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Statements

Subject Item
n2:RIV%2F60076658%3A12640%2F08%3A00009381%21RIV09-MSM-12640___
rdf:type
skos:Concept n6:Vysledek
dcterms:description
Experimental and theoretical simulations of linear and nonlinear optical susceptibilities of the novel Na3La9O3(BO3)(8), a ternary oxyborate nonlinear single crystal, are reported here. The calculations were based on one of the most accurate methods for the computation of the linear and nonlinear optical susceptibilities of solids within density functional theory. Our calculations show that the edges of optical absorption for epsilon 1/2(omega) and epsilon(parallel to)(2)(omega) are located at 5.2 eV, in good agreement with our measurements. The anisotropy is in good agreement with the theoretical data. The same is true for the birefringence. We found that our calculated and measured refractive indices are in good agreement with those obtained by previous measurements. The imaginary and real parts of the second order second harmonic generation (SHG) susceptibility chi((2))(222)(omega) and chi((2))(112)(omega) were evaluated. Our calculation shows that chi((2))(112)(omega) is the dominant component, wh Experimental and theoretical simulations of linear and nonlinear optical susceptibilities of the novel Na3La9O3(BO3)(8), a ternary oxyborate nonlinear single crystal, are reported here. The calculations were based on one of the most accurate methods for the computation of the linear and nonlinear optical susceptibilities of solids within density functional theory. Our calculations show that the edges of optical absorption for epsilon 1/2(omega) and epsilon(parallel to)(2)(omega) are located at 5.2 eV, in good agreement with our measurements. The anisotropy is in good agreement with the theoretical data. The same is true for the birefringence. We found that our calculated and measured refractive indices are in good agreement with those obtained by previous measurements. The imaginary and real parts of the second order second harmonic generation (SHG) susceptibility chi((2))(222)(omega) and chi((2))(112)(omega) were evaluated. Our calculation shows that chi((2))(112)(omega) is the dominant component, wh Je zde popsána experimentální a teoretická simulace lineární a nelineární optické simulace nového Na3La9O3(BO3)(8), ternárního oxyboritanového nelineárního jednotného krystalu. Výpočty založené na nejpřesnější metodě pro počítání lineárních a neloineárních optických citlivostí pevných látek v rámci hustoty funkční teorie. Naše výpočty ukazují, že hranice optické absorpce pro epsilon 1/2(omega) a epsilon (rovnoběžný s)(2)(omega) jsou umístěny 5,2 eV, to je v dobré shodě s našimi měřeními. Anizotropie je v dobré shodě s teoretickými daty a to samé platí pro dvojlom.
dcterms:title
Optical susceptibilities of Na3La9O3(BO3)(8), ternary oxyborate nonlinear single crystal: theory and experiment Optical susceptibilities of Na3La9O3(BO3)(8), ternary oxyborate nonlinear single crystal: theory and experiment Optická citlivost Na3La9O3(BO3)(8), ternární oxyboritanový nelineární jednotný krystal: teorie a experiment
skos:prefLabel
Optical susceptibilities of Na3La9O3(BO3)(8), ternary oxyborate nonlinear single crystal: theory and experiment Optical susceptibilities of Na3La9O3(BO3)(8), ternary oxyborate nonlinear single crystal: theory and experiment Optická citlivost Na3La9O3(BO3)(8), ternární oxyboritanový nelineární jednotný krystal: teorie a experiment
skos:notation
RIV/60076658:12640/08:00009381!RIV09-MSM-12640___
n3:aktivita
n7:Z
n3:aktivity
Z(MSM6007665808)
n3:cisloPeriodika
14
n3:dodaniDat
n16:2009
n3:domaciTvurceVysledku
Reshak, Ali Hussain
n3:druhVysledku
n12:J
n3:duvernostUdaju
n5:S
n3:entitaPredkladatele
n15:predkladatel
n3:idSjednocenehoVysledku
385030
n3:idVysledku
RIV/60076658:12640/08:00009381
n3:jazykVysledku
n14:eng
n3:klicovaSlova
Optical susceptibilities; Na3La9O3(BO3)(8),
n3:klicoveSlovo
n8:Na3La9O3%28BO3%29%288%29 n8:Optical%20susceptibilities
n3:kodStatuVydavatele
GB - Spojené království Velké Británie a Severního Irska
n3:kontrolniKodProRIV
[A908FC489F4E]
n3:nazevZdroje
Journal of Physics-Condensed Matter
n3:obor
n10:BO
n3:pocetDomacichTvurcuVysledku
1
n3:pocetTvurcuVysledku
3
n3:rokUplatneniVysledku
n16:2008
n3:svazekPeriodika
20
n3:tvurceVysledku
Reshak, Ali Hussain Auluck, S. Kityk, I. V.
n3:wos
000254175100011
n3:zamer
n17:MSM6007665808
s:issn
0953-8984
s:numberOfPages
1
n13:organizacniJednotka
12640