Observation of Coherent Transition Radiation in Super-radiant Regime and its Application for Longitudinal Diagnostics

Bibliographic Details
Parent link:Charged & Neutral Particles Channeling Phenomena – Channeling 2024: Book of Abstracts of the 10th International Conference, Riccione (RN), Italy, September 8-13, 2024. P. 71.— .— Frascati: INFN, 2024
Other Authors: Kubankin A. S. Aleksandr Sergeevich, Baldin A. A. Anton Aleksandrovich, Klenin A. A. Artemiy, Kidanova E. A. Ekaterina Alekseevna, Bushmina E. A. Elizaveta Alekseevna, Kishin I. A. Ivan, Nozdrin M. A. Mikhail, Karataev P. V. Pavel Vladimirovich, Stuchebrov S. G. Sergey Gennadevich, Alekseev S. V. Sergey, Kocharian (Kocharyan) V. R. Vagan Rashidovich, Margaryan V. Vardan, Bleko V. V. Vitold Vladislavovich
Summary:Coherent TR (CTR) is generated when the radiation wavelength is comparable to or longer than the bunch length. In that case, all particles emit radiation more or less in phase, and the radiation intensity is proportional to a square of the number of particles in a bunch. However, if we have a sequence of bunches (a train) separated by a fixed distance from one another, the radiation is generated in a so called super-radiant regime. In that case the coherent radiation generated by individual bunches interfere. The radiation spectrum, in this case, is no longer continuous, but represents a set of very narrow lines separated by the bunch sequence frequency, which is proportional (if not equal to) the accelerating (RF) frequency. The width of those lines depends on the number of bunches in the train. For example, for 7000 bunches the relative monochromaticity can reach 10^{-4} - 10^{-7} depending of which radiation harmonic is observed. With modern interferometer based Fourier Transform spectrometers or gratings it is not possible to achieve sufficient resolution to precisely measure those lines
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Published: 2024
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Online Access:https://agenda.infn.it/event/39892/contributions/239699/
Format: Electronic Book Chapter
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=678818
Description
Summary:Coherent TR (CTR) is generated when the radiation wavelength is comparable to or longer than the bunch length. In that case, all particles emit radiation more or less in phase, and the radiation intensity is proportional to a square of the number of particles in a bunch. However, if we have a sequence of bunches (a train) separated by a fixed distance from one another, the radiation is generated in a so called super-radiant regime. In that case the coherent radiation generated by individual bunches interfere. The radiation spectrum, in this case, is no longer continuous, but represents a set of very narrow lines separated by the bunch sequence frequency, which is proportional (if not equal to) the accelerating (RF) frequency. The width of those lines depends on the number of bunches in the train. For example, for 7000 bunches the relative monochromaticity can reach 10^{-4} - 10^{-7} depending of which radiation harmonic is observed. With modern interferometer based Fourier Transform spectrometers or gratings it is not possible to achieve sufficient resolution to precisely measure those lines
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