Some rigidity results for non-commutative Bernoulli shifts

On Cocycle Actions of Non-commutative Bernoulli Shifts

In this paper we investigate the cocycle actions of non-commutative Bernoulli shifts for a countable discrete group G on the AFD II1-factor N = ⊗g∈GMn(C) or ⊗g∈GR, where R is the AFD II1-factor. We show that if G contains some non-amenable exact group, then the fixed point algebra of any its cocycle action is always atomic. We also give another proof of Popa’s cocycle vanishing theorem [15] in ...

Brooks’ theorem for Bernoulli shifts

If Γ is an infinite group with finite symmetric generating set S, we consider the graph G(Γ, S) on [0, 1]Γ by relating two distinct points if an element of s sends one to the other via the shift action. We show that, aside from the cases Γ = Z and Γ = (Z/2Z) ∗ (Z/2Z), G(Γ, S) satisfies a measure-theoretic version of Brooks’ theorem: there is a G(Γ, S)-invariant conull Borel set B ⊆ [0, 1]Γ and ...

Institute for Mathematical Physics Resolving Markov Chains onto Bernoulli Shifts Resolving Markov Chains onto Bernoulli Shifts

global results on some nonlinear partial differential equations for direct and inverse problems

در این رساله به بررسی رفتار جواب های رده ای از معادلات دیفرانسیل با مشتقات جزیی در دامنه های کراندار می پردازیم . این معادلات به فرم نیم-خطی و غیر خطی برای مسایل مستقیم و معکوس مورد مطالعه قرار می گیرند . به ویژه، تاثیر شرایط مختلف فیزیکی را در مساله، نظیر وجود موانع و منابع، پراکندگی و چسبندگی در معادلات موج و گرما بررسی می کنیم و به دنبال شرایطی می گردیم که متضمن وجود سراسری یا عدم وجود سراسر...

Rigidity and Non-rigidity Results on the Sphere

It is a simple consequence of the maximum principle that a superharmonic function u on Rn(i. e. ∆u ≤ 0) which is 1 near infinity is identically 1 on Rn (throughout this paper, n ≥ 3). Geometrically this means that one can not conformally deform the Euclidean metric in a bounded region without decreasing the scalar curvature somewhere. In fact there is a much stronger result: one can not have an...