Abstract

We investigate the dynamics of a three-dimensional Bose-Einstein condensate of ultracold atomic gases with a soft-core shape long-range interaction, which is induced by laser dressing the atoms to a highly excited Rydberg state. For a homogeneous condensate, the long-range interaction drastically alters the dispersion relation of the excitation, supporting both roton and maxon modes. Rotons are typically responsible for the creation of supersolids, while maxons are normally dynamically unstable in BECs with dipolar interactions. We show that maxon modes in the Rydberg-dressed condensate, on the contrary, are dynamically stable. We find that the maxon modes can be excited through an interaction quench, i.e. turning on the soft-core interaction instantaneously. The emergence of the maxon modes is accompanied by oscillations at high frequencies in the quantum depletion, while rotons lead to much slower oscillations. The dynamically stable excitation of the roton and maxon modes leads to persistent oscillations in the quantum depletion. Through a self-consistent Bogoliubov approach, we identify the dependence of the maxon mode on the soft-core interaction. Our study shows that maxon and roton modes can be excited dynamically and simultaneously by quenching Rydberg-dressed long-range interactions. This is relevant to current studies in creating and probing exotic states of matter with ultracold atomic gases.

Highlights

  • Collective excitations induced by particle-particle interactions play an important role in the understanding of static and dynamical properties of many-body systems

  • Through a self-consistent Bogoliubov calculation, we show that the roton and maxon modes lead to non-equilibrium dynamics, where the quantum depletion exhibits slow and fast oscillations

  • Through analyzing the Bogoliubov spectra, we identify that the slow oscillations correspond to the excitation of the roton modes, while the fast oscillations come from the excitation of the maxon modes

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Summary

INTRODUCTION

Collective excitations induced by particle-particle interactions play an important role in the understanding of static and dynamical properties of many-body systems. The laser coupling generates a long-range, soft-core type interaction between Rydberg-dressed atoms [31,32,33,34,35,36,37,38,39,40,41]. We study excitations of roton and maxon modes in three dimensional (3D) Rydberg-dressed BECs in free space at zero temperature. When the soft-core interaction is strong, both the roton and maxon modes are found in the dispersion relation of the collective excitations. Starting from a weakly interacting BEC, roton and maxon modes are dynamically excited by instantaneously switching on the Rydberg-dressed interaction.

Hamiltonian of the Rydberg-dressed BEC
Time-independent Bogoliubov approach
Self-consistent Bogoliubov approach for the quench dynamics
Stationary dispersion relation
Roton and maxon excitation
Quantum depletion in the long time limit
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