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4.Classical entanglement
4.Classical entanglement

... When det M (t )  1, then this Gaussian could be the Wigner function of a pure squeezed state, so that the evolved Wigner function could be identified with a Husimi function. Then, the evolved Wigner function must be positive! The time for positivity is independent of the initial pure state. This ti ...
WAVE OPTICS
WAVE OPTICS

... Light propagates in the form of waves. In free space, light waves travel with a constant speed c, = 3.0 X lo8 m/s (30 cm/ns or 0.3 mm/ps). The range of optical wavelengths contains three bands- ultraviolet (10 to 390 nm), visible (390 to 760 nm), and infrared (760 nm to 1 mm). The corresponding ran ...
Chapter 33 . Aberration Curves in Lens Design
Chapter 33 . Aberration Curves in Lens Design

... the optical system. The most common form is the transverse ray aberration curve. It is also called lateral aberration, or ray intercept curve (also referred to by the misleading term ‘‘rim ray plots’’). These plots are generated by tracing fans of rays from a specific object point for finite object ...
The influence of coherent waves on the remotely sensed reflectance
The influence of coherent waves on the remotely sensed reflectance

The optical microscopy with virtual image breaks
The optical microscopy with virtual image breaks

... achieved a resolution of 130 nm (λ/3 far-field resolution) with <3x magnification12. Due to the SPP energy loss and sophisticated nanofabrication process, the resolutions of existing SPP-superlens and hyperlens are limited within λ/7 to λ/3. Moreover, both magnification and resolution of these lense ...
Chapter 4
Chapter 4

... From this derivation we learn that: - the conversion efficiency is proportional to the power density, so the total amount of generated light at the second harmonic is proportional to [P()] 2. Thus second harmonic generation is a process that is non-linear in the power dependence. - the efficiency i ...
CavityRingDown_Acous..
CavityRingDown_Acous..

... the aperture smaller so the beams don’t overlap, measure the rise time and peak diffraction efficiency (not diffracted power, but ratio of diffracted output to input) as a function focal spot size, varied inversely ¢ = ¸F=A by opening and closing the aperture A (or perhaps by z-shifting the AOD). No ...
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untitled - PhysRevLett.111.243901

... optimized spot had disappeared. The spatial line profile of the ensemble averaged intensity distribution at the target arrival time is plotted in Fig. 4(c). The peak intensity after the optimization is about 2 orders of magnitude higher than that before the optimization. Moreover, the observed inten ...
Principles of optics
Principles of optics

... 10.6 Some applications 10.6.1 The degree of coherence in the image of an extended incoherent quasi-monochromatic source 10.6.2 The in¯uence of the condenser on resolution in a microscope (a) Critical illumination (b) KoÈhler's illumination 10.6.3 Imaging with partially coherent quasi-monochromatic i ...
Effects of Spatial Coherence on the Angular Distribution of Radiant
Effects of Spatial Coherence on the Angular Distribution of Radiant

... W ð0Þ ð1 ;2 ;!Þ ¼ ½Sð0Þ ð1 ;!Þ1=2 ½Sð0Þ ð2 ;!Þ1=2 ð0Þ ð1 ;2 ;!Þ; (10) ...
N15_Geom_Optics - University of Arizona
N15_Geom_Optics - University of Arizona

07 Propagation of Waves
07 Propagation of Waves

... If the E-vector describes a helical (i.e., screw-like) motion in space, the projection of the E-vector onto a plane normal to the propagation direction exhibits circular motion over time, hence circular polarization. ...
Integral holography: white-light single-shot hologram
Integral holography: white-light single-shot hologram

... three different holograms, each with a different phase factor of the DOE, are recorded sequentially and superposed in the computer into a digital Fresnel hologram. A fundamentally different solution is suggested in Refs. [3,4]. According to the methods presented there, the 3-D scene is illuminated b ...
HW2 Solutions
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... energy might refract out into the air. What would be the frequency and wavelength of the sound in the air? Solution: (a) ...
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Wave Optics and Gaussian Beams

ENE 623 - web page for staff
ENE 623 - web page for staff

5_Locating Images in a Plane Mirror
5_Locating Images in a Plane Mirror

... In other words, each letter is flipped horizontally and the letters are in reverse order. This characteristic of images in plane mirrors is called lateral inversion. Emergency vehicles are labelled in reverse printing so that their signs can be viewed correctly in an automobile rear-view mirror. ...
ANSWERS - AP Physics Multiple Choice Practice – Torque
ANSWERS - AP Physics Multiple Choice Practice – Torque

... reinforcement of different λ colors due to variations in the thickness of the soap bubble. In order to see these interference results, the thickness of the film must be similar in magnitude to the wavelength of the light. Since the film is so small, this shows that light has a very small wavelength. ...
Devil physics The baddest class on campus IB Physics
Devil physics The baddest class on campus IB Physics

... incidence, i (angle between the ray and the normal to the reflecting surface at the point of incidence) is equal to the angle of reflection, r (angle between the normal and the reflected ray). ...
Lecture 10 - KFUPM Faculty List
Lecture 10 - KFUPM Faculty List

Convex Lenses and Mirrors
Convex Lenses and Mirrors

Lens equation for flat lenses made with hyperbolic
Lens equation for flat lenses made with hyperbolic

... mechanism, subwavelength resolution is only possible at near-field distance smaller than λ=4. This process differs from the evanescent amplification in perfect lenses that theoretically allows to focalize an image at distances larger than λ with a super resolution. However, in both parabolic and hyp ...
Microscopy
Microscopy

... end of the table to catch the far-field diffraction pattern. There should be a slight angle between the incoming and reflected beams. ...
Plane Mirrors
Plane Mirrors

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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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