Energy transfer and migration processes in Yb3+-ion-sensitized, rare-earth-ion-activated luminescent materials
Identifieur interne :
001367 ( Pascal/Curation );
précédent :
001366;
suivant :
001368
Energy transfer and migration processes in Yb3+-ion-sensitized, rare-earth-ion-activated luminescent materials
Auteurs : Y. Mita [
Japon] ;
T. Ide [
Japon] ;
T. Katase [
Japon] ;
H. Yamamoto [
Japon]
Source :
-
Journal of luminescence [ 0022-2313 ] ; 1997.
RBID : Pascal:97-0389705
Descripteurs français
- Pascal (Inist)
- Photoluminescence,
Transfert énergie,
Diffusion(transport),
Méthode Monte Carlo,
Etude théorique,
Etude expérimentale,
Polycristal,
Matériau dopé,
Codopage,
Addition thulium,
Addition ytterbium,
Yttrium fluorure,
Baryum fluorure,
Composé binaire,
Composé ternaire,
7855H,
BaY2F8:Tm Yb,
Ba F Y,
YF3:Tm Yb.
English descriptors
- KwdEn :
- Barium fluorides,
Binary compounds,
Codoping,
Diffusion,
Doped materials,
Energy transfer,
Experimental study,
Monte Carlo method,
Photoluminescence,
Polycrystals,
Ternary compounds,
Theoretical study,
Thulium additions,
Ytterbium additions,
Yttrium fluorides.
Abstract
Copyright (c) 1997 Elsevier Science B.V. All rights reserved.Energy migration processes between Yb3+ ions have been investigated in BaY2F8 and YF3 lattices. It has been found that energy transfer coefficient from Yb3+ to Tm3+ ions increases almost linearly with Yb3+ concentration at low Yb3+ concentrations and tends to saturate at higher Yb3+ concentrations. Comparison of the experimental results with calculated results, particularly on Monte Carlo simulation, has enabled to explain the above-mentioned results and to determine several parameters relevant to the migration processes.
pA |
A01 | 01 | 1 | | @0 0022-2313 |
---|
A02 | 01 | | | @0 JLUMA8 |
---|
A03 | | 1 | | @0 J. lumin. |
---|
A05 | | | | @2 72-74 |
---|
A08 | 01 | 1 | ENG | @1 Energy transfer and migration processes in Yb3+-ion-sensitized, rare-earth-ion-activated luminescent materials |
---|
A11 | 01 | 1 | | @1 MITA (Y.) |
---|
A11 | 02 | 1 | | @1 IDE (T.) |
---|
A11 | 03 | 1 | | @1 KATASE (T.) |
---|
A11 | 04 | 1 | | @1 YAMAMOTO (H.) |
---|
A14 | 01 | | | @1 Tokyo Engineering University, 1404, Katakura, Hachioji @2 Tokyo 192 @3 JPN @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. |
---|
A20 | | | | @1 959-960 |
---|
A21 | | | | @1 1997 |
---|
A23 | 01 | | | @0 ENG |
---|
A24 | 01 | | | @0 eng |
---|
A43 | 01 | | | @1 INIST @2 14666 @5 354000067607490728 |
---|
A44 | | | | @0 9000 @1 © 1997 Elsevier Science B.V. All rights reserved. |
---|
A47 | 01 | 1 | | @0 97-0389705 |
---|
A60 | | | | @1 P @2 C |
---|
A61 | | | | @0 A |
---|
A64 | 01 | 1 | | @0 Journal of luminescence |
---|
A66 | 01 | | | @0 NLD |
---|
C01 | 01 | | ENG | @0 Copyright (c) 1997 Elsevier Science B.V. All rights reserved.Energy migration processes between Yb3+ ions have been investigated in BaY2F8 and YF3 lattices. It has been found that energy transfer coefficient from Yb3+ to Tm3+ ions increases almost linearly with Yb3+ concentration at low Yb3+ concentrations and tends to saturate at higher Yb3+ concentrations. Comparison of the experimental results with calculated results, particularly on Monte Carlo simulation, has enabled to explain the above-mentioned results and to determine several parameters relevant to the migration processes. |
---|
C02 | 01 | 3 | | @0 001B70H55H |
---|
C03 | 01 | 3 | FRE | @0 Photoluminescence @5 01 |
---|
C03 | 01 | 3 | ENG | @0 Photoluminescence @5 01 |
---|
C03 | 02 | 3 | FRE | @0 Transfert énergie @5 02 |
---|
C03 | 02 | 3 | ENG | @0 Energy transfer @5 02 |
---|
C03 | 03 | 3 | FRE | @0 Diffusion(transport) @5 03 |
---|
C03 | 03 | 3 | ENG | @0 Diffusion @5 03 |
---|
C03 | 04 | 3 | FRE | @0 Méthode Monte Carlo @5 04 |
---|
C03 | 04 | 3 | ENG | @0 Monte Carlo method @5 04 |
---|
C03 | 05 | 3 | FRE | @0 Etude théorique @5 05 |
---|
C03 | 05 | 3 | ENG | @0 Theoretical study @5 05 |
---|
C03 | 06 | 3 | FRE | @0 Etude expérimentale @5 06 |
---|
C03 | 06 | 3 | ENG | @0 Experimental study @5 06 |
---|
C03 | 07 | 3 | FRE | @0 Polycristal @5 07 |
---|
C03 | 07 | 3 | ENG | @0 Polycrystals @5 07 |
---|
C03 | 08 | 3 | FRE | @0 Matériau dopé @5 08 |
---|
C03 | 08 | 3 | ENG | @0 Doped materials @5 08 |
---|
C03 | 09 | X | FRE | @0 Codopage @5 09 |
---|
C03 | 09 | X | ENG | @0 Codoping @5 09 |
---|
C03 | 09 | X | SPA | @0 Codrogado @5 09 |
---|
C03 | 10 | 3 | FRE | @0 Addition thulium @5 10 |
---|
C03 | 10 | 3 | ENG | @0 Thulium additions @5 10 |
---|
C03 | 11 | 3 | FRE | @0 Addition ytterbium @5 11 |
---|
C03 | 11 | 3 | ENG | @0 Ytterbium additions @5 11 |
---|
C03 | 12 | 3 | FRE | @0 Yttrium fluorure @2 NK @5 12 |
---|
C03 | 12 | 3 | ENG | @0 Yttrium fluorides @2 NK @5 12 |
---|
C03 | 13 | 3 | FRE | @0 Baryum fluorure @2 NK @5 13 |
---|
C03 | 13 | 3 | ENG | @0 Barium fluorides @2 NK @5 13 |
---|
C03 | 14 | 3 | FRE | @0 Composé binaire @5 14 |
---|
C03 | 14 | 3 | ENG | @0 Binary compounds @5 14 |
---|
C03 | 15 | 3 | FRE | @0 Composé ternaire @5 15 |
---|
C03 | 15 | 3 | ENG | @0 Ternary compounds @5 15 |
---|
C03 | 16 | 3 | FRE | @0 7855H @2 PAC @4 INC @5 56 |
---|
C03 | 17 | 3 | FRE | @0 BaY2F8:Tm Yb @4 INC @5 92 |
---|
C03 | 18 | 3 | FRE | @0 Ba F Y @4 INC @5 93 |
---|
C03 | 19 | 3 | FRE | @0 YF3:Tm Yb @4 INC @5 94 |
---|
C07 | 01 | 3 | FRE | @0 Métal transition composé @5 16 |
---|
C07 | 01 | 3 | ENG | @0 Transition element compounds @5 16 |
---|
C07 | 02 | 3 | FRE | @0 Composé minéral @5 17 |
---|
C07 | 02 | 3 | ENG | @0 Inorganic compounds @5 17 |
---|
N21 | | | | @1 237 |
---|
|
pR |
A30 | 01 | 1 | ENG | @1 ICL'96 Hala |
---|
|
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Le document en format XML
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-ion-sensitized, rare-earth-ion-activated luminescent materials</title>
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-ion-sensitized, rare-earth-ion-activated luminescent materials</title>
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<country>Japon</country>
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<author><name sortKey="Yamamoto, H" sort="Yamamoto, H" uniqKey="Yamamoto H" first="H." last="Yamamoto">H. Yamamoto</name>
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<series><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
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<imprint><date when="1997">1997</date>
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<idno type="ISSN">0022-2313</idno>
</seriesStmt>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Barium fluorides</term>
<term>Binary compounds</term>
<term>Codoping</term>
<term>Diffusion</term>
<term>Doped materials</term>
<term>Energy transfer</term>
<term>Experimental study</term>
<term>Monte Carlo method</term>
<term>Photoluminescence</term>
<term>Polycrystals</term>
<term>Ternary compounds</term>
<term>Theoretical study</term>
<term>Thulium additions</term>
<term>Ytterbium additions</term>
<term>Yttrium fluorides</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Photoluminescence</term>
<term>Transfert énergie</term>
<term>Diffusion(transport)</term>
<term>Méthode Monte Carlo</term>
<term>Etude théorique</term>
<term>Etude expérimentale</term>
<term>Polycristal</term>
<term>Matériau dopé</term>
<term>Codopage</term>
<term>Addition thulium</term>
<term>Addition ytterbium</term>
<term>Yttrium fluorure</term>
<term>Baryum fluorure</term>
<term>Composé binaire</term>
<term>Composé ternaire</term>
<term>7855H</term>
<term>BaY2F8:Tm Yb</term>
<term>Ba F Y</term>
<term>YF3:Tm Yb</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">Copyright (c) 1997 Elsevier Science B.V. All rights reserved.Energy migration processes between Yb<sup>3+</sup>
ions have been investigated in BaY<sub>2</sub>
F<sub>8</sub>
and YF<sub>3</sub>
lattices. It has been found that energy transfer coefficient from Yb<sup>3+</sup>
to Tm<sup>3+</sup>
ions increases almost linearly with Yb<sup>3+</sup>
concentration at low Yb<sup>3+</sup>
concentrations and tends to saturate at higher Yb<sup>3+</sup>
concentrations. Comparison of the experimental results with calculated results, particularly on Monte Carlo simulation, has enabled to explain the above-mentioned results and to determine several parameters relevant to the migration processes.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0022-2313</s0>
</fA01>
<fA02 i1="01"><s0>JLUMA8</s0>
</fA02>
<fA03 i2="1"><s0>J. lumin.</s0>
</fA03>
<fA05><s2>72-74</s2>
</fA05>
<fA08 i1="01" i2="1" l="ENG"><s1>Energy transfer and migration processes in Yb<sup>3+</sup>
-ion-sensitized, rare-earth-ion-activated luminescent materials</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>MITA (Y.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>IDE (T.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>KATASE (T.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>YAMAMOTO (H.)</s1>
</fA11>
<fA14 i1="01"><s1>Tokyo Engineering University, 1404, Katakura, Hachioji</s1>
<s2>Tokyo 192</s2>
<s3>JPN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14>
<fA20><s1>959-960</s1>
</fA20>
<fA21><s1>1997</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA24 i1="01"><s0>eng</s0>
</fA24>
<fA43 i1="01"><s1>INIST</s1>
<s2>14666</s2>
<s5>354000067607490728</s5>
</fA43>
<fA44><s0>9000</s0>
<s1>© 1997 Elsevier Science B.V. All rights reserved.</s1>
</fA44>
<fA47 i1="01" i2="1"><s0>97-0389705</s0>
</fA47>
<fA60><s1>P</s1>
<s2>C</s2>
</fA60>
<fA64 i1="01" i2="1"><s0>Journal of luminescence</s0>
</fA64>
<fA66 i1="01"><s0>NLD</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>Copyright (c) 1997 Elsevier Science B.V. All rights reserved.Energy migration processes between Yb<sup>3+</sup>
ions have been investigated in BaY<sub>2</sub>
F<sub>8</sub>
and YF<sub>3</sub>
lattices. It has been found that energy transfer coefficient from Yb<sup>3+</sup>
to Tm<sup>3+</sup>
ions increases almost linearly with Yb<sup>3+</sup>
concentration at low Yb<sup>3+</sup>
concentrations and tends to saturate at higher Yb<sup>3+</sup>
concentrations. Comparison of the experimental results with calculated results, particularly on Monte Carlo simulation, has enabled to explain the above-mentioned results and to determine several parameters relevant to the migration processes.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70H55H</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Photoluminescence</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Photoluminescence</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Transfert énergie</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Energy transfer</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Diffusion(transport)</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Diffusion</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Méthode Monte Carlo</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Monte Carlo method</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Etude théorique</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Theoretical study</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Etude expérimentale</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Experimental study</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Polycristal</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Polycrystals</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE"><s0>Codopage</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG"><s0>Codoping</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA"><s0>Codrogado</s0>
<s5>09</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>10</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Addition ytterbium</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Ytterbium additions</s0>
<s5>11</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Yttrium fluorure</s0>
<s2>NK</s2>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Yttrium fluorides</s0>
<s2>NK</s2>
<s5>12</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Baryum fluorure</s0>
<s2>NK</s2>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Barium fluorides</s0>
<s2>NK</s2>
<s5>13</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Composé binaire</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Binary compounds</s0>
<s5>14</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Composé ternaire</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Ternary compounds</s0>
<s5>15</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>7855H</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>BaY2F8:Tm Yb</s0>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Ba F Y</s0>
<s4>INC</s4>
<s5>93</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>YF3:Tm Yb</s0>
<s4>INC</s4>
<s5>94</s5>
</fC03>
<fC07 i1="01" i2="3" l="FRE"><s0>Métal transition composé</s0>
<s5>16</s5>
</fC07>
<fC07 i1="01" i2="3" l="ENG"><s0>Transition element compounds</s0>
<s5>16</s5>
</fC07>
<fC07 i1="02" i2="3" l="FRE"><s0>Composé minéral</s0>
<s5>17</s5>
</fC07>
<fC07 i1="02" i2="3" l="ENG"><s0>Inorganic compounds</s0>
<s5>17</s5>
</fC07>
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<pR><fA30 i1="01" i2="1" l="ENG"><s1>ICL'96 Hala</s1>
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