NONLINEAR DYNAMICS OF FEMTOSECOND OPTICAL SOLITARY WAVE-PROPAGATION AT THE ZERO DISPERSION POINT

FRANTZESKAKIS, DJ; HIZANIDIS, K; TOMBRAS, GS; BELIA, I

dc.contributor.author	FRANTZESKAKIS, DJ	en
dc.contributor.author	HIZANIDIS, K	en
dc.contributor.author	TOMBRAS, GS	en
dc.contributor.author	BELIA, I	en
dc.date.accessioned	2014-03-01T01:11:18Z
dc.date.available	2014-03-01T01:11:18Z
dc.date.issued	1995	en
dc.identifier.issn	0018-9197	en
dc.identifier.uri	https://dspace.lib.ntua.gr/xmlui/handle/123456789/11593
dc.subject	Hamiltonian Dynamics	en
dc.subject	Initial Condition	en
dc.subject	Nonlinear Dynamics	en
dc.subject	nonlinear schrodinger equation	en
dc.subject	Optical Fiber	en
dc.subject	Ordinary Differential Equation	en
dc.subject	Solitary Wave	en
dc.subject	Peak Power	en
dc.subject.classification	Engineering, Electrical & Electronic	en
dc.subject.classification	Physics, Applied	en
dc.subject.other	SCHRODINGER-EQUATION	en
dc.subject.other	PULSE-PROPAGATION	en
dc.subject.other	ANOMALOUS DISPERSION	en
dc.subject.other	DIELECTRIC FIBERS	en
dc.subject.other	SOLITONS	en
dc.subject.other	WAVELENGTH	en
dc.subject.other	TRANSMISSION	en
dc.subject.other	GUIDE	en
dc.subject.other	MODULATION	en
dc.subject.other	AMPLIFIERS	en
dc.title	NONLINEAR DYNAMICS OF FEMTOSECOND OPTICAL SOLITARY WAVE-PROPAGATION AT THE ZERO DISPERSION POINT	en
heal.type	journalArticle	en
heal.identifier.primary	10.1109/3.341724	en
heal.identifier.secondary	http://dx.doi.org/10.1109/3.341724	en
heal.language	English	en
heal.publicationDate	1995	en
heal.abstract	A perturbed nonlinear Schrodinger equation, describing nonlinear pulse propagation of femtosecond duration in optical fibers at the zero dispersion point, is considered. This equation is reduced to an ordinary differential equation, which is treated by means of Hamiltonian dynamics techniques. Conditions for solitary wave formation, as well as the solutions themselves, namely, a bright soliton, a rarefaction soliton, and a pair of dark solitons, are derived analytically. The shifts of the solitary wave velocity, the angular frequency, and the wavenumber, as well as the peak power required to launch a bright soliton are also obtained. The connection among the point initial conditions of the pulse and the type of solitary wave that can be excited is finally presented.	en
heal.publisher	IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC	en
heal.journalName	IEEE JOURNAL OF QUANTUM ELECTRONICS	en
dc.identifier.doi	10.1109/3.341724	en
dc.identifier.isi	ISI:A1995QE58800024	en
dc.identifier.volume	31	en
dc.identifier.issue	1	en
dc.identifier.spage	183	en
dc.identifier.epage	189	en