Titlebook: Coherent Sources of XUV Radiation; Soft X-Ray Lasers an Pierre Jaeglé Textbook 2006 Springer-Verlag New York 2006 Transmission.interferomet

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The Driver as the Weak Point in Interactiontaneous interferograms from rapidly evolving physical objects. Furthermore, used in grazing incidence reflection, XUV radiation is a nondestructive surface probe thanks to the peculiar properties of optical constants in this spectral range.

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缺乏

Beginningsinterval shorter than the vacancy lifetime, would offer the population inversion necessary to generate a laser action. This pumping scheme was illustrated by order-of-magnitude calculations for a sodium vapor tube and for a solid copper rod, from which laser emission could be expected at 37.2 nm and 0.154 nm, respectively.

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Recombination Lasers that the production of plasmas suitable for recombination studies requires much less energy than collisional pumping. Thereby laboratories could work on X-ray lasers with nanosecond lasers providing a few tens of Joules per pulse only.

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Time-Resolution About 100 Picosecondstaneous interferograms from rapidly evolving physical objects. Furthermore, used in grazing incidence reflection, XUV radiation is a nondestructive surface probe thanks to the peculiar properties of optical constants in this spectral range.

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Textbook 2006nge. Thanks to new sources of coherent radiation - XUV-lasers and High Order Harmonics - the use of XUV radiation, for interferometry, holography, diffractive optics, non-linear radiation-matter interaction, time-resolved study of fast and ultrafast phenomena and many other applications, including medical sciences, is ubiquitous..

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Short Survey of XUV Emission Mechanisms and Sourcesadiation. This fluctuating designation reflects the various origins of a radiation pattern which, in other respects, exhibits singular optical properties marking it off from far-ultraviolet, on one side, and X-rays, on the other. The penetration length of XUV radiation is very small in almost all ma

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XUV Opticsnd UV optical know-how to XUV wavelengths. As we briefly stated at the very outset of these introductory chapters, XUV optical properties of condensed matter are to absorb most of the radiation along less than ̃1 μm length and to offer an extremely poor reflectance, viz. ≲10., at near normal inciden