E9: Optical Kagome Lattice

From left to right: Shao-Wen Chang, Malte Schwarz, Rowan Duim

Lab room: B171 Birge
Lab phone: (510) 643-0543

Undergraduate students: John Ciavarra, Nikhil Maserang
Graduate Students: 
Malte Schwarz, Shao-Wen Chang, Rowan Duim

Former members: Claire Thomas, Thomas Barter, Masayuki Okano, Luca Bayha, Severin Daiss, Vincent Klinkhamer, Gyu-boong Jo, Jennie Guzman, Alex Liebman-Pelaez, Zephy Leung, Charles Brown, Carson Patterson, Ryan Everly

Overview

In this experiment, we study the physics of ultracold bosonic (and soon fermionic) atoms in an optical triangular superlattice, which is formed by superimposing two commensurate triangular lattices at 532nm and 1064nm. Depending on the beam polarization and the relative position between the two lattices, the combined superlattice can take on a variety of geometries, including the triangular, the normal/ trimerized Kagome lattice and the hexamerized triangular lattice.

lattices_landscape.png
Kagome band structure

Kagome band structure

The Kagome lattice is of particular interest to us because it manifests geometric frustration - the phenomenon of having a large number of degenerate ground states for geometric reasons -in various contexts. Frustration forbids ordering even at zero temperature, and often leads to exotic phases of matter. For example, the spin-1/2 antiferromagnetic Heisenberg model in a Kagome lattice is a frustrated quantum system whose ground state is believed to be a spin liquid. Yet there are many open questions about its exact properties. The Kagome lattice also manifests geometric frustration in its band structure, by having a flat excited band. In a flat band, the kinetic energy is quenched and therefore interactions are strongly accentuated, leading to the possibility of hosting subtle interaction-driven phases, including trion-superfluid and supersolid etc. The long term goal of this experiment is to study frustration-related physics and realize the aforementioned exotic phases using ultracold atoms in optical lattices.


In recent years, we have conducted a number of experiments with bosonic rubidium-87 atoms in the triangular superlattice. See below for brief descriptions on those experiments.


New Species: Potassium (Ongoing)

We are building a new apparatus for laser cooling potassium atoms. Unlike rubidium, potassium has a stable fermionic isotope: 40K. By loading a quantum degenerate fermi gas of 40K into the kagome lattice, with appropriate filling, the Pauli Exclusion Principle would allow atoms to populate the flat band in a stable manner.


Interaction-Enhanced Group Velocity of Bosons in the Flat Band of an Optical Kagome Lattice

Tsz-Him Leung, Malte N. Schwarz, Shao-Wen Chang, Charles D. Brown, Govind Unnikrishnan, and Dan Stamper-Kurn
Phys. Rev. Lett. 125, 133001 (2020)
arXiv: 2007.05928

We access the excited bands of the kagome lattice by loading atoms with non-zero momentum in the lattice frame. We are particularly interested in the properties of the third band, which is non-dispersive (flat) in the tight-binding limit. We observe atomic diffraction from such a band, and determined the group velocity from those images. Atomic interactions significantly increase the group velocity in the non-dispersive band, effectively un-flattening it. Gross-Pitaevskii-equation based calculations show good agreement with our data, demonstrating the influence of interactions over a large range of different parameters (like lattice depth or atomic density).

We’re proud that our paper was chosen as the cover of Physical Review Letters Vol. 125, Iss. 13.


Optical Trimerized Kagome lattice

Thomas H. Barter, Tsz-Him Leung, Masayuki Okano, Maxwell Block, Norman Y. Yao, Dan M. Stamper-Kurn, Spatial Coherence of a Strongly Interacting Bose Gas in the Trimerized Kagome Lattice, Phys. Rev. A 101, 011601(R) (2020) | arXiv:1906.11444

0us.png

The trimerized (breathing) Kagome lattice is different from the normal Kagome lattice in having different intra- and inter-trimer bonding. Its richer lattice structure leads to possibility of hosting exotic many-body phases. 

By studying time-of flight images, we measure the coherence of the system as it crosses the superfluid to Mott insulator transition. We show persistent short-range coherence within trimers and asymmetric revealing asymmetric correlations in the system.


Mean Field scaling of the Bose Hubbard Model

C. K. Thomas, T. H. Barter, T.-H. Leung, M. Okano, G.-B. Jo, J. Guzman, I. Kimchi, A. Vishwanath, and D. M. Stamper-Kurn, Mean-Field Scaling of the Superfluid to Mott Insulator Transition in a 2D Optical Superlattice, Phys. Rev. Lett. 119, 100402 (2017) (Editor's suggestions) | arXiv:1702.04433

mean field diffraction pictures.png
mean field scaled data.png

The mean-field treatment of the Bose-Hubbard model predicts properties of lattice-trapped gases to be insensitive to the specific lattice geometry once system energies are scaled by the lattice coordination number z. We test this scaling directly by comparing coherence properties of 87Rb gases that are driven across the superfluid to Mott insulator transition within optical lattices of either the kagome (z=4) or the triangular (z=6) geometries. 


Revealing Broken Inversion Symmetry by Kapitza-Dirac Diffraction

C. K. Thomas, T. H. Barter, T.-H. Leung, S. Daiss, D. M. Stamper-Kurn, Signatures of spatial inversion asymmetry of an optical lattice observed in matter-wave diffraction, Phys. Rev. A 93, 063613 (2016)arXiv:1601.07117.

asy diffraction pictures.png

We demonstrate that even a small potential asymmetry due to vector Stark shift, with peak-to-peak amplitude of ≤ 2.3% of the overall lattice potential, can lead to pronounced inversion asymmetry in the momentum-space diffraction pattern.


Ultracold Atoms in a Tunable Optical Kagome Lattice

kagome.png

G.-B. Jo, J. Guzman, C.K. Thomas, P. Hosur, A. Vishwanath, and D.M. Stamper-Kurn, Ultracold atoms in a tunable optical kagome latticePhysical Review Letters 108, 045305 (2012) | arXiV:1109.1591.

We report the first experimental demonstration of an optical Kagome lattice along with some other lattice geometries and techniques to characterize the lattice.