Fig. 1
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(a) Angle of incidence at which the transmittance of each CSP is maximum as a function of cavity thickness. (b) Maximum transmittance at each CSP resonance peak as a function of cavity thickness, FTIR transmission at θco without Ag for comparison. (c) Modulus and (d) phase of rLMH (lighter) and rLM (darker) as functions of the incident angle. All results correspond to a setup using silver as metal (dM = 39 nm), BK7 as prism and air filling the gap between the mirrors, at λ = 800 nm.
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