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Near Soliton Evolution for Equivariant Schrodinger Maps in Two Spatial Dimensions
  • Language: en
  • Pages: 120

Near Soliton Evolution for Equivariant Schrodinger Maps in Two Spatial Dimensions

The authors consider the Schrödinger Map equation in 2+1 dimensions, with values into \mathbb{S}^2. This admits a lowest energy steady state Q, namely the stereographic projection, which extends to a two dimensional family of steady states by scaling and rotation. The authors prove that Q is unstable in the energy space \dot H^1. However, in the process of proving this they also show that within the equivariant class Q is stable in a stronger topology X \subset \dot H^1.

Directory of Romanian Officials
  • Language: en
  • Pages: 244

Directory of Romanian Officials

  • Type: Book
  • -
  • Published: 1976
  • -
  • Publisher: Unknown

None

Directory of Officials of the Socialist Republic of Romania
  • Language: en
  • Pages: 248

Directory of Officials of the Socialist Republic of Romania

  • Type: Book
  • -
  • Published: 1976
  • -
  • Publisher: Unknown

None

Directory of Officials of the Socialist Republic of Romania
  • Language: en
  • Pages: 252

Directory of Officials of the Socialist Republic of Romania

  • Type: Book
  • -
  • Published: 1976
  • -
  • Publisher: Unknown

None

Critical Population and Error Threshold on the Sharp Peak Landscape for a Moran Model
  • Language: en
  • Pages: 100

Critical Population and Error Threshold on the Sharp Peak Landscape for a Moran Model

The goal of this work is to propose a finite population counterpart to Eigen's model, which incorporates stochastic effects. The author considers a Moran model describing the evolution of a population of size of chromosomes of length over an alphabet of cardinality . The mutation probability per locus is . He deals only with the sharp peak landscape: the replication rate is for the master sequence and for the other sequences. He studies the equilibrium distribution of the process in the regime where

Sheaves on Graphs, Their Homological Invariants, and a Proof of the Hanna Neumann Conjecture
  • Language: en
  • Pages: 124

Sheaves on Graphs, Their Homological Invariants, and a Proof of the Hanna Neumann Conjecture

In this paper the author establishes some foundations regarding sheaves of vector spaces on graphs and their invariants, such as homology groups and their limits. He then uses these ideas to prove the Hanna Neumann Conjecture of the 1950s; in fact, he proves a strengthened form of the conjecture.

A Geometric Theory for Hypergraph Matching
  • Language: en
  • Pages: 108

A Geometric Theory for Hypergraph Matching

The authors develop a theory for the existence of perfect matchings in hypergraphs under quite general conditions. Informally speaking, the obstructions to perfect matchings are geometric, and are of two distinct types: `space barriers' from convex geometry, and `divisibility barriers' from arithmetic lattice-based constructions. To formulate precise results, they introduce the setting of simplicial complexes with minimum degree sequences, which is a generalisation of the usual minimum degree condition. They determine the essentially best possible minimum degree sequence for finding an almost perfect matching. Furthermore, their main result establishes the stability property: under the same ...

Quasi-Linear Perturbations of Hamiltonian Klein-Gordon Equations on Spheres
  • Language: en
  • Pages: 92

Quasi-Linear Perturbations of Hamiltonian Klein-Gordon Equations on Spheres

The Hamiltonian ∫X(∣∂tu∣2+∣∇u∣2+m2∣u∣2)dx, defined on functions on R×X, where X is a compact manifold, has critical points which are solutions of the linear Klein-Gordon equation. The author considers perturbations of this Hamiltonian, given by polynomial expressions depending on first order derivatives of u. The associated PDE is then a quasi-linear Klein-Gordon equation. The author shows that, when X is the sphere, and when the mass parameter m is outside an exceptional subset of zero measure, smooth Cauchy data of small size ϵ give rise to almost global solutions, i.e. solutions defined on a time interval of length cNϵ−N for any N. Previous results were limited either to the semi-linear case (when the perturbation of the Hamiltonian depends only on u) or to the one dimensional problem. The proof is based on a quasi-linear version of the Birkhoff normal forms method, relying on convenient generalizations of para-differential calculus.

Local Entropy Theory of a Random Dynamical System
  • Language: en
  • Pages: 118

Local Entropy Theory of a Random Dynamical System

In this paper the authors extend the notion of a continuous bundle random dynamical system to the setting where the action of R or N is replaced by the action of an infinite countable discrete amenable group. Given such a system, and a monotone sub-additive invariant family of random continuous functions, they introduce the concept of local fiber topological pressure and establish an associated variational principle, relating it to measure-theoretic entropy. They also discuss some variants of this variational principle. The authors introduce both topological and measure-theoretic entropy tuples for continuous bundle random dynamical systems, and apply variational principles to obtain a relationship between these of entropy tuples. Finally, they give applications of these results to general topological dynamical systems, recovering and extending many recent results in local entropy theory.

Shock Waves in Conservation Laws with Physical Viscosity
  • Language: en
  • Pages: 180

Shock Waves in Conservation Laws with Physical Viscosity

The authors study the perturbation of a shock wave in conservation laws with physical viscosity. They obtain the detailed pointwise estimates of the solutions. In particular, they show that the solution converges to a translated shock profile. The strength of the perturbation and that of the shock are assumed to be small but independent. The authors' assumptions on the viscosity matrix are general so that their results apply to the Navier-Stokes equations for the compressible fluid and the full system of magnetohydrodynamics, including the cases of multiple eigenvalues in the transversal fields, as long as the shock is classical. The authors' analysis depends on accurate construction of an approximate Green's function. The form of the ansatz for the perturbation is carefully constructed and is sufficiently tight so that the author can close the nonlinear term through Duhamel's principle.