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dc.contributor.authorReshak, Ali Hussain
dc.contributor.authorI. V., Kityk
dc.contributor.authorS., Auluck
dc.date.accessioned2011-03-09T02:59:23Z
dc.date.available2011-03-09T02:59:23Z
dc.date.issued2010-12-23
dc.identifier.citationJournal of Physical Chemistry B, vol. 114(50), 2010, pages 16705-16712en_US
dc.identifier.issn1520-6106
dc.identifier.urihttp://pubs.acs.org/doi/abs/10.1021/jp1072878
dc.identifier.urihttp://dspace.unimap.edu.my/123456789/11109
dc.descriptionLink to publisher's homepage at http://pubs.acs.org/en_US
dc.description.abstractExperimental and theoretical studies of the linear and nonlinear optical susceptibilities for single crystals of potassium titanyl phosphate KTiOPO 4 are reported. The state-of-the-art full potential linear augmented plane wave method, based on the density functional theory, was applied for the theoretical investigation. The calculated direct energy band gap at γ, using the Engel-Vosko exchange correlation functional, is found to be 3.1 eV. This is in excellent agreement with the band gap obtained from the experimental optical absorption spectra (3.2 eV). We have calculated the complex dielectric susceptibility ε(Ω)dispersion, its zero-frequency limit ε1(0) and the birefringence of KTiOPO4. The calculated birefringence at the zero-frequency limit δn(0) is equal to about 0.07 and δn(Ω) at 1.165 eV (Λ = 1064 nm) is 0.074. We also report calculations of the complex second-order optical susceptibility dispersions for the principal tensor components: ξ113(2)(Ω), ξ232(2)(Ω), ξ311(2)(Ω), ξ322(2)(Ω), and ξ333(2)(Ω). The intra- and interband contributions to these susceptibilities are evaluated. The calculated total second order susceptibility tensor components |ξijk(2)(Ω)| at Λ = 1064 nm for all the five tensor components are compared with those obtained from our measurements performed by nanosecond Nd:YAG laser at the fundamental wavelength (Λ = 1064 nm). Our calculations show reasonably good agreement with our experimental nonlinear optical data and the results obtained by other authors. The calculated the microscopic second order hyperpolarizability, β333, vector component along the dipole moment direction for the dominant component ξ333(2)(Ω) is found to be 31.6 - 10-30 esu, at Λ = 1064 nm.en_US
dc.language.isoenen_US
dc.publisherAmerican Chemical Societyen_US
dc.subjectSingle crystalsen_US
dc.subjectNon-linear opticalen_US
dc.subjectKTiOPO4en_US
dc.titleInvestigation of the linear and nonlinear optical susceptibilities of KTiOPO4 single crystals: Theory and experimenten_US
dc.typeArticleen_US
dc.contributor.urlmaalidph@yahoo.co.uken_US


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