Orbital optical lattices with bosons. (25th January 2016)

• Record Type: Journal Article
• Authors: Kock, T; Hippler, C; Ewerbeck, A; Hemmerich, A
• Is Part Of: Journal of physics. Volume 49:Number 4(2016:Feb. 15)
• Publication Date: 2016-01-25
• Subjects: Bose–Einstein condensates in optical lattices -- metastable Bloch bands -- orbital degrees of freedom -- topological band degeneracy points -- unconventional superfluid order; 03.75.Lm -- 03.75.Hh -- 03.75.Nt; Atoms -- Periodicals; Molecules -- Periodicals; Optics -- Periodicals; Nuclear physics -- Periodicals; 539.6
• DOI: 10.1088/0953-4075/49/4/042001
• Languages: English
• ISSNs: 0953-4075

Abstract

Abstract: This article provides a synopsis of our recent experimental work exploring Bose–Einstein condensation in metastable higher Bloch bands of optical lattices. Bipartite lattice geometries have allowed us to implement appropriate band structures, which meet three basic requirements: the existence of metastable excited states sufficiently protected from collisional band relaxation, a mechanism to excite the atoms initially prepared in the lowest band with moderate entropy increase, and the possibility of cross-dimensional tunneling dynamics, necessary to establish coherence along all lattice axes. A variety of bands can be selectively populated and a subsequent thermalization process leads to the formation of a condensate in the lowest energy state of the chosen band. As examples the 2nd, 4th and 7th bands in a bipartite square lattice are discussed. The geometry of the 2nd and 7th bands can be tuned such that two inequivalent energetically degenerate energy minima arise at the X ± -points at the edge of the 1st Brillouin zone. In this case even a small interaction energy is sufficient to lock the phase between the two condensation points such that a complex-valued chiral superfluid order parameter can emerge, which breaks time reversal symmetry. In the 4th band a condensate can be formed at the Γ-point in the center of the 1st Brillouin zone, which can be used to explore topologically protected band touching points. The new techniques to access orbital degrees of freedom in higher bands greatly extend the class of many-body scenarios that can be explored with bosons in optical lattices.