Illustration of diffraction12/12/2023 In the far-field regime, the diffraction orders appear as the impulses of the Fourier transform of the grating’s transmission function. In addition, the intensity pattern over a plane includes the propagation axis and the grating vector (say the longitudinal plane) that is called the Talbot carpet 2. In the near-field regime, superposition of diffraction orders form self-images and sub-images of the grating’s structure at certain propagation distances. For the conventional gratings, the intensities of diffraction orders decrease with increasing the number of order of diffraction. These diffracted beams are known as diffraction orders. In the diffraction of a plane wave from a linear grating, the beam is split and diffracted into several beams travelling in different directions. The presented theory is confirmed by respective experiments.Ī conventional optical diffraction grating, say linear grating, is a periodic structure in the Cartesian coordinates. In addition, a detailed analysis of the multiplication of the diffraction pattern of an AMLPG by the 2D structure of a spatial light modulator is presented. This feature nominates them for potential applications in light sheet microscopy. We show that AMLPG-based radial carpet beams can be engineered in which they acquire sheet-like spokes. ![]() The diffraction grating introduced with controlled intensity sharing among different diffraction orders might find wide applications in many areas of optics such as optical switches. The resulting patterns over different diffraction orders are specified and their differences are determined. In comparison with the diffraction of a plane wave from radial phase gratings, the use of AMLPGs provides high contrast diffraction patterns and presents varied radial carpet beams over the different diffraction orders of the host linear phase grating. ![]() The theory of the work and experimental results are presented. We show that for a given value of the phase amplitude over the host linear phase grating, one of the diffraction orders is predominant and by increasing the value of the phase amplitude, the intensity sharing changes in favor of the higher orders. A radial carpet beam is generated in the diffraction of a plane wave from a radial phase grating. ![]() In this work, in addition to introducing AMLPGs, we present the generation of varied radial carpet beams over different diffraction orders of an AMLPG with controlled intensity sharing among the generated beams. We construct these gratings by adding an azimuthal periodic dependency to the argument of the transmission function of a linear phase grating that has a sinusoidal profile and we call them azimuthally-modified linear phase gratings (AMLPGs). Here, we introduce a new type of grating where in the diffraction of a plane wave, the intensity of a given higher order diffracted beam can be higher than the intensity of the lower orders. In the diffraction of a plane wave from a conventional grating, the intensities of diffracted beams decrease with increasing order of diffraction. The directions of the diffraction orders depend on the grating period and the wavelength of the impinging light beam so that a grating can be used as a dispersive element. The diffracted beams from a grating are commonly called diffraction orders. A diffraction grating is a periodic structure that splits and diffracts the impinging light beam into several beams travelling in different directions. Diffraction gratings are important optical components and are used in many areas of optics such as in spectroscopy.
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