Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Bulletin of the American Physical Society

Quantum phases in an asymmetric double-well optical lattice

Saurabh Paul, Eite Tiesinga

Published Jun 4, 2014• 0 citations
OpenAlex

Related papers

Effective three-body interaction in an asymmetric double-well optical lattice

Saurabh Paul, Eite Tiesinga

Bulletin of the American Physical Society•Jun 11, 2015•0 citations

Exploring the phase diagram of a double-well optical lattice

Nathan E. Lundblad, P. Lee, Ben Brown +4 more

Bulletin of the American Physical Society•Jun 7, 2007•1 citation

Phase diagram for ultracold bosons in double-well optical lattices

Ippei Danshita, JAMES E. JUN. WILLIAMS, Carlos A. R. Sá de Melo +1 more

Bulletin of the American Physical Society•Mar 7, 2007•0 citations

Interaction-induced excited-band condensate in a double-well optical lattice

Qi Zhou, J. V. Porto, S. Das Sarma

We show theoretically that interaction effects in a double-well optical lattice can induce condensates in an excited band. For a symmetric double-well lattice, bosons condense into the bottom of the excited band at the edge of the Brillouin zone if the chemical potential is above a critical value. For an asymmetric lattice, a condensate with zero momentum is automatically induced in the excited band by the condensate in the lowest band. This is due to a combined effect of interaction and lattice potential, which reduces the band gap and breaks the inversion symmetry. Our work can be generalized to a superlattice composed of multiple-well potentials at each lattice site, where condensates can be induced in even higher bands.

arXiv:1105.0012•Physical Review A•Sep 26, 2011•18 citations

Phases in an anisotropic two-dimensional optical lattice

Sara Bergkvist, Anders Rosengren, Robert Saers +3 more

Bulletin of the American Physical Society•Mar 7, 2007•0 citations

Symmetry Breaking Ground States of Bose-Einstein Condensates in 1D Double Square Well and Optical Lattice Well

YUANQing-Xin, DINGGuo-Hui

We investigate the phenomena of symmetry breaking and phase transition in the ground state of BoseEinstein condensates (BECs) trapped in a double square well and in an optical lattice well, respectively. By using standing-wave expansion method, we present symmetric and asymmetric ground state solutions of nonlinear Schrodinger equation (NLSE) with a symmetric double square well potential for attractive nonlinearity. In particular, we study the ground state wave function's properties by changing the depth of potential and atomic interactions (here we restrict ourselves to the attractive regime). By using the Fourier grid Hamiltonian method, we also reveal a phase transition of BECs trapped in one-dimensional optical lattice potential.

理论物理通讯:英文版•Jan 1, 2005•0 citations
We show theoretically that interaction effects in a double-well optical lattice can induce condensates in an excited band. For a symmetric double-well lattice, bosons condense into the bottom of the excited band at the edge of the Brillouin zone if the chemical potential is above a critical value. For an asymmetric lattice, a condensate with zero momentum is automatically induced in the excited band by the condensate in the lowest band. This is due to a combined effect of interaction and lattice potential, which reduces the band gap and breaks the inversion symmetry. Our work can be generalized to a superlattice composed of multiple-well potentials at each lattice site, where condensates can be induced in even higher bands.
We investigate the phenomena of symmetry breaking and phase transition in the ground state of BoseEinstein condensates (BECs) trapped in a double square well and in an optical lattice well, respectively. By using standing-wave expansion method, we present symmetric and asymmetric ground state solutions of nonlinear Schrodinger equation (NLSE) with a symmetric double square well potential for attractive nonlinearity. In particular, we study the ground state wave function's properties by changing the depth of potential and atomic interactions (here we restrict ourselves to the attractive regime). By using the Fourier grid Hamiltonian method, we also reveal a phase transition of BECs trapped in one-dimensional optical lattice potential.