Monolayer">
Di Huang
;
Kevin Sampson
;
Yue Ni
;
Zhida Liu
;
Danfu Liang
;
Kenji Watanabe
(National Institute for Materials Science
)
;
Takashi Taniguchi
(National Institute for Materials Science
)
;
Hebin Li
;
Eric Martin
;
Jesper Levinsen
;
Meera M. Parish
;
Emanuel Tutuc
;
Dmitry K. Efimkin
;
Xiaoqin Li
Description:
(abstract)When mobile impurities are introduced and coupled to a Fermi gas, new quasiparticles known as Fermi polarons are formed. There are two interesting, yet drastically different regimes of the Fermi polaron problem: (I) the attractive polaron branch, which connects to pairing phenomena spanning the crossover from BCS superfluidity to the Bose-Einstein condensation of molecules; and (II) the repulsive branch, which underlies the physics responsible for Stoner’s itinerant ferromagnetism. Here, we study Fermi polarons in two dimensional systems where many questions and debates regarding their nature persist. The model system we investigate is a doped MoSe2 monolayer. Remarkably, not only the energy splitting but also the quantum dynamics of attractive polarons agree with the predictions of polaron theory well. As the doping density increases, the quantum dephasing of the attractive polarons remains constant, indicative of stable quasiparticles, while the repulsive polaron dephasing rate increases nearly quadratically, as a consequence of the interplay between the electron Fermi seas in two valleys. The dynamics of Fermi polarons are of critical importance for understanding the pairing and magnetic instabilities that lead to the formation of rich quan- tum phases found in a wide range of physical systems including nuclei, cold atomic gases, and solids.
Rights:
Keyword: Fermi polarons, MoSe2 monolayer, quantum dynamics
Date published: 2023-03-02
Publisher: American Physical Society (APS)
Journal:
Funding:
Manuscript type: Publisher's version (Version of record)
MDR DOI:
First published URL: https://doi.org/10.1103/physrevx.13.011029
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Updated at: 2025-02-23 22:47:02 +0900
Published on MDR: 2025-02-23 22:47:02 +0900
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