Polarized Raman study on phase transitions in 0.24Pb(In1/2Nb1/2)O3-0.43Pb(Mg1/3Nb2/3)O3-0.33PbTiO3 single crystal
Identifieur interne : 000143 ( Chine/Analysis ); précédent : 000142; suivant : 000144Polarized Raman study on phase transitions in 0.24Pb(In1/2Nb1/2)O3-0.43Pb(Mg1/3Nb2/3)O3-0.33PbTiO3 single crystal
Auteurs : RBID : Pascal:13-0228948Descripteurs français
- Pascal (Inist)
English descriptors
- KwdEn :
Abstract
Polarized Raman spectroscopy was performed to investigate the local lattice structure and phase transitions of unpoled 0.24Pb(In1/2Nb1/2)O3-0.43Pb(Mg1/3Nb2/3)O3-0.33PbTiO3 (0.24PIN-0.43PMN-0.33PT) single crystal in the temperature range from 30 °C to 260 °C. MA- and Mc-type monoclinic phases were detected by micro-Raman spectra measured in different micro areas. Temperature dependence of Raman intensities, frequency shifts, mode merge and intensity ratios in the W and VH geometries were investigated. Our results indicated that the monoclinic-tetragonal (M-T) phase transition of the ternary relaxor-based ferroelectric single crystal 0.24PIN-0.43PMN-0.33PT occurs at 85 °C, which is verified by the mode merging from 520 cm-1 and 580 cm-1 to 500 cm-1, and the tetragonal-cubic (T-C) phase transition happens at 200 °C based on the vanishing mode at 780 cm-1 measured in the VH polarization.
Links toward previous steps (curation, corpus...)
- to stream Main, to step Corpus: 000B25
- to stream Main, to step Repository: 000693
- to stream Chine, to step Extraction: 000143
Links to Exploration step
Pascal:13-0228948Le document en format XML
<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Polarized Raman study on phase transitions in 0.24Pb(In<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>-0.43Pb(Mg<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub>-0.33PbTiO<sub>3</sub> single crystal</title><author><name>FENGMINWU</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Condensed Matter Science and Technology Institute, Harbin Institute of Technology</s1><s2>Harbin 150080</s2><s3>CHN</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>7 aut.</sZ></inist:fA14><country>République populaire de Chine</country><wicri:noRegion>Harbin 150080</wicri:noRegion></affiliation><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>College of Applied Science, Harbin University of Science and Technology</s1><s2>Harbin 150080</s2><s3>CHN</s3><sZ>1 aut.</sZ></inist:fA14><country>République populaire de Chine</country><wicri:noRegion>Harbin 150080</wicri:noRegion></affiliation></author><author><name>BINYANG</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Condensed Matter Science and Technology Institute, Harbin Institute of Technology</s1><s2>Harbin 150080</s2><s3>CHN</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>7 aut.</sZ></inist:fA14><country>République populaire de Chine</country><wicri:noRegion>Harbin 150080</wicri:noRegion></affiliation></author><author><name>ENWEISUN</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Condensed Matter Science and Technology Institute, Harbin Institute of Technology</s1><s2>Harbin 150080</s2><s3>CHN</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>7 aut.</sZ></inist:fA14><country>République populaire de Chine</country><wicri:noRegion>Harbin 150080</wicri:noRegion></affiliation></author><author><name>RUIZHANG</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Condensed Matter Science and Technology Institute, Harbin Institute of Technology</s1><s2>Harbin 150080</s2><s3>CHN</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>7 aut.</sZ></inist:fA14><country>République populaire de Chine</country><wicri:noRegion>Harbin 150080</wicri:noRegion></affiliation></author><author><name>DAPENGXU</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>School of Physics, Jilin University</s1><s2>Changchun 130023</s2><s3>CHN</s3><sZ>5 aut.</sZ><sZ>6 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>JING ZHOU</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>School of Physics, Jilin University</s1><s2>Changchun 130023</s2><s3>CHN</s3><sZ>5 aut.</sZ><sZ>6 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>WENWU CAO</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Condensed Matter Science and Technology Institute, Harbin Institute of Technology</s1><s2>Harbin 150080</s2><s3>CHN</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>7 aut.</sZ></inist:fA14><country>République populaire de Chine</country><wicri:noRegion>Harbin 150080</wicri:noRegion></affiliation><affiliation wicri:level="1"><inist:fA14 i1="04"><s1>Materials Research Institute, The Pennsylvania State University</s1><s2>University Park, PA 16802</s2><s3>USA</s3><sZ>7 aut.</sZ></inist:fA14><country>États-Unis</country><wicri:noRegion>University Park, PA 16802</wicri:noRegion></affiliation></author></titleStmt><publicationStmt><idno type="inist">13-0228948</idno><date when="2013">2013</date><idno type="stanalyst">PASCAL 13-0228948 INIST</idno><idno type="RBID">Pascal:13-0228948</idno><idno type="wicri:Area/Main/Corpus">000B25</idno><idno type="wicri:Area/Main/Repository">000693</idno><idno type="wicri:Area/Chine/Extraction">000143</idno></publicationStmt><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>Cubic lattices</term><term>Ferroelectric materials</term><term>Indium Lead Niobates Mixed</term><term>Lead magnesium niobates</term><term>Lead titanates</term><term>Local structure</term><term>Monocrystals</term><term>Phase transformations</term><term>Polarization</term><term>Raman spectra</term><term>Relaxor</term><term>Spectral line shift</term><term>Transition element compounds</term><term>Vibrational modes</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Spectre Raman</term><term>Structure locale</term><term>Transformation phase</term><term>Déplacement raie</term><term>Polarisation</term><term>Mode vibration</term><term>Monocristal</term><term>Relaxeur</term><term>Matériau ferroélectrique</term><term>Réseau cubique</term><term>Titanate de plomb</term><term>Indium Plomb Niobate Mixte</term><term>Composé de métal de transition</term><term>Magnoniobate de plomb</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">Polarized Raman spectroscopy was performed to investigate the local lattice structure and phase transitions of unpoled 0.24Pb(In<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>-0.43Pb(Mg<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub>-0.33PbTiO<sub>3</sub> (0.24PIN-0.43PMN-0.33PT) single crystal in the temperature range from 30 °C to 260 °C. M<sub>A</sub>- and M<sub>c</sub>-type monoclinic phases were detected by micro-Raman spectra measured in different micro areas. Temperature dependence of Raman intensities, frequency shifts, mode merge and intensity ratios in the W and VH geometries were investigated. Our results indicated that the monoclinic-tetragonal (M-T) phase transition of the ternary relaxor-based ferroelectric single crystal 0.24PIN-0.43PMN-0.33PT occurs at 85 °C, which is verified by the mode merging from 520 cm<sup>-1</sup> and 580 cm<sup>-1</sup> to 500 cm<sup>-1</sup>, and the tetragonal-cubic (T-C) phase transition happens at 200 °C based on the vanishing mode at 780 cm<sup>-1</sup> measured in the VH polarization.</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0925-8388</s0></fA01><fA03 i2="1"><s0>J. alloys compd.</s0></fA03><fA05><s2>551</s2></fA05><fA08 i1="01" i2="1" l="ENG"><s1>Polarized Raman study on phase transitions in 0.24Pb(In<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>-0.43Pb(Mg<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub>-0.33PbTiO<sub>3</sub> single crystal</s1></fA08><fA11 i1="01" i2="1"><s1>FENGMINWU</s1></fA11><fA11 i1="02" i2="1"><s1>BINYANG</s1></fA11><fA11 i1="03" i2="1"><s1>ENWEISUN</s1></fA11><fA11 i1="04" i2="1"><s1>RUIZHANG</s1></fA11><fA11 i1="05" i2="1"><s1>DAPENGXU</s1></fA11><fA11 i1="06" i2="1"><s1>JING ZHOU</s1></fA11><fA11 i1="07" i2="1"><s1>WENWU CAO</s1></fA11><fA14 i1="01"><s1>Condensed Matter Science and Technology Institute, Harbin Institute of Technology</s1><s2>Harbin 150080</s2><s3>CHN</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>7 aut.</sZ></fA14><fA14 i1="02"><s1>College of Applied Science, Harbin University of Science and Technology</s1><s2>Harbin 150080</s2><s3>CHN</s3><sZ>1 aut.</sZ></fA14><fA14 i1="03"><s1>School of Physics, Jilin University</s1><s2>Changchun 130023</s2><s3>CHN</s3><sZ>5 aut.</sZ><sZ>6 aut.</sZ></fA14><fA14 i1="04"><s1>Materials Research Institute, The Pennsylvania State University</s1><s2>University Park, PA 16802</s2><s3>USA</s3><sZ>7 aut.</sZ></fA14><fA20><s1>98-100</s1></fA20><fA21><s1>2013</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>1151</s2><s5>354000502447070180</s5></fA43><fA44><s0>0000</s0><s1>© 2013 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>24 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>13-0228948</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Journal of alloys and compounds</s0></fA64><fA66 i1="01"><s0>GBR</s0></fA66><fC01 i1="01" l="ENG"><s0>Polarized Raman spectroscopy was performed to investigate the local lattice structure and phase transitions of unpoled 0.24Pb(In<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>-0.43Pb(Mg<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub>-0.33PbTiO<sub>3</sub> (0.24PIN-0.43PMN-0.33PT) single crystal in the temperature range from 30 °C to 260 °C. M<sub>A</sub>- and M<sub>c</sub>-type monoclinic phases were detected by micro-Raman spectra measured in different micro areas. Temperature dependence of Raman intensities, frequency shifts, mode merge and intensity ratios in the W and VH geometries were investigated. Our results indicated that the monoclinic-tetragonal (M-T) phase transition of the ternary relaxor-based ferroelectric single crystal 0.24PIN-0.43PMN-0.33PT occurs at 85 °C, which is verified by the mode merging from 520 cm<sup>-1</sup> and 580 cm<sup>-1</sup> to 500 cm<sup>-1</sup>, and the tetragonal-cubic (T-C) phase transition happens at 200 °C based on the vanishing mode at 780 cm<sup>-1</sup> measured in the VH polarization.</s0></fC01><fC02 i1="01" i2="3"><s0>001B70G84D</s0></fC02><fC02 i1="02" i2="3"><s0>001B60C20D</s0></fC02><fC02 i1="03" i2="3"><s0>001B60D70K</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>Spectre Raman</s0><s5>02</s5></fC03><fC03 i1="01" i2="3" l="ENG"><s0>Raman spectra</s0><s5>02</s5></fC03><fC03 i1="02" i2="X" l="FRE"><s0>Structure locale</s0><s5>03</s5></fC03><fC03 i1="02" i2="X" l="ENG"><s0>Local structure</s0><s5>03</s5></fC03><fC03 i1="02" i2="X" l="SPA"><s0>Estructura local</s0><s5>03</s5></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Transformation phase</s0><s5>04</s5></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Phase transformations</s0><s5>04</s5></fC03><fC03 i1="04" i2="3" l="FRE"><s0>Déplacement raie</s0><s5>05</s5></fC03><fC03 i1="04" i2="3" l="ENG"><s0>Spectral line shift</s0><s5>05</s5></fC03><fC03 i1="05" i2="3" l="FRE"><s0>Polarisation</s0><s5>06</s5></fC03><fC03 i1="05" i2="3" l="ENG"><s0>Polarization</s0><s5>06</s5></fC03><fC03 i1="06" i2="3" l="FRE"><s0>Mode vibration</s0><s5>07</s5></fC03><fC03 i1="06" i2="3" l="ENG"><s0>Vibrational modes</s0><s5>07</s5></fC03><fC03 i1="07" i2="3" l="FRE"><s0>Monocristal</s0><s5>15</s5></fC03><fC03 i1="07" i2="3" l="ENG"><s0>Monocrystals</s0><s5>15</s5></fC03><fC03 i1="08" i2="3" l="FRE"><s0>Relaxeur</s0><s5>16</s5></fC03><fC03 i1="08" i2="3" l="ENG"><s0>Relaxor</s0><s5>16</s5></fC03><fC03 i1="09" i2="3" l="FRE"><s0>Matériau ferroélectrique</s0><s5>17</s5></fC03><fC03 i1="09" i2="3" l="ENG"><s0>Ferroelectric materials</s0><s5>17</s5></fC03><fC03 i1="10" i2="3" l="FRE"><s0>Réseau cubique</s0><s5>18</s5></fC03><fC03 i1="10" i2="3" l="ENG"><s0>Cubic lattices</s0><s5>18</s5></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Titanate de plomb</s0><s2>NK</s2><s5>19</s5></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Lead titanates</s0><s2>NK</s2><s5>19</s5></fC03><fC03 i1="12" i2="X" l="FRE"><s0>Indium Plomb Niobate Mixte</s0><s2>NC</s2><s2>NA</s2><s5>20</s5></fC03><fC03 i1="12" i2="X" l="ENG"><s0>Indium Lead Niobates Mixed</s0><s2>NC</s2><s2>NA</s2><s5>20</s5></fC03><fC03 i1="12" i2="X" l="SPA"><s0>Mixto</s0><s2>NC</s2><s2>NA</s2><s5>20</s5></fC03><fC03 i1="13" i2="3" l="FRE"><s0>Composé de métal de transition</s0><s5>48</s5></fC03><fC03 i1="13" i2="3" l="ENG"><s0>Transition element compounds</s0><s5>48</s5></fC03><fC03 i1="14" i2="3" l="FRE"><s0>Magnoniobate de plomb</s0><s4>CD</s4><s5>96</s5></fC03><fC03 i1="14" i2="3" l="ENG"><s0>Lead magnesium niobates</s0><s4>CD</s4><s5>96</s5></fC03><fC03 i1="14" i2="3" l="SPA"><s0>Niobato de Magnesio y plomo</s0><s4>CD</s4><s5>96</s5></fC03><fN21><s1>210</s1></fN21></pA></standard></inist></record>Pour manipuler ce document sous Unix (Dilib)
EXPLOR_STEP=IndiumV3/Data/Chine/Analysis
HfdSelect -h $EXPLOR_STEP/biblio.hfd -nk 000143 | SxmlIndent | more
Ou
HfdSelect -h $EXPLOR_AREA/Data/Chine/Analysis/biblio.hfd -nk 000143 | SxmlIndent | more
Pour mettre un lien sur cette page dans le réseau Wicri
{{Explor lien
|wiki= *** parameter Area/wikiCode missing ***
|area= IndiumV3
|flux= Chine
|étape= Analysis
|type= RBID
|clé= Pascal:13-0228948
|texte= Polarized Raman study on phase transitions in 0.24Pb(In1/2Nb1/2)O3-0.43Pb(Mg1/3Nb2/3)O3-0.33PbTiO3 single crystal
}}
| This area was generated with Dilib version V0.5.77. |  |