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Low-coherence heterodyne photon correlation spectroscopy
Low-coherence heterodyne photon correlation spectroscopy

Soleil-Babinet Compensator
Soleil-Babinet Compensator

A simple peak-to-average power ratio reduction
A simple peak-to-average power ratio reduction

Section 4 Diffraction_handbook of optics
Section 4 Diffraction_handbook of optics

... diffraction with every obstacle they encounter. Maxwell’s equations form a theoretical basis for describing light in propagation, diffraction, scattering and, in general, its interaction with material media. Experience has shown that the electric field E plays a central role in detection of light an ...
acta physica slovaca vol. 50 No. 4, 489 – 500 August 2000 MATRIX
acta physica slovaca vol. 50 No. 4, 489 – 500 August 2000 MATRIX

... A profile of the complex refractive index across the thin film represent this inhomogeneity. The schematic diagram of j-th inhomogeneous film (IHF) of the system is plotted in Fig. 2. It is known that the solution of the Maxwell equations expressing the wave propagation within the inhomogeneous thin ...
Document
Document

... generate circularly polarized waves. Similarly, the polarized waves in different phase and different amplitude give elliptical polarized waves [5]. Polarization at any point is expressed by the sum of the wave vector components by the principle of superposition [6]. Light passes through the magnetic ...
Surface-Enhanced Raman Scattering in Noble
Surface-Enhanced Raman Scattering in Noble

Intense, ultrashort light and dense, hot matter
Intense, ultrashort light and dense, hot matter

... power of laser pulses. The peak power is boosted by successive amplification of laser pulses in a set of light amplifiers. As peak powers go up, the larger electric fields give rise to nonlinear processes. One of the nonlinear processes discovered soon after the laser was born is self-focusing. This ...
Diffracting fractals: new paradigms in linear wave physics
Diffracting fractals: new paradigms in linear wave physics

... Figure 5: Diffraction of the Weierstrass fractal function [Eq. (1)] with random phases for different values of the dimension D at a single slit when D = 1.99. (a) NF = 5, (b) NF = 10, (c) NF = 30, (d) NF = 50. Other parameters:  = 1.2, /a = 1.0, L/k = 1, and  = 0.1. Shaded areas denote geometric ...
Full text - UvA/FNWI - University of Amsterdam
Full text - UvA/FNWI - University of Amsterdam

... is a great simplication however, for the alkali metals it is not a bad approximation and it is useful as a tool to understand the basic interactions between light and atoms. The interaction of atoms with light can be broken down in two main parts. A dissipative part and a conservative part of inter ...
Noise-related resolution limit of dispersion measurements with white
Noise-related resolution limit of dispersion measurements with white

... spectrally resolved interferometry are given in Section 6); however, a detailed comparison between spectrally resolved and spectrally integrated detection methods goes beyond the scope of this paper. Spectral resolution, the accuracy of GDD determination, and the measurement time are the key paramet ...
Optics in Astronomy
Optics in Astronomy

... complex degree of self coherence: ...
Physics Laboratory Manual PHYC 20080 Fields, Waves and Light
Physics Laboratory Manual PHYC 20080 Fields, Waves and Light

... During the laboratory practicals, students will be paired off with a partner with whom they perform the experiment and collect the data. In order to make optimal use of your time in the laboratory, please read the manual and familiarise yourself with the experiment before the laboratory practical. T ...
Refraction
Refraction

... When a light ray travels from a denser medium into a rarer medium it is refracted away from the normal. As the angle of incidence increases so does the angle of refraction. Eventually the angle i is reached that give an angle r of 90o. The angle i for which this occurs is called the critical angle. ...
2001 - Institute of Applied Physics - Friedrich-Schiller
2001 - Institute of Applied Physics - Friedrich-Schiller

Investigation of Physical Properties in II-VI
Investigation of Physical Properties in II-VI

Understanding Laser Beam Parameters Leads to Better System
Understanding Laser Beam Parameters Leads to Better System

Mirrors form images by reflecting light.
Mirrors form images by reflecting light.

... see how the light waves create images inside the human eye. Light rays bounce off objects in a very predictable way. For example, look at the diagram on the left below. Light rays from a flashlight strike a mirror at an angle of 60° as measured from the normal, an imaginary line perpendicular to the ...
“ waves, yielding a resultant irradiance that may deviate from the... component irradiances. r
“ waves, yielding a resultant irradiance that may deviate from the... component irradiances. r

Improved Intrapulse Raman Scattering Control via Asymmetric Airy
Improved Intrapulse Raman Scattering Control via Asymmetric Airy

... values of the bandwidth or σ are expected to give similar results because of the scaling properties of Airy pulses. The generalized nonlinear Schrödinger equation [18] was employed to analyze the propagation of Airy pulses in a large effective area fiber (LEAF) (see Methods in Ref. [19]). Figures 2( ...
Optical Properties of Plasmonic Ag/Ni Square Nanostructures
Optical Properties of Plasmonic Ag/Ni Square Nanostructures

Ultrafast Lasers Based on Quantum Dot Structures
Ultrafast Lasers Based on Quantum Dot Structures

Mystery of the double limit in homogenization of finitely or perfectly
Mystery of the double limit in homogenization of finitely or perfectly

\ 204 207 208 209 210 21g \ 221 /
\ 204 207 208 209 210 21g \ 221 /

The Double Etalon filter in Vernier configuration
The Double Etalon filter in Vernier configuration

< 1 ... 56 57 58 59 60 61 62 63 64 ... 223 >

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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