By Bhowmick D., Davison A.C.
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G. a sapphire plate. A desired wavelength of this continuum may be used together with radiation of the initial wavelength of 790 nm for a DFG process in a nonlinear crystal. Since energy conservation has to be fulfilled, the chosen wavelength has to be larger than 790 nm. In this context it is convenient to refer to the different beams coupled into the crystal as seed and pump beam, respectively, see Fig. 8. A part of the energy of one photon from the pump beam is used for amplification of the seed beam by stimulated emission.
Exp. 19, 4464–4471 (2011). 004464 35. S. Siegmann, Lasers (University Science Books, USA, 1986) 36. Ch. , Compact, high-throughput expansion-compression scheme for chirped pulse amplification in the 10 fs range. Opt. Commun. 120, 321–324 (1995). 1016/00304018(95)00494-S 37. A. , Sub-10-fs mirror-dispersion-controlled Ti:sapphire laser. Opt. Lett. 20, 602–604 (1995). 000602 References 27 38. , Femtosecond time-resolved photoelectron spectroscopy. Chem. Rev. 104, 1719–1758 (2004). 1021/cr020683w 39.
571743 21. Fritz Kurt Kneubühl and Markus Werner Sigrist. Laser. Vierweg + Teubner (2008) 22. F. Krausz et al. ), Ultrafast Optics IV (Springer, LLC, New York, 2004) 23. M. D. thesis. Ruperto-Carola University of Heidelberg, Germany. URN: urn:nbn:de:bsz:16-heidok-100544 (2009) 24. A. Krupp, Untersuchung der Pulsdauer und Langzeitstabilisierung eines Hohlfaserkompressors, BA thesis. Ruperto-Carola University of Heidelberg, Germany (2011) 25. M. , Sub-20-fs, kilohertz-repetition-rate Ti:sapphire amplifier.
A Laplace mixture model for identification of differential expression in microarray experiments (200 by Bhowmick D., Davison A.C.