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We study the existence and multiplicity of positive solutions for the Dirichlet problem
where λ > 0, 1 < q < 2, p = 2* = 2N/(N − 2), 0 ε Ω ⊂ ℝN, N ≥ 3, is a bounded domain with smooth boundary ∂Ω and f is a non-negative continuous function on . Assuming that f satisfies some hypothesis, we prove that the equation admits at least three positive solutions for sufficiently small λ.
where N ≥ 4, λ > 0, α1, α2, β ε ℝ, p, p > 1, p + q = 2* = 2N/(N − 2) and α1(x), a2(x) ≥ 0 have potential well. By using variational methods and the category theory, we establish the existence of least energy and multiplicity of solutions.
We give sharp conditions under which the composition of two homeomorphisms of finite distortion is of finite distortion and has integrable distortion. As an application, we obtain a generalization of the classical uniqueness theorem of homeomorphic solution to the measurable Riemann mapping problem.
For a class of non-conservative hyperbolic systems of partial differential equations endowed with a strictly convex mathematical entropy, we formulate the initial-value problem by supplementing the equations with a kinetic relation prescribing the rate of entropy dissipation across shock waves. Our condition can be regarded as a generalization to non-conservative systems of a similar concept introduced by Abeyaratne, Knowles and Truskinovsky for subsonic phase transitions and by LeFloch for non-classical undercompressive shocks to nonlinear hyperbolic systems. The proposed kinetic relation for non-conservative systems turns out to be equivalent, for the class of systems under consideration at least, to Dal Maso, LeFloch and Murat's definition based on a prescribed family of Lipschitz continuous paths. In agreement with previous theories, the kinetic relation should be derived from a phase-plane analysis of travelling-wave solutions associated with an augmented version of the non-conservative system. We illustrate with several examples that non-conservative systems arising in the applications fit in our framework, and for a typical model of turbulent fluid dynamics we provide a detailed analysis of the existence and properties of travelling waves which yields the corresponding kinetic function.
We are concerned with the solvability of nonlinear second-order elliptic partial differential equations with nonlinear boundary conditions. We study the generalized Steklov–Robin eigenproblem (with possibly singular weights) in which the spectral parameter is both in the differential equation and on the boundary. We prove the existence of solutions for nonlinear problems when both nonlinearities in the differential equation and on the boundary interact, in some sense, with the generalized spectrum. The proofs are based on variational methods and a priori estimates.
Our purpose in this monograph is to provide a concise and complete introduction to the study of arithmetic differential operators over the p-adic integers ℤp. These are the analogues of the usual differential operators over say, the ring ℂ[x], but where the role of the variable x is replaced by a prime p, and the roles of a function f(x) and its derivative df/dx are now played by an integer α ∈ ℤ and its Fermat quotient δpa = (a - ap)/p.
In making our presentation of these type of operators, we find no better way than discussing the p-adic numbers in detail also, and some of the classical differential analysis on the field of p-adic numbers, emphasizing the aspects that give rise to the philosophy behind the arithmetic differential operators. The reader is urged to contrast these ideas at will, while keeping in mind that our study is neither exhaustive nor intended to be so, and most of the time we shall content ourselves by explaining the differential aspect of an arithmetic operator by way of analogy, rather than appealing to the language of jet spaces. But even then, the importance of these operators will be justified by their significant appearance in number theoretic considerations. One of our goals will be to illustrate how different these operators are when the ground field where they are defined is rather coarse, as are the p-adic integers ℤp that we use.
In going further, we now make a fundamental use of Theorem 2.12 to introduce the notion of arithmetic differential operators over the ring ℤp. This is the essential idea in our work here. In the following chapter, we shall present the theory of these operators in general, discussing the jet spaces whose global sections give rise to them. We shall even expand our explanations to outline the general theory in the case of multiple primes, something that we start also in a simplified manner here. But when we revisit the study of these operators in the remaining chapters, there will be little that we will do beyond our discussion of them over the ring ℤp until the very end. In the very last chapter, we compare the behaviour of these operators over the p-adic integers with their behaviour over its unramified completion.
The idea leading to arithmetic operators embodies a radically different philosophy from that used up until now. This philosophy arises naturally when looking at the p-adic numbers in the setting of the analytic functions of the previous section. For we treat p-adic numbers now as functions, albeit functions on a space of “dimension zero.” These functions all admit the representation (2.4), and so they ought to be considered analytic since these representations are convergent power series in p. Once we agree with the idea of the p-adic numbers as “analytic” functions, it is then only natural to define their derivatives, the arithmetic derivatives of our work.
Let kr(n, δ) be the minimum number of r-cliques in graphs with n vertices and minimum degree at least δ. We evaluate kr(n, δ) for δ ≤ 4n/5 and some other cases. Moreover, we give a construction which we conjecture to give all extremal graphs (subject to certain conditions on n, δ and r).