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Efficient optical pumping of Zeeman spin levels in Nd3+: YVO4

Identifieur interne : 002454 ( PascalFrancis/Checkpoint ); précédent : 002453; suivant : 002455

Efficient optical pumping of Zeeman spin levels in Nd3+: YVO4

Auteurs : Mikael Afzelius [Suisse] ; Matthias U. Staudt [Suisse] ; Hugues De Riedmatten [Suisse] ; Nicolas Gisin [Suisse] ; Olivier Guillot-Noël [France] ; Philippe Goldner [France] ; Robert Marino [France] ; Pierre Porcher [France] ; Enrico Cavalli [Italie] ; Marco Bettinelli [Italie]

Source :

RBID : Pascal:10-0351218

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English descriptors

Abstract

We demonstrate that Zeeman ground-state spin levels in Nd3+: YVO4 provides the possibility to create an efficient A- system for optical pumping experiments. The branching ratio R in the A-system is measured experimentally via absorption spectroscopy and is compared to a theoretical model. We show that R can be tuned by changing the orientation of the magnetic field. These results are applied to optical pumping experiments, where significant improvement is obtained compared to previous experiments in this system. The tunability of the branching ratio in combination with its good coherence properties and the high oscillator strength makes Nd3+: YVO4 an interesting candidate for various quantum information protocols.


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<term>Absorption spectra</term>
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<term>Doping</term>
<term>Energy-level splitting</term>
<term>Ground states</term>
<term>Magnetic field effects</term>
<term>Neodymium additions</term>
<term>Optical pumping</term>
<term>Oscillator strengths</term>
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<term>Pompage optique</term>
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<term>Spectre absorption</term>
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<div type="abstract" xml:lang="en">We demonstrate that Zeeman ground-state spin levels in Nd
<sup>3+</sup>
: YVO
<sub>4</sub>
provides the possibility to create an efficient A- system for optical pumping experiments. The branching ratio R in the A-system is measured experimentally via absorption spectroscopy and is compared to a theoretical model. We show that R can be tuned by changing the orientation of the magnetic field. These results are applied to optical pumping experiments, where significant improvement is obtained compared to previous experiments in this system. The tunability of the branching ratio in combination with its good coherence properties and the high oscillator strength makes Nd
<sup>3+</sup>
: YVO
<sub>4</sub>
an interesting candidate for various quantum information protocols.</div>
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<s2>75231 Paris</s2>
<s3>FRA</s3>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
</fA14>
<fA14 i1="03">
<s1>Dipartimento di Chimica Generale ed Inorganica, Chimica Analitica e Chimica, Fisica, Università di Parma, Viale G. P. Usberti 17/a</s1>
<s2>43100 Parma</s2>
<s3>ITA</s3>
<sZ>9 aut.</sZ>
</fA14>
<fA14 i1="04">
<s1>Dipartimento Scientifico e Tecnologico, Univ. Verona Strada Le Grazie 15</s1>
<s2>37134 Verona</s2>
<s3>ITA</s3>
<sZ>10 aut.</sZ>
</fA14>
<fA15 i1="01">
<s1>Laboratoire Aimé Cotton, CNRS-UPR 3321, Univ. Paris-Sud, Bât. 505</s1>
<s2>91405 Orsay</s2>
<s3>FRA</s3>
<sZ>1 aut.</sZ>
</fA15>
<fA15 i1="02">
<s1>Laser Physics Centre, Research School of Physics and Engineering, The Australian National University</s1>
<s2>Canberra, ACT 0200</s2>
<s3>AUS</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</fA15>
<fA20>
<s1>1566-1571</s1>
</fA20>
<fA21>
<s1>2010</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>14666</s2>
<s5>354000193752120020</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2010 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>36 ref.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>10-0351218</s0>
</fA47>
<fA60>
<s1>P</s1>
<s2>C</s2>
</fA60>
<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Journal of luminescence</s0>
</fA64>
<fA66 i1="01">
<s0>NLD</s0>
</fA66>
<fC01 i1="01" l="ENG">
<s0>We demonstrate that Zeeman ground-state spin levels in Nd
<sup>3+</sup>
: YVO
<sub>4</sub>
provides the possibility to create an efficient A- system for optical pumping experiments. The branching ratio R in the A-system is measured experimentally via absorption spectroscopy and is compared to a theoretical model. We show that R can be tuned by changing the orientation of the magnetic field. These results are applied to optical pumping experiments, where significant improvement is obtained compared to previous experiments in this system. The tunability of the branching ratio in combination with its good coherence properties and the high oscillator strength makes Nd
<sup>3+</sup>
: YVO
<sub>4</sub>
an interesting candidate for various quantum information protocols.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001B70H20C</s0>
</fC02>
<fC02 i1="02" i2="3">
<s0>001B70A70E</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Pompage optique</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Optical pumping</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE">
<s0>Effet Zeeman</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG">
<s0>Zeeman effect</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Etat fondamental</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Ground states</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE">
<s0>Décomposition niveau énergie</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG">
<s0>Energy-level splitting</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Rapport branchement</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Branching ratio</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE">
<s0>Spectre absorption</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG">
<s0>Absorption spectra</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Effet champ magnétique</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Magnetic field effects</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE">
<s0>Dopage</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG">
<s0>Doping</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA">
<s0>Doping</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Force oscillateur</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Oscillator strengths</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Addition néodyme</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG">
<s0>Neodymium additions</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Yttrium Vanadate</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>15</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Yttrium Vanadates</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>15</s5>
</fC03>
<fN21>
<s1>221</s1>
</fN21>
</pA>
<pR>
<fA30 i1="01" i2="1" l="ENG">
<s1>International Conference on Hole Burning, Single Molecule, and Related Spectroscopies: Science and Applications (HBSM 2009)</s1>
<s2>10</s2>
<s3>Palm Cove AUS</s3>
<s4>2009-06-22</s4>
</fA30>
</pR>
</standard>
</inist>
<affiliations>
<list>
<country>
<li>France</li>
<li>Italie</li>
<li>Suisse</li>
</country>
<region>
<li>Canton de Genève</li>
<li>Île-de-France</li>
</region>
<settlement>
<li>Genève</li>
<li>Paris</li>
</settlement>
<orgName>
<li>Université de Genève</li>
</orgName>
</list>
<tree>
<country name="Suisse">
<region name="Canton de Genève">
<name sortKey="Afzelius, Mikael" sort="Afzelius, Mikael" uniqKey="Afzelius M" first="Mikael" last="Afzelius">Mikael Afzelius</name>
</region>
<name sortKey="De Riedmatten, Hugues" sort="De Riedmatten, Hugues" uniqKey="De Riedmatten H" first="Hugues" last="De Riedmatten">Hugues De Riedmatten</name>
<name sortKey="Gisin, Nicolas" sort="Gisin, Nicolas" uniqKey="Gisin N" first="Nicolas" last="Gisin">Nicolas Gisin</name>
<name sortKey="Staudt, Matthias U" sort="Staudt, Matthias U" uniqKey="Staudt M" first="Matthias U." last="Staudt">Matthias U. Staudt</name>
</country>
<country name="France">
<region name="Île-de-France">
<name sortKey="Guillot Noel, Olivier" sort="Guillot Noel, Olivier" uniqKey="Guillot Noel O" first="Olivier" last="Guillot-Noël">Olivier Guillot-Noël</name>
</region>
<name sortKey="Goldner, Philippe" sort="Goldner, Philippe" uniqKey="Goldner P" first="Philippe" last="Goldner">Philippe Goldner</name>
<name sortKey="Marino, Robert" sort="Marino, Robert" uniqKey="Marino R" first="Robert" last="Marino">Robert Marino</name>
<name sortKey="Porcher, Pierre" sort="Porcher, Pierre" uniqKey="Porcher P" first="Pierre" last="Porcher">Pierre Porcher</name>
</country>
<country name="Italie">
<noRegion>
<name sortKey="Cavalli, Enrico" sort="Cavalli, Enrico" uniqKey="Cavalli E" first="Enrico" last="Cavalli">Enrico Cavalli</name>
</noRegion>
<name sortKey="Bettinelli, Marco" sort="Bettinelli, Marco" uniqKey="Bettinelli M" first="Marco" last="Bettinelli">Marco Bettinelli</name>
</country>
</tree>
</affiliations>
</record>

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