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Interference I - Galileo and Einstein
Interference I - Galileo and Einstein

TEP 2.6.11-00 Fourier optics – 2f Arrangement TEP 2.6.11
TEP 2.6.11-00 Fourier optics – 2f Arrangement TEP 2.6.11

... assumption that a spherical wave emanates from each point (x,y,0) behind the diffracting structure (Huygens’ principle). This leads to Kirchhoff’s diffraction integral: ...
depending on the wave - Rowan County Schools
depending on the wave - Rowan County Schools

... Period (T): how long it takes for a single wave to pass a single point. seconds Frequency (f): number of waves that pass a given point in a time period of one second. Hertz (Hz) = 1/s Q. What is the period of a 60 Hz wave traveling at 3.0 x 108 m/s? ...
Lab 2: Abbe Theory of Imaging
Lab 2: Abbe Theory of Imaging

Interference
Interference

... • Use the following applet to help explore the different interference patterns produced by single, double and multiple slits... ...
PPT - Tensors for Tots
PPT - Tensors for Tots

... the points on a wave front. ...
Click To
Click To

Document
Document

... Fourier transform of the transparency times a spherical wavefront • The lens produces at its focal plane the Fraunhofer diffraction pattern of the transparency • When the transparency is placed exactly one focal distance behind the lens (i.e., z=f ), the Fourier transform relationship is exact. ...
Scalar Diffraction Theory and Basic Fourier Optics  [Hecht  10.2.4­10.2.6, 10.2.8, 11.2­11.3 or Fowles Ch. 5]
Scalar Diffraction Theory and Basic Fourier Optics  [Hecht  10.2.4­10.2.6, 10.2.8, 11.2­11.3 or Fowles Ch. 5]

Monochromatic plane waves ( ) Plane waves have straight wave fronts
Monochromatic plane waves ( ) Plane waves have straight wave fronts

... A homogeneous surface perpendicular to say the z direction can not change the transverse momentum. Since the propagation vector is proportional to the photon's momentum, the transverse propagation direction (kx,ky,0) must remain the same in both regions. Assuming without loss of generality a plane o ...
Fourier Spectra for Non-Homogeneous Patterns
Fourier Spectra for Non-Homogeneous Patterns

... using bands much smaller than t:.k (lop I) for any particular band centered on k. If there is reason to believe that the spectrum is relatively smooth, then one might be able to use bands much wider than this. In general, it turns out to be impossible to construct a mosaic from hands of constant t:. ...
Optics - Tensors for Tots
Optics - Tensors for Tots

... the points on a wave front. ...
$doc.title

5. GAUSSIAN BEAMS 5.1. Solution to the wave equation in
5. GAUSSIAN BEAMS 5.1. Solution to the wave equation in

Week4-figs
Week4-figs

10NonlinearOptics.pdf
10NonlinearOptics.pdf

... If the medium has an inversion symmetry, the second order nonlinearity, characterized by d, is zero. Why? Physical pictures: When the potential as a function of displacement deviates from a perfect parabola, the electrons driven by an electric field may create a polarization. For example: a DC polar ...
Gothic Cathedrals and Solar Cells (and maybe a Grail?)
Gothic Cathedrals and Solar Cells (and maybe a Grail?)

Surface waves
Surface waves

... Surface waves A semi-infinite, homogeneous medium fills the x > 0 region. The optical properties of the medium are described by a dielectric function ε = ε(ω) having real values in the frequency range of interest. A monochromatic EM wave propagates along the y-direction, parallel to the surface of t ...
Part 1
Part 1

Optical Diffraction and Image Formation
Optical Diffraction and Image Formation

... diffraction pattern from that slide, which corresponds to the intensities (= Amplitudes2) of the Fourier transformation of the slide image. If the slide, for example, shows some lines, then the distant wall will show the diffraction peaks from those lines. The Fraunhofer theory explains how that sha ...
PH4035 - Principles of Optics
PH4035 - Principles of Optics

doc - University of Rochester
doc - University of Rochester

... Ghost imaging with entangled photon pairs (biphotons) has been extensively discussed in the literature [1,2]. Recently, the question of whether the resolution of ghost imaging is improved using non-degenerate biphotons (biphotons with pairs of photons of different frequency) has been raised. In this ...
LOYOLA COLLEGE (AUTONOMOUS), CHENNAI – 600 034
LOYOLA COLLEGE (AUTONOMOUS), CHENNAI – 600 034

... (a) Explain the action of a half wave plate when a plane polarized light is incident normally on it. (b) Calculate the thickness of a half wave plate for light of wavelength 6000Å. Given µe= 1.553 and µ0=1.533.(2.5). ...
Wave equation
Wave equation

... This is the differential equation that describes the propagation of dissipationless, dispersionless waves. This derivation will be inductive and general. For each specific case like tension waves on a string or sound waves in the air, it is also possible to give a detailed deductive derivation that ...
Test Review 3
Test Review 3

< 1 ... 42 43 44 45 46 >

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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