Download Parametric X-Ray Radiation in Crystals: Theory, Experiment by Vladimir G. Baryshevsky, Ilya D. Feranchuk, Alexander P. PDF

By Vladimir G. Baryshevsky, Ilya D. Feranchuk, Alexander P. Ulyanenkov

This systematic and entire monograph is dedicated to parametric X-ray radiation (PXR). This radiation is generated by way of the movement of electrons within a crystal, wherein the emitted photons are diffracted via the crystal and the radiation depth significantly depends on the parameters of the crystal constitution. these days PXR is the topic of diverse theoretical and experimental stories through the international. the 1st a part of the publication is a theoretical therapy of PXR, which incorporates a new method of describe the radiation strategy in crystals. the second one half is a survey of PXR experimental effects and the potential purposes of PXR as a device for crystal constitution research and a resource of tunable X-ray radiation.

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12, 1149 (1970) 38, 40 31. A. Porai-Koshitz: Practical Course for X-ray Structure Analysis, vol 2 (Fizmatgiz, Moscow 1968) 33, 34, 36, 38 42 2 Classical Theory of Radiation 32. P. A. Rukhadze: Electromagnetic Properties of Plazma (Gosatomizdat, Moscow 1961) 19, 20 33. L. Ter-Mikaelian: High Energy Electromagnetic Processes in Condensed Media (in Russian: AN ArmSSR, Yerevan 1969) (in English: Wiley, New York 1972) 20 34. F. J. 1 Quantum Electrodynamics for Radiation Processes in Crystals Previous chapters demonstrate a close analogue between the theory of parametric X-ray radiation (PXR) in thin crystals and the kinematic theory of X-ray diffraction, which is used in X-ray analysis, viz.

Chumakov, O. Leupold, R. A. N. Salashchenko: Hyperfine Interact. 141/142, 119 (2002) 39 4. A. Authier: Dynamical Theory of X-ray Diffraction (Oxford University Press, New York 2001) pp 3–26 21, 22 5. N. M. S. Fadin: Radiation from Relativistic Electrons (Atomizdat, Moscow 1973) 20, 21 References 41 6. N. M. M. Strakhovenko: Electromagnetic Processes at High Energies in Oriented Single Crystals (World Scientific, Singapore 1998) 20, 21 7. G. Baryshevsky: Dokl. Akad. Sci. G. D. Feranchuk: Proc. XXI Conf.

1. Wave fields for the calculation of the transition radiation intensity (s) Wnω J ∂2N = . 18) To illustrate the above-described method, the intensity of transition radiation [21] from a constantly moving charged particle crossing the boundary between two different media is calculated below. Let us consider a semi-infinite homogeneous medium with a surface at z = 0, where the z-axis is parallel to the inward normal N to the surface. The medium possesses a dielectric permittivity and the velocity of a charged particle is parallel to the surface normal v N (Fig.

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