Los Alamos National Laboratory
Lab Home  |  Phone
Quantum Institute : 2008 Quantum Lunch Seminar Schedule


  • Coordinator
    Diego Dalvit
  • Quantum Lunch Location:
    T-Division Conference Room, TA-3,
    Building 123, Room 121

Quantum Institute: Visitor Schedule

The Quantum Lunch is regularly held on Thursdays in the Theoretical Division Conference Room, TA-3, Building 123, Room 121.
For more information, contact Diego Dalvit.

Thursday, October 2, 2008
12:30 PM to 2 PM

Speaker: A. M. Rey, JILA and University of Colorado, Department of Physics, University of Colorado

Technical Host: Eddy Timmermans

TOPIC: Exploring quantum magnetism in optical super-lattices

A fundamental problem in quantum physics is to determine whether spin-independent interactions can be the origin of the ferromagnetic or antiferromagnetic ordering observed in some materials. The Hubbard model is one of the minimal models that describes strongly correlated fermions in a lattice and was developed to study quantum magnetism in these systems. The Hubbard model is nevertheless a very complicated model and its phase diagram remains unknown except at half-lling and when there is a single hole. Spinor atoms in optical lattices are highly controllable systems ideal to investigate quantum magnetism in strongly correlated systems. They have the potential to help us understand the Hubbard model phase diagram. However, to achieve this goal we have to start by exploring the known regions rst. This is going to be the topic of this talk. In the rst part I am going to describe a novel approach to prepare, detect and control super-exchange interactions in ultracold spinor atoms loaded in double well superlattices [1]. Recently this approach was used for the rst experimental observation of super-exchange interactions in ultra-cold atoms [2]. In the second part I am going to discuss how to prepare and detect the ferromagnetic order that arises in the present of a single hole using an array of plaquettes (four lattice sites coupled in a square). The latter is also known as Nagaoka ferromagnetism.

[1] A. M. Rey, V. Gritsev,I. Bloch, E. Demler, and M. D. Lukin, PRL 99, 140601 (2007). [2] S. Trotzky, P. Cheinet, S. Folling, M. Feld, U. Schnorrberger, A.M. Rey, A. Polkovnikov, E. Demler, M. D. Lukin, and I. Bloch, Science 319, 295 (2008).

Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA

Inside | © Copyright 2007-8 Los Alamos National Security, LLC All rights reserved | Disclaimer/Privacy | Web Contact