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Modeling phase microscopy of transparent three
Modeling phase microscopy of transparent three

Advanced optics tutorials
Advanced optics tutorials

Mechanism of angular momentum transfer from microwaves to
Mechanism of angular momentum transfer from microwaves to

... and macroscopic objects, there have been several studies reporting mechanical torques on various objects. Whereas some works manipulate the radiation pressure on specifically designed complex objects [3–5], most of the experiments use the AM of light. It can either be the Spin Angular Momentum (SAM) ...
(a) n r from the center is an example of a
(a) n r from the center is an example of a

... the optical axis the optical path length (OPL) is given as (OPL)O = nmaxd At a height r, (OPL)r ≈ n(r)d. In order for the rays to converge at a focus, the planar wavefront must bend into a spherical wavefront, which defines surfaces of constant phase. ...
Subwavelength transportation of light with atomic resonances
Subwavelength transportation of light with atomic resonances

... resonance condition t(k)G(k) = 1. We also investigated the transport through atoms for straight lines of two different lengths but the same lattice spacing. The “carrier wave” periodicity remains the same for the different lengths of the chain. Generally, the resonance energy levels form a discrete ...
Digital holography of total internal reflection
Digital holography of total internal reflection

Determining Shape and Fringe Count in a Holographic
Determining Shape and Fringe Count in a Holographic

... pattern of fringes on the recording media. These fringes can be bright and dark. When the crust or trough of two waves or more waves meet, they form the bright or constructive interference. But when crust and trough of waves meet, it forms dark or destructive fringe pattern. [2, 4] The paper starts ...
Analytic design method for optimal imaging: coupling three ray sets
Analytic design method for optimal imaging: coupling three ray sets

... In contrast, direct optics design methods do not necessarily follow this design strategy. Usually, a key objective is to find a set of unrestricted free-form surfaces designed to have specific predefined characteristics. Where unrestricted means that the optical surfaces can have any shape to fulfil ...
Resolution Power And Intensity Distribution Using Synthetic Square
Resolution Power And Intensity Distribution Using Synthetic Square

... number of rows and columns are choosing (T=2,4,6,8,10),that mean the apertures allow light to pass through it are (2,8,18,32,50) . The two cases (G=1,G=-1) are solved , the result appear similar in two cases at ideal system or contain focus error and aberrations which are chosen in research. Figure ...
Do Solitonlike Self-Similar Waves Exist in Nonlinear Optical Media?
Do Solitonlike Self-Similar Waves Exist in Nonlinear Optical Media?

... fundamental bright (or dark) spatial soliton using an appropriate phase mask placed at the entrance to the gradedindex waveguide. If the amplifier gain g satisfies the condition given in Eq. (11), the entering phase-chirped spatial soliton propagates inside the amplifier as a self-similar wave found ...
Get PDF - OSA Publishing
Get PDF - OSA Publishing

... The factor hcos θ is is an asymmetry parameter of the scattering: hcos θ is is positive or negative when the scattering at the forward hemisphere is stronger or weaker relative to the scattering at the backward hemisphere. An inspection of (20) shows why even in the idealized case of negligible abso ...
Physical Properties of Lead Molybdate Relevant to Acousto
Physical Properties of Lead Molybdate Relevant to Acousto

... the positive sense of axes for nonpiezoelectric crystals, we have somewhat arbitrarily chosen +Z such that the elastic constant CI6 is positive. Our crystals were oriented with respect to this "convention" by acoustic velocity measurements. X-ray techniques could be used also to find the +Z axis, bu ...
Second harmonic generation via total internal reflection quasi
Second harmonic generation via total internal reflection quasi

... the input/output polarization of the propagating waves 2. The effective nonlinear d coefficient (deff) can also change sign after reflection depending on the selection of the input/output polarization which will result in an extra phase shift (ξπ) with ξ being 1 or 0 depending on the inversion of de ...
Wave Optics Theory and 3-D Deconvolution for the Light Field
Wave Optics Theory and 3-D Deconvolution for the Light Field

Document
Document

7_SNOM
7_SNOM

... Ex, y, z    F u, v,0  ei ux vy  wz dudv ...
Simultaneous calibration of optical tweezers spring constant and
Simultaneous calibration of optical tweezers spring constant and

... The subsequent application of high-resolution position detection methods, e.g. back focal plane detection [1, 2], and accurate calibration of the tweezers’ spring constant then readily enabled the measurement of displacements and forces by individual biomolecular motors [3–5]. When the same laser be ...
Light Field Microscopy - Stanford Computer Graphics Laboratory
Light Field Microscopy - Stanford Computer Graphics Laboratory

... system thickness is not an issue, the latter arrangement is preferred. For a microscope, where resolution of the image is critical, a field lens is essential. This choice also allows us to reuse the most critical and highly optimized component in a conventional microscope, its objective (see figure ...
The Intermediate Optical System of Laser
The Intermediate Optical System of Laser

Shedding Light on Hybrid Optics: A Tutorial in
Shedding Light on Hybrid Optics: A Tutorial in

Determination of the transfer function for optical surface topography
Determination of the transfer function for optical surface topography

... with image formation no longer describable using an OTF. Instead, the so-called transmission cross-coefficient (TCC) [36, 38] must be defined which describes the attenuation and relative phase shift upon imaging pairs of spatial frequencies (of the underlying time instantaneous field). Definition of ...
Optical bistability in a Vertical-Cavity Semiconductor Optical Amplifier
Optical bistability in a Vertical-Cavity Semiconductor Optical Amplifier

Automated Mode-Matching of Gaussian Beams
Automated Mode-Matching of Gaussian Beams

... overall beam profile. It is with this in mind that a deep optimization is then taken with these rough solutions in mind, using the same fminsearch with more iterations. From the positions found by the rough approximation, a second pass is done on these points using a max iteration value of 100. In e ...
Atmospheric Turbulence and its Influence on Adaptive Optics
Atmospheric Turbulence and its Influence on Adaptive Optics

Spherical mirrors in the paraxial approximation [Pages 181-187]. Assignment 2
Spherical mirrors in the paraxial approximation [Pages 181-187]. Assignment 2

... To use this result you need to have the object at a distance more than 10f 2 (f is the focal length of the positive lens) or use a collimated laser beam. In this formula either f1 or f2 could be the focal length of the diverging lens. If the first lens is the positive lens then the separation distan ...
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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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