A. Schmitt
;
P. Vallet
;
D. Mele
;
M. Rosticher
;
T. Taniguchi
(National Institute for Materials Science
)
;
K. Watanabe
(National Institute for Materials Science
)
;
E. Bocquillon
;
G. Fève
;
J. M. Berroir
;
C. Voisin
;
J. Cayssol
;
M. O. Goerbig
;
J. Troost
;
E. Baudin
;
B. Plaçais
Description:
(abstract)Strong electric field annihilation by particle-antiparticle pair creation, described in detail by Sauter and Schwinger, is a basic non-perturbative prediction of quantum electrodynamics. Its experimental demonstration remains elusive as Schwinger fields ES are beyond reach even for the light electron-positron pairs. Here we put forward a mesoscopic variant of the Schwinger effect in graphene, which hosts Dirac fermions with electron-hole symmetry. Using DC transport and RF noise, we report on univer- sal 1d-Schwinger conductance at the pinch-off of ballistic graphene transistors. Strong pinch-off electric fields are concentrated in a length Λ >∼ 0.1 μm at the transistor drain, and induce Schwinger e-h pair creation at saturation, for a Schwinger voltage VS = ES Λ on the order of the pinch-off voltage. This Klein-Schwinger effect (KSE) precedes an instability toward an ohmic Zener regime, which is rejected at twice the pinch-off voltage in long devices. The KSE not only gives clues to current saturation limits in ballistic graphene, but also opens new routes for quantum electrodynamic experiments in the laboratory.
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Keyword: Schwinger effect, graphene, Dirac fermions
Date published: 2023-03-09
Publisher: Springer Science and Business Media LLC
Journal:
Funding:
Manuscript type: Publisher's version (Version of record)
MDR DOI:
First published URL: https://doi.org/10.1038/s41567-023-01978-9
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Updated at: 2025-02-23 22:48:23 +0900
Published on MDR: 2025-02-23 22:48:23 +0900
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