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Wavefront Aberrations
Wavefront Aberrations

... (like V = U + P). In reality, many of the rays that are incident on a lens are NOT paraxial. So, ideal images are NOT formed. We can begin to see the effects of this if we expand the sine function in a power series expansion: sin  =   3/3! + 5/5! .... In the paraxial approximation, we keep just ...
HEAVY ION BEAM ACCELERATION
HEAVY ION BEAM ACCELERATION

... The magnetic field along the axial hole of the cyclotron magnet was calculated using the TOSCA code for various current excitations. The field, as shown in Fig. 3. is characterized by a sharp gradient at the beginning of the yoke and then it decreases gradually along the axis. The axial field near t ...
Chapter 8
Chapter 8

... axis and the wave direction. The refractive index depends on whether the Efield is parallel or perpendicular to the principal plane. Ray direction: Energy flow direction. o-ray: E-field normal to the principal plane. e-ray: E-field parallel to the principal plane. However, inside a crystal the light ...
4 Modeling of SVE fields in WaveTrain
4 Modeling of SVE fields in WaveTrain

Overview of various methods for measuring a lens focal length
Overview of various methods for measuring a lens focal length

... The lens power is measured for different positions of the source. The author of this method claims that routinely measurements are made with less than 0.5% accuracy. ...
LATTICE IMAGING IN TRANSMISSION ELECTRON MICROSCOPY
LATTICE IMAGING IN TRANSMISSION ELECTRON MICROSCOPY

Demonstration of a multiwave coherent holographic beam combiner in a polymeric substrate
Demonstration of a multiwave coherent holographic beam combiner in a polymeric substrate

... The optical setup for demonstrating a six-beam combiner is presented in Fig. 3. The input beam from the laser illuminates the hologram in the direction of reference R. The gratings act as a beam splitter, producing six diffracted waves (indicated by solid lines in the figure). The six waves are coll ...


... thin diffusion screen with the complex amplitude transmittance which is randomly changed in time. Such a screen may be created in practice by means of the electrically controlled spatial-time light modulator on the basis of a twisted nematic liquid crystal placed between two polarizers (see, for exa ...
Measuring the Real Point Spread Function of High Numerical
Measuring the Real Point Spread Function of High Numerical

... A perfect lens transforms a plane wave front into a converging spherical wave. If they are not too dramatic, any deviations from this ideal behavior can be described by introducing a complex Pupil Function P(r, q), where r is the normalized radial coordinate in the pupil plane and m is the azimuthal ...
4. characterization of phase modulation
4. characterization of phase modulation

... A twisted nematic liquid crystal display (TNLCD) is a device that changes the state of polarization of light. In a properly controlled environment, consisting in a set of suitably configured optical elements and the TNLCD, the change in the state of polarization of light can be used to modulate the ...
Optical polarization tutorial
Optical polarization tutorial

... 1 Birefringence, or double refraction, is an optical property of certain materials, primarily crystals. Birefringent materials have anisotropic structure, such that a light wave polarized along a particular direction (called optical axis) has index of refraction which is different from waves polarize ...
Chromatic and Monochromatic Aberrations
Chromatic and Monochromatic Aberrations

... the photons that emerge from a common source at any given instant in time. Or, if you think of light as a wave (like ripples when you drop a stone into a puddle), the wavefront is a.line or surface that follows the crest of any wave. For example, a point source emits light in all directions. The ray ...
Revista Mexicana de Física . Simulation of Michelson and
Revista Mexicana de Física . Simulation of Michelson and

Modulation of spatial coherence of optical field by means of liquid
Modulation of spatial coherence of optical field by means of liquid

R.J.Kasumova, Second harmonic generation in
R.J.Kasumova, Second harmonic generation in

... It should be noted that difficulty of creating metamaterials in a field of optical lengths of waves has two aspects. Above all, metallic conducting elements forming micro schemes of metamaterial of conductor and rings with split type are to be lessened to the scale of nanometers to make them smaller ...
Lecture-6-Optics
Lecture-6-Optics

... determines the light gathering ability of the lens. Field Stop (F.S.) – Limits the size or angular breadth of the object. In a camera, the edge of the film itself bounds the image plane and becomes the F.S. Entrance Pupil – Image of the A.S. as seen from the object side of the lens system (below). E ...
Optics of Anisotropic Media
Optics of Anisotropic Media

Photonic band structure theory: assessment and perspectives
Photonic band structure theory: assessment and perspectives

... The present paper offers an overview of photonic bandstructure theory. Section 1 provides an introduction to photonic bandstructure calculations as well as a discussion of the most prominent methods for the their along with some of the most important results. In Section 2, methods for and results of ...
Diffraction
Diffraction

The Absolute Sensitivity of Lens and Compound Eyes
The Absolute Sensitivity of Lens and Compound Eyes

ptical Short Course International
ptical Short Course International

... projector lens design. We know that all glasses have dispersion which means that they have a slightly different refractive index for each wavelength or color of light. Because we want to view nice vivid colors in our projected images our projection lenses must be corrected to work over the full wave ...
CfE Advanced Higher Physics – Unit 2 – Waves
CfE Advanced Higher Physics – Unit 2 – Waves

Tutorial of Telecentric Lens
Tutorial of Telecentric Lens

Flatland optics - Weizmann Institute of Science
Flatland optics - Weizmann Institute of Science

52.3: An Improved Polarizing Beamsplitter LCOS Projection
52.3: An Improved Polarizing Beamsplitter LCOS Projection

... extinction ratio as a function of angle occurs with the MacNeille beamsplitter than occurs with the Proflux™ beamsplitter, although there is greater variation with wavelength in the behavior of the Proflux™. Even with its spectral variation, however, the Proflux™ delivers performance in excess of 60 ...
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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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