The facility can operate in two modes: at high (MHz) repetition rate with flux and brilliance similar to that of a beamline at a large 2nd generation synchrotron, but with short 1. The absorption of multiple photons of the electromagnetic field by the charged particle causes the consequent emission of an X-ray or a gamma ray with energy comparable or higher with respect to the charged particle rest energy. A compact X-ray source based on inverse Compton scattering of a high-power laser on a high-brightness linac beam is described. 29 ICS based on a conventional accelerator has been under development since the 1990s, 1012 but its further. Non-linear inverse Compton scattering is a scattering process belonging to the category of light-matter interaction phenomena. REGIMES OF OPERATIONS OF INVERSE COMPTON SOURCES The fundamental elements of the Compton source are an electron beam and a laser, which interact to produce x rays or rays. Inverse Compton scattering (ICS) based on colliding an energetic electron beam with an intense laser pulse can generate high-flux energy-tunable quasi-monoenergetic short x/gamma-ray pulses, 1 with potential applications in biology, material science, and nuclear physics. Furthermore, differently from Compton scattering, this process is explicitly non-linear because the conditions for multiphoton absorption by the charged particle are reached in the presence of a very intense electromagnetic field, for example, the one produced by high-intensity lasers. The scattering kernel for Compton and inverse Compton scattering. This process is an inverted variant of Compton scattering since, contrary to it, the charged particle transfers its energy to the outgoing high-energy photon instead of receiving energy from an incoming high-energy photon. Non-linear inverse Compton scattering ( NICS), also known as non-linear Compton scattering and multiphoton Compton scattering, is the scattering of multiple low-energy photons, given by an intense electromagnetic field, in a high-energy photon ( X-ray or gamma ray) during the interaction with a charged particle, in many cases an electron. The linear inverse Compton scattering is decided by the first-order term with our analytical results. including the inverse-Compton scattering of a toy-model modi ed blackbody SED, the halo model formalism for the CIB and Compton-y elds, and the full, self-consistent calculation of the CIB monopole and its inverse-Compton-induced distortion. Electron-many photon scattering Picture of non-linear inverse Compton scattering.
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