Abstract:The revision of the previous theory of the shear Alfven vortices in a homogeneous plasma is given. The necessity of such a revision is due to the fact that in the previous papers the solutions were not matched adequately on the singular line of the vortex so that these solutions do not satisfy to the charge conservation law. The influence of the magnetic viscosity on the character of the admitted discontinuities in the shear Alfven vortices is studied. The nonlinear equations of the shear Alfven waves in the u… Show more
“…This exercise has been carried out by Mikhailovskii et al 14 and Liu and Horton, 15 and explicit expressions for the various constants had been found.…”
The linear and nonlinear properties of drift-ballooning modes in the presence of an equilibrium electric field and stationary charged dust grains are examined. It is found that the presence of these two contribute to the stability of the ballooning mode. Furthermore, the nonlinear coupling between finite amplitude drift-ballooning modes gives rise to different types of coherent vortex structures, which can affect the transport properties of an inhomogeneous magnetized plasma. The relevance of the investigation to laboratory and astrophysical plasmas is discussed.
“…This exercise has been carried out by Mikhailovskii et al 14 and Liu and Horton, 15 and explicit expressions for the various constants had been found.…”
The linear and nonlinear properties of drift-ballooning modes in the presence of an equilibrium electric field and stationary charged dust grains are examined. It is found that the presence of these two contribute to the stability of the ballooning mode. Furthermore, the nonlinear coupling between finite amplitude drift-ballooning modes gives rise to different types of coherent vortex structures, which can affect the transport properties of an inhomogeneous magnetized plasma. The relevance of the investigation to laboratory and astrophysical plasmas is discussed.
“…The important point to be noted here is that for a uniform plasma (L n -*oo), the lower bound u/a > c s is clearly attributed to the inclusion of the nonlinear parallel ion dynamics. Such an effect has been overlooked in previous studies (Shukla et al , 1986Liu & Horton 1986;Mikhailovskii et al 1987;Kaladze et al 1987). The inner solution of (25) is given by ( r\ uB A 3 J 1 (k 1 r)+A i I 1 (k 2 r) + -\-^R costf,…”
Section: ( 2 7 )mentioning
confidence: 99%
“…2 v 2 A )/p 2 . Equation (25) is a fourth-order inhomogeneous partial differential equation, whose solution can be found following Liu & Horton (1986) and Mikhailovskii et al (1987).…”
Section: P K Shuklamentioning
confidence: 99%
“…It is found that the parallel ion motion restricts the vortex speed.Recently, a number of authors (Shukla 1985;Shukla, Yu & Varma 1985;Shukla, Yu & Stenflo 1986;Liu & Horton 1986;Mikhailovskii et al 1987;Kaladze et al 1987) have investigated the formation of drift-Alfven vortices in plasmas. However, all of these studies have been restricted to the twodimensional ion-fluid and three-dimensional electron-fluid motions.…”
Drift-Alfven vortices are investigated, taking into account the nonlinear ion dynamics parallel to the external magnetic field. It is found that the parallel ion motion restricts the vortex speed.Recently, a number of authors (Shukla 1985;Shukla, Yu & Varma 1985;Shukla, Yu & Stenflo 1986;Liu & Horton 1986;Mikhailovskii et al. 1987;Kaladze et al. 1987) have investigated the formation of drift-Alfven vortices in plasmas. However, all of these studies have been restricted to the twodimensional ion-fluid and three-dimensional electron-fluid motions. It has been found that drift-Alfven vortices can propagate with sub-Alfvenic velocity with no lower bound to their speed. In this paper we incorporate the nonlinear ion dynamics parallel to the external magnetic field and show that the sound term restricts the propagation speed of drift-Alfven vortices.If we represent the electromagnetic fields as
E = -V-zc-1 d t A z ,
B = VA Z x z (2)then the perpendicular (to the external magnetic field B o z) components of the electron-and ion-fluid velocities in the drift approximation (d t v iz d z . Furthermore, in view of the low-/? (= 8nn 0 T e /Bl <£ 1) approximation, compressional magnetic field effects are neglected.From the z component of Ampere's law, we find a relationship between the parallel component of the electron-and ion-fluid velocities and the parallel vector potential. We have
“…These modes are ultimately suitably rescaled wave functions of the stationary states of a two-dimensional quantum oscillator, under the Schrödinger equation [27]. Since this latter system can properly model other interesting vortices arising in different media (as in plasmas [28], superfluids [29], and Bose-Einstein condensates [29]), the oscillator will serve as our thread, bearing in mind that the results can be immediately translated to the optical case.…”
We introduce an operator linked with the radial index in the Laguerre-Gauss modes of a two-dimensional harmonic oscillator in cylindrical coordinates. We discuss ladder operators for this variable, and confirm that they obey the commutation relations of the su(1,1) algebra. Using this fact, we examine how basic quantum optical concepts can be recast in terms of radial modes.
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