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15] J. Hecht, Semiconductor Sources advance Deeper into the Ultraviolet, Laser Focus World February 2005. p. 95. E. D. , Springer-Verlag, Berlin, 1976, p. 29.  J. Tirrel, Cavity Ring-Down Spectroscopy Makes the Leaps out of the Laboratory, Opto & Laser Europe, October 2004, p. 17.  A. G. Deacon, Rev. Sci. Instrum. 59, 2544 (1988).  J. -S. L. Hall, J. Opt. Soc. Am. B 15, 6 (1998).  M. Ducloy, Europhys. News March/April 2004, p. 40.  Laser Focus World, Issues January and February 2005, p.
If 2 probe beams are used, the emitted photon can be shifted to a wavelength shorter than the probe beam. This process is known as coherent anti resonant Raman scattering and can be mush stronger than Raman scattering. All of the spectroscopic techniques described above depend on the availability of a probe source. The simplest probe source is a black body radiator, such as a tungsten filament lamp or even the sun. Black body sources produce a wide range of wavelengths so they can be used in wavelength scanning systems.
17.  A. G. Deacon, Rev. Sci. Instrum. 59, 2544 (1988).  J. -S. L. Hall, J. Opt. Soc. Am. B 15, 6 (1998).  M. Ducloy, Europhys. News March/April 2004, p. 40.  Laser Focus World, Issues January and February 2005, p. 83 and 69, respectively, for the latest data, and previous corresponding Issues for old data RELAXATION AND DECOHERENCE: WHAT’S NEW? RALPH V. BALTZ Institut f¨ ff¨r Theorie der Kondensierten Materie Universitat ¨ Karlsruhe, D–76128 Karlsruhe, Germany ∗ 1. Introduction Relaxation and decoherence are omnipresent phenomena in macro–physics − Relaxation: evolution of an initial state towards a steady state.