Classical Nonlinear Compton Scattering with Strong Bessel Laser Beams

Descripción del Articulo

In this paper, the Hartemann-Kerman approach is numerically examined with the implementation of Bessel pulses that dramatically changes the morphology of yielded radiation. For this end it is used the covariant Bessel pulse given by J (Φ/ Δ) with J the integer-order of Bessel function whereas Φ and...

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Detalles Bibliográficos
Autor: Nieto-Chaupis, Huber
Formato: artículo
Fecha de Publicación:2022
Institución:Universidad Autónoma del Perú
Repositorio:AUTONOMA-Institucional
Lenguaje:inglés
OAI Identifier:oai:repositorio.autonoma.edu.pe:20.500.13067/1808
Enlace del recurso:https://hdl.handle.net/20.500.13067/1808
https://doi.org/10.1109/PPC40517.2021.9733051
Nivel de acceso:acceso restringido
Materia:Laser theory
Numerical analysis
Free electron lasers
Power lasers
Scattering
Quantum mechanics
Morphology
https://purl.org/pe-repo/ocde/ford#2.02.04
Descripción
Sumario:In this paper, the Hartemann-Kerman approach is numerically examined with the implementation of Bessel pulses that dramatically changes the morphology of yielded radiation. For this end it is used the covariant Bessel pulse given by J (Φ/ Δ) with J the integer-order of Bessel function whereas Φ and Δ the invariant product and the pulse width respectively. In concrete this paper is focused at the emitted radiation by a free electron that depends on the pulse amplitude as well as the normalized Doppler-shifted frequency. The numerical analysis yields that a fully nonlinear spectrum that to some extent can be interpreted as of GeV electron to interact simultaneously with a laser power of 1.36 keV and a peak intensity of order of 1000 W/cm 2 . Therefore, the usage of Bessel-like pulses would reveal the departure of a classical view to one based at electron-photon interaction as dictated by the quantum mechanics rules.
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