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One dimensional quantum gases: from few to many

Júlia Amorós-Binefa

Published Jul 7, 2016• 0 citations
OpenAlex

Abstract

Following a recent experimental study [Wenz et al. Science 342, 457 (2013)] on the achievement of the thermodynamic limit in a system of one-dimensional (1D) fermions, the project aims to investigate theoretically a similar problem for 1D Bose gases. By considering a system of bosons confined in a 1D harmonic trap and interacting with a single impurity, the plan is to calculate the binding energy of the impurity as the number of bosons in the bath is increased. The analysis will be performed by varying both the coupling strength of the bath and the interspecies interactio

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Following a recent experimental study [Wenz et al. Science 342, 457 (2013)] on the achievement of the thermodynamic limit in a system of one-dimensional (1D) fermions, the project aims to investigate theoretically a similar problem for 1D Bose gases. By considering a system of bosons confined in a 1D harmonic trap and interacting with a single impurity, the plan is to calculate the binding energy of the impurity as the number of bosons in the bath is increased. The analysis will be performed by varying both the coupling strength of the bath and the interspecies interactio
The transition from ``few to many'' has recently been probed experimentally in an ultracold harmonically confined one-dimensional lithium gas, in which a single impurity atom interacts with a background gas consisting of one, two, or more identical fermions [A. N. Wenz et al., Science 342, 457 (2013)]. For repulsive interactions between the background or majority atoms and the impurity, the interaction energy for relatively moderate system sizes was analyzed and found to converge toward the corresponding expression for an infinitely large Fermi gas. Motivated by these experimental results, we apply perturbative techniques to determine the interaction energy for weak and strong coupling strengths and derive approximate descriptions for the interaction energy for repulsive interactions with varying strength between the impurity and the majority atoms and any number of majority atoms.
Cold atomic gases have provided us with a great number of opportunities for studying various physical systems under controlled conditions that are seldom offered in other fields. We are thus at the point where one can truly do quantum simulation of models that are relevant for instance in condensed-matter or high-energy physics, i.e. we are on the verge of a ’cool’ quantum simulator as envisioned by Feynman. One of the avenues under exploration is the physics of one-dimensional systems. Until recently this was mostly in the many-body limit but now experiments can be performed with controllable particle numbers all the way down to the few-body regime. After a brief introduction to some of the relevant experiments, I will review recent theoretical work on one-dimensional quantum systems containing bosons, fermions, or mixtures of the two, with a particular emphasis on the case where the particles are held by an external trap.
Following a recent experimental study [Wenz et al. Science 342, 457 (2013)] on the achievement of the thermodynamic limit in a system of one-dimensional (1D) fermions, the project aims to investigate theoretically a similar problem for 1D Bose gases. By considering a system of bosons confined in a 1D harmonic trap and interacting with a single impurity, the plan is to calculate the binding energy of the impurity as the number of bosons in the bath is increased. The analysis will be performed by varying both the coupling strength of the bath and the interspecies interactio
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We theoretically demonstrate the feasibility of creating Bell states in multicomponent ultracold atomic gases by solely using the ability to control the interparticle interactions via Feshbach resonances. For this we consider two distinguishable impurities immersed in an atomic background cloud of a few bosons, with the entire system being confined in a one-dimensional harmonic trap. By analyzing the numerically obtained ground states we demonstrate that the two impurities can form spatially entangled bipolaron states due to mediated interactions from the bosonic bath. Our analysis is based on calculating the correlations between the two impurities in a two-mode basis, which is experimentally accessible by measuring the particle positions in the left or right sides of the trap. While interspecies interactions are crucial in order to create the strongly entangled impurity states, they can also inhibit correlations depending on the ordering of the impurities and three-body impurity-bath correlations. We show how these drawbacks can be mitigated by manipulating the properties of the bath, namely its size, mass, and intraspecies interactions, allowing one to create impurity Bell states over a wide range of impurity-impurity interactions. Published by the American Physical Society 2024