A light scattering study of non equilibrium fluctuations
... intermediate scattering function of NEFs for each wave vector covered by the NFS experiment and each delay time contained in the image sequence. Working at 1:1 magnification, the theoretically accessible wave vectors are set by the size of the area detector and the pixel size. If L is the edge lengt ...
... intermediate scattering function of NEFs for each wave vector covered by the NFS experiment and each delay time contained in the image sequence. Working at 1:1 magnification, the theoretically accessible wave vectors are set by the size of the area detector and the pixel size. If L is the edge lengt ...
Investigations on the Theory of the Transverse Doppler Effect
... Equations (1) and (2) are the formulas of the relativistic Doppler shift and of the aberration. Where u = cβ, γ = (1 − β 2 )−1/2 and c is the velocity of light in vacuum. The inverse transformation, from ν 0 and α0 to ν and α, can be easily obtained from equations (1) and (2) by straightforward calc ...
... Equations (1) and (2) are the formulas of the relativistic Doppler shift and of the aberration. Where u = cβ, γ = (1 − β 2 )−1/2 and c is the velocity of light in vacuum. The inverse transformation, from ν 0 and α0 to ν and α, can be easily obtained from equations (1) and (2) by straightforward calc ...
Optical design of reflectionless complex media by
... to an external observer and allow to transfer the electromagnetic field manipulations from the transformation optical medium to another medium. In addition, a heuristic topological design criterion was described in order to engineer the transformation optical device perfectly reflectionless. The new ...
... to an external observer and allow to transfer the electromagnetic field manipulations from the transformation optical medium to another medium. In addition, a heuristic topological design criterion was described in order to engineer the transformation optical device perfectly reflectionless. The new ...
Interference with monochromatic light
... A parallel beam of monochromatic light enters from the left side under the angle of incidence ϑ. Due to multiple reflection between the mirrors there is an infinite number of beams leaving the device to the right side; they are all laterally displaced by the same amount with respect to their neighbo ...
... A parallel beam of monochromatic light enters from the left side under the angle of incidence ϑ. Due to multiple reflection between the mirrors there is an infinite number of beams leaving the device to the right side; they are all laterally displaced by the same amount with respect to their neighbo ...
RAY OPTICS I
... 1. The first principal ray is the ray that goes through the center of the lens. Near the center of the lens, the front and back surfaces of the lens are essentially parallel, like an ordinary flat piece of glass. Just as photons going through a flat pane of glass are not significantly deflected, so ...
... 1. The first principal ray is the ray that goes through the center of the lens. Near the center of the lens, the front and back surfaces of the lens are essentially parallel, like an ordinary flat piece of glass. Just as photons going through a flat pane of glass are not significantly deflected, so ...
Anomalous transient amplification of waves in non
... gain can be exploited to engineer novel functionalities for propagating and filtering electromagnetic radiation. Here we show a generic property of optical systems that feature an unbalanced distribution of loss and gain, described by non-normal operators, namely that an overall lossy optical system ...
... gain can be exploited to engineer novel functionalities for propagating and filtering electromagnetic radiation. Here we show a generic property of optical systems that feature an unbalanced distribution of loss and gain, described by non-normal operators, namely that an overall lossy optical system ...
Phase space of partially coherent light with discontinuous surfaces
... in 1932 as a quasi-probability distribution to describe quantum mechanics in phase space. Later the Wigner function was introduced into optics by Dolin and Walther [2–4], to describe an optical signal in phase space. There are several remarkable advantages of using the Wigner function for analyzing ...
... in 1932 as a quasi-probability distribution to describe quantum mechanics in phase space. Later the Wigner function was introduced into optics by Dolin and Walther [2–4], to describe an optical signal in phase space. There are several remarkable advantages of using the Wigner function for analyzing ...
Electrostatic micromirrors for subaperturing in an
... membrane, the pixels of a DMD are not interconnected and reflect light in one of two preset directions only. Our experiments utilized the 600 800-element DMD that forms the core element of the Texas Instruments digital light processing video display system [17–20]. Each mirror pixel in the TI-DMD p ...
... membrane, the pixels of a DMD are not interconnected and reflect light in one of two preset directions only. Our experiments utilized the 600 800-element DMD that forms the core element of the Texas Instruments digital light processing video display system [17–20]. Each mirror pixel in the TI-DMD p ...
Conditions for practicing compressive Fresnel holography Yair Rivenson * and Adrian Stern
... jϕðrÞj2 , because each column is a just a circularly shifted version of ϕðrÞ. We note that in our case, ϕðrÞ is actually the discrete Fresnel propagation point spread function (PSF). This means that in order to evaluate the coherence parameter, we need only to consider the maximum absolute value of ...
... jϕðrÞj2 , because each column is a just a circularly shifted version of ϕðrÞ. We note that in our case, ϕðrÞ is actually the discrete Fresnel propagation point spread function (PSF). This means that in order to evaluate the coherence parameter, we need only to consider the maximum absolute value of ...
Computational photography with plenoptic camera and light field
... community [24]. Note that the term “light field” was first used in a translated work on illumination engineering in the 1930s [23,25], but this is not in the sense of an electromagnetic field, which underlines the principles of optics [26]. The value of Lu; v; x; y is the amount of light—known as ...
... community [24]. Note that the term “light field” was first used in a translated work on illumination engineering in the 1930s [23,25], but this is not in the sense of an electromagnetic field, which underlines the principles of optics [26]. The value of Lu; v; x; y is the amount of light—known as ...
Three-dimensional imaging by optical sectioning in the aberration
... Note that the convolution over the z coordinate is only strictly valid if the form of the probe is unchanged by scattering within the sample. In the case of isolated nanoparticles on a light support, this is a reasonable approximation. Using the convolution theorem (Bracewell 2000), the Fourier tran ...
... Note that the convolution over the z coordinate is only strictly valid if the form of the probe is unchanged by scattering within the sample. In the case of isolated nanoparticles on a light support, this is a reasonable approximation. Using the convolution theorem (Bracewell 2000), the Fourier tran ...
CHAPTER 1 PHYSICAL OPTICS: INTERFERENCE • Introduction
... But many optical phenomena cannot be adequately explained by geometrical optics. For example, the iridescence that makes the colors of a hummingbird so brilliant are not due to pigment but to an interference effect caused by structures in the feathers. ...
... But many optical phenomena cannot be adequately explained by geometrical optics. For example, the iridescence that makes the colors of a hummingbird so brilliant are not due to pigment but to an interference effect caused by structures in the feathers. ...
