Characterisation and modelling of the 450 K TSL peak of alpha alumina by the simultaneous analysis of TSL, TSC and TSEE
Identifieur interne :
006277 ( PascalFrancis/Corpus );
précédent :
006276;
suivant :
006278
Characterisation and modelling of the 450 K TSL peak of alpha alumina by the simultaneous analysis of TSL, TSC and TSEE
Auteurs : S. Guissi ;
P. Iacconi ;
R. Bindi ;
D. LaprazSource :
-
Radiation protection dosimetry [ 0144-8420 ] ; 1999.
RBID : Pascal:99-0414304
Descripteurs français
English descriptors
Abstract
The TSL peak D' (450 K) of α-alumina is commonly used for ionising radiation dosimetry. Generally, it is simultaneously accompanied by TSC and TSEE peaks. In this work, peaks D' are characterised by using a previously described model in which the defect associated with peak D' is considered as an electron trap and the TSEE resulting from the thermionic effect. The comparison with experimental data does not invalidate these basic hypotheses.
Notice en format standard (ISO 2709)
Pour connaître la documentation sur le format Inist Standard.
| pA |
| A01 | 01 | 1 | | @0 0144-8420 |
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| A02 | 01 | | | @0 RPDODE |
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| A03 | | 1 | | @0 Radiat. prot. dosim. |
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| A05 | | | | @2 84 |
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| A06 | | | | @2 1-4 |
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| A08 | 01 | 1 | ENG | @1 Characterisation and modelling of the 450 K TSL peak of alpha alumina by the simultaneous analysis of TSL, TSC and TSEE |
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| A09 | 01 | 1 | ENG | @1 Solid state dosimetry. Part I |
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| A11 | 01 | 1 | | @1 GUISSI (S.) |
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| A11 | 02 | 1 | | @1 IACCONI (P.) |
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| A11 | 03 | 1 | | @1 BINDI (R.) |
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| A11 | 04 | 1 | | @1 LAPRAZ (D.) |
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| A12 | 01 | 1 | | @1 DELGADO (A.) @9 ed. |
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| A12 | 02 | 1 | | @1 GOMEZ ROS (J. M.) @9 ed. |
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| A12 | 03 | 1 | | @1 BOS (A. J. J.) @9 ed. |
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| A12 | 04 | 1 | | @1 BØTTER-JENSEN (L.) @9 ed. |
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| A12 | 05 | 1 | | @1 HOROWITZ (Y. S.) @9 ed. |
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| A12 | 06 | 1 | | @1 JULIUS (H. W.) @9 ed. |
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| A12 | 07 | 1 | | @1 KLEMIC (G.) @9 ed. |
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| A12 | 08 | 1 | | @1 KRON (T.) @9 ed. |
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| A14 | 01 | | | @1 LPES-CRESA, Université de Nice-Sophia Antipolis, Parc Valrose @2 06108 - Nice @3 FRA @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. |
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| A15 | 01 | | | @1 CIEMAT @3 ESP @Z 1 aut. |
|---|
| A15 | 02 | | | @1 Delft T. University @3 NLD @Z 3 aut. |
|---|
| A15 | 03 | | | @1 Ben Gurion University @3 ISR @Z 5 aut. |
|---|
| A15 | 04 | | | @1 TNO @3 NLD @Z 6 aut. |
|---|
| A15 | 05 | | | @1 EML (DOE) @3 USA @Z 7 aut. |
|---|
| A15 | 06 | | | @1 Newcastle Mater Misericordiae Hospital @3 AUS @Z 8 aut. |
|---|
| A20 | | | | @1 247-251 |
|---|
| A21 | | | | @1 1999 |
|---|
| A23 | 01 | | | @0 ENG |
|---|
| A43 | 01 | | | @1 INIST @2 19318 @5 354000085782220540 |
|---|
| A44 | | | | @0 0000 @1 © 1999 INIST-CNRS. All rights reserved. |
|---|
| A45 | | | | @0 8 ref. |
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| A47 | 01 | 1 | | @0 99-0414304 |
|---|
| A60 | | | | @1 P @2 C |
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| A61 | | | | @0 A |
|---|
| A64 | 01 | 1 | | @0 Radiation protection dosimetry |
|---|
| A66 | 01 | | | @0 GBR |
|---|
| C01 | 01 | | ENG | @0 The TSL peak D' (450 K) of α-alumina is commonly used for ionising radiation dosimetry. Generally, it is simultaneously accompanied by TSC and TSEE peaks. In this work, peaks D' are characterised by using a previously described model in which the defect associated with peak D' is considered as an electron trap and the TSEE resulting from the thermionic effect. The comparison with experimental data does not invalidate these basic hypotheses. |
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| C02 | 01 | X | | @0 002A08F05 |
|---|
| C03 | 01 | X | FRE | @0 Mesure simultanée @5 01 |
|---|
| C03 | 01 | X | ENG | @0 Simultaneous measurement @5 01 |
|---|
| C03 | 01 | X | SPA | @0 Medición simultánea @5 01 |
|---|
| C03 | 02 | X | FRE | @0 Modélisation @5 02 |
|---|
| C03 | 02 | X | ENG | @0 Modeling @5 02 |
|---|
| C03 | 02 | X | SPA | @0 Modelización @5 02 |
|---|
| C03 | 03 | X | FRE | @0 Dosimètre @5 03 |
|---|
| C03 | 03 | X | ENG | @0 Dosimeter @5 03 |
|---|
| C03 | 03 | X | SPA | @0 Dosímetro @5 03 |
|---|
| C03 | 04 | X | FRE | @0 Thermoluminescence @5 04 |
|---|
| C03 | 04 | X | ENG | @0 Thermoluminescence @5 04 |
|---|
| C03 | 04 | X | SPA | @0 Termoluminescencia @5 04 |
|---|
| C03 | 05 | X | FRE | @0 Emission exoélectronique @5 05 |
|---|
| C03 | 05 | X | ENG | @0 Exoelectron emission @5 05 |
|---|
| C03 | 05 | X | SPA | @0 Emisión exoelectrónica @5 05 |
|---|
| C03 | 06 | X | FRE | @0 Conductivité électrique @5 06 |
|---|
| C03 | 06 | X | ENG | @0 Electrical conductivity @5 06 |
|---|
| C03 | 06 | X | SPA | @0 Conductividad eléctrica @5 06 |
|---|
| C03 | 07 | X | FRE | @0 Alumine @2 NK @5 07 |
|---|
| C03 | 07 | X | ENG | @0 Alumina @2 NK @5 07 |
|---|
| C03 | 07 | X | SPA | @0 Alúmina @2 NK @5 07 |
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| C03 | 08 | X | FRE | @0 Piégeage @5 09 |
|---|
| C03 | 08 | X | ENG | @0 Trapping @5 09 |
|---|
| C03 | 08 | X | SPA | @0 Captura @5 09 |
|---|
| C03 | 09 | X | FRE | @0 Détecteur thermoionique @5 10 |
|---|
| C03 | 09 | X | ENG | @0 Thermoionic detector @5 10 |
|---|
| C03 | 09 | X | SPA | @0 Detector termoiónico @5 10 |
|---|
| C03 | 10 | X | FRE | @0 Mécanisme action @5 11 |
|---|
| C03 | 10 | X | ENG | @0 Mechanism of action @5 11 |
|---|
| C03 | 10 | X | SPA | @0 Mecanismo acción @5 11 |
|---|
| N21 | | | | @1 263 |
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|
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| pR |
| A30 | 01 | 1 | ENG | @1 International Conference on Solid State Dosimetry @2 12 @3 Burgos ESP @4 1998-07-05 |
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|
|---|
Format Inist (serveur)
| NO : | PASCAL 99-0414304 INIST |
|---|
| ET : | Characterisation and modelling of the 450 K TSL peak of alpha alumina by the simultaneous analysis of TSL, TSC and TSEE |
|---|
| AU : | GUISSI (S.); IACCONI (P.); BINDI (R.); LAPRAZ (D.); DELGADO (A.); GOMEZ ROS (J. M.); BOS (A. J. J.); BØTTER-JENSEN (L.); HOROWITZ (Y. S.); JULIUS (H. W.); KLEMIC (G.); KRON (T.) |
|---|
| AF : | LPES-CRESA, Université de Nice-Sophia Antipolis, Parc Valrose/06108 - Nice/France (1 aut., 2 aut., 3 aut., 4 aut.); CIEMAT/Espagne (1 aut.); Delft T. University/Pays-Bas (3 aut.); Ben Gurion University/Israël (5 aut.); TNO/Pays-Bas (6 aut.); EML (DOE)/Etats-Unis (7 aut.); Newcastle Mater Misericordiae Hospital/Australie (8 aut.) |
|---|
| DT : | Publication en série; Congrès; Niveau analytique |
|---|
| SO : | Radiation protection dosimetry; ISSN 0144-8420; Coden RPDODE; Royaume-Uni; Da. 1999; Vol. 84; No. 1-4; Pp. 247-251; Bibl. 8 ref. |
|---|
| LA : | Anglais |
|---|
| EA : | The TSL peak D' (450 K) of α-alumina is commonly used for ionising radiation dosimetry. Generally, it is simultaneously accompanied by TSC and TSEE peaks. In this work, peaks D' are characterised by using a previously described model in which the defect associated with peak D' is considered as an electron trap and the TSEE resulting from the thermionic effect. The comparison with experimental data does not invalidate these basic hypotheses. |
|---|
| CC : | 002A08F05 |
|---|
| FD : | Mesure simultanée; Modélisation; Dosimètre; Thermoluminescence; Emission exoélectronique; Conductivité électrique; Alumine; Piégeage; Détecteur thermoionique; Mécanisme action |
|---|
| ED : | Simultaneous measurement; Modeling; Dosimeter; Thermoluminescence; Exoelectron emission; Electrical conductivity; Alumina; Trapping; Thermoionic detector; Mechanism of action |
|---|
| SD : | Medición simultánea; Modelización; Dosímetro; Termoluminescencia; Emisión exoelectrónica; Conductividad eléctrica; Alúmina; Captura; Detector termoiónico; Mecanismo acción |
|---|
| LO : | INIST-19318.354000085782220540 |
|---|
| ID : | 99-0414304 |
|---|
Links to Exploration step
Pascal:99-0414304
Le document en format XML
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<sZ>2 aut.</sZ>
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<sZ>4 aut.</sZ>
</inist:fA14><series><title level="j" type="main">Radiation protection dosimetry</title>
<title level="j" type="abbreviated">Radiat. prot. dosim.</title>
<idno type="ISSN">0144-8420</idno>
<imprint><date when="1999">1999</date>
</imprint><seriesStmt><title level="j" type="main">Radiation protection dosimetry</title>
<title level="j" type="abbreviated">Radiat. prot. dosim.</title>
<idno type="ISSN">0144-8420</idno>
</seriesStmt><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Alumina</term>
<term>Dosimeter</term>
<term>Electrical conductivity</term>
<term>Exoelectron emission</term>
<term>Mechanism of action</term>
<term>Modeling</term>
<term>Simultaneous measurement</term>
<term>Thermoionic detector</term>
<term>Thermoluminescence</term>
<term>Trapping</term>
</keywords><keywords scheme="Pascal" xml:lang="fr"><term>Mesure simultanée</term>
<term>Modélisation</term>
<term>Dosimètre</term>
<term>Thermoluminescence</term>
<term>Emission exoélectronique</term>
<term>Conductivité électrique</term>
<term>Alumine</term>
<term>Piégeage</term>
<term>Détecteur thermoionique</term>
<term>Mécanisme action</term>
</keywords><front><div type="abstract" xml:lang="en">The TSL peak D' (450 K) of α-alumina is commonly used for ionising radiation dosimetry. Generally, it is simultaneously accompanied by TSC and TSEE peaks. In this work, peaks D' are characterised by using a previously described model in which the defect associated with peak D' is considered as an electron trap and the TSEE resulting from the thermionic effect. The comparison with experimental data does not invalidate these basic hypotheses.</div>
</front><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0144-8420</s0>
</fA01><fA02 i1="01"><s0>RPDODE</s0>
</fA02><fA03 i2="1"><s0>Radiat. prot. dosim.</s0>
</fA03><fA06><s2>1-4</s2>
</fA06><fA08 i1="01" i2="1" l="ENG"><s1>Characterisation and modelling of the 450 K TSL peak of alpha alumina by the simultaneous analysis of TSL, TSC and TSEE</s1>
</fA08><fA09 i1="01" i2="1" l="ENG"><s1>Solid state dosimetry. Part I</s1>
</fA09><fA11 i1="01" i2="1"><s1>GUISSI (S.)</s1>
</fA11><fA11 i1="02" i2="1"><s1>IACCONI (P.)</s1>
</fA11><fA11 i1="03" i2="1"><s1>BINDI (R.)</s1>
</fA11><fA11 i1="04" i2="1"><s1>LAPRAZ (D.)</s1>
</fA11><fA12 i1="01" i2="1"><s1>DELGADO (A.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="02" i2="1"><s1>GOMEZ ROS (J. M.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="03" i2="1"><s1>BOS (A. J. J.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="04" i2="1"><s1>BØTTER-JENSEN (L.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="05" i2="1"><s1>HOROWITZ (Y. S.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="06" i2="1"><s1>JULIUS (H. W.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="07" i2="1"><s1>KLEMIC (G.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="08" i2="1"><s1>KRON (T.)</s1>
<s9>ed.</s9>
</fA12><fA14 i1="01"><s1>LPES-CRESA, Université de Nice-Sophia Antipolis, Parc Valrose</s1>
<s2>06108 - Nice</s2>
<s3>FRA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14><fA15 i1="01"><s1>CIEMAT</s1>
<s3>ESP</s3>
<sZ>1 aut.</sZ>
</fA15><fA15 i1="02"><s1>Delft T. University</s1>
<s3>NLD</s3>
<sZ>3 aut.</sZ>
</fA15><fA15 i1="03"><s1>Ben Gurion University</s1>
<s3>ISR</s3>
<sZ>5 aut.</sZ>
</fA15><fA15 i1="04"><s1>TNO</s1>
<s3>NLD</s3>
<sZ>6 aut.</sZ>
</fA15><fA15 i1="05"><s1>EML (DOE)</s1>
<s3>USA</s3>
<sZ>7 aut.</sZ>
</fA15><fA15 i1="06"><s1>Newcastle Mater Misericordiae Hospital</s1>
<s3>AUS</s3>
<sZ>8 aut.</sZ>
</fA15><fA20><s1>247-251</s1>
</fA20><fA21><s1>1999</s1>
</fA21><fA23 i1="01"><s0>ENG</s0>
</fA23><fA43 i1="01"><s1>INIST</s1>
<s2>19318</s2>
<s5>354000085782220540</s5>
</fA43><fA44><s0>0000</s0>
<s1>© 1999 INIST-CNRS. All rights reserved.</s1>
</fA44><fA45><s0>8 ref.</s0>
</fA45><fA47 i1="01" i2="1"><s0>99-0414304</s0>
</fA47><fA60><s1>P</s1>
<s2>C</s2>
</fA60><fA64 i1="01" i2="1"><s0>Radiation protection dosimetry</s0>
</fA64><fA66 i1="01"><s0>GBR</s0>
</fA66><fC01 i1="01" l="ENG"><s0>The TSL peak D' (450 K) of α-alumina is commonly used for ionising radiation dosimetry. Generally, it is simultaneously accompanied by TSC and TSEE peaks. In this work, peaks D' are characterised by using a previously described model in which the defect associated with peak D' is considered as an electron trap and the TSEE resulting from the thermionic effect. The comparison with experimental data does not invalidate these basic hypotheses.</s0>
</fC01><fC02 i1="01" i2="X"><s0>002A08F05</s0>
</fC02><fC03 i1="01" i2="X" l="FRE"><s0>Mesure simultanée</s0>
<s5>01</s5>
</fC03><fC03 i1="01" i2="X" l="ENG"><s0>Simultaneous measurement</s0>
<s5>01</s5>
</fC03><fC03 i1="01" i2="X" l="SPA"><s0>Medición simultánea</s0>
<s5>01</s5>
</fC03><fC03 i1="02" i2="X" l="FRE"><s0>Modélisation</s0>
<s5>02</s5>
</fC03><fC03 i1="02" i2="X" l="ENG"><s0>Modeling</s0>
<s5>02</s5>
</fC03><fC03 i1="02" i2="X" l="SPA"><s0>Modelización</s0>
<s5>02</s5>
</fC03><fC03 i1="03" i2="X" l="FRE"><s0>Dosimètre</s0>
<s5>03</s5>
</fC03><fC03 i1="03" i2="X" l="ENG"><s0>Dosimeter</s0>
<s5>03</s5>
</fC03><fC03 i1="03" i2="X" l="SPA"><s0>Dosímetro</s0>
<s5>03</s5>
</fC03><fC03 i1="04" i2="X" l="FRE"><s0>Thermoluminescence</s0>
<s5>04</s5>
</fC03><fC03 i1="04" i2="X" l="ENG"><s0>Thermoluminescence</s0>
<s5>04</s5>
</fC03><fC03 i1="04" i2="X" l="SPA"><s0>Termoluminescencia</s0>
<s5>04</s5>
</fC03><fC03 i1="05" i2="X" l="FRE"><s0>Emission exoélectronique</s0>
<s5>05</s5>
</fC03><fC03 i1="05" i2="X" l="ENG"><s0>Exoelectron emission</s0>
<s5>05</s5>
</fC03><fC03 i1="05" i2="X" l="SPA"><s0>Emisión exoelectrónica</s0>
<s5>05</s5>
</fC03><fC03 i1="06" i2="X" l="FRE"><s0>Conductivité électrique</s0>
<s5>06</s5>
</fC03><fC03 i1="06" i2="X" l="ENG"><s0>Electrical conductivity</s0>
<s5>06</s5>
</fC03><fC03 i1="06" i2="X" l="SPA"><s0>Conductividad eléctrica</s0>
<s5>06</s5>
</fC03><fC03 i1="07" i2="X" l="FRE"><s0>Alumine</s0>
<s2>NK</s2>
<s5>07</s5>
</fC03><fC03 i1="07" i2="X" l="ENG"><s0>Alumina</s0>
<s2>NK</s2>
<s5>07</s5>
</fC03><fC03 i1="07" i2="X" l="SPA"><s0>Alúmina</s0>
<s2>NK</s2>
<s5>07</s5>
</fC03><fC03 i1="08" i2="X" l="FRE"><s0>Piégeage</s0>
<s5>09</s5>
</fC03><fC03 i1="08" i2="X" l="ENG"><s0>Trapping</s0>
<s5>09</s5>
</fC03><fC03 i1="08" i2="X" l="SPA"><s0>Captura</s0>
<s5>09</s5>
</fC03><fC03 i1="09" i2="X" l="FRE"><s0>Détecteur thermoionique</s0>
<s5>10</s5>
</fC03><fC03 i1="09" i2="X" l="ENG"><s0>Thermoionic detector</s0>
<s5>10</s5>
</fC03><fC03 i1="09" i2="X" l="SPA"><s0>Detector termoiónico</s0>
<s5>10</s5>
</fC03><fC03 i1="10" i2="X" l="FRE"><s0>Mécanisme action</s0>
<s5>11</s5>
</fC03><fC03 i1="10" i2="X" l="ENG"><s0>Mechanism of action</s0>
<s5>11</s5>
</fC03><fC03 i1="10" i2="X" l="SPA"><s0>Mecanismo acción</s0>
<s5>11</s5>
</fC03><fN21><s1>263</s1>
</fN21><pR><fA30 i1="01" i2="1" l="ENG"><s1>International Conference on Solid State Dosimetry</s1>
<s2>12</s2>
<s3>Burgos ESP</s3>
<s4>1998-07-05</s4>
</fA30><server><NO>PASCAL 99-0414304 INIST</NO>
<ET>Characterisation and modelling of the 450 K TSL peak of alpha alumina by the simultaneous analysis of TSL, TSC and TSEE</ET>
<AU>GUISSI (S.); IACCONI (P.); BINDI (R.); LAPRAZ (D.); DELGADO (A.); GOMEZ ROS (J. M.); BOS (A. J. J.); BØTTER-JENSEN (L.); HOROWITZ (Y. S.); JULIUS (H. W.); KLEMIC (G.); KRON (T.)</AU>
<AF>LPES-CRESA, Université de Nice-Sophia Antipolis, Parc Valrose/06108 - Nice/France (1 aut., 2 aut., 3 aut., 4 aut.); CIEMAT/Espagne (1 aut.); Delft T. University/Pays-Bas (3 aut.); Ben Gurion University/Israël (5 aut.); TNO/Pays-Bas (6 aut.); EML (DOE)/Etats-Unis (7 aut.); Newcastle Mater Misericordiae Hospital/Australie (8 aut.)</AF>
<DT>Publication en série; Congrès; Niveau analytique</DT>
<SO>Radiation protection dosimetry; ISSN 0144-8420; Coden RPDODE; Royaume-Uni; Da. 1999; Vol. 84; No. 1-4; Pp. 247-251; Bibl. 8 ref.</SO>
<LA>Anglais</LA>
<EA>The TSL peak D' (450 K) of α-alumina is commonly used for ionising radiation dosimetry. Generally, it is simultaneously accompanied by TSC and TSEE peaks. In this work, peaks D' are characterised by using a previously described model in which the defect associated with peak D' is considered as an electron trap and the TSEE resulting from the thermionic effect. The comparison with experimental data does not invalidate these basic hypotheses.</EA>
<CC>002A08F05</CC>
<FD>Mesure simultanée; Modélisation; Dosimètre; Thermoluminescence; Emission exoélectronique; Conductivité électrique; Alumine; Piégeage; Détecteur thermoionique; Mécanisme action</FD>
<ED>Simultaneous measurement; Modeling; Dosimeter; Thermoluminescence; Exoelectron emission; Electrical conductivity; Alumina; Trapping; Thermoionic detector; Mechanism of action</ED>
<SD>Medición simultánea; Modelización; Dosímetro; Termoluminescencia; Emisión exoelectrónica; Conductividad eléctrica; Alúmina; Captura; Detector termoiónico; Mecanismo acción</SD>
<LO>INIST-19318.354000085782220540</LO>
<ID>99-0414304</ID>
</server>
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