Theory of preparation and relaxation of a p-orbital atomic Mott insulator
arXiv:0901.3696 · doi:10.1103/PhysRevA.79.043609
Abstract
We develop a theoretical framework to understand the preparation and relaxation of a metastable Mott insulator state within the first excited band of a 1D optical lattice. The state is loaded by "lifting" atoms from the ground to the first excited band by means of a stimulated Raman transition. We determine the effect of pulse duration on the accuracy of the state preparation for the case of a Gaussian pulse shape. Relaxation of the prepared state occurs in two major stages: double-occupied sites occurring due to quantum fluctuations initially lead to interband transitions followed by a spreading of particles in the trap and thermalization. We find the characteristic relaxation times at the earliest stage and at asymptotically long times approaching equilibrium. Our theory is applicable to recent experiments performed with 1D optical lattices [T. Müller, S. Fölling, A. Widera, and I. Bloch, Phys. Rev. Lett. \textbf{99}, 200405 (2007)].
27 pages, 23 figures: Edited figures, added references
References in corpus (12)
- Many-Body Physics with Ultracold Gases
- Flat bands and Wigner crystallization in the honeycomb optical lattice
- Breakdown of the adiabatic limit in low dimensional gapless systems
- Supplementary Information to the paper ``Breakdown of the adiabatic limit in low dimensional gapless systems''
- State preparation and dynamics of ultracold atoms in higher lattice orbitals
- Atomic matter of non-zero momentum Bose-Einstein condensation and orbital current order
- Breakdown of integrability in a quasi-one-dimensional ultracold bosonic gas
- Unconventional Bose-Einstein Condensations Beyond the "No-node" Theorem
- Prediction of quantum stripe ordering in optical lattices
- Bond algebraic liquid phase in strongly correlated multiflavor cold atom systems
- Unconventional strongly interacting Bose-Einstein condensates in optical lattices
- Incommensurate superfluidity of bosons in a double-well optical lattice