Strong Coulomb drag and broken symmetry in double-layer graphene

Gorbachev, R. V. and Geim, A. K. and Katsnelson, M. I. and Novoselov, K. S. and Tudorovskiy, T. and Grigorieva, I. V. and MacDonald, A. H. and Morozov, S. V. and Watanabe, K. and Taniguchi, T. and Ponomarenko, L. A. (2012) Strong Coulomb drag and broken symmetry in double-layer graphene. Nature physics, 8 (12). pp. 896-901. ISSN 1745-2473

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Abstract

Coulomb drag is a frictional coupling between electric currents flowing in spatially separated conducting layers. It is caused by interlayer electron–electron interactions. Previously, only the regime of weak (ddouble greater thanl) to intermediate (d~l) coupling could be studied experimentally, where dis the interlayer separation and l is the characteristic distance between charge carriers. Here we use graphene–boron-nitride heterostructures with d down to 1 nm to probe Coulomb drag in the limit dless doublel such that the two Dirac liquids effectively nest within the same plane, but can still be tuned and measured independently. The strongly interacting regime reveals many unexpected features. In particular, although drag vanishes because of electron–hole symmetry when either layer is neutral, we often find drag strongest when both layers are neutral. Under this circumstance, drag is positive in zero magnetic field but changes its sign and rapidly grows in strength with field. The drag remains strong at room temperature. The broken electron–hole symmetry is attributed to mutual polarization of closely spaced interacting layers.

Item Type:
Journal Article
Journal or Publication Title:
Nature physics
Uncontrolled Keywords:
/dk/atira/pure/subjectarea/asjc/3100
Subjects:
ID Code:
66715
Deposited By:
Deposited On:
23 Sep 2013 15:07
Refereed?:
Yes
Published?:
Published
Last Modified:
24 Jun 2020 02:17