CW and Temporal Theoretical Model Predictions and Experimental Results for Tm:YAG and Ho:YAG Lasers
Identifieur interne :
000526 ( Pascal/Corpus );
précédent :
000525;
suivant :
000527
CW and Temporal Theoretical Model Predictions and Experimental Results for Tm:YAG and Ho:YAG Lasers
Auteurs : Eric K. Gorton ;
John G. Benerton ;
David A. Orchard ;
Brian J. Perrett ;
Paul D. Mason ;
Ian F. ElderSource :
-
Proceedings of SPIE - The International Society for Optical Engineering [ 0277-786X ] ; 2008.
RBID : Pascal:09-0151999
Descripteurs français
- Pascal (Inist)
- Etat fondamental,
Composé ternaire,
Grenat aluminium yttrium,
Thulium,
Temps retard,
Holmium,
Contremesure,
Méthode mesure,
Méthode optique,
YAG,
Y3Al5O12,
Al O Y,
0130C,
0760.
English descriptors
Abstract
We describe the development of a time dependent thulium laser model. The model is used to predict both the CW and temporal behaviour of a Tm:YAG laser. Experimental results from a diode-pumped Tm:YAG laser are obtained and the model is used to obtain good agreement with these observations for both the CW and temporal behaviour of the laser. Particular results relate to switch-on time delays and the effect of pump diode modulation on Tm laser efficiency. The laser model has been extended to the case of the Ho:YAG laser where other important effects due to ground state depletion and self re-absorption must be taken into account. The holmium laser model has recently been used to predict reported experimental results from a thulium fibre laser pumped Ho:YAG laser.
Notice en format standard (ISO 2709)
Pour connaître la documentation sur le format Inist Standard.
| pA |
| A01 | 01 | 1 | | @0 0277-786X |
|---|
| A05 | | | | @2 7115 |
|---|
| A08 | 01 | 1 | ENG | @1 CW and Temporal Theoretical Model Predictions and Experimental Results for Tm:YAG and Ho:YAG Lasers |
|---|
| A09 | 01 | 1 | ENG | @1 Technologies for optical countermeasures V : 15-16 September 2008, Cardiff, Wales, United Kingdom |
|---|
| A11 | 01 | 1 | | @1 GORTON (Eric K.) |
|---|
| A11 | 02 | 1 | | @1 BENERTON (John G.) |
|---|
| A11 | 03 | 1 | | @1 ORCHARD (David A.) |
|---|
| A11 | 04 | 1 | | @1 PERRETT (Brian J.) |
|---|
| A11 | 05 | 1 | | @1 MASON (Paul D.) |
|---|
| A11 | 06 | 1 | | @1 ELDER (Ian F.) |
|---|
| A12 | 01 | 1 | | @1 TITTERTON (David H.) @9 ed. |
|---|
| A12 | 02 | 1 | | @1 RICHARDSON (Mark A.) @9 ed. |
|---|
| A14 | 01 | | | @1 QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem @2 Worcestershire, WR14 3PS @3 GBR @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. |
|---|
| A14 | 02 | | | @1 SELEX Galileo, Crewe Toll House, Ferry Road @2 Edinburgh EH5 2XS @3 GBR @Z 6 aut. |
|---|
| A18 | 01 | 1 | | @1 SPIE Europe @3 INC @9 org-cong. |
|---|
| A18 | 02 | 1 | | @1 Great Britain. Ministry of Defence @3 GBR @9 org-cong. |
|---|
| A18 | 03 | 1 | | @1 SPIE @3 USA @9 org-cong. |
|---|
| A20 | | | | @2 71150U.1-71150U.8 |
|---|
| A21 | | | | @1 2008 |
|---|
| A23 | 01 | | | @0 ENG |
|---|
| A26 | 01 | | | @0 978-0-8194-7347-9 |
|---|
| A43 | 01 | | | @1 INIST @2 21760 @5 354000172939790230 |
|---|
| A44 | | | | @0 0000 @1 © 2009 INIST-CNRS. All rights reserved. |
|---|
| A45 | | | | @0 10 ref. |
|---|
| A47 | 01 | 1 | | @0 09-0151999 |
|---|
| A60 | | | | @1 P @2 C |
|---|
| A61 | | | | @0 A |
|---|
| A64 | 01 | 1 | | @0 Proceedings of SPIE - The International Society for Optical Engineering |
|---|
| A66 | 01 | | | @0 USA |
|---|
| C01 | 01 | | ENG | @0 We describe the development of a time dependent thulium laser model. The model is used to predict both the CW and temporal behaviour of a Tm:YAG laser. Experimental results from a diode-pumped Tm:YAG laser are obtained and the model is used to obtain good agreement with these observations for both the CW and temporal behaviour of the laser. Particular results relate to switch-on time delays and the effect of pump diode modulation on Tm laser efficiency. The laser model has been extended to the case of the Ho:YAG laser where other important effects due to ground state depletion and self re-absorption must be taken into account. The holmium laser model has recently been used to predict reported experimental results from a thulium fibre laser pumped Ho:YAG laser. |
|---|
| C02 | 01 | 3 | | @0 001B00A30C |
|---|
| C02 | 02 | 3 | | @0 001B00G60 |
|---|
| C03 | 01 | 3 | FRE | @0 Etat fondamental @5 41 |
|---|
| C03 | 01 | 3 | ENG | @0 Ground states @5 41 |
|---|
| C03 | 02 | 3 | FRE | @0 Composé ternaire @5 50 |
|---|
| C03 | 02 | 3 | ENG | @0 Ternary compounds @5 50 |
|---|
| C03 | 03 | 3 | FRE | @0 Grenat aluminium yttrium @5 51 |
|---|
| C03 | 03 | 3 | ENG | @0 YAG @5 51 |
|---|
| C03 | 04 | 3 | FRE | @0 Thulium @2 NC @5 61 |
|---|
| C03 | 04 | 3 | ENG | @0 Thulium @2 NC @5 61 |
|---|
| C03 | 05 | 3 | FRE | @0 Temps retard @5 62 |
|---|
| C03 | 05 | 3 | ENG | @0 Time delay @5 62 |
|---|
| C03 | 06 | 3 | FRE | @0 Holmium @2 NC @5 63 |
|---|
| C03 | 06 | 3 | ENG | @0 Holmium @2 NC @5 63 |
|---|
| C03 | 07 | X | FRE | @0 Contremesure @5 64 |
|---|
| C03 | 07 | X | ENG | @0 Countermeasurement @5 64 |
|---|
| C03 | 07 | X | SPA | @0 Contramedida @5 64 |
|---|
| C03 | 08 | 3 | FRE | @0 Méthode mesure @5 65 |
|---|
| C03 | 08 | 3 | ENG | @0 Measuring methods @5 65 |
|---|
| C03 | 09 | X | FRE | @0 Méthode optique @5 66 |
|---|
| C03 | 09 | X | ENG | @0 Optical method @5 66 |
|---|
| C03 | 09 | X | SPA | @0 Método óptico @5 66 |
|---|
| C03 | 10 | 3 | FRE | @0 YAG @4 INC @5 71 |
|---|
| C03 | 11 | 3 | FRE | @0 Y3Al5O12 @4 INC @5 72 |
|---|
| C03 | 12 | 3 | FRE | @0 Al O Y @4 INC @5 75 |
|---|
| C03 | 13 | 3 | FRE | @0 0130C @4 INC @5 83 |
|---|
| C03 | 14 | 3 | FRE | @0 0760 @4 INC @5 84 |
|---|
| N21 | | | | @1 110 |
|---|
| N44 | 01 | | | @1 OTO |
|---|
| N82 | | | | @1 OTO |
|---|
|
|---|
| pR |
| A30 | 01 | 1 | ENG | @1 Technologies for optical countermeasures @2 5 @3 Cardiff GBR @4 2008 |
|---|
|
|---|
Format Inist (serveur)
| NO : | PASCAL 09-0151999 INIST |
|---|
| ET : | CW and Temporal Theoretical Model Predictions and Experimental Results for Tm:YAG and Ho:YAG Lasers |
|---|
| AU : | GORTON (Eric K.); BENERTON (John G.); ORCHARD (David A.); PERRETT (Brian J.); MASON (Paul D.); ELDER (Ian F.); TITTERTON (David H.); RICHARDSON (Mark A.) |
|---|
| AF : | QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem/Worcestershire, WR14 3PS/Royaume-Uni (1 aut., 2 aut., 3 aut., 4 aut., 5 aut.); SELEX Galileo, Crewe Toll House, Ferry Road/Edinburgh EH5 2XS/Royaume-Uni (6 aut.) |
|---|
| DT : | Publication en série; Congrès; Niveau analytique |
|---|
| SO : | Proceedings of SPIE - The International Society for Optical Engineering; ISSN 0277-786X; Etats-Unis; Da. 2008; Vol. 7115; 71150U.1-71150U.8; Bibl. 10 ref. |
|---|
| LA : | Anglais |
|---|
| EA : | We describe the development of a time dependent thulium laser model. The model is used to predict both the CW and temporal behaviour of a Tm:YAG laser. Experimental results from a diode-pumped Tm:YAG laser are obtained and the model is used to obtain good agreement with these observations for both the CW and temporal behaviour of the laser. Particular results relate to switch-on time delays and the effect of pump diode modulation on Tm laser efficiency. The laser model has been extended to the case of the Ho:YAG laser where other important effects due to ground state depletion and self re-absorption must be taken into account. The holmium laser model has recently been used to predict reported experimental results from a thulium fibre laser pumped Ho:YAG laser. |
|---|
| CC : | 001B00A30C; 001B00G60 |
|---|
| FD : | Etat fondamental; Composé ternaire; Grenat aluminium yttrium; Thulium; Temps retard; Holmium; Contremesure; Méthode mesure; Méthode optique; YAG; Y3Al5O12; Al O Y; 0130C; 0760 |
|---|
| ED : | Ground states; Ternary compounds; YAG; Thulium; Time delay; Holmium; Countermeasurement; Measuring methods; Optical method |
|---|
| SD : | Contramedida; Método óptico |
|---|
| LO : | INIST-21760.354000172939790230 |
|---|
| ID : | 09-0151999 |
|---|
Links to Exploration step
Pascal:09-0151999
Le document en format XML
<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">CW and Temporal Theoretical Model Predictions and Experimental Results for Tm:YAG and Ho:YAG Lasers</title>
<author><name sortKey="Gorton, Eric K" sort="Gorton, Eric K" uniqKey="Gorton E" first="Eric K." last="Gorton">Eric K. Gorton</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Benerton, John G" sort="Benerton, John G" uniqKey="Benerton J" first="John G." last="Benerton">John G. Benerton</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Orchard, David A" sort="Orchard, David A" uniqKey="Orchard D" first="David A." last="Orchard">David A. Orchard</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Perrett, Brian J" sort="Perrett, Brian J" uniqKey="Perrett B" first="Brian J." last="Perrett">Brian J. Perrett</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Mason, Paul D" sort="Mason, Paul D" uniqKey="Mason P" first="Paul D." last="Mason">Paul D. Mason</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Elder, Ian F" sort="Elder, Ian F" uniqKey="Elder I" first="Ian F." last="Elder">Ian F. Elder</name>
<affiliation><inist:fA14 i1="02"><s1>SELEX Galileo, Crewe Toll House, Ferry Road</s1>
<s2>Edinburgh EH5 2XS</s2>
<s3>GBR</s3>
<sZ>6 aut.</sZ>
</inist:fA14><publicationStmt><idno type="wicri:source">INIST</idno>
<idno type="inist">09-0151999</idno>
<date when="2008">2008</date>
<idno type="stanalyst">PASCAL 09-0151999 INIST</idno>
<idno type="RBID">Pascal:09-0151999</idno>
<idno type="wicri:Area/Pascal/Corpus">000526</idno>
</publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">CW and Temporal Theoretical Model Predictions and Experimental Results for Tm:YAG and Ho:YAG Lasers</title>
<author><name sortKey="Gorton, Eric K" sort="Gorton, Eric K" uniqKey="Gorton E" first="Eric K." last="Gorton">Eric K. Gorton</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Benerton, John G" sort="Benerton, John G" uniqKey="Benerton J" first="John G." last="Benerton">John G. Benerton</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Orchard, David A" sort="Orchard, David A" uniqKey="Orchard D" first="David A." last="Orchard">David A. Orchard</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Perrett, Brian J" sort="Perrett, Brian J" uniqKey="Perrett B" first="Brian J." last="Perrett">Brian J. Perrett</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Mason, Paul D" sort="Mason, Paul D" uniqKey="Mason P" first="Paul D." last="Mason">Paul D. Mason</name>
<affiliation><inist:fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><author><name sortKey="Elder, Ian F" sort="Elder, Ian F" uniqKey="Elder I" first="Ian F." last="Elder">Ian F. Elder</name>
<affiliation><inist:fA14 i1="02"><s1>SELEX Galileo, Crewe Toll House, Ferry Road</s1>
<s2>Edinburgh EH5 2XS</s2>
<s3>GBR</s3>
<sZ>6 aut.</sZ>
</inist:fA14><series><title level="j" type="main">Proceedings of SPIE - The International Society for Optical Engineering</title>
<idno type="ISSN">0277-786X</idno>
<imprint><date when="2008">2008</date>
</imprint><seriesStmt><title level="j" type="main">Proceedings of SPIE - The International Society for Optical Engineering</title>
<idno type="ISSN">0277-786X</idno>
</seriesStmt><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Countermeasurement</term>
<term>Ground states</term>
<term>Holmium</term>
<term>Measuring methods</term>
<term>Optical method</term>
<term>Ternary compounds</term>
<term>Thulium</term>
<term>Time delay</term>
<term>YAG</term>
</keywords><keywords scheme="Pascal" xml:lang="fr"><term>Etat fondamental</term>
<term>Composé ternaire</term>
<term>Grenat aluminium yttrium</term>
<term>Thulium</term>
<term>Temps retard</term>
<term>Holmium</term>
<term>Contremesure</term>
<term>Méthode mesure</term>
<term>Méthode optique</term>
<term>YAG</term>
<term>Y3Al5O12</term>
<term>Al O Y</term>
<term>0130C</term>
<term>0760</term>
</keywords><front><div type="abstract" xml:lang="en">We describe the development of a time dependent thulium laser model. The model is used to predict both the CW and temporal behaviour of a Tm:YAG laser. Experimental results from a diode-pumped Tm:YAG laser are obtained and the model is used to obtain good agreement with these observations for both the CW and temporal behaviour of the laser. Particular results relate to switch-on time delays and the effect of pump diode modulation on Tm laser efficiency. The laser model has been extended to the case of the Ho:YAG laser where other important effects due to ground state depletion and self re-absorption must be taken into account. The holmium laser model has recently been used to predict reported experimental results from a thulium fibre laser pumped Ho:YAG laser.</div>
</front><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0277-786X</s0>
</fA01><fA05><s2>7115</s2>
</fA05><fA08 i1="01" i2="1" l="ENG"><s1>CW and Temporal Theoretical Model Predictions and Experimental Results for Tm:YAG and Ho:YAG Lasers</s1>
</fA08><fA09 i1="01" i2="1" l="ENG"><s1>Technologies for optical countermeasures V : 15-16 September 2008, Cardiff, Wales, United Kingdom</s1>
</fA09><fA11 i1="01" i2="1"><s1>GORTON (Eric K.)</s1>
</fA11><fA11 i1="02" i2="1"><s1>BENERTON (John G.)</s1>
</fA11><fA11 i1="03" i2="1"><s1>ORCHARD (David A.)</s1>
</fA11><fA11 i1="04" i2="1"><s1>PERRETT (Brian J.)</s1>
</fA11><fA11 i1="05" i2="1"><s1>MASON (Paul D.)</s1>
</fA11><fA11 i1="06" i2="1"><s1>ELDER (Ian F.)</s1>
</fA11><fA12 i1="01" i2="1"><s1>TITTERTON (David H.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="02" i2="1"><s1>RICHARDSON (Mark A.)</s1>
<s9>ed.</s9>
</fA12><fA14 i1="01"><s1>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem</s1>
<s2>Worcestershire, WR14 3PS</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</fA14><fA14 i1="02"><s1>SELEX Galileo, Crewe Toll House, Ferry Road</s1>
<s2>Edinburgh EH5 2XS</s2>
<s3>GBR</s3>
<sZ>6 aut.</sZ>
</fA14><fA18 i1="01" i2="1"><s1>SPIE Europe</s1>
<s3>INC</s3>
<s9>org-cong.</s9>
</fA18><fA18 i1="02" i2="1"><s1>Great Britain. Ministry of Defence</s1>
<s3>GBR</s3>
<s9>org-cong.</s9>
</fA18><fA18 i1="03" i2="1"><s1>SPIE</s1>
<s3>USA</s3>
<s9>org-cong.</s9>
</fA18><fA20><s2>71150U.1-71150U.8</s2>
</fA20><fA21><s1>2008</s1>
</fA21><fA23 i1="01"><s0>ENG</s0>
</fA23><fA26 i1="01"><s0>978-0-8194-7347-9</s0>
</fA26><fA43 i1="01"><s1>INIST</s1>
<s2>21760</s2>
<s5>354000172939790230</s5>
</fA43><fA44><s0>0000</s0>
<s1>© 2009 INIST-CNRS. All rights reserved.</s1>
</fA44><fA45><s0>10 ref.</s0>
</fA45><fA47 i1="01" i2="1"><s0>09-0151999</s0>
</fA47><fA60><s1>P</s1>
<s2>C</s2>
</fA60><fA64 i1="01" i2="1"><s0>Proceedings of SPIE - The International Society for Optical Engineering</s0>
</fA64><fA66 i1="01"><s0>USA</s0>
</fA66><fC01 i1="01" l="ENG"><s0>We describe the development of a time dependent thulium laser model. The model is used to predict both the CW and temporal behaviour of a Tm:YAG laser. Experimental results from a diode-pumped Tm:YAG laser are obtained and the model is used to obtain good agreement with these observations for both the CW and temporal behaviour of the laser. Particular results relate to switch-on time delays and the effect of pump diode modulation on Tm laser efficiency. The laser model has been extended to the case of the Ho:YAG laser where other important effects due to ground state depletion and self re-absorption must be taken into account. The holmium laser model has recently been used to predict reported experimental results from a thulium fibre laser pumped Ho:YAG laser.</s0>
</fC01><fC02 i1="01" i2="3"><s0>001B00A30C</s0>
</fC02><fC02 i1="02" i2="3"><s0>001B00G60</s0>
</fC02><fC03 i1="01" i2="3" l="FRE"><s0>Etat fondamental</s0>
<s5>41</s5>
</fC03><fC03 i1="01" i2="3" l="ENG"><s0>Ground states</s0>
<s5>41</s5>
</fC03><fC03 i1="02" i2="3" l="FRE"><s0>Composé ternaire</s0>
<s5>50</s5>
</fC03><fC03 i1="02" i2="3" l="ENG"><s0>Ternary compounds</s0>
<s5>50</s5>
</fC03><fC03 i1="03" i2="3" l="FRE"><s0>Grenat aluminium yttrium</s0>
<s5>51</s5>
</fC03><fC03 i1="03" i2="3" l="ENG"><s0>YAG</s0>
<s5>51</s5>
</fC03><fC03 i1="04" i2="3" l="FRE"><s0>Thulium</s0>
<s2>NC</s2>
<s5>61</s5>
</fC03><fC03 i1="04" i2="3" l="ENG"><s0>Thulium</s0>
<s2>NC</s2>
<s5>61</s5>
</fC03><fC03 i1="05" i2="3" l="FRE"><s0>Temps retard</s0>
<s5>62</s5>
</fC03><fC03 i1="05" i2="3" l="ENG"><s0>Time delay</s0>
<s5>62</s5>
</fC03><fC03 i1="06" i2="3" l="FRE"><s0>Holmium</s0>
<s2>NC</s2>
<s5>63</s5>
</fC03><fC03 i1="06" i2="3" l="ENG"><s0>Holmium</s0>
<s2>NC</s2>
<s5>63</s5>
</fC03><fC03 i1="07" i2="X" l="FRE"><s0>Contremesure</s0>
<s5>64</s5>
</fC03><fC03 i1="07" i2="X" l="ENG"><s0>Countermeasurement</s0>
<s5>64</s5>
</fC03><fC03 i1="07" i2="X" l="SPA"><s0>Contramedida</s0>
<s5>64</s5>
</fC03><fC03 i1="08" i2="3" l="FRE"><s0>Méthode mesure</s0>
<s5>65</s5>
</fC03><fC03 i1="08" i2="3" l="ENG"><s0>Measuring methods</s0>
<s5>65</s5>
</fC03><fC03 i1="09" i2="X" l="FRE"><s0>Méthode optique</s0>
<s5>66</s5>
</fC03><fC03 i1="09" i2="X" l="ENG"><s0>Optical method</s0>
<s5>66</s5>
</fC03><fC03 i1="09" i2="X" l="SPA"><s0>Método óptico</s0>
<s5>66</s5>
</fC03><fC03 i1="10" i2="3" l="FRE"><s0>YAG</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03><fC03 i1="11" i2="3" l="FRE"><s0>Y3Al5O12</s0>
<s4>INC</s4>
<s5>72</s5>
</fC03><fC03 i1="12" i2="3" l="FRE"><s0>Al O Y</s0>
<s4>INC</s4>
<s5>75</s5>
</fC03><fC03 i1="13" i2="3" l="FRE"><s0>0130C</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03><fC03 i1="14" i2="3" l="FRE"><s0>0760</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03><fN21><s1>110</s1>
</fN21><fN44 i1="01"><s1>OTO</s1>
</fN44><fN82><s1>OTO</s1>
</fN82><pR><fA30 i1="01" i2="1" l="ENG"><s1>Technologies for optical countermeasures</s1>
<s2>5</s2>
<s3>Cardiff GBR</s3>
<s4>2008</s4>
</fA30><server><NO>PASCAL 09-0151999 INIST</NO>
<ET>CW and Temporal Theoretical Model Predictions and Experimental Results for Tm:YAG and Ho:YAG Lasers</ET>
<AU>GORTON (Eric K.); BENERTON (John G.); ORCHARD (David A.); PERRETT (Brian J.); MASON (Paul D.); ELDER (Ian F.); TITTERTON (David H.); RICHARDSON (Mark A.)</AU>
<AF>QinetiQ, Malvem Technology Centre, St Andrews Road, Great Malvem/Worcestershire, WR14 3PS/Royaume-Uni (1 aut., 2 aut., 3 aut., 4 aut., 5 aut.); SELEX Galileo, Crewe Toll House, Ferry Road/Edinburgh EH5 2XS/Royaume-Uni (6 aut.)</AF>
<DT>Publication en série; Congrès; Niveau analytique</DT>
<SO>Proceedings of SPIE - The International Society for Optical Engineering; ISSN 0277-786X; Etats-Unis; Da. 2008; Vol. 7115; 71150U.1-71150U.8; Bibl. 10 ref.</SO>
<LA>Anglais</LA>
<EA>We describe the development of a time dependent thulium laser model. The model is used to predict both the CW and temporal behaviour of a Tm:YAG laser. Experimental results from a diode-pumped Tm:YAG laser are obtained and the model is used to obtain good agreement with these observations for both the CW and temporal behaviour of the laser. Particular results relate to switch-on time delays and the effect of pump diode modulation on Tm laser efficiency. The laser model has been extended to the case of the Ho:YAG laser where other important effects due to ground state depletion and self re-absorption must be taken into account. The holmium laser model has recently been used to predict reported experimental results from a thulium fibre laser pumped Ho:YAG laser.</EA>
<CC>001B00A30C; 001B00G60</CC>
<FD>Etat fondamental; Composé ternaire; Grenat aluminium yttrium; Thulium; Temps retard; Holmium; Contremesure; Méthode mesure; Méthode optique; YAG; Y3Al5O12; Al O Y; 0130C; 0760</FD>
<ED>Ground states; Ternary compounds; YAG; Thulium; Time delay; Holmium; Countermeasurement; Measuring methods; Optical method</ED>
<SD>Contramedida; Método óptico</SD>
<LO>INIST-21760.354000172939790230</LO>
<ID>09-0151999</ID>
</server>
Pour manipuler ce document sous Unix (Dilib)
EXPLOR_STEP=$WICRI_ROOT/Wicri/Terre/explor/ThuliumV1/Data/Pascal/Corpus
HfdSelect -h $EXPLOR_STEP/biblio.hfd -nk 000526 | SxmlIndent | more
Ou
HfdSelect -h $EXPLOR_AREA/Data/Pascal/Corpus/biblio.hfd -nk 000526 | SxmlIndent | more
Pour mettre un lien sur cette page dans le réseau Wicri
{{Explor lien
|wiki= Wicri/Terre
|area= ThuliumV1
|flux= Pascal
|étape= Corpus
|type= RBID
|clé= Pascal:09-0151999
|texte= CW and Temporal Theoretical Model Predictions and Experimental Results for Tm:YAG and Ho:YAG Lasers
}}
| This area was generated with Dilib version V0.6.21.
Data generation: Thu May 12 08:27:09 2016. Site generation: Thu Mar 7 22:33:44 2024 |  |
