1967
DOI: 10.1070/pu1967v009n06abeh003226
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Nonlinear Effects in a Plasma

Abstract: Doctor of Physicomathematical Sciences. Prior to 1956 his scientific interests centered on quantum electrodynamics. From 1957 to 1960 he elaborated the theory proposed by Wexler for coherent methods of charged particle acceleration. Since 1959 he has studied plasma physics and astrophysics. Tsytovich has been responsible, in particular, for investigations of the properties of relativistic plasma, the physics of turbulent plasma, and nonlinear effects in plasma.The original Russian text, first published by Nauk… Show more

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Cited by 203 publications
(156 citation statements)
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“…This method is similar to that described by Tsytovich. 16 The field perturbation δE and velocity perturbation δv along with the density perturbation δn represent the electrostatic component of the lower-band whistler mode, while the perpendicular components of the primed perturbations represent its electromagnetic component.…”
Section: Theoretical Analysis On Lower Band Cascadementioning
confidence: 99%
“…This method is similar to that described by Tsytovich. 16 The field perturbation δE and velocity perturbation δv along with the density perturbation δn represent the electrostatic component of the lower-band whistler mode, while the perpendicular components of the primed perturbations represent its electromagnetic component.…”
Section: Theoretical Analysis On Lower Band Cascadementioning
confidence: 99%
“…This process has been considered by several groups in the different cases: vacuum [12], electron plasma [13][14][15][16][17][18], magnetic fields of different configurations [19][20][21][22][23] and magnetized plasma [24][25][26]. The main point of the work we have done [26] was to extend the previous analysis by including the modified photon dispersion relation.…”
Section: Introductionmentioning
confidence: 99%
“…An influence of an external magnetic field on properties of leptons and their interactions becomes especially important when the field strength reaches the critical Schwinger value of B e = m 2 e /e = 4.41 × 10 13 Gauss, where m e is the electron mass and e is the elementary charge. Such fields are not accessible in accelerator experiments but can exist in strongly magnetized neutron stars called "magnetars" [1][2][3].…”
Section: Introductionmentioning
confidence: 99%
“…The first theory of plasma emission was put forth by Ginzburg & Zhelezniakov (1958) and many modifications and improvements have been made over the past six decades (Tsytovich 1967;Kaplan & Tsytovich 1968;Zheleznyakov & Zaitsev 1970;Melrose 1982;Goldman & Dubois 1982;Goldman 1983;Cairns 1987;Robinson & Cairns 1998;Mel'Nik et al 1999;Kontar 2001;Ledenev et al 2004;Li et al 2005Li et al , 2006aLi et al ,b, 2008aLi & Cairns 2013;. Although the essential theoretical framework based upon EM weak turbulence theory, which describes the entire process starting from the beam-generated Langmuir turbulence to the radiation generation, was available, complete numerical solution of the entire set of EM weak turbulence equations have not been done until quite recently, when Ziebell et al (2014aZiebell et al ( ,b,c, 2015 numerically solved the complete equations of EM weak turbulence theory for the first time.…”
Section: Introductionmentioning
confidence: 99%