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Coherent polarization radiation from crystals irradiated with relativistic charged particles
Institution:1. Guangdong Provincial Key Laboratory of Brain Connectome and Behavior, CAS Key Laboratory of Brain Connectome and Manipulation, the Brain Cognition and Brain Disease Institute (BCBDI), Shenzhen Key Laboratory of Translational Research for Brain Diseases, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen-Hong Kong Institute of Brain Science-Shenzhen Fundamental Research Institutions, Shenzhen 518055, China;2. State Key Laboratory of Robotics, Shenyang Institute of Automation, Chinese Academy of Sciences, Shenyang 110016, China;3. Institutes for Robotics and Intelligent Manufacturing, Chinese Academy of Sciences, Shenyang 110169, China;4. University of Chinese Academy of Sciences, Beijing 100049, China;5. Institute of Neuroinformatics, the University of Zürich and Swiss Federal Institute of Technology (ETH), Zurich CH-8057, Switzerland;6. European Molecular Biology Laboratory (EMBL), Monterotondo 00015, Italy;7. School of Systems Science, Beijing Normal University, Beijing 100875, China;1. Department of Neurobiology & Anatomy, McGovern Medical School, University of Texas, Houston, TX 77030, USA;1. BBS Program, Harvard Medical School, 220 Longwood Avenue, Boston, MA 02115, USA;2. Department of Neurology, F.M. Kirby Neurobiology Center, Boston Children’s Hospital, 300 Longwood Avenue, Boston, MA 02115, USA;3. Program in Neuroscience, Harvard Medical School, 220 Longwood Avenue, Boston, MA 02115, USA;1. Huygens-Kamerlingh Onnes Laboratory, Leiden Institute of Physics, Leiden University, P.O. Box 9504, 2300 RA Leiden, The Netherlands;2. SPECS GmbH, Voltastrasse 5, D-13355 Berlin, Germany;3. IBM T.J. Watson Research Center, 1101 Kitchawan Road, P.O. Box 218, Yorktown Heights, NY 10598, USA
Abstract:When polarization radiation (polarization bremsstrahlung) occurs in a crystal, the radiation becomes coherent in X-ray wavelengths. This radiation, called coherent polarization radiation (CPR) in this paper, is considered as a possible compact X-ray source because CPR is intense, monochromatic, tunable, small background, and easy to extract. We present a simple theory of CPR with emphasis on its relation to Cherenkov radiation and transition radiation. Various properties of CPR are also discussed.
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