physics 415/416 supplemental problems
... is blazed to operate in the first order. Refer to the sheet and answer the following questions. (a) What is the line separation a of this grating? (b) What is the linear dispersion (in mm/nm) of this grating near the blaze wavelength? Calculate it using L=1/4 m. (c) From your answer in (b), calculat ...
... is blazed to operate in the first order. Refer to the sheet and answer the following questions. (a) What is the line separation a of this grating? (b) What is the linear dispersion (in mm/nm) of this grating near the blaze wavelength? Calculate it using L=1/4 m. (c) From your answer in (b), calculat ...
Photorefractive cyclometalated complexes
... substituting electronics with photonics, since, in principle, photons can carry much more information and more rapidly than electrons. Within this frame, materials with physical properties that can be modulated by light are very interesting, among these are photoconducting media [1], which exhibit a ...
... substituting electronics with photonics, since, in principle, photons can carry much more information and more rapidly than electrons. Within this frame, materials with physical properties that can be modulated by light are very interesting, among these are photoconducting media [1], which exhibit a ...
The Intermediate Optical System of Laser
... Ordinary photographic cameras use a single lens to form an image. This has the property that the magnification varies with the distance of the object from the lens. As a result, in pictures of high buildings taken from ground level, the edges are tilted towards the image’s top center. This phenomeno ...
... Ordinary photographic cameras use a single lens to form an image. This has the property that the magnification varies with the distance of the object from the lens. As a result, in pictures of high buildings taken from ground level, the edges are tilted towards the image’s top center. This phenomeno ...
2. Spectral Stray Light
... measurements (Damm 2007) are illustrated in fig. 3. It can be seen that the spectral stray light can span 60 or more channels. The gap around channel 0 is due to the fact that only the out-of-band channels are shown (Damm 2007). While this method quantifies the stray light over “long ranges”, it is ...
... measurements (Damm 2007) are illustrated in fig. 3. It can be seen that the spectral stray light can span 60 or more channels. The gap around channel 0 is due to the fact that only the out-of-band channels are shown (Damm 2007). While this method quantifies the stray light over “long ranges”, it is ...
Metamaterials at Optical Frequencies: Fabrication and Measurements
... Masks are generally made using electron-beam lithography (EBL), which has been employed as the tool of choice in the fabrication of near-infrared or optical-frequency metamaterials because of its high resolution, moderate cost and flexibility (allowing designs to be easily changed). However, for mas ...
... Masks are generally made using electron-beam lithography (EBL), which has been employed as the tool of choice in the fabrication of near-infrared or optical-frequency metamaterials because of its high resolution, moderate cost and flexibility (allowing designs to be easily changed). However, for mas ...
Lecture_22
... The sign conventions are slightly different: 1. The focal length is positive for converging lenses and negative for diverging. 2. The object distance is positive when the object is on the same side as the light entering the lens (not an issue except in compound systems); otherwise it is ...
... The sign conventions are slightly different: 1. The focal length is positive for converging lenses and negative for diverging. 2. The object distance is positive when the object is on the same side as the light entering the lens (not an issue except in compound systems); otherwise it is ...
Lab 7: Fabry-Perot Interferometer
... the Fabry-Perot cavity. To ensure this is the case, adjust the mirrors so the reflected laser beam goes back on itself into the laser. You should see the slightly expanded beam reflected back on to the laser aperture. Now that the beam is incident perpendicular to the first glass plate, we must adju ...
... the Fabry-Perot cavity. To ensure this is the case, adjust the mirrors so the reflected laser beam goes back on itself into the laser. You should see the slightly expanded beam reflected back on to the laser aperture. Now that the beam is incident perpendicular to the first glass plate, we must adju ...
Exam 4 problems
... 2. For a monochromatic electric field in a dispersive medium, write the general expression for the frequency dependent electric susceptibility (). What is the limit of () as infinity? What is the high frequency limit of the dielectric polarization P? 3. Write Newton’s equation for the motio ...
... 2. For a monochromatic electric field in a dispersive medium, write the general expression for the frequency dependent electric susceptibility (). What is the limit of () as infinity? What is the high frequency limit of the dielectric polarization P? 3. Write Newton’s equation for the motio ...
Images in Lenses
... students understand each part, as various incident rays behave differently in other parts of the illustration. Ask students questions such as, Is this incident ray parallel or angled? Where is the light source now? What happens when it emerges and why? • As you work through the illustrations with st ...
... students understand each part, as various incident rays behave differently in other parts of the illustration. Ask students questions such as, Is this incident ray parallel or angled? Where is the light source now? What happens when it emerges and why? • As you work through the illustrations with st ...
Low-coherence heterodyne photon correlation spectroscopy
... fluid, making the polystyrene spheres neutrally buoyant. The volume fractions utilized ranged from 0.001% to 0.01% yielding from one-third to three scattering mean-free-path lengths across our 1 cm sample cell. We find that the number of scattering path lengths across the sample cell (L, where i ...
... fluid, making the polystyrene spheres neutrally buoyant. The volume fractions utilized ranged from 0.001% to 0.01% yielding from one-third to three scattering mean-free-path lengths across our 1 cm sample cell. We find that the number of scattering path lengths across the sample cell (L, where i ...
Supplementary Material for
... in which the real part of the spatial field correlation function decays to half its maximum value. The correlation length was determined from measurements made with a collimated incident beam (500-m diameter) with small angular divergence (0.046°). Measurements of for different values of L ...
... in which the real part of the spatial field correlation function decays to half its maximum value. The correlation length was determined from measurements made with a collimated incident beam (500-m diameter) with small angular divergence (0.046°). Measurements of
ppt
... Regions where the field of geometrical optics diverges (i.e. where at least one radius of curvature is zero and the density of rays is infinitely high). ...
... Regions where the field of geometrical optics diverges (i.e. where at least one radius of curvature is zero and the density of rays is infinitely high). ...
Template for Technical Memo - MZA Associates Corporation
... Subject: How to choose mesh spacings and mesh dimensions for wave optics simulation. In wave optics simulation, optical wavefronts are represented using two-dimensional rectangular complex meshes. In order to obtain correct simulation results, it is important to choose mesh spacings small enough to ...
... Subject: How to choose mesh spacings and mesh dimensions for wave optics simulation. In wave optics simulation, optical wavefronts are represented using two-dimensional rectangular complex meshes. In order to obtain correct simulation results, it is important to choose mesh spacings small enough to ...
Retroreflector
A retroreflector (sometimes called a retroflector or cataphote) is a device or surface that reflects light back to its source with a minimum of scattering. In a retroreflector an electromagnetic wavefront is reflected back along a vector that is parallel to but opposite in direction from the wave's source. The angle of incidence at which the device or surface reflects light in this way is greater than zero, unlike a planar mirror, which does this only if the mirror is exactly perpendicular to the wave front, having a zero angle of incidence.