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The Fractional Fourier Transform. with Applications in Optics and Signal
The Fractional Fourier Transform. with Applications in Optics and Signal

... covering both theory and applications. As a generalisation of the Fourier transform, the fractional Fourier transform is richer in theory and more flexible in applications but not more costly in implementation. This text consolidates knowledge on the transform and illustrates its application in dive ...
Is the Magnetosphere a Lens to MHD Waves?
Is the Magnetosphere a Lens to MHD Waves?

... the magnetotailand can have significantimplicationsfor the dynamics of substorms. The objectiveof this letter is to presentthe basicphysics underlyingthe idea of the magnetosphereas a lens by using a simplified analysisthat relies on conventionaltechniques of optics. More detailedanalysisand modelin ...
Wavefront shaping of infrared light through a subwavelength hole
Wavefront shaping of infrared light through a subwavelength hole

VII-3
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In Situ Imaging of Cold Atomic Gases
In Situ Imaging of Cold Atomic Gases

... In the limit of small phase shifts (ϕ), the phase modulated light leaving the atom cloud can be decomposed into the original plane wave and a small secondary plane wave that is π/2 out of phase. At the detector, we can write the complex electric field produced by the incoming plane wave as: ...
Engineering Optics and Optical Techniques
Engineering Optics and Optical Techniques

... SP-2: Collimated light containing the wavelengths 600 nm and 610 nm is diffracted by a plane grating ruled with 60 lines to the millimeter. If a lens of 2 m focal length is used to focus the light on a screen, what is the linear distance between these two lines in the first order? ...
Irradiance transport equation from geometrical - E
Irradiance transport equation from geometrical - E

... theorem together with the representation of the Poynting vector in the eikonal approximation. It is shown that the irradiance transport equation is a particular case of a more general conservation equation and is valid in the paraxial regime. An analysis of the range of validity of the irradiance tr ...
Mirrors and Lenses
Mirrors and Lenses

... First ray: parallel to optical axis and refracting through focal point.  Second ray: called the chief ray passes from the object through the center of the lens un-refracted.  Third ray: through the focal point and refracting parallel to optical ...
Optical forces on particles of arbitrary shape and size
Optical forces on particles of arbitrary shape and size

Properties of Waves
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... The distance between a sound and an object can be found by using the wave equation – but remember, it will be double the distance between the sound and the hard surface s = 2d/t Where s is the speed of sound in air (or whatever medium it is travelling through), d is distance and t is ...
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... e−(kx +ky )(w0 /4+iz/2k) ei(kx x+ky y) dkx dky 4π Here, we used the paraxial approximation: r kx2 + ky2 kx2 + ky2 kz = k 1 − ...
waveplates - CVI Laser Optics
waveplates - CVI Laser Optics

... For the full-, half-, and quarter-wave waveplate examples given in standard waveplates, the order of the waveplate is given by the integer m. For m > 0, the waveplate is termed a multiple-order waveplate. For m = 0, we have a zero order waveplate. The birefringence of crystal quartz near 500 nm is a ...
Properties of Multilayer Optics
Properties of Multilayer Optics

... As seen from the plots, phase retardation based on reflection can be quite effective, producing Δφ≈45 degrees. Because of the necessity of operating near 45 degrees for decent phase shifts, the reflectivity of the p-component is quite low (≤0.1), which is extended to ≤0.01(two reflections) if it is ...
Lesson 1 - primalight
Lesson 1 - primalight

Lecture 11
Lecture 11

... what this is saying is that, in some sense, wave phenomena are absent in the paraxial approximation. As we will see, this transformation rule applies in more general situations as long as the paraxial approximation holds. But let痴 focus on the Gaussian beam for concreteness. The Gaussian beam stays ...
Microscopy Basics
Microscopy Basics

... Bright field microscopy is based on absorption of light in the sample. Most biological objects, however, absorb only weakly in the visible spectrum. This lead to: • Development of specific staining (nowadays almost entirely replaced by fluorescent labeling) • Development of UV microscopy (Köhler) fa ...
Localized superluminal solutions to the wave equation in
Localized superluminal solutions to the wave equation in

... where Dx  Dxþ or Dx . Because of the nonsymmetric character of spectrum (5), let us call Dxþ ð> 0) the bandwidth to the right, and Dx (< 0) the bandwidth to the left of the spectrum central frequency xc ; so that Dx ¼ Dxþ  Dx . It should be noted, however, that, already for small values of m ( ...
Gaurav Chetna Josan - Department of Electrical Engineering
Gaurav Chetna Josan - Department of Electrical Engineering

... Linear optics- ‘Optics of weak light’: Light is deflected or delayed but its frequency is unchanged. ...
Li_Fang_Report
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PPT Lecture Notes

... • What are the evolutionary advantages of being sensitive to light, per se (versus some other part of the E.M. spectrum)? • Light is “bouncy”. Unlike longer-wave energy, which passes through many opaque objects, light can be reflected (‘bounced’) off of objects, making them visible. Light’s a better ...
5 Convolution of Two Functions - School of Physics and Astronomy
5 Convolution of Two Functions - School of Physics and Astronomy

... Of more importance, if we consider f (x) to be the “signal” and h(x) to be the “target” then we see that the correlation gives a peak where the “signal” matches the “target”. This gives the basis of the simples method of target detection2 . In the Fourier Domain the Correlation Theorem becomes C(u) ...
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244061

Image formation and optical transfer function in a course of
Image formation and optical transfer function in a course of

... values [different sizes of the effective light source]: Fig. 4a S=O.2, Fig. 4b S=O.5, Fig. 4c S=oo. Each figure shows the images of the five bars on different defocused planes: W200, W200. 17, W200.34, W200.51, and W200.68. A common behaviour shown in all the figures is that the contrast of the bars ...
Chapter 23: Electromagnetic waves What will we learn in this chapter?
Chapter 23: Electromagnetic waves What will we learn in this chapter?

Chapter 23: Electromagnetic waves What will we learn in this chapter?
Chapter 23: Electromagnetic waves What will we learn in this chapter?

... stretched strings. In an EM wave, the E and B field are sinusoidal in time. This is similar to the rudimentary wave in that the fields are uniform in the propagation front. We call such a wave a plane wave. EM waves can be described by wave functions: ...
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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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