Analysis of the Spectral Resolution of a TeO2 based Noncollinear
... such as laser wavelength tuning, spectral analysis, spectral imaging [1-3], and etc. TeO2 is a kind of A-O crystal with many applications in the large angular aperture noncollinear AOTF. Light diffraction by acoustic wave propagating in the A-O crystal is the foundation of the operation of an AOTF. ...
... such as laser wavelength tuning, spectral analysis, spectral imaging [1-3], and etc. TeO2 is a kind of A-O crystal with many applications in the large angular aperture noncollinear AOTF. Light diffraction by acoustic wave propagating in the A-O crystal is the foundation of the operation of an AOTF. ...
Diffraction-free beams in thin films *
... and B共kx兲 are simply the Airy formulas corresponding to the transmittance and reflectance coefficients through the slab [31]. Thus, the matrix elements A and B quantify the contribution of reflected and transmitted wavelets to the scattered fields R±n. We confirm that Ũ±n = F̃±n = R̃±n under perfec ...
... and B共kx兲 are simply the Airy formulas corresponding to the transmittance and reflectance coefficients through the slab [31]. Thus, the matrix elements A and B quantify the contribution of reflected and transmitted wavelets to the scattered fields R±n. We confirm that Ũ±n = F̃±n = R̃±n under perfec ...
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... sphere, that is suspended in a fixed position from the top of the tank. Measurements of the relative photon density (17) are made by positioning one end of a detection fiber in the Intralipid at a known location relative to the source and attaching the other end to a photomultiplier tube. The signal ...
... sphere, that is suspended in a fixed position from the top of the tank. Measurements of the relative photon density (17) are made by positioning one end of a detection fiber in the Intralipid at a known location relative to the source and attaching the other end to a photomultiplier tube. The signal ...
Singularities of interference of three waves with different polarization
... (along the x-axis). The third wave coming from the second arm of proposed polarization interferometer is linearly or circularly polarized with linearly changed phase difference along the y-axis. The interference of three plane waves with different polarization states (LLL – linear-linear-linear or L ...
... (along the x-axis). The third wave coming from the second arm of proposed polarization interferometer is linearly or circularly polarized with linearly changed phase difference along the y-axis. The interference of three plane waves with different polarization states (LLL – linear-linear-linear or L ...
JOURNAL OF T O THE EUROPEAN OPTI CAL SOCI ETY
... is located between the aperture stop and the entrance pupil. A theory of aberrational vignetting has been developed using the eikonal theory. [DOI: 10.2971/jeos.2009.09046] Keywords: aberration, apertures, eikonal theory, radiometry, vignetting ...
... is located between the aperture stop and the entrance pupil. A theory of aberrational vignetting has been developed using the eikonal theory. [DOI: 10.2971/jeos.2009.09046] Keywords: aberration, apertures, eikonal theory, radiometry, vignetting ...
Parallel-plate MEMS Mirror Design for Large On
... another silicon wafer, thus eliminating the need for the release step associated with surface micromachining. To test the device in the laboratory, both the mirror and the back electrode were mounted on separate 1” tip-tilt optical mounts, and placed on translation stages. The plane faces were align ...
... another silicon wafer, thus eliminating the need for the release step associated with surface micromachining. To test the device in the laboratory, both the mirror and the back electrode were mounted on separate 1” tip-tilt optical mounts, and placed on translation stages. The plane faces were align ...
Lectures on Theoretical Physics Linear Response Theory
... 5 Dielectric susceptibility 5.1 Polarization of matter . . . . . . . . . . . . . . . . . . . . . . . . . 5.2 Dielectric susceptibility . . . . . . . . . . . . . . . . . . . . . . . . 5.3 Susceptibility proper and optical activity . . . . . . . . . . . . . . . ...
... 5 Dielectric susceptibility 5.1 Polarization of matter . . . . . . . . . . . . . . . . . . . . . . . . . 5.2 Dielectric susceptibility . . . . . . . . . . . . . . . . . . . . . . . . 5.3 Susceptibility proper and optical activity . . . . . . . . . . . . . . . ...
Computer-generated holograms for three
... sometimes referred to as ray tracing.2 However, there are also wave-oriented methods to calculate object fields in which fields emitted from objects defined as planar segments9,10 or 3-D distributions of field strength11 are calculated by methods based on wave optics. The major advantage of wave-ori ...
... sometimes referred to as ray tracing.2 However, there are also wave-oriented methods to calculate object fields in which fields emitted from objects defined as planar segments9,10 or 3-D distributions of field strength11 are calculated by methods based on wave optics. The major advantage of wave-ori ...
Fresnel Equations. In Encyclopedia of Optical Engineering
... where n1 and n2 are the refractive indices of the two media. The angle θr of the reflected wave is equal to θi according to the law of reflection. We denote the amplitudes of these two waves as Et and Er, respectively. Our goal is to determine these amplitudes. To accomplish this, we apply the bound ...
... where n1 and n2 are the refractive indices of the two media. The angle θr of the reflected wave is equal to θi according to the law of reflection. We denote the amplitudes of these two waves as Et and Er, respectively. Our goal is to determine these amplitudes. To accomplish this, we apply the bound ...