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Numerical Study of Wave Propagation in Uniaxially Anisotropic
Numerical Study of Wave Propagation in Uniaxially Anisotropic

Surface Electromagnetic Waves Thermally Excited: Radiative Heat
Surface Electromagnetic Waves Thermally Excited: Radiative Heat

... charge oscillations. It was shown in [2] that the van der Waals force between a molecule and a surface can become repulsive depending on the relative position of the molecule and the surface resonances. Enhanced scattering due to the resonant excitation of surface charges has also been demonstrated ...
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Part A One reason that Fraunhofer diffraction is relatively easy to
Part A One reason that Fraunhofer diffraction is relatively easy to

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High-order Harmonic Generation in Gases (HHG)
High-order Harmonic Generation in Gases (HHG)

... Link time / frequency • A LASER pulse is made of many wavelengths inside a spectral width Δω • Its duration Δt is not « free »: Δω ∙ Δt ≥ ½ • Δω ∙ Δt = ½: Gaussian envelop – pulse « limited by Fourier transform » • If the spectral components ω are not in phase, the pulse is lengthened: there is a ch ...
Notes II for phy132
Notes II for phy132

Plane Waves and Wave Propagation
Plane Waves and Wave Propagation

[SSM] True or false: (a) Maxwell`s equations apply only to electric
[SSM] True or false: (a) Maxwell`s equations apply only to electric

... The intensity of the sunlight striking Earth’s upper atmosphere is 1.37 kW/m2. (a) Find the rms values of the magnetic and electric fields of this light. (b) Find the average power output of the Sun. (c) Find the intensity and the radiation pressure at the surface of the Sun. Picture the Problem We ...
Diffraction of dust acoustic waves by a circular cylinder (Physics of
Diffraction of dust acoustic waves by a circular cylinder (Physics of

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This chapter is the second on electromagnetic waves. We begin with

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Lecture-8-Optics

... 1  cos2km x  2mt  I  E02  4E01 cos 2 km x  mt   2 E01 ...
Electromagnetic waves
Electromagnetic waves

... a handle on, for a number of reasons. First, the things that are oscillating are electric and magnetic fields, which are much harder to see (which is an ironic statement, considering that we see with light, which is an electromagnetic wave). Second, the fields can have components in various directio ...
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EM Waves

... Examples Unpolarized light can be thought of as a collection of many separate light waves, each linearly-polarized in different and random directions. A The intensity is reduced to 1/2 by the first polarizer: I out = (I in cos2 θ) avg = ...
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(a) n r from the center is an example of a

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Potential Energy - McMaster Physics and Astronomy

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Measuring the Speed of Light: Roemer

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chapter - WebAssign

... rotating it 90, we can produce a wave linearly polarized in the horizontal direction, rather than in the vertical direction. By rotating the laser through some other angle we can get polarization in any direction perpendicular to the beam. Most natural light sources and many lasers have random pola ...
Electromagnetic Waves
Electromagnetic Waves

... be B ⫽ E/c ⫽ 5 ⫻ 10⫺6 T. These values then allow us to calculate the energy density, from Equation (19.4) to be 2 ⫻ 10⫺5 J/m3. Alternatively we can use Equation (19.5) directly to find the same result. The Poynting vector then has an amplitude given by Equation (19.6) to be Smax ⫽ (PE/V)c ⫽ 6000 W/m ...
Polarimetry in astronomy
Polarimetry in astronomy

... Measuring Polarization • This means measuring flux differences along different electric field oscillation planes • In principle one would be able to measure linear polarization simply rotating a linear polarizer and measuring the light intensity as a function of rotation angle. In the presence of p ...
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Coherent Optical Photons from Shock Waves in Crystals * Marin Soljacˇic´,
Coherent Optical Photons from Shock Waves in Crystals * Marin Soljacˇic´,

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Nature and Properties of Electromagnetic Waves

Surface excitation of hypersound in piezoelectric crystals by
Surface excitation of hypersound in piezoelectric crystals by

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Coherence (physics)

In physics, two wave sources are perfectly coherent if they have a constant phase difference and the same frequency. It is an ideal property of waves that enables stationary (i.e. temporally and spatially constant) interference. It contains several distinct concepts, which are limiting cases that never quite occur in reality but allow an understanding of the physics of waves, and has become a very important concept in quantum physics. More generally, coherence describes all properties of the correlation between physical quantities of a single wave, or between several waves or wave packets. Interference is nothing more than the addition, in the mathematical sense, of wave functions. A single wave can interfere with itself, but this is still an addition of two waves (see Young's slits experiment). Constructive or destructive interferences are limit cases, and two waves always interfere, even if the result of the addition is complicated or not remarkable.When interfering, two waves can add together to create a wave of greater amplitude than either one (constructive interference) or subtract from each other to create a wave of lesser amplitude than either one (destructive interference), depending on their relative phase. Two waves are said to be coherent if they have a constant relative phase. The amount of coherence can readily be measured by the interference visibility, which looks at the size of the interference fringes relative to the input waves (as the phase offset is varied); a precise mathematical definition of the degree of coherence is given by means of correlation functions. Spatial coherence describes the correlation (or predictable relationship) between waves at different points in space, either lateral or longitudinal. Temporal coherence describes the correlation between waves observed at different moments in time. Both are observed in the Michelson–Morley experiment and Young's interference experiment. Once the fringes are obtained in the Michelson–Morley experiment, when one of the mirrors is moved away gradually, the time for the beam to travel increases and the fringes become dull and finally are lost, showing temporal coherence. Similarly, if in Young's double slit experiment the space between the two slits is increased, the coherence dies gradually and finally the fringes disappear, showing spatial coherence.
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