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.
The derivative of the field at thez=d interface can be written as the sum of the three spatial sectors, e′(d−) =e ′(d−) z0<0 +e ′(d−) 0<z0<d +e ′(d−) z0>d
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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.