Singular continuous spectrum

Speaker: 

Fan Yang

Institution: 

Ocean University, visiting UCI

Time: 

Thursday, January 14, 2016 - 2:00pm

Location: 

rh 340p

For singular operators of the form (H_{\alpha,\theta}u)_n=u_{n+1}+u_{n-1}+
\frac{g(\theta+n\alpha)}{f(\theta+n\alpha)} u_n, we prove such operators
have purely singular continuous spectrum on the set
{E: \delta{(\alpha,\theta)}>L(E)\}, where f and g are both analytic functions
on T.

 

 

 

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Singular continuous spectrum for singular potentials

Speaker: 

Fan Yang

Institution: 

Ocean University

Time: 

Thursday, January 7, 2016 - 2:00pm

Location: 

RH 340P

We prove that Schrodinger operators with meromorphic potentials have purely singular continuous spectrum on the set {E: \delta{(\alpha,\theta)}>L(E)\} where \alpha is the frequency, \theta is the phase, delta is an explicit function, and L is the Lyapunov exponent. This extends a result of Jitomirskaya and Liu for the Maryland model to the general class of meromorphic potentials.

Full measure reducibility and localization for quasiperiodic Jacobi operators.

Speaker: 

Rui Han

Institution: 

UCI

Time: 

Thursday, December 10, 2015 - 2:00pm

Location: 

RH 340 P

In this talk we show that if the normalized cocycle related to a quasiperiodic Jacobi operator H_{v,c} (where v being the potential and c being the off-diagonal term) is reducible to a constant rotation for almost all energies with respect to the density of states measure, then its dual model has either purely point spectrum for almost all phase or purely absolutely continuous spectrum for almost all phase, depending on the winding number of c. As a corollary, we obtain the complete phase-transition of extended Harper's model in the positive Lyapunov exponent region.

Reductions of discrete nonlinear wave equations

Speaker: 

Chris Ormerod

Institution: 

Caltech

Time: 

Monday, November 23, 2015 - 2:00pm

Location: 

NSII 1201

 

The exact solutions of the Korteweg-de Vries (KdV) equation obtained by travelling wave and similarity reductions may be expressed in terms of elliptic functions and Painleve transcendents respectively. Discrete versions of the KdV equation may be obtained from chains of commuting Backlund transformations of the KdV equation. These systems are considered integrable in their own right. This introductory talk will demonstrate how solutions obtained as reductions of the discrete KdV equation give us discrete analogues of elliptic equations and discrete Painleve equations, mimicking the case for the KdV equation.

 

Many-body localization and mobility edges (joint Mathematical Physics and Condensed Matter Physics seminar)

Speaker: 

François Huveneers

Institution: 

Université Paris-Dauphine

Time: 

Monday, November 9, 2015 - 1:00pm

Host: 

Location: 

RH 188

Many-body localization (MBL) generalizes Anderson localization to interacting many-body systems. MBL challenges many fundamental notions of statistical physics. In this talk I will introduce what MBL is from a math-phys perspective. Then I will discuss some striking difference between Anderson localization and MBL, in particular the existence/absence of a mobility edge, i.e. a critical energy (or energy density for many-bod physics) that separates localized states from extended states. (Joint work with W. De Roeck, M. Müller, M. Schiulaz.)

Second phase transition line of the almost Mathieu operator.

Speaker: 

Qi Zhou

Institution: 

Nanjing University

Time: 

Friday, October 16, 2015 - 2:00pm

Location: 

RH 340 P

 

  For the second  phase transition line $\lambda=e^{\beta}$ of  the almost Mathieu operator, we prove that for dense $\alpha$, the operator has purely singular continuous spectrum for every phases, and  for dense $\alpha$, the operator has pure point spectrum for almost every phases. This is joint work with Artur Avila and Svetlana Jitomirskaya. 

Title: Second phase transition line of the almost Mathieu operator.

Speaker: 

Qi Zhou

Institution: 

Nanjing University

Time: 

Thursday, October 29, 2015 - 2:00pm

Location: 

RH 340 P

 

 

Abstract:  For the second  phase transition line $\lambda=e^{\beta}$ of  almost Mathieu operator, we prove that for dense $\alpha$, the operator has purely singular continuous spectrum for every phases, and  for dense $\alpha$, the operator has pure point spectrum for almost every phases. This is joint work with Artur Avila and Svetlana Jitomirskaya. 

Jaksic-Last Theorem for Higher Rank Perturbations

Speaker: 

Anish Mallick

Institution: 

Institute of Mathematical Sciences, Chennai

Time: 

Thursday, November 5, 2015 - 2:00pm

Host: 

Location: 

RH 340P

Consider the generalized Anderson Model
$H^\omega=\Delta+\sum_{n\in\mathcal{N}}\omega_n P_n$, where $\mathcal{N}$ is a countable set, $\{\omega_n\}_{n\in\mathcal{N}}$ are iid randomvariables and $P_n$ are rank $N<\infty$ projections. For these models one can prove theorems analogous to that of Jak\v{s}i\'{c}-Last on the
equivalence of measures.

We show that if the projection $Q_m^\omega P_n$ (where $Q^\omega_m$ is
cannonical projection on the subspace generated by $H^\omega$ and range of
$P_m$) has same rank as $P_n$, then the trace measure
$\sigma_i(\cdot)=tr(P_iE_{H^\omega}(\cdot)P_i)$ and absolute continuous
part of the measure $P_iE_{H^\omega}(\cdot)P_i$ are equivalent for $i=n,m$.
 

Nodal sets in conformal geometry

Speaker: 

Dmitry Jakobson

Institution: 

McGill University

Time: 

Tuesday, September 29, 2015 - 3:00pm to 4:00pm

Host: 

Location: 

RH 340N

We study conformal invariants that arise from nodal sets and negative eigenvalues of conformally covariant operators, which include the Yamabe and Paneitz operators. We give several applications to curvature prescription problems. We establish a version in conformal geometry of Courant's Nodal Domain Theorem. We also show that on any manifold of dimension at least 3, there exist many metrics for which our invariants are nontrivial. We prove that the Yamabe operator can have an arbitrarily large number of negative eigenvalues on any manifold of dimension n>=3. We obtain similar results for some higher order GJMS operators on some Einstein and Heisenberg manifolds. This is joint work with Yaiza Canzani, Rod Gover and Raphael Ponge. If time permits, we shall discuss related results for operators on graphs.

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