Figure 6
From: Real-time detection of influenza A virus using semiconductor nanophotonics

Conic measurement of BSA physisorption on the QW-SPR device. (a) The dispersion relation of the SPR is projected on a skewed set of axes I(E–ky,kx).15 The image reveals the projection of two ellipses, obtained from the projection of the SPR dispersion on the E–ky space. Measuring the distance in kx between the two ellipses provides direct information on the SPR conditions. In this case, the quality of the signal as a function of E–ky depends on the luminescence intensity of the QW. (b) ΔSPR as a function of E–ky and time, as the BSA solution is injected over the device and rinsed. The periodic modulations in E–ky are attributed to the interactions of the SPs with the grating as predicted in the literature.15,16 (c) Cumulative SPR shift in time for the BSA physisorption, where the SNR, bulk shift (ΔB) and surficial shift (ΔS) are measured. BSA, bovine serum albumin; QW, quantum well; SNR, signal-to-noise ratio; SP, surface plasmon; SPR, surface plasmon resonance.