By Professor Dr. Werner Lauterborn, Dr. rer. nat. Thomas Kurz, Dipl.-Phys. Martin Wiesenfeldt (auth.)
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Additional resources for Coherent Optics: Fundamentals and Applications
Light in the large range in between these two limiting cases is called partially coherent. Therefore, the following cases are distinguished (-r :t:. 0, lr(O)I = 1): lr( -r)l - 1 completely coherent, 0 ::;; lr(-r)l ::;; 1 partially coherent, lr( -r)l - 0 completely incoherent. Many natural and artificial light sources have a monotonously decreasing contrast function; for instance, the light from a spectral lamp. 6 shows typical graphs of the field amplitude, the self coherence function, and the contrast function for light from a mercury lamp.
Progress in Optics, Vol. : "Coherence and indistinguishability", Opt. Lett. 16, 1882-1883 (1991) Marathay A. , T. Kuga, M. Baba, M. Matsuoka: "Measurement of ultrafast optical pulses with two-photon interference", Opt. Lett. 18, 900-902 (1993) Ou, Z. , E. C. Gage, B. E. Magill, L. Mandel: "Fourth-order interference technique for determining the coherence time of a light beam", J. Opt. Soc. Am.
Both reflected beams are divided again into two by the beam splitter, whereby one beam from each mirror propagates to a screen. The idea of this arrangement is to superimpose a light wave with a time-shifted copy of itself. We now set out for a mathematical description. On the screen, we have a superposition of two waves, E 1 and E 2 . Let E 1 be the light wave that reaches the screen via the first mirror and E 2 the one that reaches the screen via the movable mirror. 1) The wave E 2 thus has to start earlier to reach the screen at time t because of the additional path oflength 2d.
Coherent Optics: Fundamentals and Applications by Professor Dr. Werner Lauterborn, Dr. rer. nat. Thomas Kurz, Dipl.-Phys. Martin Wiesenfeldt (auth.)