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

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Preface<br />

N certain materials, the spreading <strong>of</strong> a laser beam owing to diffracti<strong>on</strong><br />

I can be compensated by the material n<strong>on</strong>linearity and as a result the<br />

beam propagates without any change in its shape. Such n<strong>on</strong>-diffracting<br />

beams are known as spatial solit<strong>on</strong>s. These solit<strong>on</strong>s have been observed<br />

in various n<strong>on</strong>linear media including Kerr, photorefractive, quadratic and<br />

liquid crystals. Solit<strong>on</strong>s arc ubiquitous in nature and have been studied<br />

in many branches <strong>of</strong> science. In the field <strong>of</strong> optics, temporal solit<strong>on</strong>s,<br />

short temporal pulses that do not change shape as they propagate in a<br />

dispersive material such as an optical fiber, has been studied widely. It<br />

was first proposed in the year 1973 by Hasegawa and Tappert and observed<br />

experimentally in 1980 by ·:'dollenauer et al.<br />

In this thesis, we have studied the propagati<strong>on</strong> <strong>of</strong> light beam through<br />

various n<strong>on</strong>linear media like the cubic-quintic medium, the photorcfractive<br />

medium and the photopolymer system. The fundamental mechanism<br />

resp<strong>on</strong>sible for the refractive index modulati<strong>on</strong> in each <strong>of</strong> the three media<br />

are different.<br />

Chapter 1 gives a basic introducti<strong>on</strong> to the c<strong>on</strong>cept <strong>of</strong> solit<strong>on</strong>s. Different<br />

terms and c<strong>on</strong>cepts associated with solit<strong>on</strong> theory are introduced. Its<br />

historical development and current status are also given. A comprehensive<br />

review in the area <strong>of</strong> spatial solit<strong>on</strong>s is presented. An introducti<strong>on</strong> to the<br />

basic analytical and numerical methods used in this thesis is given.<br />

In Chapter 2, wc have studied two kinds <strong>of</strong> solit<strong>on</strong>s, the (2 + 1) D<br />

spatial soli t<strong>on</strong>s and the (3 + l)D spatio-temporal solit<strong>on</strong>s in a cubic-quintic<br />

medium. The change in refractive index in such a medium occurs due to<br />

two competing effects, focusing due to the third order n<strong>on</strong>linearity and<br />

defocusing due to the fifth order n<strong>on</strong>linearity. We have studied the propagati<strong>on</strong><br />

<strong>of</strong> an optical high power cylindrically symmetric beam in such<br />

a medium both analytically and numerically. In this case, we have to<br />

c<strong>on</strong>sider the self-defocusing effect caused by the presence <strong>of</strong> free electr<strong>on</strong>s<br />

produced due to plasma formati<strong>on</strong>. Multiphot<strong>on</strong> absorpti<strong>on</strong> is a n<strong>on</strong>linear<br />

process, in c<strong>on</strong>trast with the <strong>on</strong>e-phot<strong>on</strong> absorpti<strong>on</strong> process. It has a<br />

self defocusing effect <strong>on</strong> the material. The counteracting self-defocusing<br />

effect <strong>of</strong> both photoi<strong>on</strong>ized free electr<strong>on</strong>s and the quintic n<strong>on</strong> linearity restricts<br />

the unbounded growth <strong>of</strong> the Kerr n<strong>on</strong>linearity. Variati<strong>on</strong>al method<br />

is used to study the system analytically. Finite Difference <strong>Beam</strong> Propagati<strong>on</strong><br />

Method is used for the numerical analysis. In the sec<strong>on</strong>d part<br />

<strong>of</strong> this chapter, we have studied the propagati<strong>on</strong> <strong>of</strong> spatio-ternporal solit<strong>on</strong>s<br />

(<strong>Light</strong> Bullets) through a cubic-quintic medium. The same approach<br />

is used to study the propagati<strong>on</strong> <strong>of</strong> a pulsed high power beam through<br />

ix

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