RADAR CROSS-SECTION STUDIES OF SPHERICAL LENS
... practical SLRs varies within the range 5 ≤ 2r1 /λ ≤ 200, though our code enables us to advance into the extremely deep optical region where the parameter 2 r1 /λ may take values up to 10000 (k0 r1 ∼ 30000). The dielectric constant εr varies from 2.1 (PTFE) to 3.8 (fused quartz). The dB-scaled distri ...
... practical SLRs varies within the range 5 ≤ 2r1 /λ ≤ 200, though our code enables us to advance into the extremely deep optical region where the parameter 2 r1 /λ may take values up to 10000 (k0 r1 ∼ 30000). The dielectric constant εr varies from 2.1 (PTFE) to 3.8 (fused quartz). The dB-scaled distri ...
WAVE PLATES
... component is retarded by one half-wave, it will also be a maximum, but 180° out of phase, or pointing along the negative slow axis. If we follow the wave further, we see that the slow component remains exactly 180° out of phase with the original slow component, relative to the fast component. This d ...
... component is retarded by one half-wave, it will also be a maximum, but 180° out of phase, or pointing along the negative slow axis. If we follow the wave further, we see that the slow component remains exactly 180° out of phase with the original slow component, relative to the fast component. This d ...
Kursat Sendur 2009 Opex1
... Due to the large number of geometry, material composition, and source-related parameters, the development of efficient and accurate modeling and simulation tools for nearfield optical systems is necessary. In this study, an integral equation based numerical solution is developed for nano-optical par ...
... Due to the large number of geometry, material composition, and source-related parameters, the development of efficient and accurate modeling and simulation tools for nearfield optical systems is necessary. In this study, an integral equation based numerical solution is developed for nano-optical par ...
Étendue and spectral resolution
... The finesse is a measure of the spectral resolution that can be achieved with an interferometer for a specified FSR – which is determined by experimental requirements. Ideally the interferometer plates should be illuminated by parallel rays of light and these rays should be in the wedge plane of the ...
... The finesse is a measure of the spectral resolution that can be achieved with an interferometer for a specified FSR – which is determined by experimental requirements. Ideally the interferometer plates should be illuminated by parallel rays of light and these rays should be in the wedge plane of the ...
Computer-generated holograms of three
... wave front on the rear focal plane of a spherical lens when the object is located near the front focal point and illuminated by a plane wave. Therefore the computed matrix can be used as a CGH after it is encoded to a real positive-valued transparency. When such CGH is illuminated by a plane wave, a ...
... wave front on the rear focal plane of a spherical lens when the object is located near the front focal point and illuminated by a plane wave. Therefore the computed matrix can be used as a CGH after it is encoded to a real positive-valued transparency. When such CGH is illuminated by a plane wave, a ...
PowerPoint Presentation - Tip-tilt mirror and sensor configuration
... • Description of diffraction depends on how far you are from the source (Fresnel, Fraunhofer) • Geometric and diffractive phenomena seen in the lab (Rayleigh range, diffraction limit, depth of focus…) • Image formation with wave optics Page 65 ...
... • Description of diffraction depends on how far you are from the source (Fresnel, Fraunhofer) • Geometric and diffractive phenomena seen in the lab (Rayleigh range, diffraction limit, depth of focus…) • Image formation with wave optics Page 65 ...
Plane-wave scattering by a dielectric circular cylinder
... Figure 1 shows the geometrical layout of our problem: A monochromatic plane wave with wavelength l impinges on a dielectric circular cylinder of radius a and refractive index n c . The cylinder axis is placed at a distance h from a general reflecting flat surface. This diffractive structure is assum ...
... Figure 1 shows the geometrical layout of our problem: A monochromatic plane wave with wavelength l impinges on a dielectric circular cylinder of radius a and refractive index n c . The cylinder axis is placed at a distance h from a general reflecting flat surface. This diffractive structure is assum ...
Sign convention
... 1. A ray through the center of the lens is undeviated 2. An incident ray parallel to the optic axis appears to emerge from the front focal point 3. An incident ray directed towards the back focal point emerges parallel to the optic axis. and occasionally useful 4. Two rays that are parallel in front ...
... 1. A ray through the center of the lens is undeviated 2. An incident ray parallel to the optic axis appears to emerge from the front focal point 3. An incident ray directed towards the back focal point emerges parallel to the optic axis. and occasionally useful 4. Two rays that are parallel in front ...
The Physics 431 Final Exam Wed, DECEMBER 15, 2010
... This condition means going a distance away: z >> kD2/2 = πD2/λ If D = 1 mm and λ = 1 micron, then z >> 3 m. ...
... This condition means going a distance away: z >> kD2/2 = πD2/λ If D = 1 mm and λ = 1 micron, then z >> 3 m. ...
RESOLUTION OF ICCD CAMERAS
... system to transfer various levels of detail from object to image. It is defined by the ratio of percentage modulation of a sinusoidal signal leaving to that entering the device over the range of frequencies of interest (see figure 1 below). It is mathematically obtainable from the point spread funct ...
... system to transfer various levels of detail from object to image. It is defined by the ratio of percentage modulation of a sinusoidal signal leaving to that entering the device over the range of frequencies of interest (see figure 1 below). It is mathematically obtainable from the point spread funct ...