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The phase speed of the SPP wave varies mainly as a function of the tilt of the CTF columns.
The plot of the position of the central wavelength as a function of the tilt angle is shown in Figure 3. Figure 3 Comparison of simulated shift of the central wavelength for low-doped and high-doped silicon photonic crystals.
The measured shift of the central wavelength as a function of the tilt angle is shown in Figure 5.Measurements for demonstration of the dual tunability induced by tilting and pore-filling were performed using a rugate photonic crystal having 32 periods and a central wavelength at 700 nm.
At the localisation plane on the retina, the interference pattern produced by the virtual point sources S′1 and S′2 due to the actual point source S of the extended source Σ is only a function of the tilt α.
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The visibility for each data point was measured in the same way as in Fig. 4. The decrease of the visibility is evaluated as a function of the tilts.
Fig. 8 Observed tilt angle of wavevector anisotropy as a function of the true tilt angle at different values of spectral slopes (top panel) (alpha = 1) (black), (alpha = 2) (gray), and (alpha = 3) (light gray).
The normalized values are shown in Fig. 4. Fig. 4 Substorm probability as a function of the total tilt.
The purpose of this paper is to statistically confirm the influence of tail current configuration on substorm onset by investigating the following phenomena: (1) substorm probability during periods with different dipole tilt angles and SW flow directions, (2) AL index dependence on the current sheet bending, and (3) the magnetotail lobe field magnitude as a function of the dipole tilt angle.
The output power of the photovoltaic system depends directly on the amount of tilted global irradiance absorbed by the surface which is a function of the incident tilted global irradiance, air mass and angle of incidence [20].
The results of these measurements are depicted in Fig. 5. Fig. 5 Visibility as a function of the relative tilted and thus in the reference plane shifted interfering TEM00-modes of the single signal photons in tangential and radial direction.
Figure 3a plots the ultimate efficiency η as a function of the nanowire array tilt angle β. η = 29.7% for the vertical nanowire array (β = 0°).
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