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Studies on Some Aspects of Light Beam Propagation Through ...

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Introducti<strong>on</strong><br />

. l've effects are less important in this case. The main mechanism<br />

d Ispers<br />

behind the filament formati<strong>on</strong> is related to a dynamic balance between the<br />

Kerr self-focusing and the defocusing ind ueed by the plasma. 16<br />

We study the propagati<strong>on</strong> <strong>of</strong> an optical high power beam through a<br />

PTS like medium. In this high energy regime, we have to c<strong>on</strong>sider the phenomen<strong>on</strong><br />

<strong>of</strong> plasma generati<strong>on</strong> through multiphot<strong>on</strong> absorpti<strong>on</strong>. 17 1\·1 ultiphot<strong>on</strong><br />

absorpti<strong>on</strong> is a n<strong>on</strong>linear process, in c<strong>on</strong>trast with the <strong>on</strong>e-phot<strong>on</strong><br />

absorpti<strong>on</strong> process. It has a self defoeusing effect OIl the material. The<br />

counteracting self-de focusing effect <strong>of</strong> both photoi<strong>on</strong>ized free electr<strong>on</strong>s and<br />

the quintic n<strong>on</strong>linearity restricts the unbounded growth <strong>of</strong> the Kerr n<strong>on</strong>linearity.<br />

The study <strong>of</strong> spatial solit<strong>on</strong>s in a bulk Kerr medium with multiphot<strong>on</strong><br />

i<strong>on</strong>izati<strong>on</strong> has been carried out by Herrmann et al. 1S Couair<strong>on</strong> 19<br />

has studied the dynamics <strong>of</strong> light filaments formed when a femtosec<strong>on</strong>d<br />

laser pulse propagates in air taking into c<strong>on</strong>siderati<strong>on</strong> the plasma generated<br />

using photoi<strong>on</strong>izati<strong>on</strong> and has given an extensive review20 <strong>on</strong> the<br />

main aspects <strong>of</strong> ult.rashort laser pulse filament-ati<strong>on</strong> in various transparent<br />

media such as air (gases), transparent solids and liquids. The refractive<br />

index now takes the form<br />

29<br />

(2.2)<br />

where Ne is the number density <strong>of</strong> free electr<strong>on</strong>s and NeT' is the critical<br />

plasma density. The beam evoluti<strong>on</strong> is studied using the cubic-quintic<br />

n<strong>on</strong> linear Schrodinger equati<strong>on</strong> with the effect <strong>of</strong> multiphot<strong>on</strong> i<strong>on</strong>izati<strong>on</strong>.<br />

Now, when a pulsed optical beam propagates through a bulk n<strong>on</strong>linear<br />

medium, it is affected by diffracti<strong>on</strong> and dispersi<strong>on</strong> simultaneously and at<br />

the same time the two effects become coupled through the Il<strong>on</strong>linearity<br />

<strong>of</strong> the medium. Such a space-time coupling leads to various n<strong>on</strong> linear effects<br />

like the possibility <strong>of</strong> spatio-temporal collapse or pulse splitting and<br />

the formati<strong>on</strong> <strong>of</strong> light bullets. The idea <strong>of</strong> "light bullets" was first proposed<br />

by Silberberg. 21 Optical spatiotcmporal solit<strong>on</strong>s, or the so called<br />

"light bullets", have attracted growing interest because <strong>of</strong> their potential<br />

applicati<strong>on</strong>s in ultra fast all-optical switching in a bulk medium. The binary<br />

informati<strong>on</strong> <strong>on</strong>ce brought by temporal soli t<strong>on</strong>s has to be retreated<br />

in all-optical systems. Therefore, there is a growing interest in spatiotemporal<br />

solit<strong>on</strong>s. 22 In a medium with purely cubic Il<strong>on</strong>linear resp<strong>on</strong>se<br />

light bullets (LB) formally exist. But in the higher dimensi<strong>on</strong>s (2D and<br />

3D) they are unstable against the spatiotemporal collapse induced by the<br />

combined effects <strong>of</strong> n<strong>on</strong>linearity and anomalous dispersi<strong>on</strong>. They are not<br />

stable in the uniform self-focusing Kerr medium 23 uut stability ca.n be

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