Photoinduced nonlinear optical effects in the Pr doped BiB306 glass nanoparticles incorporated into the polymer matrices
Identifieur interne : 004D96 ( Main/Repository ); précédent : 004D95; suivant : 004D97Photoinduced nonlinear optical effects in the Pr doped BiB306 glass nanoparticles incorporated into the polymer matrices
Auteurs : RBID : Pascal:10-0034253Descripteurs français
- Pascal (Inist)
- Effet photoinduit, Optique non linéaire, Addition indium, Nanomatériau, Génération harmonique 2, Propriété optique, Carbonate polymère, Laser YAG, Rayonnement laser, Faisceau laser, Harmonique 2, Ordre 2, Commutation, Nanocomposite, Verre, Nanoparticule, Polymère, Bismuth Borate, Méthacrylate de méthyle polymère, BiB3O6, 4265K, 4270M, Triborate de bismuth.
- Wicri :
English descriptors
- KwdEn :
- Bismuth Borates, Bismuth triborate, Glass, Indium additions, Laser beams, Laser radiation, Nanocomposites, Nanoparticles, Nanostructured materials, Nonlinear optics, Optical properties, PMMA, Photoinduced effect, Polycarbonates, Polymers, Second harmonic, Second harmonic generation, Second order, Switching, YAG laser.
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:10-0034253Le document en format XML
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0<sub>6</sub>
glass nanoparticles incorporated into the polymer matrices</title>
<author><name sortKey="Majchrowski, A" uniqKey="Majchrowski A">A. Majchrowski</name>
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<s2>00-908 Warsaw</s2>
<s3>POL</s3>
<sZ>1 aut.</sZ>
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<wicri:noRegion>00-908 Warsaw</wicri:noRegion>
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<author><name sortKey="Ebothe, J" uniqKey="Ebothe J">J. Ebothe</name>
<affiliation wicri:level="3"><inist:fA14 i1="02"><s1>Laboratoire de Microscopies & d'Etude de Nanostructures, E.A. n°3799, UFR Sciences, Université de Reims, B.P. 138, 21 rue Clément Ader</s1>
<s2>51685 Reims</s2>
<s3>FRA</s3>
<sZ>2 aut.</sZ>
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<placeName><region type="region" nuts="2">Champagne-Ardenne</region>
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<author><name sortKey="Gondek, E" uniqKey="Gondek E">E. Gondek</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Institute of Physics, Krakow Technological University, ul.Podchorazych 1</s1>
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<author><name sortKey="Ozga, K" uniqKey="Ozga K">K. Ozga</name>
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<sZ>4 aut.</sZ>
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<author><name sortKey="Kityk, I V" uniqKey="Kityk I">I. V. Kityk</name>
<affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Electrical Engineering Department, Czestochowa Technological University, Al. Armii Krajowej 17/19</s1>
<s2>Czestochowa</s2>
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<sZ>5 aut.</sZ>
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</author>
<author><name sortKey="Reshak, A H" uniqKey="Reshak A">A. H. Reshak</name>
<affiliation wicri:level="1"><inist:fA14 i1="06"><s1>Institute of Physical Biology, South Bohemia University, Zamek 136</s1>
<s2>37333 Nove Hrady</s2>
<s3>CZE</s3>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>République tchèque</country>
<wicri:noRegion>37333 Nove Hrady</wicri:noRegion>
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</author>
<author><name sortKey="Lukasiewicz, T" uniqKey="Lukasiewicz T">T. Lukasiewicz</name>
<affiliation wicri:level="1"><inist:fA14 i1="07"><s1>Institute of Electronic Materials Technology, Wolczynska 133</s1>
<s2>01-919 Warsaw</s2>
<s3>POL</s3>
<sZ>7 aut.</sZ>
</inist:fA14>
<country>Pologne</country>
<wicri:noRegion>01-919 Warsaw</wicri:noRegion>
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<publicationStmt><idno type="inist">10-0034253</idno>
<date when="2009">2009</date>
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<seriesStmt><idno type="ISSN">0925-8388</idno>
<title level="j" type="abbreviated">J. alloys compd.</title>
<title level="j" type="main">Journal of alloys and compounds</title>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><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>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><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>
<term>Harmonique 2</term>
<term>Ordre 2</term>
<term>Commutation</term>
<term>Nanocomposite</term>
<term>Verre</term>
<term>Nanoparticule</term>
<term>Polymère</term>
<term>Bismuth Borate</term>
<term>Méthacrylate de méthyle polymère</term>
<term>BiB3O6</term>
<term>4265K</term>
<term>4270M</term>
<term>Triborate de bismuth</term>
</keywords>
<keywords scheme="Wicri" type="concept" xml:lang="fr"><term>Verre</term>
<term>Polymère</term>
</keywords>
</textClass>
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<front><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>
</front>
</TEI>
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</fA03>
<fA05><s2>485</s2>
</fA05>
<fA06><s2>1-2</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Photoinduced nonlinear optical effects in the Pr doped BiB<sub>3</sub>
0<sub>6</sub>
glass nanoparticles incorporated into the polymer matrices</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>MAJCHROWSKI (A.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>EBOTHE (J.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>GONDEK (E.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>OZGA (K.)</s1>
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<fA11 i1="05" i2="1"><s1>KITYK (I. V.)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>RESHAK (A. H.)</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>LUKASIEWICZ (T.)</s1>
</fA11>
<fA14 i1="01"><s1>Institute of Applied Physics, Military University of Technology, Kaliskiego 2</s1>
<s2>00-908 Warsaw</s2>
<s3>POL</s3>
<sZ>1 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Laboratoire de Microscopies & d'Etude de Nanostructures, E.A. n°3799, UFR Sciences, Université de Reims, B.P. 138, 21 rue Clément Ader</s1>
<s2>51685 Reims</s2>
<s3>FRA</s3>
<sZ>2 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Institute of Physics, Krakow Technological University, ul.Podchorazych 1</s1>
<s2>Krakow</s2>
<s3>POL</s3>
<sZ>3 aut.</sZ>
</fA14>
<fA14 i1="04"><s1>Chair of Public Health, Czestochowa Technological University, Al. Armii Krajowej 36A</s1>
<s2>Czestochowa</s2>
<s3>POL</s3>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="05"><s1>Electrical Engineering Department, Czestochowa Technological University, Al. Armii Krajowej 17/19</s1>
<s2>Czestochowa</s2>
<s3>POL</s3>
<sZ>5 aut.</sZ>
</fA14>
<fA14 i1="06"><s1>Institute of Physical Biology, South Bohemia University, Zamek 136</s1>
<s2>37333 Nove Hrady</s2>
<s3>CZE</s3>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="07"><s1>Institute of Electronic Materials Technology, Wolczynska 133</s1>
<s2>01-919 Warsaw</s2>
<s3>POL</s3>
<sZ>7 aut.</sZ>
</fA14>
<fA20><s1>29-32</s1>
</fA20>
<fA21><s1>2009</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
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<fA43 i1="01"><s1>INIST</s1>
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<s1>© 2010 INIST-CNRS. All rights reserved.</s1>
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<fA47 i1="01" i2="1"><s0>10-0034253</s0>
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<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
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<fA64 i1="01" i2="1"><s0>Journal of alloys and compounds</s0>
</fA64>
<fA66 i1="01"><s0>CHE</s0>
</fA66>
<fC01 i1="01" l="ENG"><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>
</fC01>
<fC02 i1="01" i2="3"><s0>001B40B70M</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B40B65K</s0>
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<fC03 i1="01" i2="X" l="FRE"><s0>Effet photoinduit</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG"><s0>Photoinduced effect</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA"><s0>Efecto fotoinducido</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Optique non linéaire</s0>
<s5>02</s5>
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<fC03 i1="02" i2="3" l="ENG"><s0>Nonlinear optics</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Addition indium</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Indium additions</s0>
<s5>03</s5>
</fC03>
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<s5>04</s5>
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<s5>04</s5>
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<s5>05</s5>
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<s5>05</s5>
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<s5>06</s5>
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<s5>06</s5>
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<fC03 i1="07" i2="3" l="FRE"><s0>Carbonate polymère</s0>
<s2>NK</s2>
<s5>07</s5>
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<fC03 i1="07" i2="3" l="ENG"><s0>Polycarbonates</s0>
<s2>NK</s2>
<s5>07</s5>
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<s5>08</s5>
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<fC03 i1="08" i2="X" l="SPA"><s0>Laser YAG</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Rayonnement laser</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Laser radiation</s0>
<s5>09</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Faisceau laser</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Laser beams</s0>
<s5>10</s5>
</fC03>
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<s5>11</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG"><s0>Second harmonic</s0>
<s5>11</s5>
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<s5>11</s5>
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<s5>12</s5>
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<s5>12</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA"><s0>Orden 2</s0>
<s5>12</s5>
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<fC03 i1="13" i2="3" l="FRE"><s0>Commutation</s0>
<s5>13</s5>
</fC03>
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<s5>13</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Nanocomposite</s0>
<s5>14</s5>
</fC03>
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<s5>14</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Verre</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Glass</s0>
<s5>15</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Nanoparticule</s0>
<s5>16</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG"><s0>Nanoparticles</s0>
<s5>16</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Polymère</s0>
<s5>17</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG"><s0>Polymers</s0>
<s5>17</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Bismuth Borate</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>18</s5>
</fC03>
<fC03 i1="18" i2="3" l="ENG"><s0>Bismuth Borates</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>18</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>Méthacrylate de méthyle polymère</s0>
<s2>NK</s2>
<s5>19</s5>
</fC03>
<fC03 i1="19" i2="3" l="ENG"><s0>PMMA</s0>
<s2>NK</s2>
<s5>19</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>BiB3O6</s0>
<s4>INC</s4>
<s5>46</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>4265K</s0>
<s4>INC</s4>
<s5>65</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE"><s0>4270M</s0>
<s4>INC</s4>
<s5>66</s5>
</fC03>
<fC03 i1="23" i2="3" l="FRE"><s0>Triborate de bismuth</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="23" i2="3" l="ENG"><s0>Bismuth triborate</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="23" i2="3" l="SPA"><s0>Triborato de bismuto</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fN21><s1>025</s1>
</fN21>
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