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Profiling Atmospheric Turbulence with Single Star
Profiling Atmospheric Turbulence with Single Star

pdf
pdf

Optical path function.
Optical path function.

Introduction to optical fibers
Introduction to optical fibers

... The single mode fibers do not exhibit intermodal dispersion (which will be discussed in Chapter 3), thus the light pulse reaches the end of the fiber only slightly distorted. Therefore, the single mode fiber is suitable for long-distance transmission since the light pulse can be transmitted without ...
Label-free super-resolution imaging of adenoviruses by submerged
Label-free super-resolution imaging of adenoviruses by submerged

Interference and Interferometry [Pedrotti^3 Ch. 7 & Ch. 8]
Interference and Interferometry [Pedrotti^3 Ch. 7 & Ch. 8]

... As shown on previous pages, most available light sources emit a range wavelengths. For many photonic applications it is desirable to have a "monochromatic" (ideal) point light source. An ideal light source would emit only one exact frequency f0 and its physical size would be infinitely small (an ide ...
OPTICAL TWEEZERS: Characterization and Systems
OPTICAL TWEEZERS: Characterization and Systems

... mathematics. This work investigates a modern tool of micro-manipulation of microscopic particles that is used primarily by bio-physicists and bio-chemists for single cell, single molecule studies. This tool called the Optical Tweezers can trap microscopic dielectric particles using radiation pressur ...
Modeling of Lithium Niobate Ridge Waveguides - Rays
Modeling of Lithium Niobate Ridge Waveguides - Rays

... Waveguides are used in order to guide electromagnetic waves and an example of a waveguide is optical fibers. Problems arise with waveguides when propagation losses are induced, and the aim of this study is to model optical guidance, field profiles and effective indices in ridge type waveguides and p ...
Theory and Practice of Scanning Optical Microscopy - X
Theory and Practice of Scanning Optical Microscopy - X

Physics and Computation of Aero-Optics
Physics and Computation of Aero-Optics

Evanescent Waves in the Near- and the Far Field
Evanescent Waves in the Near- and the Far Field

... The advantage of the fact that each partial wave in the angular spectrum is a solution of the free-space Maxwell equations can not be overemphasized. For instance, when the source is located near an interface, each partial wave reflects and refracts in the usual way, and this can be accounted for b ...
ComplexLightBookChapterEG
ComplexLightBookChapterEG

The Optical Resonator
The Optical Resonator

... § All the modes would have comparable Q in the 3D resonator – To be avoided in a laser as it would cause all the atoms to emit power into a large number of modes (would differ in their frequency and spatial characteristics) § Large, open resonators consisting of opposite flat/curved reflectors mus ...
Scattering of a Plane Electromagnetic Wave by a Small Conducting
Scattering of a Plane Electromagnetic Wave by a Small Conducting

... is the Poynting vector (in Gaussian units) and c is the speed of light in vacuum. Because the incident wavelength is large compared to the radius of the cylinder, and the wave is normally incident, the incident fields are essentially uniform over the cylinder, and we might suppose the induced fields n ...
Optical Waveguide Modes
Optical Waveguide Modes

... A system like that shown in Fig. 2.3 is particularly useful for analysis of mode shapes in semiconductor waveguides, which generally support only one or two modes because of the relatively small Δn at the waveguide-substrate interface. Generally, the position of the focused input laser beam can be m ...
What Brown saw, and you can too
What Brown saw, and you can too

Creation of gap solitons in Bose
Creation of gap solitons in Bose

... in the gaps associated with avoided crossings. Gap solitons have previously been studied in a variety of physical contexts, but particularly in nonlinear optics [12]. They were also studied in the framework of nonlinear atom optics [7], but in this case the two states involved are connected by an op ...
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Lecture Notes 07: EM Waves, Wave Propagation in Conducting Media
Lecture Notes 07: EM Waves, Wave Propagation in Conducting Media

1.5% root-mean-square flat-intensity laser beam
1.5% root-mean-square flat-intensity laser beam

... the lowest potential region. Finally, in our application, we can sacrifice some degree of conversion efficiency from the input Gaussian profile beam to the desired profile in order to achieve a high degree of beam shape control and a minimum root-meansquare (RMS) deviation from the targeted beam sha ...
Spatiotemporal pattern formation in
Spatiotemporal pattern formation in

... 21. As long as u E 0 u is smaller than a critical value, there is a region of stability for any transverse mode. At a critical value E 0 c ' 21.7E d a finite band of transverse modes around a critical mode fK c 2 ' 3.6w 0 22 is predicted to become unstable through a Hopf bifurcation with a character ...
Measuring the Modulation Transfer Function of
Measuring the Modulation Transfer Function of

... generate than sinewave targets, while the ratio of the modulation of the scanned image to the modulation of the original image is defined as contrast transfer function (CTF). It is different from the MTF. There are formulas to transfer between the MTF and the CTF.4 In addition, we also can use the F ...
P510/2 - Sharebility
P510/2 - Sharebility

Basic Interferometry and Optical Testing Two
Basic Interferometry and Optical Testing Two

Diffraction - ICT for IST
Diffraction - ICT for IST

... Dimension of slits/obstacles and wavelength It also seems very effective to systematically present diffraction phenomena using both obstacles and openings (slits) and to emphasize the important relation between the size (dimension „u‟) of obstacles (or slits) and the wavelength (lambda). Again the s ...
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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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