dc.contributor.author |
Karapetyan, GG |
en |
dc.contributor.author |
Baghclasaryan, HV |
en |
dc.contributor.author |
Daryan, AV |
en |
dc.contributor.author |
Uzunoglu, NK |
en |
dc.date.accessioned |
2014-03-01T01:15:05Z |
|
dc.date.available |
2014-03-01T01:15:05Z |
|
dc.date.issued |
1999 |
en |
dc.identifier.issn |
0895-2477 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/13335 |
|
dc.subject |
chromatic dispersion |
en |
dc.subject |
dispersion distortion |
en |
dc.subject |
linear dispersion |
en |
dc.subject |
quadratic dispersion |
en |
dc.subject.classification |
Engineering, Electrical & Electronic |
en |
dc.subject.classification |
Optics |
en |
dc.subject.other |
Electromagnetic wave propagation |
en |
dc.subject.other |
Optical communication |
en |
dc.subject.other |
Optical links |
en |
dc.subject.other |
Signal distortion |
en |
dc.subject.other |
Chromatic dispersion |
en |
dc.subject.other |
Electromagnetic pulse propagation |
en |
dc.subject.other |
Linear dispersion |
en |
dc.subject.other |
Pulse dispersive distortion |
en |
dc.subject.other |
Quadratic dispersion |
en |
dc.subject.other |
Single mode fibers |
en |
dc.title |
Pulse-dispersive distortion in a single-mode fiber |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1002/(SICI)1098-2760(19990620)21:6<428::AID-MOP10>3.0.CO;2-2 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1002/(SICI)1098-2760(19990620)21:6<428::AID-MOP10>3.0.CO;2-2 |
en |
heal.language |
English |
en |
heal.publicationDate |
1999 |
en |
heal.abstract |
Electromagnetic pulse propagation in an arbitrary dispersive medium is investigated. A quasimonochromatic pulse is assumed, and for this case, separate analytical investigations for two cases of dispersion, called linear and quadratic dispersion, ara carried out. Exact and convenient calculation formulas for envelopes of rectangular and trapezoidal (triangular) initial pulses in the case of linear dispersion are obtained The same is obtained for a rectangular initial pulse in the case of quadratic dispersion. On the basis of this observation, the appropriate calculation formulas for an arbitrary initial pulse given by step-size amplitudes are created. The pulse distortion in the general case when it is impossible to separate linear and quadratic dispersion is investigated. The obtained formulas are convenient for practical calculations. (C) 1999 John Wiley & Sons, Inc. |
en |
heal.publisher |
John Wiley & Sons Inc, New York, NY, United States |
en |
heal.journalName |
Microwave and Optical Technology Letters |
en |
dc.identifier.doi |
10.1002/(SICI)1098-2760(19990620)21:6<428::AID-MOP10>3.0.CO;2-2 |
en |
dc.identifier.isi |
ISI:000080627500010 |
en |
dc.identifier.volume |
21 |
en |
dc.identifier.issue |
6 |
en |
dc.identifier.spage |
428 |
en |
dc.identifier.epage |
433 |
en |