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Axial intensity of apertured Bessel beams
Axial intensity of apertured Bessel beams

... have attracted the attention of many scientists, who have proposed a great number of applications.8–12 Since finite-aperture optical elements are always present in any practical realization,13–18 a more realistic model for a Bessel beam has to include the presence, at a certain plane (z 5 0), of a w ...
Ray Optics - Sakshi Education
Ray Optics - Sakshi Education

... used as a rear-view mirror. 36. Concave mirror is an ideal one for shaving purposes. Ophthalmoscope consists of a concave mirror. It is also used by dentists. REFRACTION : 1. When a light ray travels from one medium to another, it suffers a change of direction at the surface of separation of the two ...
3D locations of the object directly from in
3D locations of the object directly from in

Surface Water Waves
Surface Water Waves

... from chromatic aberrations. Using metamaterials they would enable light of visible wavelengths to be deflected around an object and continue its path on the far side as though the object were not there. This phenomenon has been achieved at microwave frequencies[1][2] however, achieving this effect a ...
Waveguide electro-optic modulation in micro-engineered
Waveguide electro-optic modulation in micro-engineered

Effect of spatial distribution of partial information on the accurate
Effect of spatial distribution of partial information on the accurate

Electrical Excitation of Surface Plasmons
Electrical Excitation of Surface Plasmons

Radiative Transfer Theory - UCL Department of Geography
Radiative Transfer Theory - UCL Department of Geography

... propagation direction, or energy that is scattered from other directions) and energy losses from the volume (either scattering out of the propagation direction, or absorption losses). Whilst optical modelling generally exploits a scalar radiative transfer equation, in microwave scattering, we deal u ...
Coupled-mode theory for electromagnetic pulse propagation in
Coupled-mode theory for electromagnetic pulse propagation in

... be the z direction, but they can have any sort of nonuniformity in the transverse direction r⊥ , i.e., the dispersive permittivity of the structure (defined in the frequency domain) is given by  = (r⊥ ,ω). This is the natural waveguide geometry, which obviously includes also uniform media. Howev ...
Student Text, pp. 444-452
Student Text, pp. 444-452

... source is straight. We confine ourselves for the moment to waves from sources with a constant frequency. As a wave moves away from its constant-frequency source, the spacing between successive crests or successive troughs—the wavelength—remains the same provided the speed of the wave does not change ...
Lecture 3 -- Electromagnetic Principles
Lecture 3 -- Electromagnetic Principles

Wormald Coupland On measuring 3D flow within inkjet droplet
Wormald Coupland On measuring 3D flow within inkjet droplet

... instrument was focused approximately at the position of the nozzle axis. Figure 7. shows the reconstructed hologram of a droplet close to the nozzle exit approximately 1ms after the solenoid valve opened. At this stage the droplet is in the form of an extruded filament of fluid. Out-of-focus and ab ...
Optical Solitons with Fourth Order Dispersion and Dual
Optical Solitons with Fourth Order Dispersion and Dual

... materials such as LiNbO3 . The propagation of ultrashort optical pulses in a nonlinear media can be charaterized by the nonliner refractive index that is given by [2, 6, 7] n = n0 + n2 |E|2m + n4 |E|4m ...
ROGUE WAVES - University of Surrey
ROGUE WAVES - University of Surrey

Generation of diffractive optical elements onto a photopolymer using a
Generation of diffractive optical elements onto a photopolymer using a

Coherence - Studentportalen
Coherence - Studentportalen

... The angle is thus much smaller, and naturally the angle should be much smaller than the one corresponding to the first diffraction minimum. The transverse coherence width at a distance z from the aperture is then lt  ...
Mathematical models and numerical methods for high frequency
Mathematical models and numerical methods for high frequency

... With consistent initial and boundary data, φ(t, x) = φ̃(x) − t. We note that, since the family of curves {x | φ(t, x) = φ̃(x) − t = 0}, parametrized by t ≥ 0, describe a propagating wave front in (11), we often directly interpret the frequency domain phase φ̃(x) as the travel time of a wave. The dif ...
Page 251 - eCM Journal
Page 251 - eCM Journal

... astigmatism and other axial aberrations grow also in importance. To reduce the effect of aberrations, methods for coma-free alignment of electron microscopes and accurate determination of aberration coefficients are, therefore, required. A method for coma-free alignment was originally proposed in an ...
Document
Document

Ultra–large field-of-view two-photon microscopy
Ultra–large field-of-view two-photon microscopy

... The design of the scan system begins with the selection of the objective. We seek a field-ofview that encompasses 10 mm, a numerical aperture (NA) to achieve 1-µm resolution, and a back aperture that does not exceed 25 mm. The singular choice is a 4-times magnification (f = 45 mm), 0.28 NA air-immer ...
A nanometer notch filter with high rejection and throughput
A nanometer notch filter with high rejection and throughput

Multimode Interferometer for Guided Matter Waves
Multimode Interferometer for Guided Matter Waves

... even below the Fermi temperature. The multimode interferometer is built by combining two Y-shaped beam splitters [4], capable of coherently splitting or recombining many incoming transverse modes, and arranging the interferometer geometry so that all the different transverse states give the same pha ...
One-parameter two-term HenyeyŒGreenstein phase function for
One-parameter two-term HenyeyŒGreenstein phase function for

... To compare results of modeling with the seawater TTHG phase function with the experimental data, a set of random pairs of backscattering probability and single-scattering albedos 共B, ␻0兲 was generated. These pairs, being homogeneously distributed in the rectangle 共0 ⱕ B ⱕ 0.5, 0 ⱕ ␻0 ⱕ 1兲, simulate ...
The effects of longitudinal chromatic aberration and a shift in the
The effects of longitudinal chromatic aberration and a shift in the

... retinal image with defocus from LCA, and calculation of M-cone contrast of the defocused retinal image when the peak sensitivity of the M-cone fundamental is varied. Because M-cone contrast varies with the plane of focus we calculated M-cone contrast when the eye is focused to maximize luminance con ...
3-D Ultrahigh Resolution Optical Coherence Tomography with
3-D Ultrahigh Resolution Optical Coherence Tomography with

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Fourier optics

Fourier optics is the study of classical optics using Fourier transforms, in which the wave is regarded as a superposition of plane waves that are not related to any identifiable sources; instead they are the natural modes of the propagation medium itself. Fourier optics can be seen as the dual of the Huygens–Fresnel principle, in which the wave is regarded as a superposition of expanding spherical waves which radiate outward from actual (physically identifiable) current sources via a Green's function relationship (see Double-slit experiment)A curved phasefront may be synthesized from an infinite number of these ""natural modes"" i.e., from plane wave phasefronts oriented in different directions in space. Far from its sources, an expanding spherical wave is locally tangent to a planar phase front (a single plane wave out of the infinite spectrum), which is transverse to the radial direction of propagation. In this case, a Fraunhofer diffraction pattern is created, which emanates from a single spherical wave phase center. In the near field, no single well-defined spherical wave phase center exists, so the wavefront isn't locally tangent to a spherical ball. In this case, a Fresnel diffraction pattern would be created, which emanates from an extended source, consisting of a distribution of (physically identifiable) spherical wave sources in space. In the near field, a full spectrum of plane waves is necessary to represent the Fresnel near-field wave, even locally. A ""wide"" wave moving forward (like an expanding ocean wave coming toward the shore) can be regarded as an infinite number of ""plane wave modes"", all of which could (when they collide with something in the way) scatter independently of one other. These mathematical simplifications and calculations are the realm of Fourier analysis and synthesis – together, they can describe what happens when light passes through various slits, lenses or mirrors curved one way or the other, or is fully or partially reflected. Fourier optics forms much of the theory behind image processing techniques, as well as finding applications where information needs to be extracted from optical sources such as in quantum optics. To put it in a slightly more complex way, similar to the concept of frequency and time used in traditional Fourier transform theory, Fourier optics makes use of the spatial frequency domain (kx, ky) as the conjugate of the spatial (x,y) domain. Terms and concepts such as transform theory, spectrum, bandwidth, window functions and sampling from one-dimensional signal processing are commonly used.
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