For an MIM device in equilibrium, any carriers excited by ZPFs and injected into the insulator from the upper electrode would be balanced by ZPF-excited hot carriers from the base electrode. We hypothesize that
the presence of the Casimir cavity breaks this balance, resulting in a change in the net injection rate and hence increased G. This imbalance is discussed in greater detail after the presentation of the results. Because cavities
suppress zero-point electromagnetic modes having wavelengths greater than twice the cavity thickness, reducing the cavity thickness increases the range of suppressed wavelengths. We would therefore expect an increase in G for decreasing cavity thickness, a trend that can be seen in Fig.
3(b).
Examining the results of Fig.
3(b) further,
we would expect wavelengths in the visible range to dominate the response because, for near-UV wavelengths <250nm, the PMMA becomes highly absorptive
[40], and the infrared response is limited because the available vacuum energy density falls off with the cube of the wavelength. Although the vacuum energy density in ideal Casimir cavities varies inversely with the thickness cubed
[7], we would not expect the conductance to exhibit such a cubic dependence because there are multiple energy-dependent mechanisms in play, including (i) variations of photoinjection yield with photon energy, as described by extensions of Fowler's theory of photoemission
[41]; (ii) the interband transition threshold of Pd
[42], which limits the transport of high-energy carriers; (iii) the energy-dependent reflectivity of the mirrors and absorptivity of the transparent dielectric; and (iv) the energy dependence of hot carrier scattering
[43].