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Photoinduced nonlinear optical effects in the Pr doped BiB306 glass nanoparticles incorporated into the polymer matrices

Identifieur interne : 004D96 ( Main/Repository ); précédent : 004D95; suivant : 004D97

Photoinduced nonlinear optical effects in the Pr doped BiB306 glass nanoparticles incorporated into the polymer matrices

Auteurs : RBID : Pascal:10-0034253

Descripteurs français

English descriptors

Abstract

Photoinduced second harmonic generation was studied in Pr3+ doped bismuth triborate glasses (BiB3O6:Pr) and their nanoparticles (NP) incorporated into the polymethylmethacrylate (PMMA) and polycarbonate (PC) matrices. The process of photoinduction was performed using the simultaneous treatment by 10 ns 1064 nm Nd:YAG laser beam and its second harmonic transformed signal. It was shown that maximal effective second-order susceptibilities (up to 3.7 pm/V) were achieved for content of BiB3O6:Pr NP equal to about 4-6% in weighting units in the PC polymer matrices. After switching off of the phototreatement the decrease of the second-order susceptibility did not exceed 14%.

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Pascal:10-0034253

Le document en format XML

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<title xml:lang="en" level="a">Photoinduced nonlinear optical effects in the Pr doped BiB
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0
<sub>6</sub>
glass nanoparticles incorporated into the polymer matrices</title>
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<term>Bismuth Borates</term>
<term>Bismuth triborate</term>
<term>Glass</term>
<term>Indium additions</term>
<term>Laser beams</term>
<term>Laser radiation</term>
<term>Nanocomposites</term>
<term>Nanoparticles</term>
<term>Nanostructured materials</term>
<term>Nonlinear optics</term>
<term>Optical properties</term>
<term>PMMA</term>
<term>Photoinduced effect</term>
<term>Polycarbonates</term>
<term>Polymers</term>
<term>Second harmonic</term>
<term>Second harmonic generation</term>
<term>Second order</term>
<term>Switching</term>
<term>YAG laser</term>
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<term>Effet photoinduit</term>
<term>Optique non linéaire</term>
<term>Addition indium</term>
<term>Nanomatériau</term>
<term>Génération harmonique 2</term>
<term>Propriété optique</term>
<term>Carbonate polymère</term>
<term>Laser YAG</term>
<term>Rayonnement laser</term>
<term>Faisceau laser</term>
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<term>Bismuth Borate</term>
<term>Méthacrylate de méthyle polymère</term>
<term>BiB3O6</term>
<term>4265K</term>
<term>4270M</term>
<term>Triborate de bismuth</term>
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<div type="abstract" xml:lang="en">Photoinduced second harmonic generation was studied in Pr
<sup>3+</sup>
doped bismuth triborate glasses (BiB
<sub>3</sub>
O
<sub>6</sub>
:Pr) and their nanoparticles (NP) incorporated into the polymethylmethacrylate (PMMA) and polycarbonate (PC) matrices. The process of photoinduction was performed using the simultaneous treatment by 10 ns 1064 nm Nd:YAG laser beam and its second harmonic transformed signal. It was shown that maximal effective second-order susceptibilities (up to 3.7 pm/V) were achieved for content of BiB
<sub>3</sub>
O
<sub>6</sub>
:Pr NP equal to about 4-6% in weighting units in the PC polymer matrices. After switching off of the phototreatement the decrease of the second-order susceptibility did not exceed 14%.</div>
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<sub>3</sub>
0
<sub>6</sub>
glass nanoparticles incorporated into the polymer matrices</s1>
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<s0>Photoinduced second harmonic generation was studied in Pr
<sup>3+</sup>
doped bismuth triborate glasses (BiB
<sub>3</sub>
O
<sub>6</sub>
:Pr) and their nanoparticles (NP) incorporated into the polymethylmethacrylate (PMMA) and polycarbonate (PC) matrices. The process of photoinduction was performed using the simultaneous treatment by 10 ns 1064 nm Nd:YAG laser beam and its second harmonic transformed signal. It was shown that maximal effective second-order susceptibilities (up to 3.7 pm/V) were achieved for content of BiB
<sub>3</sub>
O
<sub>6</sub>
:Pr NP equal to about 4-6% in weighting units in the PC polymer matrices. After switching off of the phototreatement the decrease of the second-order susceptibility did not exceed 14%.</s0>
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