2017
DOI: 10.1063/1.4981386
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Magnetic field effect on the self-focusing of an intense laser pulse interacting with a bulk medium of graphite nanoparticles

Abstract: The motivation of the present work is the study of self-focusing of an intense laser beam propagating through a magnetized bulk medium consisting of metallic nanoparticles. Using a perturbative method, the wave equation describing the nonlinear interaction of the intense laser beam with metallic magnetized nanoparticles is derived. Evolution of the laser spot size for the circular polarization with the Gaussian profile is considered. A graphite nanoparticle medium is introduced as a good candidate for self-foc… Show more

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Cited by 16 publications
(14 citation statements)
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“…An identical behavior to [39,40,52] for their investigation on size of nanoparticles has also been obtained in our scheme when height-to-radius ratio of the cylinders is evaluated on the THz field. Moreover, higher efficiency has been obtained in our case as compared to [39,40,[52][53][54]. Overall we can conclude that our results are in agreement with the observations of the other researchers [26,[35][36][37][38][39][40][52][53][54] while the amplitude of the emitted THz radiation and the efficiency in our case is much higher.…”
Section: Resultssupporting
confidence: 92%
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“…An identical behavior to [39,40,52] for their investigation on size of nanoparticles has also been obtained in our scheme when height-to-radius ratio of the cylinders is evaluated on the THz field. Moreover, higher efficiency has been obtained in our case as compared to [39,40,[52][53][54]. Overall we can conclude that our results are in agreement with the observations of the other researchers [26,[35][36][37][38][39][40][52][53][54] while the amplitude of the emitted THz radiation and the efficiency in our case is much higher.…”
Section: Resultssupporting
confidence: 92%
“…Moreover, higher efficiency has been obtained in our case as compared to [39,40,[52][53][54]. Overall we can conclude that our results are in agreement with the observations of the other researchers [26,[35][36][37][38][39][40][52][53][54] while the amplitude of the emitted THz radiation and the efficiency in our case is much higher. In addition, our proposal of a medium containing conductive nanocylinders which is illuminated by the hat-top lasers is quite effective based on which we can tune the emitted THz radiation in terms of its frequency, focus and intensity.…”
Section: Resultssupporting
confidence: 92%
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“…All the mentioned facts in this paragraph, may emphasize on the importance of considering restoring force in dynamical problems related to the interaction of EMWs with MNPs in the classical regime. In some studies related to the interaction of EMWs with systems including MNPs, in classical momentum equation, the restoring force which can predict the resonance frequency is considered [54][55][56][57][58][59][60][61][62][63][64][65][66][67] but surprisingly it is absent in the dynamics of the most of the studies related to the Drude-based problems and as it is mentioned in the previous paragraph, they considered only the free path limitation on the dynamics of conduction electrons in MNPs. In some studies related to the plasmonics of metallic nanostructures, for extraction of permittivity of system by Drude-based models, in the equation of motion of damped harmonic oscillation, the restoring force is considered and the related spring constant is determined by simulation [68][69][70][71][72][73].…”
Section: Introductionmentioning
confidence: 99%
“…( 2) is related to the restoration force caused by the separation of electrons from the positive background ions and parameter ξ is for adjustment of experimental data with the theory. In most of theoretical studies related to the interaction of laser beam with MNPs [33][34][35][36][37][38][39][40], in an ideal case of rigid body approximation in which all conduction electrons are replaced equally, its value is 1/3, however in the real situation, its value depending on the diameter of NP is less than 1/3 and it vanishes for the large particles which shows the transition to bulk medium situation [32]. E 1 is the electric field at the place of the first NP which is the sum of the incident wave electric field E L and interaction term E 2→1 where E 2→1 is the electric field at the place of first NP r 01 caused by the electric dipole moment of the second NP (p 2 = −Zer 2 , where Z = n 0 V is the total conduction electrons of each NP and V is the volume of NP) that can be represented as…”
Section: Introductionmentioning
confidence: 99%