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Kumar, Gaurav, Malik, Hitendra K.. (1402). Excitation of R- and L-waves by laser propagation through over-dense magnetized plasma and their verification. , 17(2), -. doi: 10.57647/J.JTAP.2023.1702.24
Gaurav Kumar; Hitendra K. Malik. "Excitation of R- and L-waves by laser propagation through over-dense magnetized plasma and their verification". , 17, 2, 1402, -. doi: 10.57647/J.JTAP.2023.1702.24
Kumar, Gaurav, Malik, Hitendra K.. (1402). 'Excitation of R- and L-waves by laser propagation through over-dense magnetized plasma and their verification', , 17(2), pp. -. doi: 10.57647/J.JTAP.2023.1702.24
Kumar, Gaurav, Malik, Hitendra K.. Excitation of R- and L-waves by laser propagation through over-dense magnetized plasma and their verification. , 1402; 17(2): -. doi: 10.57647/J.JTAP.2023.1702.24

Excitation of R- and L-waves by laser propagation through over-dense magnetized plasma and their verification

Journal of Theoretical and Applied Physics
مقاله 9، دوره 17، شماره 2، مرداد و شهریور 2023  XML
نوع مقاله: Scientific Research Manuscript
شناسه دیجیتال (DOI): 10.57647/J.JTAP.2023.1702.24
نویسندگان
Gaurav Kumar؛ Hitendra K. Malik email orcid
Department of Physics, Indian Institute of Technology Delhi, New Delhi, India.
چکیده
Laser-plasma interaction is a fascinating subject in view of its various applications in wave generation, particle acceleration, radiation generation, etc. The laser beam gets reflected at the vacuum-plasma interface if the plasma density is equal or larger than the critical density. However, in the presence of strong magnetic field in the order of kilo Tesla, the beam can travel some distance through over-dense plasma. Here E×B heating and pondermotive force play role for the laser beams to propagate through the over-dense plasma. In the present article, taking the external magnetic field along the propagation direction of the laser beam we have observed the R- and L- waves to be excited. The applied magnetic field is chosen in such way that the laser frequency 𝜔𝑙 falls between the electron cyclotron frequency 𝜔𝑐𝑒 and ion cyclotron frequency 𝜔𝑐𝑖. Under this situation, it generates only an R-wave. If the laser frequency is considered to be less than the ion cyclotron frequency ( 𝜔𝑙𝑎𝑠𝑒𝑟<𝜔𝑐𝑖) then an L-wave is additionally generated. In both the cases, an electrostatic disturbance is also formed with different but significant electric field amplitudes. We simulate these R- and L-waves in 1-D by using Particle-in-Cell (PIC) simulation using the EPOCH-4.17.10. Specifically, the electric and magnetic fields are studied that are associated with these waves, and the waves are verified based on the dispersion relation and the polarization studies.
کلیدواژه‌ها
Particle-In-Cell؛ R-wave؛ L-wave؛ Electron cyclotron frequency؛ Ion cyclotron frequency
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