2010
DOI: 10.1063/1.3480106
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Power law decay of harmonic spectra in ultrarelativistic laser-plasma interactions

Abstract: Imaging spectroscopy diagnosis of internal electron temperature and density distributions of plasma cloud surrounding hydrogen pellet in the Large Helical Device Rev. Sci. Instrum. 83, 093506 (2012) Density and temperature effects on Compton scattering in plasmas Phys. Plasmas 19, 093115 (2012) Synchronized operation by field programmable gate array based signal controller for the Thomson scattering diagnostic system in KSTAR Rev. Sci. Instrum. 83, 093505 (2012) Microwave scattering from laser spark in air

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Cited by 4 publications
(3 citation statements)
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“…We note in passing that all three signatures of this spectrum, namely plasma emission at ω p and its harmonics, spectral decay with p = 5/3 and a cut-off in a range typically 100 m c 300 are consistent with the BOR spectra reported in references [6] and [9]. Furthermore, the localized electrostatic structures in their strongly turbulent state, the so-called soliton, is consistent with the trajectory crossings, as shown in figure 2.…”
Section: Plasma and Harmonic Emission From Relativistic Electrons Persupporting
confidence: 71%
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“…We note in passing that all three signatures of this spectrum, namely plasma emission at ω p and its harmonics, spectral decay with p = 5/3 and a cut-off in a range typically 100 m c 300 are consistent with the BOR spectra reported in references [6] and [9]. Furthermore, the localized electrostatic structures in their strongly turbulent state, the so-called soliton, is consistent with the trajectory crossings, as shown in figure 2.…”
Section: Plasma and Harmonic Emission From Relativistic Electrons Persupporting
confidence: 71%
“…These structures were identified as sources of emission at the plasma frequency and at its harmonics. Particle-in-cell simulations where used to explore the harmonic power decay in ultrarelativistic laser-plasma interactions by BOR [7][8][9] and spectral decays characterized by prevalent indexes p = 5/3 were found and, less commonly, p = 4/3 in p-polarized light incident on dense plasma targets. When the incident laser pulse is normal to the plasma surface, the spectrum is invariantly characterized by a power law described by the index 8/3, regardless of the combination of parameters (a 0 , n e /n c ), as shown in figure 1(a) [9].…”
Section: Plasma Effectsmentioning
confidence: 99%
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