Theory of relativistic optical harmonic generation
... circularly polarized input beam [14]. Physically, this result can be understood from the perspective that under nonrelativistic conditions, each electron (whether bound or free) is induced to rotate in a circular orbit at the fundamental frequency of the incident laser light. For a bound electron, t ...
... circularly polarized input beam [14]. Physically, this result can be understood from the perspective that under nonrelativistic conditions, each electron (whether bound or free) is induced to rotate in a circular orbit at the fundamental frequency of the incident laser light. For a bound electron, t ...
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... This coherence volume determines the maximum domain size over which the fields can be considered correlated. In general an extended source, such as an incandescent filament, may have spectral properties that vary from point to point. It is convenient to discuss spatial correlations at each freque ...
... This coherence volume determines the maximum domain size over which the fields can be considered correlated. In general an extended source, such as an incandescent filament, may have spectral properties that vary from point to point. It is convenient to discuss spatial correlations at each freque ...
Chapter 25 - Heartland Community College
... • The most basic limitation on the length of the fiber-optic link is loss in the fiber, connectors, and splices • If the length is too great, the optical power level at the receiver will be insufficient to produce an acceptable signal-to-noise ratio • Given the optical power output of the transmitte ...
... • The most basic limitation on the length of the fiber-optic link is loss in the fiber, connectors, and splices • If the length is too great, the optical power level at the receiver will be insufficient to produce an acceptable signal-to-noise ratio • Given the optical power output of the transmitte ...
Superprism phenomena in planar photonic crystals
... studying the iso-frequency contours of a semiconductor waveguide PhC in the similar way as that of Kosaka, we succeeded in demonstrating the superprism effect in a planar configuration. The angular dispersion is almost an order of magnitude larger than that estimated by Lin and two orders of magnitu ...
... studying the iso-frequency contours of a semiconductor waveguide PhC in the similar way as that of Kosaka, we succeeded in demonstrating the superprism effect in a planar configuration. The angular dispersion is almost an order of magnitude larger than that estimated by Lin and two orders of magnitu ...
Regenerating evanescent waves from a silver superlens
... (LHMs) [2] is an example of a new exciting area in physics. A medium of this type [3] exhibits a unique negative refractive index in the design of negative effective permittivity and permeability simultaneously over certain frequency bands, and thus it is also termed a negative refractive-index medi ...
... (LHMs) [2] is an example of a new exciting area in physics. A medium of this type [3] exhibits a unique negative refractive index in the design of negative effective permittivity and permeability simultaneously over certain frequency bands, and thus it is also termed a negative refractive-index medi ...
Analysis of the detective quantum efficiency of
... The resulting combined MTF, T,,(f), is given by the magnitude of the Fourier transform of L,(x). It should be noted that the effect of fl,,““’as well as the fact that the transmittancesdecreaseas a function of ‘angle,actually reducesthe LSF width, and therefore improves the MTF at the ...
... The resulting combined MTF, T,,(f), is given by the magnitude of the Fourier transform of L,(x). It should be noted that the effect of fl,,““’as well as the fact that the transmittancesdecreaseas a function of ‘angle,actually reducesthe LSF width, and therefore improves the MTF at the ...
Ultrafast electronic dynamics in polyatomic molecules studied using
... and second harmonic beams. The relative polarization of two beams is parallel to each other. The pulse energies of the fundamental and the second harmonic are 0.43 and 0.37 mJ, respectively. When the ω and 2ω pulses overlap temporally and spatially, a bright filament (plasma column) with the length ...
... and second harmonic beams. The relative polarization of two beams is parallel to each other. The pulse energies of the fundamental and the second harmonic are 0.43 and 0.37 mJ, respectively. When the ω and 2ω pulses overlap temporally and spatially, a bright filament (plasma column) with the length ...