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chapter 6—light and telescopes
chapter 6—light and telescopes

TEP Zeeman Effect with a variable magnetic system and a CMOS
TEP Zeeman Effect with a variable magnetic system and a CMOS

... As early as 1862, Faraday investigated whether the spectrum of coloured flames changes under the influence of a magnetic field, but without success. It was not until 1885 that Fievez from Belgium was able to Fig. 3: Magnetic flux density B in the centre of the gap without Cd-lamp as demonstrate an e ...
CHAPTER 6—LIGHT AND TELESCOPES
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Determination of guided-mode resonances in photonic crystal slabs
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High visibility six-photon entanglement Magnus R˚ admark
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... Such states can be applied to e.g. decoherence-free encoding, quantum communication without sharing a common reference frame, quantum telecloning, secret sharing and remote state preparation schemes. In the experimental implementation we use a single source of entangled photon pairs and extract the ...
Results from an Extremely Sensitive Rayleigh
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... For the lowest altitude channel, Raman scattering will be observed rather that Rayleigh or Mie. Raman scattering differs greatly from the first two types because it involves inelastic scattering between the incident light and particle scatterer. In Raman scattering, the incident light excites the at ...
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Narrowband photon pair generation and waveform reshaping

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... demonstrated by an excellent correspondence between experimental results and theoretical calculations. The high dynamic range and signal-to-noise ratio is due to the fact that the total signals (∼10 nA at 10 mW laser power) are 3−4 orders of magnitude higher than the noise level of typical nanopores ...
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A method for characterizing longitudinal chromatic aberration of

... cooled to – 308C). The camera now gives an ‘image’ in which the horizontal axis represents wavelength, the vertical axis represents the axial z-position of the plane mirror and the image intensity denotes the intensity of the axial response. The z-motion axis was calibrated interferometrically and s ...
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Transverse and longitudinal angular momenta of light

... light. If the mean momentum of the beam (in units of  per photon) can be associated with its mean wave vector k , then such beam carries the corresponding spin AM S = σ k / k . Here σ is the helicity parameter, i.e., the degree of circular polarization. In turn, the orbital AM of a uniformly-polari ...
Semiconductor Lasers: Device Physics and Applications
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... Our group fabricates precision optics via the injection molding process. Specifications for these optics typically have tolerances at the sub-micron level. To successfully fabricate such parts, it becomes critical to have a greater understanding and control of all the processes involved in molding o ...
Chapter 36 . Optical Properties of Semiconductors
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... Careful consideration was given in choosing the materials used as the low and high index optical layers in the FPI as well as their deposition processes to insure compatibility with those required for patterning the electrodes and the wafers. Optical layers, without further treatment, would not surv ...
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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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