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Photorefractive Solitons (Chapter in Springer book ... - Tripod

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2 E. DelRe, M. Segev, D. Christodoulides, B. Crosignani, and G. Salamo<br />

tive solitons have evolved <strong>in</strong>to a major subject contribut<strong>in</strong>g to research at<br />

the cutt<strong>in</strong>g edge of nonl<strong>in</strong>ear science. The <strong>in</strong>tr<strong>in</strong>sic complexity of the photorefractive<br />

light-<strong>in</strong>duced <strong>in</strong>dex-change, driven by several charge transport<br />

mechanisms, utiliz<strong>in</strong>g l<strong>in</strong>ear and quadratic electro-optic effects, and hav<strong>in</strong>g<br />

a polarization-dependent tensorial behavior, contributes <strong>in</strong> giv<strong>in</strong>g rise to a<br />

rich phenomenology. Much is understood now about the formation processes<br />

of the various types of photorefractive solitons, and many of the parameters<br />

can be controlled <strong>in</strong>dividually: at the same time numerous questions<br />

are still open. Also important, research on solitons <strong>in</strong> photorefractives has<br />

benefited not only the soliton community, but has also <strong>in</strong>troduced a number<br />

of new <strong>in</strong>gredients to photorefractive studies at large. For example, understand<strong>in</strong>g<br />

the propagation dynamics of beams <strong>in</strong> photorefractives (rather than<br />

two- and four-wave-mix<strong>in</strong>g), <strong>in</strong>clud<strong>in</strong>g the formation of self-oscillators (e.g.,<br />

the so-called ”double phase conjugator”) has considerably benefited from the<br />

understand<strong>in</strong>g ga<strong>in</strong>ed <strong>in</strong> photorefrative soliton research. Likewise, explor<strong>in</strong>g<br />

spatially-localized effects that emerge and f<strong>in</strong>d their full realization directly<br />

with<strong>in</strong> the sample, such as <strong>in</strong>stabilities and spontaneous pattern formation,<br />

with and without a cavity, is now nicely understood through the <strong>in</strong>timate<br />

connection between solitons and modulation <strong>in</strong>stability [4]. These dist<strong>in</strong>guish<br />

soliton phenomenology from holographic and wave-mix<strong>in</strong>g schemes, which, by<br />

nature, deal pr<strong>in</strong>cipally with the manipulation of light as a device to an effect<br />

which occurs outside the crystal. In this <strong>Chapter</strong>, we attempt to provide an<br />

updated overview on the fasc<strong>in</strong>at<strong>in</strong>g phenomenon of photorefractive solitons,<br />

which cont<strong>in</strong>uously br<strong>in</strong>gs <strong>in</strong> new surprises, new effects, new excitement, to<br />

the photorefractives community, to the much broader nonl<strong>in</strong>ear optics community,<br />

and to soliton science at large.<br />

2 The discovery of solitons <strong>in</strong> photorefractives<br />

In the wake of renewed <strong>in</strong>terest <strong>in</strong> soliton propagation, triggered by studies<br />

on temporal solitons <strong>in</strong> an ever more competitive fiber optic network, the beg<strong>in</strong>n<strong>in</strong>g<br />

of the 1990s see an <strong>in</strong>tense effort aimed at f<strong>in</strong>d<strong>in</strong>g accessible physical<br />

systems <strong>in</strong> which to experimentally <strong>in</strong>vestigate spatial solitons. Conventional<br />

Kerr-type nonl<strong>in</strong>ear schemes presented crippl<strong>in</strong>g limitations connected to the<br />

extremely high optical <strong>in</strong>tensities <strong>in</strong>volved, and suffer<strong>in</strong>g from the fundamental<br />

constra<strong>in</strong>ts associated with the <strong>in</strong>stabilities and catastrophic collapse of<br />

Kerr solitons <strong>in</strong> bulk media. Motivated by the strong nonl<strong>in</strong>ear response of<br />

photorefractive crystals, even at low optical <strong>in</strong>tensities, M. Segev, B. Crosignani,<br />

and A. Yariv, were able to formulate <strong>in</strong> 1992 the first photorefractionbased<br />

self-trapp<strong>in</strong>g mechanism. This embryonic idea sets the beg<strong>in</strong>n<strong>in</strong>g of the<br />

field, and, <strong>in</strong>deed, of our description [5].<br />

A spatial soliton is a beam which, by virtue of a robust balance between<br />

diffraction and nonl<strong>in</strong>earity, does not change its shape dur<strong>in</strong>g propagation. A<br />

direct observation of a spatial soliton <strong>in</strong> photorefractives is shown <strong>in</strong> Fig.(1).

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