Axion dark matter induces a resonantly enhanced pressure between graphene plates whose peaks and widths are controlled by graphene conductivity, chemical potential and dissipation, yielding projected sensitivities competitive in optimistic regimes.
In particular, the graphene conductivity de- pends not only on the chemical potential, but also on the probing frequency, or equivalently the axion mass
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Axion-Induced Casimir Interaction Between Graphene Plates
Axion dark matter induces a resonantly enhanced pressure between graphene plates whose peaks and widths are controlled by graphene conductivity, chemical potential and dissipation, yielding projected sensitivities competitive in optimistic regimes.