variable and x as a parameter, we have the following.
Equation (
1.2
) admits a unique formal solution
Let us write the coefficients
In the two previous articles [21,25] (see also [17], and [22,24,26] for more general equations), the author studied, in the framework of the Euler–Lagrange equation (1.3), the Gevrey regularity and the 1-summability of the formal solution
(Gevrey regularity [25]).
Let
(Summability [21]).
Let Moreover, the 1-sum
Observe that, even in the case that really matters physically speaking, that is
In this article, we propose to prove that these two results remain true in the case of the generalized Boussinesq equation (1.2) with the same noteworthy dichotomy on the Gevrey data: above 1-Gevrey, the formal solution
The organization of the article is as follows. Section 2 is devoted to the study of the Gevrey regularity of the formal solution
Gevrey regularity of
As said at the beginning of Section 1.2, we consider the time t as the variable and the space x as a parameter. Thereby, to define the notion of Gevrey formal power series in
Main result
Before stating our main result on the Gevrey regularity of the formal solution
(s-Gevrey formal series).
Let
In other words, Definition 2.1 means that
Observe that the set
Observe also that the sets
([2,17]).
Let
Let us now state the result in view in this section.
Let
Observe that Theorem 2.3 coincides with Proposition 1.3 in the case of the Euler–Lagrange equation (1.3), that is in the case where the polynomials P and Q are both zero.
Observe also that Theorem 2.3 provides the Gevrey regularity of the classical Boussinesq equation (1.1).
The formal solution
Corollary 2.4 will be improved later for some special values of its coefficients (see Proposition 2.13). The proof of Theorem 2.3 is detailed in the next two sections. The first point is the most technical and the most complicated. Its proof is based on the Nagumo norms, a technique of majorant series and a fixed point procedure (see Section 2.2). As for the second point, it stems both from the first one and from Proposition 2.13 that gives an explicit example for which
According to Proposition 2.2, it is clear that
Reciprocally, let us fix
We must prove that the coefficients
Before starting the calculations, let us first recall for the convenience of the reader the definition of the Nagumo norms and some of their properties which are needed in the sequel.
Nagumo norms
Let
Following Proposition 2.6, whose a proof can be found for instance in [19], gives us some properties of the Nagumo norms.
Let
Inequalities 4–5 of Proposition 2.6 are the most important properties. Observe besides that the same index r occurs on their both sides, allowing thus to get estimates for the product
Let us now turn to the proof of the first point of Theorem 2.3.
From the recurrence relations (1.4), we first derive for all
Applying then the Nagumo norms of indices
For all
For all
For all
Let us first observe that the assumption On the other hand, applying successively the Vandermonde Inequality (see Proposition A.2) and Proposition A.4, we get
Inequality (2.3) follows. The proof of inequalities (2.4) and (2.5) is similar and is left to the reader.
□
Applying Lemma 2.8 to the previous relations (2.2), we finally get the inequalities
The following result, which will be useful in the next section, provides some bounds on these various terms.
There exist two positive constants
Given the hypothesis on the coefficients
We shall now bound the Nagumo norms
Let us consider the formal power series
The following inequalities hold for all
According to the initial conditions on the for all for all
Consequently, using the fact that
Following Proposition 2.11 allows us to bound the
The formal series
It is sufficient to prove the convergence of
First of all, let us start by observing that
Notice that the convergence of
Let us now assume
We are left to prove the convergence of
According to Lemma 2.10 and Proposition 2.11, we can now bound the Nagumo norms
Let
We are now able to conclude the proof of the first point of Theorem 2.3.
We must prove on the sup-norm of the
Proof of Theorem 2.3: Second point
Let us fix
To conclude that we can not say better about the Gevrey order of
Let us consider the inhomogeneous Boussinesq equation
Then, the formal solution
According to the remark above, it is sufficient to prove that
First of all, let us rewrite Eq. (2.11) in the form
Let us now suppose that
This achieves the proof of the second point of Theorem 2.3.
In this section, we consider the critical value
1-Summable formal series
Still considering t as the variable and x as a parameter, one extends, in the similar way as the s-Gevrey formal series (see Definition 2.1), the classical notion of 1-summability of formal series in
Among the many equivalent definitions of 1-summability in a given direction
(1-summability).
A formal series u is defined and holomorphic on for any for any proper2 A subsector Σ of a sector
Notice that, for any fixed
Notice also that the 1-sum of a 1-summable formal series
Denote by
Let
With respect to t, the 1-sum
The operator of 1-summation
The following result investigates the 1-summability of the analytic functions at the origin
Let
Let us fix a direction
Let us now turn to the study of the 1-summability of the formal solution
Before stating our main result, let us start with a preliminary remark. Let us write the coefficients
We are now able to state the main result in view in this section.
Let Moreover, the 1-sum
Observe that Theorem 3.5 coincides with Proposition 1.4 in the case of the Euler–Lagrange equation (1.3), that is in the case where the polynomials P and Q are both zero.
First of all, let us observe that the necessary condition of the first point is straightforward from Proposition 3.2, and that the second point stems obvious from Corollary 3.3. Consequently, we are left to prove the sufficient condition of the first point. To this end, we fix from now on a direction θ and we suppose that the inhomogeneity
First step: An associated equation
Let us set
Second step: The fixed point procedure
Let us set
Observe that
Let us now respectively denote by
To end the proof, it remains to prove that the series
Third step: Some estimates on the
’s
According to Definition 3.1 and Proposition 3.4, there exists a radius
Let us now fix a proper subsector
Let
Then, the following inequalities
The proof proceeds by recursion on μ. The case
According to the relations (3.2), we derive from the generalized Leibniz Formula, from the inequalities (3.3) and (3.5), and from the fact that
Let
Let
□
Let us now bound the polynomials
Let B be the positive real number defined by
The left inequality is obvious since all the coefficients of the
The case
Applying the recurrence relation (3.4) and the fact that
The constant
Let us now prove that
Consequently,
We are now able to improve the bounds of the functions
Let us set
Applying Propositions 3.6 and 3.8, we get
We are now able to complete the proof of Theorem 3.5.
Let us now choose for Σ a sector containing a proper subsector
Thanks to Corollary 3.9, the series
To prove the second condition of Definition 3.1, we proceed as follows. The Removable Singularities Theorem implies the existence of
This achieves the proof of the sufficient condition of the first point of Theorem 3.5, which ends its full proof.
Footnotes
Some technical results on the binomial and multinomial coefficients
In combinatorial analysis, the binomial coefficients
Using the fact that
