By M. L. Ter-Mikayelyan (auth.), Helmut Wiedemann (eds.)
ISBN-10: 140200267X
ISBN-13: 9781402002670
ISBN-10: 940100367X
ISBN-13: 9789401003674
A complete survey of modern theoretical and experimental development within the zone of electron-photon interplay and dense media. A state of the art dialogue of radiation construction, with descriptions of latest rules and applied sciences that increase the construction of X-rays within the type of channelling, transition and parametric X-ray construction. development in electron beam physics to provide sub-picosecond electron bunches from low-energy linear accelerators give the opportunity to provide coherent, excessive brightness, submillimeter radiation and sub-picosecond X-ray pulses. Micro-undulators within the kind of bent crystalline constructions carry nice promise as destiny X-ray sources.
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Extra resources for Electron-Photon Interaction in Dense Media
Example text
The presented relations allow one to consider atomic electrons as being free during PB process and to neglect the Compton shift of the frequency of emitted photons. It is very important that the electron coordinates r s are approximately constant during the process of relativistic electron interaction with an atom. In the formula (2) A is the vector potential of electromagnetic field. Equation where following from eqs. (1) and (2) allows us to take into account both individual and collective contributions of medium electrons to the process of elastic scattering of virtual photons forming the Coulomb field of a fast particle.
Here § = 1§lci , where ci is the unit vector specifying the deflection of crystal microblocks from the average direction §o = (§). The vector §o is perpendicular to the crystal plane. It is rotated through the angle (7r /2 - BB) about the beam axis. The diffraction plane is determined by vectors ii and§. j€(1 - cos 2B) , (21) where ii' is the vector specifying the direction of the diffracted photon. j€ (22) A number of mosaic crystal blocks that satisfy the equation . B _ (§ii) _ [nxgx + nygy + nzgz] sm - I§I - I§I (23) meet this requirement.
0. ° "".. ' ,. '. -------. J c Figure 25. Channeling-radiation spectra for 54-MeV electrons incident along the (III) plane in LiH (part a) and LiD (part b). The location of the tunnelingtransition peak is indicated by the arrows; it is clearly present in LiD {from Bennan et al. [l8]} . ', :0. e. Parke. I. L. et al. (1970) Phys. Rev. Lett. 25, 5. 2. D. (1975) Phys. Rev. A 11,736. 3. (1976) Phys. Lett. 57,17. 4. Terhune, RW. H. (1977) Appl. Phys. Lett. 30, 265. 5. Alguard, MJ. et al. (1979) Phys.
Electron-Photon Interaction in Dense Media by M. L. Ter-Mikayelyan (auth.), Helmut Wiedemann (eds.)
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