Abstract
Some Diophantine equations related to the soliton solutions of the Korteweg-de Vries equation are resolved. The main tools are the connection with Bernoulli polynomials and the application of certain computational number-theoretical results.
MSC:11D41, 14H45, 11Y50.
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Dedication
Dedicated to Professor Hari M Srivastava
1 Introduction
In the paper [1], Fairlie and Veselov obtained a relation of the Bernoulli polynomials with the theory of the Korteweg-de Vries (KdV) equation
This equation has infinitely many conservation laws (that is, certain laws, which show that a particular measurable property of an isolated physical system, like mass, energy, momentum, etc., does not change as the system evolves) of the form
where are some polynomials of the function u and its x-derivatives up to order m, see [2]. For example,
and
The KdV equation possesses a remarkable family of so-called n-soliton solutions corresponding to the initial profile . For some recent generalizations and applications of the Korteweg-de Vries equation, we refer to [3, 4] and [5] and the references given therein.
Using the spectral theory of Schrödinger operators, see [6], Fairlie and Veselov [1] proved that there is a strong connection between the improver integrals related to the functions above and the well-known discrete sums of power values, namely,
for .
Now, let be fixed integers with , and suppose that
One can ask how often can these integrals be equal for given k and l? In other words, what is the cardinality of the set of solutions m, n to the equation
where k and l are fixed distinct integers? Of course, one can consider the much more general problem, when k and l are also unknown integers; however, in this case, the solution of the corresponding equation seems beyond the reach of current techniques.
Applying some recent results by Rakaczki, see [7] and [8], it is not too hard to give some ineffective and effective finiteness statements for the solutions m and n to equation (1). However, the purpose of this note is to resolve (1) for certain values of m and n, including an infinite family of the parameters.
Theorem 1 For and , equation (1) has only one solution, namely, .
Theorem 2 Assume that and l is a positive integer such that is prime. Then (1) has no solution in positive integers m and n.
2 Auxiliary results
In our first lemma, we summarize some classical properties of Bernoulli polynomials. For the proofs of these results, we refer to [9].
Lemma 1 Let denote the jth Bernoulli polynomial and , . Further, let be the denominator of . Then we have
-
(A)
,
-
(B)
,
-
(C)
, , ,
-
(D)
(von Staudt-Clausen) ,
-
(E)
(in ),
-
(F)
.
Consider the hyperelliptic curve
where . Let α be a root of F, and let be the Jacobian of the curve . We have that
where and κ comes from a finite set. By knowing the Mordell-Weil group of the curve , it is possible to provide a method to compute such a finite set. To each coset representative of , we associate
where the set is stable under the action of Galois, all are non-zero and , where is an algebraic integer and . If , are conjugate, then we may suppose that , and so, , are conjugate. We have the following lemma (Lemma 3.1 in [10]).
Lemma 2 Let be a set of κ values, associated as above to a complete set of coset representatives of . Then is a finite subset of , and if is an integral point on the curve (2), then for some and .
As an application of his theory of lower bounds for linear forms in logarithms, Baker [11] gave an explicit upper bound for the size of integral solutions of hyperelliptic curves. This result has been improved by many authors (see, e.g., [12–18] and [19]).
In [10], an improved completely explicit upper bound were proved combining ideas from [15, 19–25]. Now we will state the theorem, which gives the improved bound. We introduce some notation. Let K be a number field of degree d, and let r be its unit rank, and let R be its regulator. For , we denote by the logarithmic height of the element α. Let
and let
Define the constants
Let
where are number fields. Define
The following result will be used to get an upper bound for the size of the integral solutions of our equations. It is Theorem 3 in [10].
Lemma 3 Let α be an algebraic integer of degree at least 3, and let κ be an integer belonging to K. Denote by , , distinct conjugates of α and by , , the corresponding conjugates of κ. Let
and
In what follows R stands for an upper bound for the regulators of , and , and r denotes the maximum of the unit ranks of , , . Let
and let
and let
Define
and
If satisfies for some then
To obtain a lower bound for the possible unknown integer solutions, we are going to use the so-called Mordell-Weil sieve. The Mordell-Weil sieve has been successfully applied to prove the non-existence of rational points on curves (see, e.g., [26–28] and [29]).
Let be a smooth projective curve (in our case a hyperelliptic curve) of genus . Let J be its Jacobian. We assume the knowledge of some rational point on C, so let D be a fixed rational point on C, and let ȷ be the corresponding Abel-Jacobi map
Let W be the image in J of the known rational points on C and generators for the free part of . By using the Mordell-Weil sieve, we are going to obtain a very large and smooth integer B such that
Let
so that the image of ϕ is the free part of . The variant of the Mordell-Weil sieve explained in [10] provides a method to obtain a very long decreasing sequence of lattices in
such that
for .
The next lemma [[10], Lemma 12.1] gives a lower bound for the size of rational points, whose images are not in the set W.
Lemma 4 Let W be a finite subset of , and let L be a sublattice of . Suppose that . Let be a lower bound for and
Denote by M the height-pairing matrix for the Mordell-Weil basis , and let be its eigenvalues. Let
and let be the Euclidean norm of the shortest non-zero vector of L. Then, for any , either or
The following lemma plays a crucial role in the proof of Theorem 1.
Lemma 5 The integral solutions of the equation
are
Proof of Lemma 5 Let be the Jacobian of the genus two curve (3). Using MAGMA, we determine a Mordell-Weil basis, which is given by
Let , and let α be a root of f. We will choose for coset representatives of the linear combinations , where . Then
where , and is constructed as described in Lemma 2. We have that . By local arguments, it is possible to restrict the set further (see, e.g., [26, 30]). In our case, one can eliminate
by local computations in . We apply Lemma 3 to get a large upper bound for in the remaining cases. A MAGMA code was written to obtain the bounds that appeared in [10]; they can be found at http://www.warwick.ac.uk/~maseap/progs/intpoint/bounds.m. We obtain that these bounds are as in Table 1.
The set of known rational points on the curve (3) is . Let W be the image of this set in . Applying the Mordell-Weil sieve, implemented by Bruin and Stoll and explained in [10], we obtain that , where
that is
Now, we use an extension of the Mordell-Weil sieve due to Samir Siksek to obtain a very long decreasing sequence of lattices in . After that, we apply Lemma 4 to obtain a lower bound for possible unknown rational points. We get that if is an unknown integral point, then
This contradicts the bound for that we obtained by Baker’s method. □
3 Proofs of the theorems
Proof of Theorem 1 For and , we have the Diophantine equations
and
respectively. One can see that the first three equations are elliptic Diophantine equations, thus using the program package MAGMA, subroutines IntegralPoints or IntegralQuarticPoints are just a straightforward calculation to solve them. In these cases, the unique solution is . The forth equation can be written as follows
So, we easily obtain a hyperelliptic curve
where and . By Lemma 5, we have that . Therefore, we have that , a contradiction and there is no solution in positive integers of (7). □
Proof of Theorem 2 Now and is a prime. From (1), we get
Let m and n be an arbitrary but fixed solution. An elementary number theoretical argument and Lemma 1 yield that and
Suppose that , and let d be the smallest positive integer such that , and let . Since is divisible by p for and , we have that p is not a divisor of d. The constant term of the polynomial is , and, by von Staudt-Clausen theorem, it is not divisible by p. On the other hand, p is a divisor of m and , we have a contradiction. If , then we can repeat the previous argument using the fact , cf. Lemma 1. □
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Acknowledgements
The work is supported by the TÁMOP-4.2.2.C-11/1/KONV-2012-0010 project. The project is implemented through the New Hungary Development Plan, co-financed by the European Social Fund and the European Regional Development Fund. Research was supported in part by the Hungarian Academy of Sciences, OTKA grants K75566, K100339, NK101680, NK104208 (ÁP) and OTKA grants PD75264, NK104208, K100339 and János Bolyai Research Scholarship of the Hungarian Academy of Sciences (ST). The authors are grateful to the reviewers for their helpful remarks.
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Pintér, Á., Tengely, S. The Korteweg-de Vries equation and a Diophantine problem related to Bernoulli polynomials. Adv Differ Equ 2013, 245 (2013). https://doi.org/10.1186/1687-1847-2013-245
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DOI: https://doi.org/10.1186/1687-1847-2013-245