ABSTRACT
Department of Physics, Colorado School of Mines, Golden, CO 80401, U.S.A.
Rina Kanamoto Division of Advanced Sciences, Ochadai Academic Production, Ochanomizu University, Bunkyo-ku, Tokyo 112-8610 Japan
Masahito Ueda Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033 Japan
Ultracold quantum gases offer a wonderful playground for quantum manybody physics [1], as experimental systems are widely controllable, both statically and dynamically. One such system is the one-dimensional (1D) Bose gas on a ring. In this system binary contact interactions between the constituent bosonic atoms, usually alkali metals, can be controlled in both sign and magnitude; a recent experiment has tuned interactions over seven orders of magnitude [2], using an atom-molecule resonance called a Feshbach resonance. Thus one can directly realize the Lieb-Liniger Hamiltonian (LLH) [3,4], from the weakly-to the strongly-interacting regime. At the same time there are a number of experiments utilizing ring traps [5]. The ring geometry affords us the opportunity to study topological properties of this system as well; one of the main properties of a superfluid is the quantized circulation in which the average angular momentum per particle, L/N , is quantized under rotation [6]. Thus we focus on a tunable 1D Bose system for which the main control parameters are interaction and rotation. We will show that there is a critical boundary in the interaction-rotation control-parameter plane over which the topological properties of the system change. This is the basis of our concept of metastable quantum phase transitions (QPTs). Moreover, we will show that the finite domain of the ring is necessary for the QPT to occur at all because the zero-point kinetic pressure can induce QPTs, i.e., the system must be finite; we thus seek to generalize the concept of QPTs to inherently finite, mesoscopic or nanoscopic systems.1
