Photoinduced electrooptics in the In2O3 nanocrystals incorporated into PMMA matrixes
Identifieur interne : 007323 ( Main/Repository ); précédent : 007322; suivant : 007324Photoinduced electrooptics in the In2O3 nanocrystals incorporated into PMMA matrixes
Auteurs : RBID : Pascal:07-0096538Descripteurs français
- Pascal (Inist)
- Effet électrooptique, Rayonnement polarisé, Eclairement, Effet dimensionnel, Polarisation périodique, Microscopie électronique transmission, Diffusion lumière, Microscopie force atomique, Traitement par laser, Effet photoinduit, Morphologie, Nanocomposite, Indium oxyde, Nanocristal, Méthacrylate de méthyle polymère, Matériau composite, In2O3, 7867B.
- Wicri :
- concept : Matériau composite.
English descriptors
- KwdEn :
Abstract
We have observed an appearance of clear morphological structure in composites containing In2O3 nanocrystals (NCs) incorporated into polymethyl methacrylite (PMMA) matrices under optical treatment by a polarized femtosecond laser. The initial photoinduced treatment was carried out using a Ti:sapphire femtosecond laser emitting 140 fs p-polarized light at a maximum spectral wavelength 775 nm with pulse repetition 1 kHz. It was found that the average morphological radius is varied maximally only during illumination at liquid helium temperature (T = 4.2 K). The morphological average mean radius is strictly dependent on the sizes of incorporated In2O3 NCs. Afterwards we measured the linear electrooptic effect at cw He-Ne laser wavelength 633 nm during simultaneous treatment by 1060 and 530 nm coherent beams of a Nd-YAG picosecond laser. We have established that a decrease of the average morphological mean radius favours an increase of the optically poled linear electrooptic coefficient. The diameters of In2O3 NCs were evaluated using transmission electron microscopy (TEM) and light-scattering techniques, whereas the NC sizes and morphological average mean radius of formed nanocomposites were estimated by atomic force microscopy (AFM). A relationship between the diameter of the NC, composite morphological mean average radius and effective linear electrooptic coefficient was established.
Links toward previous steps (curation, corpus...)
- to stream Main, to step Corpus: 008201
Links to Exploration step
Pascal:07-0096538Le document en format XML
<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Photoinduced electrooptics in the In<sub>2</sub>O<sub>3</sub> nanocrystals incorporated into PMMA matrixes</title><author><name sortKey="Kityk, I V" uniqKey="Kityk I">I. V. Kityk</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Institute of Physics, J Dlugosz University Czestochowa, Alcja Armii Krajowej 13/15</s1><s2>Czestochowa</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ></inist:fA14><country>Pologne</country><wicri:noRegion>Czestochowa</wicri:noRegion></affiliation></author><author><name sortKey="Ebothe, J" uniqKey="Ebothe J">J. Ebothe</name><affiliation wicri:level="3"><inist:fA14 i1="02"><s1>Laboratoire de Microscopiset d'Etude de Nanstructures, E A N3799, Boite Postale 138, 21, rue Clement Ader</s1><s2>51685, Reims</s2><s3>FRA</s3><sZ>2 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Champagne-Ardenne</region><settlement type="city">Reims</settlement></placeName></affiliation></author><author><name sortKey="Tkaczyk, S" uniqKey="Tkaczyk S">S. Tkaczyk</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Institute of Physics, J Dlugosz University Czestochowa, Alcja Armii Krajowej 13/15</s1><s2>Czestochowa</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ></inist:fA14><country>Pologne</country><wicri:noRegion>Czestochowa</wicri:noRegion></affiliation></author><author><name sortKey="Miedzinski, R" uniqKey="Miedzinski R">R. Miedzinski</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Institute of Physics, J Dlugosz University Czestochowa, Alcja Armii Krajowej 13/15</s1><s2>Czestochowa</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ></inist:fA14><country>Pologne</country><wicri:noRegion>Czestochowa</wicri:noRegion></affiliation></author><author><name sortKey="Nzoghe Mendome, L" uniqKey="Nzoghe Mendome L">L. Nzoghe-Mendome</name><affiliation wicri:level="3"><inist:fA14 i1="02"><s1>Laboratoire de Microscopiset d'Etude de Nanstructures, E A N3799, Boite Postale 138, 21, rue Clement Ader</s1><s2>51685, Reims</s2><s3>FRA</s3><sZ>2 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Champagne-Ardenne</region><settlement type="city">Reims</settlement></placeName></affiliation></author><author><name>JIBAO HE</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Central Instrumental Facilities, Tulane University</s1><s2>New Orleans, LA 701 18</s2><s3>USA</s3><sZ>6 aut.</sZ></inist:fA14><country>États-Unis</country><wicri:noRegion>New Orleans, LA 701 18</wicri:noRegion></affiliation></author><author><name>XIANGCHENG SUN</name><affiliation wicri:level="1"><inist:fA14 i1="04"><s1>College of Engineering, University of Michigan</s1><s2>Ann Arbor, MI 48109</s2><s3>USA</s3><sZ>7 aut.</sZ><sZ>8 aut.</sZ></inist:fA14><country>États-Unis</country><wicri:noRegion>Ann Arbor, MI 48109</wicri:noRegion></affiliation></author><author><name>KAI SUN</name><affiliation wicri:level="1"><inist:fA14 i1="04"><s1>College of Engineering, University of Michigan</s1><s2>Ann Arbor, MI 48109</s2><s3>USA</s3><sZ>7 aut.</sZ><sZ>8 aut.</sZ></inist:fA14><country>États-Unis</country><wicri:noRegion>Ann Arbor, MI 48109</wicri:noRegion></affiliation></author><author><name>QINGSHENG LIU</name><affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Department of Chemistry, State University of New York at Binghamton</s1><s2>Binghamton, NY 13902-6000</s2><s3>USA</s3><sZ>9 aut.</sZ><sZ>10 aut.</sZ><sZ>12 aut.</sZ></inist:fA14><country>États-Unis</country><wicri:noRegion>Binghamton, NY 13902-6000</wicri:noRegion></affiliation></author><author><name>ZHAOYONG SUN</name><affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Department of Chemistry, State University of New York at Binghamton</s1><s2>Binghamton, NY 13902-6000</s2><s3>USA</s3><sZ>9 aut.</sZ><sZ>10 aut.</sZ><sZ>12 aut.</sZ></inist:fA14><country>États-Unis</country><wicri:noRegion>Binghamton, NY 13902-6000</wicri:noRegion></affiliation></author><author><name>JUN LIN</name><affiliation wicri:level="1"><inist:fA14 i1="06"><s1>Changchun Institute of Applied Chemistry, Chinese Academy of Sciences</s1><s2>Changchun 130022</s2><s3>CHN</s3><sZ>11 aut.</sZ></inist:fA14><country>République populaire de Chine</country><placeName><settlement type="city">Changchun</settlement><region type="province">Jilin</region><region type="groupement">Dongbei</region></placeName></affiliation></author><author><name>JIYE FANG</name><affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Department of Chemistry, State University of New York at Binghamton</s1><s2>Binghamton, NY 13902-6000</s2><s3>USA</s3><sZ>9 aut.</sZ><sZ>10 aut.</sZ><sZ>12 aut.</sZ></inist:fA14><country>États-Unis</country><wicri:noRegion>Binghamton, NY 13902-6000</wicri:noRegion></affiliation></author></titleStmt><publicationStmt><idno type="inist">07-0096538</idno><date when="2007">2007</date><idno type="stanalyst">PASCAL 07-0096538 INIST</idno><idno type="RBID">Pascal:07-0096538</idno><idno type="wicri:Area/Main/Corpus">008201</idno><idno type="wicri:Area/Main/Repository">007323</idno></publicationStmt><seriesStmt><idno type="ISSN">0953-8984</idno><title level="j" type="abbreviated">J. phys., Condens. matter : (Print)</title><title level="j" type="main">Journal of physics. Condensed matter : (Print)</title></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Atomic force microscopy</term><term>Composite materials</term><term>Electro-optical effects</term><term>Illumination</term><term>Indium oxides</term><term>Laser assisted processing</term><term>Light scattering</term><term>Morphology</term><term>Nanocomposites</term><term>Nanocrystal</term><term>PMMA</term><term>Photoinduced effect</term><term>Polarized radiation</term><term>Poling</term><term>Size effect</term><term>Transmission electron microscopy</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Effet électrooptique</term><term>Rayonnement polarisé</term><term>Eclairement</term><term>Effet dimensionnel</term><term>Polarisation périodique</term><term>Microscopie électronique transmission</term><term>Diffusion lumière</term><term>Microscopie force atomique</term><term>Traitement par laser</term><term>Effet photoinduit</term><term>Morphologie</term><term>Nanocomposite</term><term>Indium oxyde</term><term>Nanocristal</term><term>Méthacrylate de méthyle polymère</term><term>Matériau composite</term><term>In2O3</term><term>7867B</term></keywords><keywords scheme="Wicri" type="concept" xml:lang="fr"><term>Matériau composite</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">We have observed an appearance of clear morphological structure in composites containing In<sub>2</sub>O<sub>3</sub> nanocrystals (NCs) incorporated into polymethyl methacrylite (PMMA) matrices under optical treatment by a polarized femtosecond laser. The initial photoinduced treatment was carried out using a Ti:sapphire femtosecond laser emitting 140 fs p-polarized light at a maximum spectral wavelength 775 nm with pulse repetition 1 kHz. It was found that the average morphological radius is varied maximally only during illumination at liquid helium temperature (T = 4.2 K). The morphological average mean radius is strictly dependent on the sizes of incorporated In<sub>2</sub>O<sub>3</sub> NCs. Afterwards we measured the linear electrooptic effect at cw He-Ne laser wavelength 633 nm during simultaneous treatment by 1060 and 530 nm coherent beams of a Nd-YAG picosecond laser. We have established that a decrease of the average morphological mean radius favours an increase of the optically poled linear electrooptic coefficient. The diameters of In<sub>2</sub>O<sub>3</sub> NCs were evaluated using transmission electron microscopy (TEM) and light-scattering techniques, whereas the NC sizes and morphological average mean radius of formed nanocomposites were estimated by atomic force microscopy (AFM). A relationship between the diameter of the NC, composite morphological mean average radius and effective linear electrooptic coefficient was established.</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0953-8984</s0></fA01><fA02 i1="01"><s0>JCOMEL</s0></fA02><fA03 i2="1"><s0>J. phys., Condens. matter : (Print)</s0></fA03><fA05><s2>19</s2></fA05><fA06><s2>1</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>Photoinduced electrooptics in the In<sub>2</sub>O<sub>3</sub> nanocrystals incorporated into PMMA matrixes</s1></fA08><fA11 i1="01" i2="1"><s1>KITYK (I. V.)</s1></fA11><fA11 i1="02" i2="1"><s1>EBOTHE (J.)</s1></fA11><fA11 i1="03" i2="1"><s1>TKACZYK (S.)</s1></fA11><fA11 i1="04" i2="1"><s1>MIEDZINSKI (R.)</s1></fA11><fA11 i1="05" i2="1"><s1>NZOGHE-MENDOME (L.)</s1></fA11><fA11 i1="06" i2="1"><s1>JIBAO HE</s1></fA11><fA11 i1="07" i2="1"><s1>XIANGCHENG SUN</s1></fA11><fA11 i1="08" i2="1"><s1>KAI SUN</s1></fA11><fA11 i1="09" i2="1"><s1>QINGSHENG LIU</s1></fA11><fA11 i1="10" i2="1"><s1>ZHAOYONG SUN</s1></fA11><fA11 i1="11" i2="1"><s1>JUN LIN</s1></fA11><fA11 i1="12" i2="1"><s1>JIYE FANG</s1></fA11><fA14 i1="01"><s1>Institute of Physics, J Dlugosz University Czestochowa, Alcja Armii Krajowej 13/15</s1><s2>Czestochowa</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ></fA14><fA14 i1="02"><s1>Laboratoire de Microscopiset d'Etude de Nanstructures, E A N3799, Boite Postale 138, 21, rue Clement Ader</s1><s2>51685, Reims</s2><s3>FRA</s3><sZ>2 aut.</sZ><sZ>5 aut.</sZ></fA14><fA14 i1="03"><s1>Central Instrumental Facilities, Tulane University</s1><s2>New Orleans, LA 701 18</s2><s3>USA</s3><sZ>6 aut.</sZ></fA14><fA14 i1="04"><s1>College of Engineering, University of Michigan</s1><s2>Ann Arbor, MI 48109</s2><s3>USA</s3><sZ>7 aut.</sZ><sZ>8 aut.</sZ></fA14><fA14 i1="05"><s1>Department of Chemistry, State University of New York at Binghamton</s1><s2>Binghamton, NY 13902-6000</s2><s3>USA</s3><sZ>9 aut.</sZ><sZ>10 aut.</sZ><sZ>12 aut.</sZ></fA14><fA14 i1="06"><s1>Changchun Institute of Applied Chemistry, Chinese Academy of Sciences</s1><s2>Changchun 130022</s2><s3>CHN</s3><sZ>11 aut.</sZ></fA14><fA20><s2>016204.1-016204.10</s2></fA20><fA21><s1>2007</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>577E2</s2><s5>354000159670610160</s5></fA43><fA44><s0>0000</s0><s1>© 2007 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>19 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>07-0096538</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Journal of physics. Condensed matter : (Print)</s0></fA64><fA66 i1="01"><s0>GBR</s0></fA66><fC01 i1="01" l="ENG"><s0>We have observed an appearance of clear morphological structure in composites containing In<sub>2</sub>O<sub>3</sub> nanocrystals (NCs) incorporated into polymethyl methacrylite (PMMA) matrices under optical treatment by a polarized femtosecond laser. The initial photoinduced treatment was carried out using a Ti:sapphire femtosecond laser emitting 140 fs p-polarized light at a maximum spectral wavelength 775 nm with pulse repetition 1 kHz. It was found that the average morphological radius is varied maximally only during illumination at liquid helium temperature (T = 4.2 K). The morphological average mean radius is strictly dependent on the sizes of incorporated In<sub>2</sub>O<sub>3</sub> NCs. Afterwards we measured the linear electrooptic effect at cw He-Ne laser wavelength 633 nm during simultaneous treatment by 1060 and 530 nm coherent beams of a Nd-YAG picosecond laser. We have established that a decrease of the average morphological mean radius favours an increase of the optically poled linear electrooptic coefficient. The diameters of In<sub>2</sub>O<sub>3</sub> NCs were evaluated using transmission electron microscopy (TEM) and light-scattering techniques, whereas the NC sizes and morphological average mean radius of formed nanocomposites were estimated by atomic force microscopy (AFM). A relationship between the diameter of the NC, composite morphological mean average radius and effective linear electrooptic coefficient was established.</s0></fC01><fC02 i1="01" i2="3"><s0>001B70H67B</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>Effet électrooptique</s0><s5>02</s5></fC03><fC03 i1="01" i2="3" l="ENG"><s0>Electro-optical effects</s0><s5>02</s5></fC03><fC03 i1="02" i2="X" l="FRE"><s0>Rayonnement polarisé</s0><s5>03</s5></fC03><fC03 i1="02" i2="X" l="ENG"><s0>Polarized radiation</s0><s5>03</s5></fC03><fC03 i1="02" i2="X" l="SPA"><s0>Radiación polarizada</s0><s5>03</s5></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Eclairement</s0><s5>04</s5></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Illumination</s0><s5>04</s5></fC03><fC03 i1="04" i2="3" l="FRE"><s0>Effet dimensionnel</s0><s5>05</s5></fC03><fC03 i1="04" i2="3" l="ENG"><s0>Size effect</s0><s5>05</s5></fC03><fC03 i1="05" i2="3" l="FRE"><s0>Polarisation périodique</s0><s5>06</s5></fC03><fC03 i1="05" i2="3" l="ENG"><s0>Poling</s0><s5>06</s5></fC03><fC03 i1="06" i2="3" l="FRE"><s0>Microscopie électronique transmission</s0><s5>07</s5></fC03><fC03 i1="06" i2="3" l="ENG"><s0>Transmission electron microscopy</s0><s5>07</s5></fC03><fC03 i1="07" i2="3" l="FRE"><s0>Diffusion lumière</s0><s5>08</s5></fC03><fC03 i1="07" i2="3" l="ENG"><s0>Light scattering</s0><s5>08</s5></fC03><fC03 i1="08" i2="3" l="FRE"><s0>Microscopie force atomique</s0><s5>09</s5></fC03><fC03 i1="08" i2="3" l="ENG"><s0>Atomic force microscopy</s0><s5>09</s5></fC03><fC03 i1="09" i2="3" l="FRE"><s0>Traitement par laser</s0><s5>10</s5></fC03><fC03 i1="09" i2="3" l="ENG"><s0>Laser assisted processing</s0><s5>10</s5></fC03><fC03 i1="10" i2="X" l="FRE"><s0>Effet photoinduit</s0><s5>11</s5></fC03><fC03 i1="10" i2="X" l="ENG"><s0>Photoinduced effect</s0><s5>11</s5></fC03><fC03 i1="10" i2="X" l="SPA"><s0>Efecto fotoinducido</s0><s5>11</s5></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Morphologie</s0><s5>12</s5></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Morphology</s0><s5>12</s5></fC03><fC03 i1="12" i2="3" l="FRE"><s0>Nanocomposite</s0><s5>13</s5></fC03><fC03 i1="12" i2="3" l="ENG"><s0>Nanocomposites</s0><s5>13</s5></fC03><fC03 i1="13" i2="3" l="FRE"><s0>Indium oxyde</s0><s2>NK</s2><s5>15</s5></fC03><fC03 i1="13" i2="3" l="ENG"><s0>Indium oxides</s0><s2>NK</s2><s5>15</s5></fC03><fC03 i1="14" i2="X" l="FRE"><s0>Nanocristal</s0><s5>16</s5></fC03><fC03 i1="14" i2="X" l="ENG"><s0>Nanocrystal</s0><s5>16</s5></fC03><fC03 i1="14" i2="X" l="SPA"><s0>Nanocristal</s0><s5>16</s5></fC03><fC03 i1="15" i2="3" l="FRE"><s0>Méthacrylate de méthyle polymère</s0><s2>NK</s2><s5>17</s5></fC03><fC03 i1="15" i2="3" l="ENG"><s0>PMMA</s0><s2>NK</s2><s5>17</s5></fC03><fC03 i1="16" i2="3" l="FRE"><s0>Matériau composite</s0><s5>18</s5></fC03><fC03 i1="16" i2="3" l="ENG"><s0>Composite materials</s0><s5>18</s5></fC03><fC03 i1="17" i2="3" l="FRE"><s0>In2O3</s0><s4>INC</s4><s5>52</s5></fC03><fC03 i1="18" i2="3" l="FRE"><s0>7867B</s0><s4>INC</s4><s5>60</s5></fC03><fC07 i1="01" i2="3" l="FRE"><s0>8107B</s0><s4>INC</s4><s5>63</s5></fC07><fN21><s1>064</s1></fN21></pA></standard></inist></record>Pour manipuler ce document sous Unix (Dilib)
EXPLOR_STEP=IndiumV3/Data/Main/Repository
HfdSelect -h $EXPLOR_STEP/biblio.hfd -nk 007323 | SxmlIndent | more
Ou
HfdSelect -h $EXPLOR_AREA/Data/Main/Repository/biblio.hfd -nk 007323 | SxmlIndent | more
Pour mettre un lien sur cette page dans le réseau Wicri
{{Explor lien
|wiki= *** parameter Area/wikiCode missing ***
|area= IndiumV3
|flux= Main
|étape= Repository
|type= RBID
|clé= Pascal:07-0096538
|texte= Photoinduced electrooptics in the In2O3 nanocrystals incorporated into PMMA matrixes
}}
| This area was generated with Dilib version V0.5.77. |  |