Femtosecond envelope of the high-harmonic emission from ablation plasmas
Identifieur interne : 001B89 ( Main/Repository ); précédent : 001B88; suivant : 001B90Femtosecond envelope of the high-harmonic emission from ablation plasmas
Auteurs : RBID : Pascal:12-0229889Descripteurs français
- Pascal (Inist)
- Conversion fréquence optique, Harmonique supérieur, Génération harmonique optique, Corrélation croisée, Ionisation, Transition radiative, Impulsion ultracourte, Laser IR, Source rayonnement, Optique non linéaire, Faisceau laser, Rayonnement UV, Domaine temps fs, Durée impulsion, Domaine temps as, Plasma, Indium, Etain, Optique ultrarapide, Plasma produit par laser, Panache plasma, Attoseconde, 5250J, 0785F, 4265K, 4265R.
English descriptors
- KwdEn :
- Cross correlations, Higher harmonic, Indium, Infrared laser, Ionization, Laser beams, Laser-produced plasma, Nonlinear optics, Optical frequency conversion, Optical harmonic generation, Plasma, Pulse width, Radiation sources, Radiative transition, Tin, Ultrafast optics, Ultrashort pulse, Ultraviolet radiation, as range, fs range.
Abstract
We characterize the temporal profile of the high-order harmonic emission from ablation plasma plumes using cross-correlations with the infrared (IR) laser beam provided by two-photon harmonic+IR ionization of rare gas atoms. We study both non-resonant plasmas (lead, gold and chrome) and resonant plasmas (indium and tin), i.e. plasmas presenting in the singly charged ions a strong radiative transition coinciding with a harmonic order. The cross-correlation traces are found to be very similar for all harmonic orders and all plasma targets. The recovered harmonic pulse durations are very similar to the driving laser, with a tendency towards being shorter, demonstrating that the emission is a directly laser-driven process even in the case of resonant harmonics. This provides a valuable input for theories describing resonant-harmonic emission and opens the perspective of a very high flux tabletop XUV source for applications.
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Pascal:12-0229889Le document en format XML
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Haessler</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>CEA Saclay, IRAMIS, Service des Photons, Atomes et Molecules</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ><sZ>7 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Île-de-France</region><settlement type="city">Gif-sur-Yvette</settlement></placeName></affiliation><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Photonics Institute, Vienna University of Technology, Gusshausstrasse 27/387</s1><s2>1040 Vienna</s2><s3>AUT</s3><sZ>1 aut.</sZ></inist:fA14><country>Autriche</country><wicri:noRegion>1040 Vienna</wicri:noRegion></affiliation></author><author><name sortKey="Elouga Bom, L B" uniqKey="Elouga Bom L">L. B. Elouga Bom</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Institut National de la Recherche Scientifique, Centre Energie, Materiaux et Telecommunications, 1650 Lionel-Boulet</s1><s2>Varennes, Quebec J3X 1S2</s2><s3>CAN</s3><sZ>2 aut.</sZ><sZ>8 aut.</sZ></inist:fA14><country>Canada</country><wicri:noRegion>Varennes, Quebec J3X 1S2</wicri:noRegion></affiliation></author><author><name sortKey="Gobert, O" uniqKey="Gobert O">O. Gobert</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>CEA Saclay, IRAMIS, Service des Photons, Atomes et Molecules</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ><sZ>7 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Île-de-France</region><settlement type="city">Gif-sur-Yvette</settlement></placeName></affiliation></author><author><name sortKey="Hergott, J F" uniqKey="Hergott J">J.-F. Hergott</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>CEA Saclay, IRAMIS, Service des Photons, Atomes et Molecules</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ><sZ>7 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Île-de-France</region><settlement type="city">Gif-sur-Yvette</settlement></placeName></affiliation></author><author><name sortKey="Lepetit, F" uniqKey="Lepetit F">F. Lepetit</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>CEA Saclay, IRAMIS, Service des Photons, Atomes et Molecules</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ><sZ>7 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Île-de-France</region><settlement type="city">Gif-sur-Yvette</settlement></placeName></affiliation></author><author><name sortKey="Perdrix, M" uniqKey="Perdrix M">M. Perdrix</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>CEA Saclay, IRAMIS, Service des Photons, Atomes et Molecules</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ><sZ>7 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Île-de-France</region><settlement type="city">Gif-sur-Yvette</settlement></placeName></affiliation></author><author><name sortKey="Carre, B" uniqKey="Carre B">B. Carre</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>CEA Saclay, IRAMIS, Service des Photons, Atomes et Molecules</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ><sZ>7 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Île-de-France</region><settlement type="city">Gif-sur-Yvette</settlement></placeName></affiliation></author><author><name sortKey="Ozaki, T" uniqKey="Ozaki T">T. Ozaki</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Institut National de la Recherche Scientifique, Centre Energie, Materiaux et Telecommunications, 1650 Lionel-Boulet</s1><s2>Varennes, Quebec J3X 1S2</s2><s3>CAN</s3><sZ>2 aut.</sZ><sZ>8 aut.</sZ></inist:fA14><country>Canada</country><wicri:noRegion>Varennes, Quebec J3X 1S2</wicri:noRegion></affiliation></author><author><name sortKey="Salieres, P" uniqKey="Salieres P">P. Salieres</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>CEA Saclay, IRAMIS, Service des Photons, Atomes et Molecules</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ><sZ>7 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Île-de-France</region><settlement type="city">Gif-sur-Yvette</settlement></placeName></affiliation></author></titleStmt><publicationStmt><idno type="inist">12-0229889</idno><date when="2012">2012</date><idno type="stanalyst">PASCAL 12-0229889 INIST</idno><idno type="RBID">Pascal:12-0229889</idno><idno type="wicri:Area/Main/Corpus">001D31</idno><idno type="wicri:Area/Main/Repository">001B89</idno></publicationStmt><seriesStmt><idno type="ISSN">0953-4075</idno><title level="j" type="abbreviated">J. phys., B, At. mol. opt. phys. : (Print)</title><title level="j" type="main">Journal of physics. B. Atomic, molecular and optical physics : (Print)</title></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Cross correlations</term><term>Higher harmonic</term><term>Indium</term><term>Infrared laser</term><term>Ionization</term><term>Laser beams</term><term>Laser-produced plasma</term><term>Nonlinear optics</term><term>Optical frequency conversion</term><term>Optical harmonic generation</term><term>Plasma</term><term>Pulse width</term><term>Radiation sources</term><term>Radiative transition</term><term>Tin</term><term>Ultrafast optics</term><term>Ultrashort pulse</term><term>Ultraviolet radiation</term><term>as range</term><term>fs range</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Conversion fréquence optique</term><term>Harmonique supérieur</term><term>Génération harmonique optique</term><term>Corrélation croisée</term><term>Ionisation</term><term>Transition radiative</term><term>Impulsion ultracourte</term><term>Laser IR</term><term>Source rayonnement</term><term>Optique non linéaire</term><term>Faisceau laser</term><term>Rayonnement UV</term><term>Domaine temps fs</term><term>Durée impulsion</term><term>Domaine temps as</term><term>Plasma</term><term>Indium</term><term>Etain</term><term>Optique ultrarapide</term><term>Plasma produit par laser</term><term>Panache plasma</term><term>Attoseconde</term><term>5250J</term><term>0785F</term><term>4265K</term><term>4265R</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">We characterize the temporal profile of the high-order harmonic emission from ablation plasma plumes using cross-correlations with the infrared (IR) laser beam provided by two-photon harmonic+IR ionization of rare gas atoms. We study both non-resonant plasmas (lead, gold and chrome) and resonant plasmas (indium and tin), i.e. plasmas presenting in the singly charged ions a strong radiative transition coinciding with a harmonic order. The cross-correlation traces are found to be very similar for all harmonic orders and all plasma targets. The recovered harmonic pulse durations are very similar to the driving laser, with a tendency towards being shorter, demonstrating that the emission is a directly laser-driven process even in the case of resonant harmonics. This provides a valuable input for theories describing resonant-harmonic emission and opens the perspective of a very high flux tabletop XUV source for applications.</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0953-4075</s0></fA01><fA02 i1="01"><s0>JPAPEH</s0></fA02><fA03 i2="1"><s0>J. phys., B, At. mol. opt. phys. : (Print)</s0></fA03><fA05><s2>45</s2></fA05><fA06><s2>7</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>Femtosecond envelope of the high-harmonic emission from ablation plasmas</s1></fA08><fA09 i1="01" i2="1" l="ENG"><s1>10th anniversary of attosecond pulses</s1></fA09><fA11 i1="01" i2="1"><s1>HAESSLER (S.)</s1></fA11><fA11 i1="02" i2="1"><s1>ELOUGA BOM (L. B.)</s1></fA11><fA11 i1="03" i2="1"><s1>GOBERT (O.)</s1></fA11><fA11 i1="04" i2="1"><s1>HERGOTT (J.-F.)</s1></fA11><fA11 i1="05" i2="1"><s1>LEPETIT (F.)</s1></fA11><fA11 i1="06" i2="1"><s1>PERDRIX (M.)</s1></fA11><fA11 i1="07" i2="1"><s1>CARRE (B.)</s1></fA11><fA11 i1="08" i2="1"><s1>OZAKI (T.)</s1></fA11><fA11 i1="09" i2="1"><s1>SALIERES (P.)</s1></fA11><fA12 i1="01" i2="1"><s1>KIENBERGER (Reinhard)</s1><s9>ed.</s9></fA12><fA12 i1="02" i2="1"><s1>CHANG (Zenghu)</s1><s9>ed.</s9></fA12><fA12 i1="03" i2="1"><s1>CHANG HEE NAM</s1><s9>ed.</s9></fA12><fA14 i1="01"><s1>CEA Saclay, IRAMIS, Service des Photons, Atomes et Molecules</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ><sZ>7 aut.</sZ><sZ>9 aut.</sZ></fA14><fA14 i1="02"><s1>Photonics Institute, Vienna University of Technology, Gusshausstrasse 27/387</s1><s2>1040 Vienna</s2><s3>AUT</s3><sZ>1 aut.</sZ></fA14><fA14 i1="03"><s1>Institut National de la Recherche Scientifique, Centre Energie, Materiaux et Telecommunications, 1650 Lionel-Boulet</s1><s2>Varennes, Quebec J3X 1S2</s2><s3>CAN</s3><sZ>2 aut.</sZ><sZ>8 aut.</sZ></fA14><fA15 i1="01"><s1>Technische Universität München and Max-Planck-Institut für Quantenoptik</s1><s2>Garching</s2><s3>DEU</s3><sZ>1 aut.</sZ></fA15><fA15 i1="02"><s1>University of Central Florida</s1><s2>Orlando</s2><s3>USA</s3><sZ>2 aut.</sZ></fA15><fA15 i1="03"><s1>KAIST</s1><s2>Daejon</s2><s3>KOR</s3><sZ>3 aut.</sZ></fA15><fA20><s2>074012.1-074012.10</s2></fA20><fA21><s1>2012</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>577D</s2><s5>354000509691050120</s5></fA43><fA44><s0>0000</s0><s1>© 2012 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>50 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>12-0229889</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Journal of physics. B. Atomic, molecular and optical physics : (Print)</s0></fA64><fA66 i1="01"><s0>GBR</s0></fA66><fC01 i1="01" l="ENG"><s0>We characterize the temporal profile of the high-order harmonic emission from ablation plasma plumes using cross-correlations with the infrared (IR) laser beam provided by two-photon harmonic+IR ionization of rare gas atoms. We study both non-resonant plasmas (lead, gold and chrome) and resonant plasmas (indium and tin), i.e. plasmas presenting in the singly charged ions a strong radiative transition coinciding with a harmonic order. The cross-correlation traces are found to be very similar for all harmonic orders and all plasma targets. The recovered harmonic pulse durations are very similar to the driving laser, with a tendency towards being shorter, demonstrating that the emission is a directly laser-driven process even in the case of resonant harmonics. This provides a valuable input for theories describing resonant-harmonic emission and opens the perspective of a very high flux tabletop XUV source for applications.</s0></fC01><fC02 i1="01" i2="3"><s0>001B40B65K</s0></fC02><fC02 i1="02" i2="3"><s0>001B40B65R</s0></fC02><fC02 i1="03" i2="3"><s0>001B50B50J</s0></fC02><fC02 i1="04" i2="3"><s0>001B00G85F</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>Conversion fréquence optique</s0><s5>01</s5></fC03><fC03 i1="01" i2="3" l="ENG"><s0>Optical frequency conversion</s0><s5>01</s5></fC03><fC03 i1="02" i2="X" l="FRE"><s0>Harmonique supérieur</s0><s5>03</s5></fC03><fC03 i1="02" i2="X" l="ENG"><s0>Higher harmonic</s0><s5>03</s5></fC03><fC03 i1="02" i2="X" l="SPA"><s0>Armónica superior</s0><s5>03</s5></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Génération harmonique optique</s0><s5>04</s5></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Optical harmonic generation</s0><s5>04</s5></fC03><fC03 i1="04" i2="3" l="FRE"><s0>Corrélation croisée</s0><s5>05</s5></fC03><fC03 i1="04" i2="3" l="ENG"><s0>Cross correlations</s0><s5>05</s5></fC03><fC03 i1="05" i2="3" l="FRE"><s0>Ionisation</s0><s5>06</s5></fC03><fC03 i1="05" i2="3" l="ENG"><s0>Ionization</s0><s5>06</s5></fC03><fC03 i1="06" i2="X" l="FRE"><s0>Transition radiative</s0><s5>07</s5></fC03><fC03 i1="06" i2="X" l="ENG"><s0>Radiative transition</s0><s5>07</s5></fC03><fC03 i1="06" i2="X" l="SPA"><s0>Transición radiativa</s0><s5>07</s5></fC03><fC03 i1="07" i2="X" l="FRE"><s0>Impulsion ultracourte</s0><s5>08</s5></fC03><fC03 i1="07" i2="X" l="ENG"><s0>Ultrashort pulse</s0><s5>08</s5></fC03><fC03 i1="07" i2="X" l="SPA"><s0>Impulsión ultracorto</s0><s5>08</s5></fC03><fC03 i1="08" i2="X" l="FRE"><s0>Laser IR</s0><s5>11</s5></fC03><fC03 i1="08" i2="X" l="ENG"><s0>Infrared laser</s0><s5>11</s5></fC03><fC03 i1="08" i2="X" l="SPA"><s0>Laser IR</s0><s5>11</s5></fC03><fC03 i1="09" i2="3" l="FRE"><s0>Source rayonnement</s0><s5>12</s5></fC03><fC03 i1="09" i2="3" l="ENG"><s0>Radiation sources</s0><s5>12</s5></fC03><fC03 i1="10" i2="3" l="FRE"><s0>Optique non linéaire</s0><s5>17</s5></fC03><fC03 i1="10" i2="3" l="ENG"><s0>Nonlinear optics</s0><s5>17</s5></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Faisceau laser</s0><s5>37</s5></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Laser beams</s0><s5>37</s5></fC03><fC03 i1="12" i2="3" l="FRE"><s0>Rayonnement UV</s0><s5>38</s5></fC03><fC03 i1="12" i2="3" l="ENG"><s0>Ultraviolet radiation</s0><s5>38</s5></fC03><fC03 i1="13" i2="3" l="FRE"><s0>Domaine temps fs</s0><s5>41</s5></fC03><fC03 i1="13" i2="3" l="ENG"><s0>fs range</s0><s5>41</s5></fC03><fC03 i1="14" i2="X" l="FRE"><s0>Durée impulsion</s0><s5>42</s5></fC03><fC03 i1="14" i2="X" l="ENG"><s0>Pulse width</s0><s5>42</s5></fC03><fC03 i1="14" i2="X" l="SPA"><s0>Duración impulso</s0><s5>42</s5></fC03><fC03 i1="15" i2="3" l="FRE"><s0>Domaine temps as</s0><s5>43</s5></fC03><fC03 i1="15" i2="3" l="ENG"><s0>as range</s0><s5>43</s5></fC03><fC03 i1="16" i2="3" l="FRE"><s0>Plasma</s0><s5>61</s5></fC03><fC03 i1="16" i2="3" l="ENG"><s0>Plasma</s0><s5>61</s5></fC03><fC03 i1="17" i2="3" l="FRE"><s0>Indium</s0><s2>NC</s2><s5>62</s5></fC03><fC03 i1="17" i2="3" l="ENG"><s0>Indium</s0><s2>NC</s2><s5>62</s5></fC03><fC03 i1="18" i2="3" l="FRE"><s0>Etain</s0><s2>NC</s2><s5>63</s5></fC03><fC03 i1="18" i2="3" l="ENG"><s0>Tin</s0><s2>NC</s2><s5>63</s5></fC03><fC03 i1="19" i2="3" l="FRE"><s0>Optique ultrarapide</s0><s5>64</s5></fC03><fC03 i1="19" i2="3" l="ENG"><s0>Ultrafast optics</s0><s5>64</s5></fC03><fC03 i1="20" i2="3" l="FRE"><s0>Plasma produit par laser</s0><s5>65</s5></fC03><fC03 i1="20" i2="3" l="ENG"><s0>Laser-produced plasma</s0><s5>65</s5></fC03><fC03 i1="21" i2="3" l="FRE"><s0>Panache plasma</s0><s4>INC</s4><s5>83</s5></fC03><fC03 i1="22" i2="3" l="FRE"><s0>Attoseconde</s0><s4>INC</s4><s5>84</s5></fC03><fC03 i1="23" i2="3" l="FRE"><s0>5250J</s0><s4>INC</s4><s5>85</s5></fC03><fC03 i1="24" i2="3" l="FRE"><s0>0785F</s0><s4>INC</s4><s5>86</s5></fC03><fC03 i1="25" i2="3" l="FRE"><s0>4265K</s0><s4>INC</s4><s5>91</s5></fC03><fC03 i1="26" i2="3" l="FRE"><s0>4265R</s0><s4>INC</s4><s5>92</s5></fC03><fN21><s1>177</s1></fN21></pA></standard></inist></record>Pour manipuler ce document sous Unix (Dilib)
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