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THEORY Geometrical optics, or ray optics, describes geometric
THEORY Geometrical optics, or ray optics, describes geometric

... With such surfaces, the direction of the reflected ray is determined by the angle the incident ray makes with the surface normal, a line perpendicular to the surface face at the point where the ray hits. The incident and reflected rays lie in a single plane, and the angle between the reflected ray a ...
Suppression of stimulated Brillouin scattering in
Suppression of stimulated Brillouin scattering in

Statistical Distribution of Field Scattered by 1
Statistical Distribution of Field Scattered by 1

Reflection and Refraction
Reflection and Refraction

Optical Pumping of Natural Rubidium
Optical Pumping of Natural Rubidium

... FIG. 3: Observed resonances during the low field optical pumping trials. The large dip to the left represents the zero-field transition, and the two dips to the right represent the Rb-87 and Rb-85 Zeeman resonances, respectively. Note that the magnetic field strength increases to the right and the t ...
Axial birefringence in high-numerical-aperture optical
Axial birefringence in high-numerical-aperture optical

... The information on optical disks is read out by focusing light of wavelength ␭ and numerical aperture (NA) on the information layer through a protective cover layer of thickness d. To increase the information density the wavelength is decreased and the numerical aperture is increased, as the spot si ...
Magnetic Plasmon Propagation Along a Chain of Connected Subwavelength Resonators
Magnetic Plasmon Propagation Along a Chain of Connected Subwavelength Resonators

... Strong wave dissipation has been one of the major obstacles for utilization of surface plasmons in optical devices. The subdiffraction-sized MP transmission line, proposed in this Letter, promises a considerable improvement in the wave transmission as shown in Fig. 3(c). For most of the propagation ...
PPT - DOE Plasma Science Center
PPT - DOE Plasma Science Center

Quasi Phase Matching Devices for Optical
Quasi Phase Matching Devices for Optical

Phys. Rev. Lett. 101, 074102(1-4) - APS Link Manager
Phys. Rev. Lett. 101, 074102(1-4) - APS Link Manager

Lesson-2 Light Microscopy
Lesson-2 Light Microscopy

... Conjugate foci: Object placed at one end of lens will form a clear image on a screen kept at other side of lens. Conjugate foci vary in position. If object is nearer the lens, the image will be formed further away, at a greater magnification and inverted. This “real” image is formed by objective len ...
OCS`08
OCS`08

Superresolution in total internal reflection tomography
Superresolution in total internal reflection tomography

Non-specular reflection of convergent beams from Iiquid-solid interface
Non-specular reflection of convergent beams from Iiquid-solid interface

Physics 425L Optics Laboratory Chromatic Aberration
Physics 425L Optics Laboratory Chromatic Aberration

Quasi Light Fields: A Model of Coherent Image Formation
Quasi Light Fields: A Model of Coherent Image Formation

... along rays. The light field is an important tool in incoherent imaging applications, where it is used to dynamically generate different viewpoints for computer graphics rendering, computational photography, and 3D displays [1–3]. Coherent imaging researchers have recognized the value of decomposing ...
DUAL NATURE OF MATTER AND RADIATION
DUAL NATURE OF MATTER AND RADIATION

... 3. Explanation of kinetic energy. If v >v₀ , then Kmax =½mvmax ∝ v i.e., above the threshold frequency, the maximum kinetic energy of the electrons increases linearly with the frequency v of the incident radiation. Moreover, the increase in intensity ...
Extraordinary optical transmission through subwavelength holes Dye-Zone A. Chen
Extraordinary optical transmission through subwavelength holes Dye-Zone A. Chen

... The optical constants used in these calculations were taken from published values.14 Overall, there is very good agreement between the calculated and measured spectra. The gross features of the spectrum are clearly reproduced, as is much of the small scale structure. The small discrepancy between th ...
Optics and Quantum Electronics E. P. Ippen
Optics and Quantum Electronics E. P. Ippen

interferometer_2014
interferometer_2014

... beam splitter and mirrors and then blow the beam up for viewing at the end. We use a laser pointer because you get a surprisingly good and reliable light source for under $25. By keeping the distances between the end mirrors and the beam splitter nearly equal, we mitigate problems caused by multimod ...
conclusion
conclusion

TS2
TS2

... Fig. 3. An assortment of optical (OM) and scanning electron (SEM) to wait until the technolomicrographs of PCF structures. (A) SEM of an endlessly single-mode gy had advanced to the solid core PCF. (B) Far-field optical pattern produced by (A) when point where larger air-fillexcited by red and green ...
Light confinement in ordered plasmonic metallic arrays and in microcavity structures
Light confinement in ordered plasmonic metallic arrays and in microcavity structures

Supplementary Methods and References
Supplementary Methods and References

... in our system). This equation shows that the depth-resolved phase term p ( zopl ) captures the combined effect of two aspects of refractive index profile of the object within the coherence gate. The first term of Eq. (5), given by  zopl , is the sub-resolution offset that measures the subresolutio ...
O A
O A

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Nonlinear optics

Nonlinear optics (NLO) is the branch of optics that describes the behavior of light in nonlinear media, that is, media in which the dielectric polarization P responds nonlinearly to the electric field E of the light. This nonlinearity is typically only observed at very high light intensities (values of the electric field comparable to interatomic electric fields, typically 108 V/m) such as those provided by lasers. Above the Schwinger limit, the vacuum itself is expected to become nonlinear. In nonlinear optics, the superposition principle no longer holds.Nonlinear optics remained unexplored until the discovery of Second harmonic generation shortly after demonstration of the first laser. (Peter Franken et al. at University of Michigan in 1961)
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