By Pierre Jaeglé
ISBN-10: 0387230076
ISBN-13: 9780387230078
Severe ultraviolet radiation, also known as tender X-rays or XUV, bargains very precise optical houses. The X-UV refractive index of subject is such that standard mirrored image can't happen on polished surfaces while beam transmission via one micrometer of virtually all fabrics reduces to 0. accordingly, it has lengthy been a tough activity to visualize and to enforce units designed for complicated optics experiments during this wavelength diversity. because of new assets of coherent radiation - XUV-lasers and excessive Order Harmonics - using XUV radiation, for interferometry, holography, diffractive optics, non-linear radiation-matter interplay, time-resolved examine of speedy and ultrafast phenomena and plenty of different functions, together with scientific sciences, is ubiquitous.
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Extra info for Coherent Sources of XUV Radiation: Soft X-Ray Lasers and High-Order Harmonic Generation (Springer Series in Optical Sciences)
Example text
7. Reflectivity of silica and gold versus photon energy for the same glancing angle smaller, in both cases, than the critical angle [35]. Fig. 8. Reflectivity of silica and gold versus photon energy for the critical incidence angle of each material [35]. 47) 2 viz. 48) As shown previously, the 45◦ -incidence reflectance at a single interface is much too small to be useful to build polarizers. But due to the fact that the magnitude of θB does not depend much on the nature of the material, multilayer mirrors can provide high linear polarization of intense beams reflected near 45◦ -incidence.
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This theorem states that the (equal-time) complex degree of coherence is equal to the amplitude of the diffraction pattern around this point, of an aperture of the same size as the light source. 14) may be neglected. 19) in calculations. 5 shows the main components used in the j (r1 , r2 ) calculation. Let us consider a couple of source points S1 (r1 )and S2 (r2 ), in the source area (σ). The vectors r1 and r2 are vectorial coordinates of S1 and S2 . 16). All contributions are then summed, giving the total intensities in P1 and P2 .
Coherent Sources of XUV Radiation: Soft X-Ray Lasers and High-Order Harmonic Generation (Springer Series in Optical Sciences) by Pierre Jaeglé
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