Understanding the low dielectric constant of nanoconfined water capacitors
ORAL
Abstract
The relative out of plane dielectric constant of nano confined water in graphene capacitors
was shown to be as low as 2.1 for capacitor thickness below 1 nm by Fumagalli et al. (Science 360, 2018). This
study motivated a plethora of theoretical studies aiming to explain this surprising behavior. It is surprising because such low
measured value is even lower than the high frequency dielectric constant of ice.
In this work we show that both experimental and theoretical studies suffer from intrinsic arbitrariness
associated to the ill defined concept of a macroscopic dielectric constant in a microscopic 2D limit.
We show that the two-dimensional transverse polarizability is the natural choice to characterize the
response of a nanoconfined dielectric in a capacitor. This polarizability can also be connected to
the actual experimental measurements of differential capacitance, providing a clean way of comparing
both experimental and theoretical results, eliminating the need for intermediate arbitrary choices needed
for the computation of the dielectric constant.
was shown to be as low as 2.1 for capacitor thickness below 1 nm by Fumagalli et al. (Science 360, 2018). This
study motivated a plethora of theoretical studies aiming to explain this surprising behavior. It is surprising because such low
measured value is even lower than the high frequency dielectric constant of ice.
In this work we show that both experimental and theoretical studies suffer from intrinsic arbitrariness
associated to the ill defined concept of a macroscopic dielectric constant in a microscopic 2D limit.
We show that the two-dimensional transverse polarizability is the natural choice to characterize the
response of a nanoconfined dielectric in a capacitor. This polarizability can also be connected to
the actual experimental measurements of differential capacitance, providing a clean way of comparing
both experimental and theoretical results, eliminating the need for intermediate arbitrary choices needed
for the computation of the dielectric constant.
* MFS aknowledges funding from the U.S. Department of Energy, Office of Science, Basic Energy Sciences, under Award No. DE-SC0019394, as part of the CCS Program
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Presenters
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Emilio Artacho
Nanogune, Ikerbasque and Univ of Cambridge
Authors
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Marivi Fernandez-Serra
Stony Brook University
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Emilio Artacho
Nanogune, Ikerbasque and Univ of Cambridge
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Matthew Dawber
State Univ of NY - Stony Brook
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Jon Zubeltzu
University of el Pais Vasco