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for diffraction orders ±1 of the grating.
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c Schematic illustration of modes existing in 1D PhC terminated by a periodically profiled metal film in p-polarization for various diffraction orders: 0 (solid lines), " −1" (dotted lines) and " +1" (dashed lines).
RCWA is an exact solution of Maxwell's equations for the electromagnetic diffraction by grating structures which is generally applicable for 2D plane with 1D periodicity; however, RCWA may suffer numerical difficulties in presence of evanescent orders and it requires a large amount of calculation for retaining several diffraction orders.
Then, we observe the recording of a stationary phase grating with many diffraction orders for a probe beam.
On the contrary, the Littrow conical diffraction spectrometer proposed by [12] includes an additional prism for separating the overlapping diffraction orders of the echelle grating to produce two-dimensional high dispersion without requiring a large field of view.
Translated dispersions for " +1" and " −1" diffraction orders in the case of 1D periodic relief (along x-axis) are presented in Fig. 1 c by dashed and dotted lines, respectively.
Furthermore, the phases of those diffraction orders for this type of gratings are only two-valued in the far field, which leads to a great simplification of phase matching during the procedure of coherent beam combination.
Because sufficiently accurate FC phase angles can be extracted by CRISP as part of its electron crystallography [44] support functionality, reciprocal lattice vector magnitudes must be extracted with a precision of better than one half of a pixel (in reciprocal space) for even the highest diffraction orders [21].
Red lines correspond to the dispersion of SPP for " −1" diffraction order in the case of flat interface between gold and uniform dielectric with refractive index n 1.
Specific points were chosen to trace the changes in the spatial distribution of the electric field for all modes (except the topmost p-polarized mode) outside of their intersection and for "-1" diffraction order.
Such dispersions for " −1" diffraction order coincide with transmittance peculiarities in Fig. 2. In the case of N L -folds, Bragg mirror there N L modes in s-polarisation and (N L +1) modes in p-polarisation.
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