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. 2015 Dec 9;10(2):1756–1763. doi: 10.1021/acsnano.5b06631

Figure 6.

Figure 6

(a) Confocal real space imaging and BFP imaging setup. (b) Scheme illustrating the BFP radiation pattern created by a point-dipole emitter. p⃗, dipole moment; Φ, orientation angle of dipole axis in sample plane; θ, emission angle; θs, incident angle complementary to θ; ϕ, azimuthal angle in back aperture; r, radial distance from optical axis.19 (c) Calculated BFP patterns of an in-plane point dipole on an air–glass interface oriented with Φ = 0° recorded for parallel (Φ = 0°, α = 0° and Φ = 90°, α = 90°) and crossed polarization (Φ = 0°, α = 90° and Φ = 90°, α = 0°), with α the orientation of the analyzer transmission (detection polarization). The emission detected for cross-polarization is due to polarization mixing caused by the air–glass interface.