By Baldassare Di Bartolo; John Collins
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Additional resources for Biophotonics: Spectroscopy, Imaging, Sensing, and Manipulation : [proceedings of the NATO Advanced Study Institute on Bio-Photonics: Spectroscopy, Imaging, Sensing, and Manipulation, Erice, Sicily, Italy 2 - 17 July 2009]
Rev. Lett. 93, 197401:1–4. PHOTONS AND PHOTON CORRELATION SPECTROSCOPY RALPH VON BALTZ* Institut für Theorie der Kondensierten Materie Universität Karlsruhe, D–76128 Karlsruhe, Germany 1. Introduction The majority of optical phenomena and even most of photonics can be well understood on the basis of Classical Electrodynamics. The Maxwell-Theory is perfectly adequate for understanding diffraction, interference, image formation, photonic-band-gap and negative-index materials, and even most nonlinear phenomena such as frequency doubling, mixing or short pulse physics.
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2 Steady states: In a steady state values of all observables (which don’t explicitly depend on time) are time-independent. Such states exist if Hˆ is time-independent ______ 2 Equation (6) holds not only for non-relativistic particles but also for photons. R. VON BALTZ 30 | (t ) e iEt / = | , Hˆ | E | . e. E = En, ψ = ψn. Pure and mixed states: Ket-vectors | describe so-called pure states which have zero entropy. They are – loosely speaking – analogs of the mechanical states with fixed q, p or the states of the classical EMF with fixed electrical and magnetic fields (“signals”).