dc.contributor.author |
Savatinova, I |
en |
dc.contributor.author |
Savova, I |
en |
dc.contributor.author |
Tonchev, S |
en |
dc.contributor.author |
Liarokapis, E |
en |
dc.contributor.author |
Armenise, MN |
en |
dc.date.accessioned |
2014-03-01T01:15:06Z |
|
dc.date.available |
2014-03-01T01:15:06Z |
|
dc.date.issued |
1999 |
en |
dc.identifier.issn |
0921-4526 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/13348 |
|
dc.subject |
LiNbO3 |
en |
dc.subject |
waveguides |
en |
dc.subject |
Raman scattering |
en |
dc.subject.classification |
Physics, Condensed Matter |
en |
dc.subject.other |
Annealing |
en |
dc.subject.other |
Cooling |
en |
dc.subject.other |
Crystal lattices |
en |
dc.subject.other |
Dielectric films |
en |
dc.subject.other |
Ferroelectric devices |
en |
dc.subject.other |
Hydrogen |
en |
dc.subject.other |
Lithium niobate |
en |
dc.subject.other |
Protons |
en |
dc.subject.other |
Raman scattering |
en |
dc.subject.other |
Raman spectroscopy |
en |
dc.subject.other |
Refractive index |
en |
dc.subject.other |
Thin film devices |
en |
dc.subject.other |
Multimode proton exchanged waveguides |
en |
dc.subject.other |
Thin film waveguides |
en |
dc.subject.other |
Optical waveguides |
en |
dc.title |
Raman study of protonated H:LiNbO3 thin film waveguides |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1016/S0921-4526(98)01293-9 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1016/S0921-4526(98)01293-9 |
en |
heal.language |
English |
en |
heal.publicationDate |
1999 |
en |
heal.abstract |
Multimode proton exchanged waveguides HxLi1-xNbO3 have been formed in congruent z-cut substrates using benzoic acid for proton source. The H concentration was changed by annealing, applying two different rates of cooling - quick (q) and slow (s). The samples were characterized by measuring their extraordinary refractive index profiles and waveguide Raman scattering. At high proton concentrations (x > 0.56), where the beta(i) phases are supposed to be existing the s- (equilibrium beta(2)/beta P-1 combination) and q- (metastable beta(1) phase) type of samples show very different Raman spectra, being also different from the scattering of the pure substrate. This is an evidence for lattice transformations probably related to the large differences in the electrooptic and nonlinear properties of the phases. (C) 1999 Elsevier Science B.V. All rights reserved. |
en |
heal.publisher |
Elsevier Science Publishers B.V., Amsterdam, Netherlands |
en |
heal.journalName |
Physica B: Condensed Matter |
en |
dc.identifier.doi |
10.1016/S0921-4526(98)01293-9 |
en |
dc.identifier.isi |
ISI:000079362700225 |
en |
dc.identifier.volume |
263-264 |
en |
dc.identifier.spage |
819 |
en |
dc.identifier.epage |
821 |
en |