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. |
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A15 | 02 | | | @1 Delft T. University @3 NLD @Z 3 aut. |
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A15 | 03 | | | @1 Ben Gurion University @3 ISR @Z 5 aut. |
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A15 | 04 | | | @1 TNO @3 NLD @Z 6 aut. |
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A15 | 05 | | | @1 EML (DOE) @3 USA @Z 7 aut. |
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A15 | 06 | | | @1 Newcastle Mater Misericordiae Hospital @3 AUS @Z 8 aut. |
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A20 | | | | @1 247-251 |
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A21 | | | | @1 1999 |
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A23 | 01 | | | @0 ENG |
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A43 | 01 | | | @1 INIST @2 19318 @5 354000085782220540 |
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A44 | | | | @0 0000 @1 © 1999 INIST-CNRS. All rights reserved. |
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A45 | | | | @0 8 ref. |
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A47 | 01 | 1 | | @0 99-0414304 |
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A60 | | | | @1 P @2 C |
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A61 | | | | @0 A |
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A64 | 01 | 1 | | @0 Radiation protection dosimetry |
---|
A66 | 01 | | | @0 GBR |
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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 |
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C03 | 01 | X | FRE | @0 Mesure simultanée @5 01 |
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C03 | 01 | X | ENG | @0 Simultaneous measurement @5 01 |
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C03 | 01 | X | SPA | @0 Medición simultánea @5 01 |
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C03 | 02 | X | FRE | @0 Modélisation @5 02 |
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C03 | 02 | X | ENG | @0 Modeling @5 02 |
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C03 | 02 | X | SPA | @0 Modelización @5 02 |
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C03 | 03 | X | FRE | @0 Dosimètre @5 03 |
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C03 | 03 | X | ENG | @0 Dosimeter @5 03 |
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C03 | 03 | X | SPA | @0 Dosímetro @5 03 |
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C03 | 04 | X | FRE | @0 Thermoluminescence @5 04 |
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C03 | 04 | X | ENG | @0 Thermoluminescence @5 04 |
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C03 | 04 | X | SPA | @0 Termoluminescencia @5 04 |
---|
C03 | 05 | X | FRE | @0 Emission exoélectronique @5 05 |
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C03 | 05 | X | ENG | @0 Exoelectron emission @5 05 |
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C03 | 05 | X | SPA | @0 Emisión exoelectrónica @5 05 |
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C03 | 06 | X | FRE | @0 Conductivité électrique @5 06 |
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C03 | 06 | X | ENG | @0 Electrical conductivity @5 06 |
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C03 | 06 | X | SPA | @0 Conductividad eléctrica @5 06 |
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C03 | 07 | X | FRE | @0 Alumine @2 NK @5 07 |
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C03 | 07 | X | ENG | @0 Alumina @2 NK @5 07 |
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C03 | 07 | X | SPA | @0 Alúmina @2 NK @5 07 |
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C03 | 08 | X | FRE | @0 Piégeage @5 09 |
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C03 | 08 | X | ENG | @0 Trapping @5 09 |
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C03 | 08 | X | SPA | @0 Captura @5 09 |
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C03 | 09 | X | FRE | @0 Détecteur thermoionique @5 10 |
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C03 | 09 | X | ENG | @0 Thermoionic detector @5 10 |
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C03 | 09 | X | SPA | @0 Detector termoiónico @5 10 |
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C03 | 10 | X | FRE | @0 Mécanisme action @5 11 |
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C03 | 10 | X | ENG | @0 Mechanism of action @5 11 |
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C03 | 10 | X | SPA | @0 Mecanismo acción @5 11 |
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N21 | | | | @1 263 |
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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 |
---|
|
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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<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>
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<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>
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<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>
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<s5>05</s5>
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<s5>06</s5>
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<s5>06</s5>
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<s5>06</s5>
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<s5>07</s5>
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<s5>07</s5>
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<s5>07</s5>
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<s5>09</s5>
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<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>
</pA>
<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>
</pR>
</standard>
<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>
</inist>
</record>
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