Charge Friedel oscillations in a Mott insulator

When a metal undergoes a transition to an insulator it will lose its electronic Fermi surface. Interestingly, in some situations a “ghost” Fermi surface of electrically neutral spin carrying fermions may survive into the insulator. Such a novel ghost Fermi surface has been proposed to underlie the p...

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Main Authors: Mross, David Fabian, Todadri, Senthil
Other Authors: Massachusetts Institute of Technology. Department of Physics
Format: Article
Language:en_US
Published: American Physical Society 2011
Online Access:http://hdl.handle.net/1721.1/67061
https://orcid.org/0000-0003-4203-4148
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author Mross, David Fabian
Todadri, Senthil
author2 Massachusetts Institute of Technology. Department of Physics
author_facet Massachusetts Institute of Technology. Department of Physics
Mross, David Fabian
Todadri, Senthil
author_sort Mross, David Fabian
collection MIT
description When a metal undergoes a transition to an insulator it will lose its electronic Fermi surface. Interestingly, in some situations a “ghost” Fermi surface of electrically neutral spin carrying fermions may survive into the insulator. Such a novel ghost Fermi surface has been proposed to underlie the properties of a few different materials but its direct detection has proven elusive. In this paper, we show that the ghost Fermi surface leads to slowly decaying spatial oscillations of the electron density near impurities or other defects. These and related oscillations stem from the sharpness of the ghost Fermi surface and are direct analogs of the familiar Friedel oscillations in metals. The oscillation period contains geometric information about the shape of the ghost Fermi surface, which can be potentially exploited to detect its existence.
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spelling mit-1721.1/670612022-10-01T14:27:02Z Charge Friedel oscillations in a Mott insulator Mross, David Fabian Todadri, Senthil Massachusetts Institute of Technology. Department of Physics Senthil, Todadri Mross, David Fabian Todadri, Senthil When a metal undergoes a transition to an insulator it will lose its electronic Fermi surface. Interestingly, in some situations a “ghost” Fermi surface of electrically neutral spin carrying fermions may survive into the insulator. Such a novel ghost Fermi surface has been proposed to underlie the properties of a few different materials but its direct detection has proven elusive. In this paper, we show that the ghost Fermi surface leads to slowly decaying spatial oscillations of the electron density near impurities or other defects. These and related oscillations stem from the sharpness of the ghost Fermi surface and are direct analogs of the familiar Friedel oscillations in metals. The oscillation period contains geometric information about the shape of the ghost Fermi surface, which can be potentially exploited to detect its existence. National Science Foundation (U.S.) (Grant DMR-0705255) 2011-11-18T18:58:36Z 2011-11-18T18:58:36Z 2011-07 2011-06 Article http://purl.org/eprint/type/JournalArticle 1098-0121 1550-235X http://hdl.handle.net/1721.1/67061 Mross, David, and T. Senthil. “Charge Friedel oscillations in a Mott insulator.” Physical Review B 84 (2011): n. pag. Web. 18 Nov. 2011. © 2011 American Physical Society https://orcid.org/0000-0003-4203-4148 en_US http://dx.doi.org/10.1103/PhysRevB.84.041102 Physical Review B Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. application/pdf American Physical Society APS
spellingShingle Mross, David Fabian
Todadri, Senthil
Charge Friedel oscillations in a Mott insulator
title Charge Friedel oscillations in a Mott insulator
title_full Charge Friedel oscillations in a Mott insulator
title_fullStr Charge Friedel oscillations in a Mott insulator
title_full_unstemmed Charge Friedel oscillations in a Mott insulator
title_short Charge Friedel oscillations in a Mott insulator
title_sort charge friedel oscillations in a mott insulator
url http://hdl.handle.net/1721.1/67061
https://orcid.org/0000-0003-4203-4148
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