2004
DOI: 10.1063/1.1712976
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Growth of a ring ripple on a Gaussian beam in a plasma

Abstract: The growth of a ring ripple, riding on an intense Gaussian laser beam, through plasma has been studied. The amplitude ratio p of the ripple and the beam and the dimensionless width ρ1 of the ripple are chosen as significant coordinates. It is observed that the positive quadrant of the p, ρ1 space can be divided in three distinct regions corresponding to steady divergence, oscillatory divergence and oscillatory convergence of the ripple. The variation of ripple width with distance of propagation has been obtain… Show more

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Cited by 17 publications
(7 citation statements)
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“…This assumption leads to the same dielectric function for both the ring ripple part as well as a Gaussian part of the electromagnetic beam and hence the same focusing factors (valid in the vicinity of the maximum of the ripple). This is in contrast to the earlier analyses [62][63][64][65][66][67][68][69], which separately consider the beam and the ripple, leading to incorrect results.…”
Section: Introductioncontrasting
confidence: 89%
See 1 more Smart Citation
“…This assumption leads to the same dielectric function for both the ring ripple part as well as a Gaussian part of the electromagnetic beam and hence the same focusing factors (valid in the vicinity of the maximum of the ripple). This is in contrast to the earlier analyses [62][63][64][65][66][67][68][69], which separately consider the beam and the ripple, leading to incorrect results.…”
Section: Introductioncontrasting
confidence: 89%
“…The other approach is based on the direct [52,53] and indirect [54] evidence, suggesting that the filamentational instability in nonlinear media is caused by the occurrence of strong irradiance spikes, riding on an incident smooth-looking irradiance distribution in the plane, transverse to the direction of propagation. On the basis of the paraxial theory formulated by Akhmanov et al [55] and developed by Sodha et al [39,56], the growth of a Gaussian ripple on a plane uniform beam [57][58][59][60][61] and of a ring ripple on a Gaussian electromagnetic beam [62][63][64][65][66][67][68][69] in a plasma have been investigated to a significant extent. An interesting critique of the two approaches has been made by Sodha and Sharma [70].…”
Section: Introductionmentioning
confidence: 99%
“…(42a) and (42b) in Eq. (40) and equating the coefficient of r 2 , we obtain the dimensionless width parameters of the scattered beam (f S )…”
Section: Stimulated Raman Scaterringmentioning
confidence: 99%
“…Ponderomotive force is a nonlinear force that a charged particle experiences in an inhomogeneous oscillatory electromagnetic field, reforming the plasma electron density distribution and effective dielectric constant of medium, which has been extensively considered in ultraintense standing wave propagation, nonisothermal plasma, magnetoplasma, co-axial electromagnetic wave propagation, and ring ripple formation. [14][15][16][17][18][19][20] Malik and Aria presented the spatial electron density distribution in the microwave and plasma interaction for different electron temperatures, and they regarded the electrons equilibrated by ponderomotive force and plasma pressure gradient force as the starting point. 21 Drude model was first proposed by Paul and Drude in 1900 to explain the transport properties of electrons in materials.…”
Section: Introductionmentioning
confidence: 99%