Abstract

Understanding the behavior of an impurity strongly interacting with a Fermi sea is a long-standing challenge in many-body physics. When the interactions are short-ranged, two vastly different ground states exist: a polaron quasiparticle and a molecule dressed by the majority atoms. In the single-impurity limit, it is predicted that at a critical interaction strength, a first-order transition occurs between these two states. Experiments, however, are always conducted in the finite temperature and impurity density regime. The fate of the polaron-to-molecule transition under these conditions, where the statistics of quantum impurities and thermal effects become relevant, is still unknown. Here, we address this question experimentally and theoretically. Our experiments are performed with a spin-imbalanced ultracold Fermi gas with tunable interactions. Utilizing a novel Raman spectroscopy combined with a high-sensitivity fluorescence detection technique, we isolate the quasiparticle contribution and extract the polaron energy, spectral weight, and the contact parameter. As the interaction strength is increased, we observe a continuous variation of all observables, in particular a smooth reduction of the quasiparticle weight as it goes to zero beyond the transition point. Our observation is in good agreement with a theoretical model where polaron and molecule quasiparticle states are thermally occupied according to their quantum statistics. At the experimental conditions, polaron states are hence populated even at interactions where the molecule is the ground state and vice versa. The emerging physical picture is thus that of a smooth transition between polarons and molecules and a coexistence of both in the region around the expected transition.

Highlights

  • In order to understand the motion of an electron through an ionic lattice, Landau suggested treating the electron and the phonons that accompany its movement as a new quasiparticle named “polaron” [1]

  • Understanding the properties of polarons coupled to a bosonic bath is still an ongoing effort in areas ranging from solid-state physics [7,8] and ultracold atoms [9,10,11] to quantum chemistry [12]

  • IV we develop a fitting routine for the experimental spectra which allows us to extract physical quantities, such as the polaron energy, the quasiparticle spectral weight, and the contact parameter

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Summary

Introduction

In order to understand the motion of an electron through an ionic lattice, Landau suggested treating the electron and the phonons that accompany its movement as a new quasiparticle named “polaron” [1]. The concept of the polaron was later found to be applicable in many other systems, including semiconductors [2], high-temperature superconductors [3], alkali halide insulators [4], and transition metal oxides [5] We find that up to a rescaling by a factor, the shapes of the background spectra from polarons and molecules are similar Based on this identification, we are able to develop a fit model for the transition probability that is largely model independent and reflects the line shape of the coherent and background signals: PðωÞ 1⁄4 Z Pcohðω; Tp; ε0pol; mÃÞ þ ð1 − Z ÞPbgðω; Tbg; EbÞ: ð6Þ. The probability FðkrelÞ that a pair will be dissociated with a relative momentum krel is determined by its relative envelope wave function, resulting in [67]

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