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Electromagnetic forces for an arbitrary optical trapping of a spherical
Electromagnetic forces for an arbitrary optical trapping of a spherical

mirrors, combination of mirrors and catadioptric systems
mirrors, combination of mirrors and catadioptric systems

Superluminal group velocity in an anisotropic metamaterial
Superluminal group velocity in an anisotropic metamaterial

Technical Information on Optics
Technical Information on Optics

Location of Cardinal Points from the ABCD Matrix for the General
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The Physics of the Optical Fibre
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... bed. In fact, the link from the UK to the English Channel Islands is achieved directly without any submerged regenerators. The world's first international optical fibre submarine cable was laid by BT in 1986 between the UK and Belgium. It is 112Km in length and has only 3 regenerators. BT was a majo ...
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... eol and mol optical switches.  FIBERTech RoMack’s switch has proven effective in a number of  complex applications including  spectroscopy (mol series), laser scan  microscopy, multichannel optical  performance monitoring, fiber bragg  sensors, testing of fiber optical cables and  environmental trac ...
Transmisi Optik Pertemuan 10
Transmisi Optik Pertemuan 10

... • Uses a much smaller junction area than that in LED and the concentration of injected carriers (holes and electrons) is much higher • Can produce large amount of optical output power (20 to 100 mW) with a very narrow output spectrum • Produces a very tightly directed beam with small NA which can be ...
Microsoft Word Format - McMaster University > ECE
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Encoding and Decoding Non-separable States of Polarization and Spatial Mode of Single Photons
Encoding and Decoding Non-separable States of Polarization and Spatial Mode of Single Photons

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Excited States, Lasers and Non-Linear Optics

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219_cha.pdf

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Reversing Light: Negative Refraction
Reversing Light: Negative Refraction

... necessary for a passive material. This briefly stated argument shows why the material Veselago pondered years ago is so unique: the index of refraction is negative. A negative refractive index implies that the phase of a wave advancing through the medium will be negative rather than positive. As Ves ...
TIE-29 Refractive Index and Dispersion
TIE-29 Refractive Index and Dispersion

... The determination of the coefficients was performed for all glass types on the basis of precision measurements by fitting the dispersion equation to the measurement values. The ­coefficients are listed in the data sheets. The dispersion equation is only valid within the spectral region in which refr ...
TIE-29 Refractive Index and Dispersion
TIE-29 Refractive Index and Dispersion

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Nonlinear optical properties of nanocomposite materials

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WHAT IS THE OPTICAL COMPUTING?

... vertical cavity surface emitting laser diode that emits light in a cylindrical beam vertically from the surface of a fabricated wafer. ...
Multidimensional and inhomogeneity effects on scattering
Multidimensional and inhomogeneity effects on scattering

Ultrahigh Precision Absolute and Relative Rotation Sensing using
Ultrahigh Precision Absolute and Relative Rotation Sensing using

... ∆φ = 4π mAΩ / h , where m is the rest mass, can be derived from eqn. 2 by substituting matter wave wavelength by the so-called Compton wavelength. In presence of optical waves in Sagnac interferometer consisting of a refractive medium, the generic phase shift ∆φo in eqn. 2 is independent of the refr ...
Polarization of x-gamma radiation produced by a Thomson and
Polarization of x-gamma radiation produced by a Thomson and

IOSR Journal of Applied Physics (IOSR-JAP)
IOSR Journal of Applied Physics (IOSR-JAP)

... It provides a measure of disorder in the amorphous and crystalline solids [22]. In amorphous materials, tructural disorder dominates and this could be due to the presence of structural defects like dangling bonds or non bridging oxygen atoms [23]. In borate based glass network, the higher the concen ...
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Birefringence



Birefringence is the optical property of a material having a refractive index that depends on the polarization and propagation direction of light. These optically anisotropic materials are said to be birefringent (or birefractive). The birefringence is often quantified as the maximum difference between refractive indices exhibited by the material. Crystals with asymmetric crystal structures are often birefringent, as are plastics under mechanical stress.Birefringence is responsible for the phenomenon of double refraction whereby a ray of light, when incident upon a birefringent material, is split by polarization into two rays taking slightly different paths. This effect was first described by the Danish scientist Rasmus Bartholin in 1669, who observed it in calcite, a crystal having one of the strongest birefringences. However it was not until the 19th century that Augustin-Jean Fresnel described the phenomenon in terms of polarization, understanding light as a wave with field components in transverse polarizations (perpendicular to the direction of the wave vector).
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