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Solitons in Nonlocal Media

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1<br />

Introduction<br />

1.1 <strong>Solitons</strong> <strong>in</strong> Nonl<strong>in</strong>ear Physics<br />

Nonl<strong>in</strong>earity has an important role <strong>in</strong> many discipl<strong>in</strong>es such as physics, economics,<br />

chemistry, biology and so on. In fact, most natural phenomena are <strong>in</strong>tr<strong>in</strong>sically non-<br />

l<strong>in</strong>ear, be<strong>in</strong>g l<strong>in</strong>ear only when small excitations are considered. Up to the twentieth<br />

century, scientists focused on l<strong>in</strong>ear phenomena, firstly because of the large availability<br />

of analytical solutions and secondly, but not less important, because of the possibility to<br />

use superimposition pr<strong>in</strong>ciple, which provides the complete knowledge of a system after<br />

study<strong>in</strong>g its response to limited sets of excitations. This pr<strong>in</strong>ciple is largely adopted <strong>in</strong><br />

eng<strong>in</strong>eer<strong>in</strong>g and physics, for example <strong>in</strong> harmonic analysis. E<strong>in</strong>ste<strong>in</strong>’s general relativity,<br />

one of the most successful physical theories <strong>in</strong> 1900’s, is based on nonl<strong>in</strong>ear equations.<br />

With the advent of modern computers <strong>in</strong> the 50’s, the available computation power<br />

allowed to study nonl<strong>in</strong>ear problems numerically: among pioneer<strong>in</strong>g work I rem<strong>in</strong>d the<br />

Fermi, Pasta and Ulam paper concern<strong>in</strong>g energy distribution <strong>in</strong> a nonl<strong>in</strong>ear vibrat<strong>in</strong>g<br />

str<strong>in</strong>g (1; 2) and the Lorenz article about chaos <strong>in</strong> meteorology (3).<br />

One of the most strik<strong>in</strong>g features of nonl<strong>in</strong>ear systems is the formation of waves with<br />

an <strong>in</strong>variant profile along their propagation due to the <strong>in</strong>terplay between l<strong>in</strong>ear and<br />

nonl<strong>in</strong>ear effects, called solitons. Strictly speak<strong>in</strong>g, solitons are solutions of <strong>in</strong>tegrable<br />

models 1 , which can be solved by the <strong>in</strong>verse scatter<strong>in</strong>g technique (4). In non <strong>in</strong>tegrable<br />

models, shape-preserv<strong>in</strong>g solutions are called solitary waves but, as usual <strong>in</strong> the spe-<br />

1 In this context <strong>in</strong>tegrability means that the differential equations compos<strong>in</strong>g the model encompass<br />

an <strong>in</strong>f<strong>in</strong>ite set of conserved quantities.<br />

1

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