Inverse compton scattering1/19/2024 ![]() High energy and high brightness laser Compton backscattering gamma-ray source at IHEP. Guangyi Tang et al., The circular electron-positron collider beam energy measurement with Compton scattering and beam tracking method. Viti, ILC beam energy measurement by means of laser Compton backscattering. Xue et al., Generation of highly-polarized high energy brilliant \(\gamma \) - rays via laser-plasma interaction’. Zhang et al., Compact broadband high-resolution Compton spectroscopy for laser-driven high-flux gamma rays. Ma et al., Region-of-interest micro-focus computed tomography based on an all-optical inverse Compton scattering source. Luo et al., X-ray generation from slanting laser-Compton scattering for future energy-tunable Shanghai Laser Electron Gamma Source. (World Scientific Publishing Company, 2016) Suliman et al., “Gamma beam industrial applications at ELI-NP.” International Journal of Modern Physics: Conference Series, vol. Ohkuma et al., “Production of MeV photons by the laser Compton scattering using a far infrared laser at SPring-8.” Proceedings of EPAC. Our results could also provide a new way to generate wave sources with strong practical value, such as the terahertz waves, the ultra-violet (EUV) waves, or the mid-infrared beams. As an important application of our results in astrophysics, corresponding ground verification devices can be designed to perform experimental verifications on the prediction of the Sunyaev–Zeldovich (SZ) effect of the cosmic microwave background radiation. Therefore, with corresponding corrections of the cross section formula of the classical Compton scattering, the cross section of the linear or nonlinear microwave Compton scattering in the local space can be described accurately. ![]() Fortunately, with the Fourier expansion of Bessel functions, the local electromagnetic field can be considered as the superposition of a series of plane waves. Although Bessel functions can form a complete set of orthogonal basis, it is difficult to quantify them directly as fundamental wave functions. In the local space of the cavity, the electromagnetic field is expressed by Bessel functions. The new scheme of the energy measurement of the extremely high energy electron beam with the inverse Compton scattering between electrons and microwave photons requires the precise calculation of the interaction cross section of electrons and microwave photons in a resonant cavity.
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