Lattice dynamics of fluoride scheelites: I. Raman and infrared study of LiYF4 and LiLnF4 (Ln = Ho, Er, Tm and Yb)
Identifieur interne : 001327 ( Pascal/Checkpoint ); précédent : 001326; suivant : 001328Lattice dynamics of fluoride scheelites: I. Raman and infrared study of LiYF4 and LiLnF4 (Ln = Ho, Er, Tm and Yb)
Auteurs : S. Salaün [France] ; M. T. Fornoni [France] ; A. Bulou [France] ; M. Rousseau [France] ; P. Simon [France] ; J. Y. Gesland [France]Source :
- Journal of physics. Condensed matter [ 0953-8984 ] ; 1997.
Descripteurs français
- Pascal (Inist)
- Mode phonon, Dynamique réticulaire, Spectre Raman, Spectre IR, Spectre réflexion, Polarisation, Structure scheelite, Interaction électron phonon, Champ cristallin, Décomposition niveau énergie, Charge effective, Lithium fluorure, Yttrium fluorure, Holmium fluorure, Erbium fluorure, Thulium fluorure, Ytterbium fluorure, LiErF4, Er F Li, LiTmF4, F Li Tm, 6320D, LiYbF4, F Li Yb, Composé ternaire, Etude expérimentale, LiYF4, F Li Y, LiHoF4, F Ho Li.
English descriptors
- KwdEn :
- Crystal field, Effective charge, Electron phonon interaction, Energy-level splitting, Erbium fluorides, Experimental study, Holmium fluorides, Infrared spectra, Lattice dynamics, Lithium fluorides, Phonon mode, Polarization, Raman spectra, Reflection spectrum, Scheelite structure, Ternary compounds, Thulium fluorides, Ytterbium fluorides, Yttrium fluorides.
Abstract
IR and Raman active modes have been measured in several fluoride scheelites, namely the laser matrix LiYF4 (studied as a reference) and four LiLnF4 compounds (Ln = Ho, Er, Tm and Yb). The observed phonons have been assigned in accordance with the various irreducible representations of the point group of the crystal. In LiYF4 three modes never observed before have been measured. The polarized experimental IR reflection spectra have been analysed through a 'four-parameters' model to give the mode frequencies and dampings. For the whole set of the compounds, the frequency dependence of the dielectric function, optical indices and absorption coefficient have been deduced from the IR study. The electronic Raman effect has been shown in the low-temperature Raman spectra for Ln = Tm, Ho and Yb. The corresponding measured wavenumbers are compared with the calculated energies between crystal-field levels of LSJ states, each being associated to an irreducible representation of the ion-site group S4.
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Simon</name><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>CRPHT, CNRS-1D, Avenue de la Recherche Scientifique</s1><s2>45071 Orléans</s2><s3>FRA</s3><sZ>5 aut.</sZ></inist:fA14><country>France</country><wicri:noRegion>45071 Orléans</wicri:noRegion><wicri:noRegion>Avenue de la Recherche Scientifique</wicri:noRegion><wicri:noRegion>45071 Orléans</wicri:noRegion></affiliation></author><author><name sortKey="Gesland, J Y" sort="Gesland, J Y" uniqKey="Gesland J" first="J. Y." last="Gesland">J. Y. Gesland</name><affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Laboratoire de Physique de l'Etat Condensé, Faculté des Sciences, Université du Maine, Avenue O Messiaen</s1><s2>72017 Le Mans</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country><wicri:noRegion>72017 Le Mans</wicri:noRegion><wicri:noRegion>Avenue O Messiaen</wicri:noRegion><wicri:noRegion>72017 Le Mans</wicri:noRegion><orgName type="university">Université du Maine</orgName><placeName><settlement type="city">Le Mans</settlement><region type="region" nuts="2">Pays de la Loire</region></placeName></affiliation></author></titleStmt><publicationStmt><idno type="wicri:source">INIST</idno><idno type="inist">97-0435689</idno><date when="1997">1997</date><idno type="stanalyst">PASCAL 97-0435689 INIST</idno><idno type="RBID">Pascal:97-0435689</idno><idno type="wicri:Area/Pascal/Corpus">001359</idno><idno type="wicri:Area/Pascal/Curation">001359</idno><idno type="wicri:Area/Pascal/Checkpoint">001327</idno><idno type="wicri:explorRef" wicri:stream="Pascal" wicri:step="Checkpoint">001327</idno></publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Lattice dynamics of fluoride scheelites: I. Raman and infrared study of LiYF<sub>4</sub> and LiLnF<sub>4</sub> (Ln = Ho, Er, Tm and Yb)</title><author><name sortKey="Salaun, S" sort="Salaun, S" uniqKey="Salaun S" first="S." last="Salaün">S. Salaün</name><affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Laboratoire de Physique de l'Etat Condensé, Faculté des Sciences, Université du Maine, Avenue O Messiaen</s1><s2>72017 Le Mans</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Pays de la Loire</region><settlement type="city">Le Mans</settlement><settlement type="city">Le Mans</settlement></placeName><orgName type="university">Université du Maine</orgName></affiliation></author><author><name sortKey="Fornoni, M T" sort="Fornoni, M T" uniqKey="Fornoni M" first="M. T." last="Fornoni">M. T. Fornoni</name><affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Laboratoire de Physique de l'Etat Condensé, Faculté des Sciences, Université du Maine, Avenue O Messiaen</s1><s2>72017 Le Mans</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country><wicri:noRegion>72017 Le Mans</wicri:noRegion><wicri:noRegion>Avenue O Messiaen</wicri:noRegion><wicri:noRegion>72017 Le Mans</wicri:noRegion><orgName type="university">Université du Maine</orgName><placeName><settlement type="city">Le Mans</settlement><region type="region" nuts="2">Pays de la Loire</region></placeName></affiliation></author><author><name sortKey="Bulou, A" sort="Bulou, A" uniqKey="Bulou A" first="A." last="Bulou">A. Bulou</name><affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Laboratoire de Physique de l'Etat Condensé, Faculté des Sciences, Université du Maine, Avenue O Messiaen</s1><s2>72017 Le Mans</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country><wicri:noRegion>72017 Le Mans</wicri:noRegion><wicri:noRegion>Avenue O Messiaen</wicri:noRegion><wicri:noRegion>72017 Le Mans</wicri:noRegion><orgName type="university">Université du Maine</orgName><placeName><settlement type="city">Le Mans</settlement><region type="region" nuts="2">Pays de la Loire</region></placeName></affiliation></author><author><name sortKey="Rousseau, M" sort="Rousseau, M" uniqKey="Rousseau M" first="M." last="Rousseau">M. Rousseau</name><affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Laboratoire de Physique de l'Etat Condensé, Faculté des Sciences, Université du Maine, Avenue O Messiaen</s1><s2>72017 Le Mans</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country><wicri:noRegion>72017 Le Mans</wicri:noRegion><wicri:noRegion>Avenue O Messiaen</wicri:noRegion><wicri:noRegion>72017 Le Mans</wicri:noRegion><orgName type="university">Université du Maine</orgName><placeName><settlement type="city">Le Mans</settlement><region type="region" nuts="2">Pays de la Loire</region></placeName></affiliation></author><author><name sortKey="Simon, P" sort="Simon, P" uniqKey="Simon P" first="P." last="Simon">P. Simon</name><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>CRPHT, CNRS-1D, Avenue de la Recherche Scientifique</s1><s2>45071 Orléans</s2><s3>FRA</s3><sZ>5 aut.</sZ></inist:fA14><country>France</country><wicri:noRegion>45071 Orléans</wicri:noRegion><wicri:noRegion>Avenue de la Recherche Scientifique</wicri:noRegion><wicri:noRegion>45071 Orléans</wicri:noRegion></affiliation></author><author><name sortKey="Gesland, J Y" sort="Gesland, J Y" uniqKey="Gesland J" first="J. Y." last="Gesland">J. Y. Gesland</name><affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Laboratoire de Physique de l'Etat Condensé, Faculté des Sciences, Université du Maine, Avenue O Messiaen</s1><s2>72017 Le Mans</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country><wicri:noRegion>72017 Le Mans</wicri:noRegion><wicri:noRegion>Avenue O Messiaen</wicri:noRegion><wicri:noRegion>72017 Le Mans</wicri:noRegion><orgName type="university">Université du Maine</orgName><placeName><settlement type="city">Le Mans</settlement><region type="region" nuts="2">Pays de la Loire</region></placeName></affiliation></author></analytic><series><title level="j" type="main">Journal of physics. Condensed matter</title><title level="j" type="abbreviated">J. phys., Condens. matter</title><idno type="ISSN">0953-8984</idno><imprint><date when="1997">1997</date></imprint></series></biblStruct></sourceDesc><seriesStmt><title level="j" type="main">Journal of physics. Condensed matter</title><title level="j" type="abbreviated">J. phys., Condens. matter</title><idno type="ISSN">0953-8984</idno></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Crystal field</term><term>Effective charge</term><term>Electron phonon interaction</term><term>Energy-level splitting</term><term>Erbium fluorides</term><term>Experimental study</term><term>Holmium fluorides</term><term>Infrared spectra</term><term>Lattice dynamics</term><term>Lithium fluorides</term><term>Phonon mode</term><term>Polarization</term><term>Raman spectra</term><term>Reflection spectrum</term><term>Scheelite structure</term><term>Ternary compounds</term><term>Thulium fluorides</term><term>Ytterbium fluorides</term><term>Yttrium fluorides</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Mode phonon</term><term>Dynamique réticulaire</term><term>Spectre Raman</term><term>Spectre IR</term><term>Spectre réflexion</term><term>Polarisation</term><term>Structure scheelite</term><term>Interaction électron phonon</term><term>Champ cristallin</term><term>Décomposition niveau énergie</term><term>Charge effective</term><term>Lithium fluorure</term><term>Yttrium fluorure</term><term>Holmium fluorure</term><term>Erbium fluorure</term><term>Thulium fluorure</term><term>Ytterbium fluorure</term><term>LiErF4</term><term>Er F Li</term><term>LiTmF4</term><term>F Li Tm</term><term>6320D</term><term>LiYbF4</term><term>F Li Yb</term><term>Composé ternaire</term><term>Etude expérimentale</term><term>LiYF4</term><term>F Li Y</term><term>LiHoF4</term><term>F Ho Li</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">IR and Raman active modes have been measured in several fluoride scheelites, namely the laser matrix LiYF<sub>4</sub> (studied as a reference) and four LiLnF<sub>4</sub> compounds (Ln = Ho, Er, Tm and Yb). The observed phonons have been assigned in accordance with the various irreducible representations of the point group of the crystal. In LiYF<sub>4</sub> three modes never observed before have been measured. The polarized experimental IR reflection spectra have been analysed through a 'four-parameters' model to give the mode frequencies and dampings. For the whole set of the compounds, the frequency dependence of the dielectric function, optical indices and absorption coefficient have been deduced from the IR study. The electronic Raman effect has been shown in the low-temperature Raman spectra for Ln = Tm, Ho and Yb. The corresponding measured wavenumbers are compared with the calculated energies between crystal-field levels of LSJ states, each being associated to an irreducible representation of the ion-site group S<sub>4</sub>.</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</s0></fA03><fA05><s2>9</s2></fA05><fA06><s2>32</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>Lattice dynamics of fluoride scheelites: I. Raman and infrared study of LiYF<sub>4</sub> and LiLnF<sub>4</sub> (Ln = Ho, Er, Tm and Yb)</s1></fA08><fA11 i1="01" i2="1"><s1>SALAÜN (S.)</s1></fA11><fA11 i1="02" i2="1"><s1>FORNONI (M. T.)</s1></fA11><fA11 i1="03" i2="1"><s1>BULOU (A.)</s1></fA11><fA11 i1="04" i2="1"><s1>ROUSSEAU (M.)</s1></fA11><fA11 i1="05" i2="1"><s1>SIMON (P.)</s1></fA11><fA11 i1="06" i2="1"><s1>GESLAND (J. Y.)</s1></fA11><fA14 i1="01"><s1>Laboratoire de Physique de l'Etat Condensé, Faculté des Sciences, Université du Maine, Avenue O Messiaen</s1><s2>72017 Le Mans</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>6 aut.</sZ></fA14><fA14 i1="02"><s1>CRPHT, CNRS-1D, Avenue de la Recherche Scientifique</s1><s2>45071 Orléans</s2><s3>FRA</s3><sZ>5 aut.</sZ></fA14><fA20><s1>6941-6956</s1></fA20><fA21><s1>1997</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>577E2</s2><s5>354000068177700160</s5></fA43><fA44><s0>0000</s0><s1>© 1997 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>31 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>97-0435689</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Journal of physics. Condensed matter</s0></fA64><fA66 i1="01"><s0>GBR</s0></fA66><fC01 i1="01" l="ENG"><s0>IR and Raman active modes have been measured in several fluoride scheelites, namely the laser matrix LiYF<sub>4</sub> (studied as a reference) and four LiLnF<sub>4</sub> compounds (Ln = Ho, Er, Tm and Yb). The observed phonons have been assigned in accordance with the various irreducible representations of the point group of the crystal. In LiYF<sub>4</sub> three modes never observed before have been measured. The polarized experimental IR reflection spectra have been analysed through a 'four-parameters' model to give the mode frequencies and dampings. For the whole set of the compounds, the frequency dependence of the dielectric function, optical indices and absorption coefficient have been deduced from the IR study. The electronic Raman effect has been shown in the low-temperature Raman spectra for Ln = Tm, Ho and Yb. The corresponding measured wavenumbers are compared with the calculated energies between crystal-field levels of LSJ states, each being associated to an irreducible representation of the ion-site group S<sub>4</sub>.</s0></fC01><fC02 i1="01" i2="3"><s0>001B60C20D</s0></fC02><fC03 i1="01" i2="X" l="FRE"><s0>Mode phonon</s0><s5>01</s5></fC03><fC03 i1="01" i2="X" l="ENG"><s0>Phonon mode</s0><s5>01</s5></fC03><fC03 i1="01" i2="X" l="SPA"><s0>Modo fonón</s0><s5>01</s5></fC03><fC03 i1="02" i2="3" l="FRE"><s0>Dynamique réticulaire</s0><s5>02</s5></fC03><fC03 i1="02" i2="3" l="ENG"><s0>Lattice dynamics</s0><s5>02</s5></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Spectre Raman</s0><s5>03</s5></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Raman spectra</s0><s5>03</s5></fC03><fC03 i1="04" i2="3" l="FRE"><s0>Spectre IR</s0><s5>04</s5></fC03><fC03 i1="04" i2="3" l="ENG"><s0>Infrared spectra</s0><s5>04</s5></fC03><fC03 i1="05" i2="X" l="FRE"><s0>Spectre réflexion</s0><s5>05</s5></fC03><fC03 i1="05" i2="X" l="ENG"><s0>Reflection spectrum</s0><s5>05</s5></fC03><fC03 i1="05" i2="X" l="SPA"><s0>Espectro reflexión</s0><s5>05</s5></fC03><fC03 i1="06" i2="3" l="FRE"><s0>Polarisation</s0><s5>06</s5></fC03><fC03 i1="06" i2="3" l="ENG"><s0>Polarization</s0><s5>06</s5></fC03><fC03 i1="07" i2="X" l="FRE"><s0>Structure scheelite</s0><s5>07</s5></fC03><fC03 i1="07" i2="X" l="ENG"><s0>Scheelite structure</s0><s5>07</s5></fC03><fC03 i1="07" i2="X" l="SPA"><s0>Estructura scheelita</s0><s5>07</s5></fC03><fC03 i1="08" i2="X" l="FRE"><s0>Interaction électron phonon</s0><s5>08</s5></fC03><fC03 i1="08" i2="X" l="ENG"><s0>Electron phonon interaction</s0><s5>08</s5></fC03><fC03 i1="08" i2="X" l="GER"><s0>Elektron Phonon Wechselwirkung</s0><s5>08</s5></fC03><fC03 i1="08" i2="X" l="SPA"><s0>Interacción electrón fonón</s0><s5>08</s5></fC03><fC03 i1="09" i2="3" l="FRE"><s0>Champ cristallin</s0><s5>09</s5></fC03><fC03 i1="09" i2="3" l="ENG"><s0>Crystal field</s0><s5>09</s5></fC03><fC03 i1="10" i2="3" l="FRE"><s0>Décomposition niveau énergie</s0><s5>10</s5></fC03><fC03 i1="10" i2="3" l="ENG"><s0>Energy-level splitting</s0><s5>10</s5></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Charge effective</s0><s5>11</s5></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Effective charge</s0><s5>11</s5></fC03><fC03 i1="12" i2="3" l="FRE"><s0>Lithium fluorure</s0><s2>NK</s2><s5>12</s5></fC03><fC03 i1="12" i2="3" l="ENG"><s0>Lithium fluorides</s0><s2>NK</s2><s5>12</s5></fC03><fC03 i1="13" i2="3" l="FRE"><s0>Yttrium fluorure</s0><s2>NK</s2><s5>13</s5></fC03><fC03 i1="13" i2="3" l="ENG"><s0>Yttrium fluorides</s0><s2>NK</s2><s5>13</s5></fC03><fC03 i1="14" i2="3" l="FRE"><s0>Holmium fluorure</s0><s2>NK</s2><s5>14</s5></fC03><fC03 i1="14" i2="3" l="ENG"><s0>Holmium fluorides</s0><s2>NK</s2><s5>14</s5></fC03><fC03 i1="15" i2="3" l="FRE"><s0>Erbium fluorure</s0><s2>NK</s2><s5>15</s5></fC03><fC03 i1="15" i2="3" l="ENG"><s0>Erbium fluorides</s0><s2>NK</s2><s5>15</s5></fC03><fC03 i1="16" i2="3" l="FRE"><s0>Thulium fluorure</s0><s2>NK</s2><s5>16</s5></fC03><fC03 i1="16" i2="3" l="ENG"><s0>Thulium fluorides</s0><s2>NK</s2><s5>16</s5></fC03><fC03 i1="17" i2="3" l="FRE"><s0>Ytterbium fluorure</s0><s2>NK</s2><s5>17</s5></fC03><fC03 i1="17" i2="3" l="ENG"><s0>Ytterbium fluorides</s0><s2>NK</s2><s5>17</s5></fC03><fC03 i1="18" i2="3" l="FRE"><s0>LiErF4</s0><s4>INC</s4><s5>52</s5></fC03><fC03 i1="19" i2="3" l="FRE"><s0>Er F Li</s0><s4>INC</s4><s5>53</s5></fC03><fC03 i1="20" i2="3" l="FRE"><s0>LiTmF4</s0><s4>INC</s4><s5>54</s5></fC03><fC03 i1="21" i2="3" l="FRE"><s0>F Li Tm</s0><s4>INC</s4><s5>55</s5></fC03><fC03 i1="22" i2="3" l="FRE"><s0>6320D</s0><s2>PAC</s2><s4>INC</s4><s5>56</s5></fC03><fC03 i1="23" i2="3" l="FRE"><s0>LiYbF4</s0><s4>INC</s4><s5>60</s5></fC03><fC03 i1="24" i2="3" l="FRE"><s0>F Li Yb</s0><s4>INC</s4><s5>61</s5></fC03><fC03 i1="25" i2="3" l="FRE"><s0>Composé ternaire</s0><s5>83</s5></fC03><fC03 i1="25" i2="3" l="ENG"><s0>Ternary compounds</s0><s5>83</s5></fC03><fC03 i1="26" i2="3" l="FRE"><s0>Etude expérimentale</s0><s5>84</s5></fC03><fC03 i1="26" i2="3" l="ENG"><s0>Experimental study</s0><s5>84</s5></fC03><fC03 i1="27" i2="3" l="FRE"><s0>LiYF4</s0><s4>INC</s4><s5>92</s5></fC03><fC03 i1="28" i2="3" l="FRE"><s0>F Li Y</s0><s4>INC</s4><s5>93</s5></fC03><fC03 i1="29" i2="3" l="FRE"><s0>LiHoF4</s0><s4>INC</s4><s5>94</s5></fC03><fC03 i1="30" i2="3" l="FRE"><s0>F Ho Li</s0><s4>INC</s4><s5>95</s5></fC03><fC07 i1="01" i2="3" l="FRE"><s0>Lanthanide composé</s0><s5>18</s5></fC07><fC07 i1="01" i2="3" l="ENG"><s0>Rare earth compounds</s0><s5>18</s5></fC07><fC07 i1="02" i2="3" l="FRE"><s0>Métal transition composé</s0><s5>81</s5></fC07><fC07 i1="02" i2="3" l="ENG"><s0>Transition element compounds</s0><s5>81</s5></fC07><fC07 i1="03" i2="3" l="FRE"><s0>Composé minéral</s0><s5>82</s5></fC07><fC07 i1="03" i2="3" l="ENG"><s0>Inorganic compounds</s0><s5>82</s5></fC07><fN21><s1>265</s1></fN21></pA></standard></inist><affiliations><list><country><li>France</li></country><region><li>Pays de la Loire</li></region><settlement><li>Le Mans</li></settlement><orgName><li>Université du Maine</li></orgName></list><tree><country name="France"><region name="Pays de la Loire"><name sortKey="Salaun, S" sort="Salaun, S" uniqKey="Salaun S" first="S." last="Salaün">S. Salaün</name></region><name sortKey="Bulou, A" sort="Bulou, A" uniqKey="Bulou A" first="A." last="Bulou">A. Bulou</name><name sortKey="Fornoni, M T" sort="Fornoni, M T" uniqKey="Fornoni M" first="M. T." last="Fornoni">M. T. Fornoni</name><name sortKey="Gesland, J Y" sort="Gesland, J Y" uniqKey="Gesland J" first="J. Y." last="Gesland">J. Y. Gesland</name><name sortKey="Rousseau, M" sort="Rousseau, M" uniqKey="Rousseau M" first="M." last="Rousseau">M. Rousseau</name><name sortKey="Simon, P" sort="Simon, P" uniqKey="Simon P" first="P." last="Simon">P. Simon</name></country></tree></affiliations></record>Pour manipuler ce document sous Unix (Dilib)
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|texte= Lattice dynamics of fluoride scheelites: I. Raman and infrared study of LiYF4 and LiLnF4 (Ln = Ho, Er, Tm and Yb)
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