ThuliumV1, Pascal, Curation, bibRecord, 000568

Optical investigation of nuclear spin coherence in Tm:YAG

Identifieur interne : 000568 ( Pascal/Curation ); précédent : 000567; suivant : 000569

Optical investigation of nuclear spin coherence in Tm:YAG

Auteurs : A. Louchet [France] ; Y. Le Du [France] ; T. Brouri [France] ; F. Bretenaker [France] ; T. Chaneliere [France] ; F. Goldfarb [France] ; I. Lorgere [France] ; J.-L. Le Gouët [France]

Source :

Solid state sciences [ 1293-2558 ] ; 2008.

RBID : Pascal:09-0032391

Descripteurs français

Pascal (Inist)
- Spin nucléaire, Addition thulium, Durée vie, Ordinateur quantique, Spectrométrie Raman, Décomposition hyperfine, Champ extérieur, Effet champ magnétique, Etat électronique, Propriété électronique, Structure électronique, Densité état électron, Etat fondamental, Oxyde d'aluminium, Grenat aluminium yttrium, Oxyde d'yttrium, Cristal quantique, Matériau dopé, Dopage, Addition lanthanide, Système 3 niveaux, Détection hétérodyne, Tm, 0367L.
Wicri :
- topic : Dopage.

English descriptors

KwdEn :
- Aluminium oxide, Doped materials, Doping, Electron state, Electronic density of states, Electronic properties, Electronic structure, External fields, Ground states, Heterodyne detection, Hyperfine splitting, Lifetime, Magnetic field effects, Nuclear spin, Quantum computer, Quantum crystals, Raman spectroscopy, Rare earth additions, Three-level systems, Thulium additions, YAG, Yttrium oxide.

Abstract

With all-optical means, the nuclear spin coherence lifetime is measured for the first time in a crystal doped with low-concentration thulium. A novel Raman echo scheme is demonstrated. The hyperfine splitting is varied over a 15 MHz-wide range with the help of an external magnetic field. Over this range the spin coherence lifetime remains close to 350 [is in the electronic ground state. Thulium-doped materials are proved to be interesting substitutes to other rare earth ion-doped crystals as quantum memory candidates, thanks to their convenient wavelength, their adjustable three-level system and their stable and long spin coherence lifetime.

A01	`01`	`1`		`@0 1293-2558`
A03		`1`		`@0 Solid state sci.`
A05				`@2 10`
A06				`@2 10`
A08	`01`	`1`	`ENG`	`@1 Optical investigation of nuclear spin coherence in Tm:YAG`
A11	`01`	`1`		`@1 LOUCHET (A.)`
A11	`02`	`1`		`@1 LE DU (Y.)`
A11	`03`	`1`		`@1 BROURI (T.)`
A11	`04`	`1`		`@1 BRETENAKER (F.)`
A11	`05`	`1`		`@1 CHANELIERE (T.)`
A11	`06`	`1`		`@1 GOLDFARB (F.)`
A11	`07`	`1`		`@1 LORGERE (I.)`
A11	`08`	`1`		`@1 LE GOUËT (J.-L.)`
A14	`01`			`@1 Laboratoire Aimé Cotton, CNRS-UPR 3321, Université Paris Sud, Bâtiment 505 @2 91405 Orsay @3 FRA @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. @Z 6 aut. @Z 7 aut. @Z 8 aut.`
A20				`@1 1374-1378`
A21				`@1 2008`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 11118 @5 354000184267920170`
A44				`@0 0000 @1 © 2009 INIST-CNRS. All rights reserved.`
A45				`@0 27 ref.`
A47	`01`	`1`		`@0 09-0032391`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Solid state sciences`
A66	`01`			`@0 FRA`
C01	`01`		`ENG`	@0 With all-optical means, the nuclear spin coherence lifetime is measured for the first time in a crystal doped with low-concentration thulium. A novel Raman echo scheme is demonstrated. The hyperfine splitting is varied over a 15 MHz-wide range with the help of an external magnetic field. Over this range the spin coherence lifetime remains close to 350 [is in the electronic ground state. Thulium-doped materials are proved to be interesting substitutes to other rare earth ion-doped crystals as quantum memory candidates, thanks to their convenient wavelength, their adjustable three-level system and their stable and long spin coherence lifetime.
C02	`01`	`3`		`@0 001B00C67L`
C03	`01`	`3`	`FRE`	`@0 Spin nucléaire @5 01`
C03	`01`	`3`	`ENG`	`@0 Nuclear spin @5 01`
C03	`02`	`3`	`FRE`	`@0 Addition thulium @5 02`
C03	`02`	`3`	`ENG`	`@0 Thulium additions @5 02`
C03	`03`	`3`	`FRE`	`@0 Durée vie @5 03`
C03	`03`	`3`	`ENG`	`@0 Lifetime @5 03`
C03	`04`	`3`	`FRE`	`@0 Ordinateur quantique @5 04`
C03	`04`	`3`	`ENG`	`@0 Quantum computer @5 04`
C03	`05`	`3`	`FRE`	`@0 Spectrométrie Raman @5 06`
C03	`05`	`3`	`ENG`	`@0 Raman spectroscopy @5 06`
C03	`06`	`X`	`FRE`	`@0 Décomposition hyperfine @5 07`
C03	`06`	`X`	`ENG`	`@0 Hyperfine splitting @5 07`
C03	`06`	`X`	`SPA`	`@0 Descomposición hiperfina @5 07`
C03	`07`	`3`	`FRE`	`@0 Champ extérieur @5 08`
C03	`07`	`3`	`ENG`	`@0 External fields @5 08`
C03	`08`	`3`	`FRE`	`@0 Effet champ magnétique @5 09`
C03	`08`	`3`	`ENG`	`@0 Magnetic field effects @5 09`
C03	`09`	`X`	`FRE`	`@0 Etat électronique @5 10`
C03	`09`	`X`	`ENG`	`@0 Electron state @5 10`
C03	`09`	`X`	`SPA`	`@0 Estado electrónico @5 10`
C03	`10`	`X`	`FRE`	`@0 Propriété électronique @5 11`
C03	`10`	`X`	`ENG`	`@0 Electronic properties @5 11`
C03	`10`	`X`	`SPA`	`@0 Propiedad electrónica @5 11`
C03	`11`	`3`	`FRE`	`@0 Structure électronique @5 12`
C03	`11`	`3`	`ENG`	`@0 Electronic structure @5 12`
C03	`12`	`3`	`FRE`	`@0 Densité état électron @5 13`
C03	`12`	`3`	`ENG`	`@0 Electronic density of states @5 13`
C03	`13`	`3`	`FRE`	`@0 Etat fondamental @5 14`
C03	`13`	`3`	`ENG`	`@0 Ground states @5 14`
C03	`14`	`X`	`FRE`	`@0 Oxyde d'aluminium @5 15`
C03	`14`	`X`	`ENG`	`@0 Aluminium oxide @5 15`
C03	`14`	`X`	`SPA`	`@0 Aluminio óxido @5 15`
C03	`15`	`3`	`FRE`	`@0 Grenat aluminium yttrium @5 16`
C03	`15`	`3`	`ENG`	`@0 YAG @5 16`
C03	`16`	`X`	`FRE`	`@0 Oxyde d'yttrium @5 17`
C03	`16`	`X`	`ENG`	`@0 Yttrium oxide @5 17`
C03	`16`	`X`	`SPA`	`@0 Ytrio óxido @5 17`
C03	`17`	`3`	`FRE`	`@0 Cristal quantique @5 18`
C03	`17`	`3`	`ENG`	`@0 Quantum crystals @5 18`
C03	`18`	`3`	`FRE`	`@0 Matériau dopé @5 29`
C03	`18`	`3`	`ENG`	`@0 Doped materials @5 29`
C03	`19`	`X`	`FRE`	`@0 Dopage @5 30`
C03	`19`	`X`	`ENG`	`@0 Doping @5 30`
C03	`19`	`X`	`SPA`	`@0 Doping @5 30`
C03	`20`	`3`	`FRE`	`@0 Addition lanthanide @5 31`
C03	`20`	`3`	`ENG`	`@0 Rare earth additions @5 31`
C03	`21`	`3`	`FRE`	`@0 Système 3 niveaux @5 33`
C03	`21`	`3`	`ENG`	`@0 Three-level systems @5 33`
C03	`22`	`3`	`FRE`	`@0 Détection hétérodyne @5 34`
C03	`22`	`3`	`ENG`	`@0 Heterodyne detection @5 34`
C03	`23`	`3`	`FRE`	`@0 Tm @4 INC @5 46`
C03	`24`	`3`	`FRE`	`@0 0367L @4 INC @5 65`
N21				`@1 022`

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Pascal:09-0032391

Le document en format XML

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<author><name sortKey="Le Gouet, J L" sort="Le Gouet, J L" uniqKey="Le Gouet J" first="J.-L." last="Le Gouët">J.-L. Le Gouët</name>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Aluminium oxide</term>
<term>Doped materials</term>
<term>Doping</term>
<term>Electron state</term>
<term>Electronic density of states</term>
<term>Electronic properties</term>
<term>Electronic structure</term>
<term>External fields</term>
<term>Ground states</term>
<term>Heterodyne detection</term>
<term>Hyperfine splitting</term>
<term>Lifetime</term>
<term>Magnetic field effects</term>
<term>Nuclear spin</term>
<term>Quantum computer</term>
<term>Quantum crystals</term>
<term>Raman spectroscopy</term>
<term>Rare earth additions</term>
<term>Three-level systems</term>
<term>Thulium additions</term>
<term>YAG</term>
<term>Yttrium oxide</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Spin nucléaire</term>
<term>Addition thulium</term>
<term>Durée vie</term>
<term>Ordinateur quantique</term>
<term>Spectrométrie Raman</term>
<term>Décomposition hyperfine</term>
<term>Champ extérieur</term>
<term>Effet champ magnétique</term>
<term>Etat électronique</term>
<term>Propriété électronique</term>
<term>Structure électronique</term>
<term>Densité état électron</term>
<term>Etat fondamental</term>
<term>Oxyde d'aluminium</term>
<term>Grenat aluminium yttrium</term>
<term>Oxyde d'yttrium</term>
<term>Cristal quantique</term>
<term>Matériau dopé</term>
<term>Dopage</term>
<term>Addition lanthanide</term>
<term>Système 3 niveaux</term>
<term>Détection hétérodyne</term>
<term>Tm</term>
<term>0367L</term>
</keywords>
<keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Dopage</term>
</keywords>
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<front><div type="abstract" xml:lang="en">With all-optical means, the nuclear spin coherence lifetime is measured for the first time in a crystal doped with low-concentration thulium. A novel Raman echo scheme is demonstrated. The hyperfine splitting is varied over a 15 MHz-wide range with the help of an external magnetic field. Over this range the spin coherence lifetime remains close to 350 [is in the electronic ground state. Thulium-doped materials are proved to be interesting substitutes to other rare earth ion-doped crystals as quantum memory candidates, thanks to their convenient wavelength, their adjustable three-level system and their stable and long spin coherence lifetime.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>1293-2558</s0>
</fA01>
<fA03 i2="1"><s0>Solid state sci.</s0>
</fA03>
<fA05><s2>10</s2>
</fA05>
<fA06><s2>10</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Optical investigation of nuclear spin coherence in Tm:YAG</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>LOUCHET (A.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>LE DU (Y.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>BROURI (T.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>BRETENAKER (F.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>CHANELIERE (T.)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>GOLDFARB (F.)</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>LORGERE (I.)</s1>
</fA11>
<fA11 i1="08" i2="1"><s1>LE GOUËT (J.-L.)</s1>
</fA11>
<fA14 i1="01"><s1>Laboratoire Aimé Cotton, CNRS-UPR 3321, Université Paris Sud, Bâtiment 505</s1>
<s2>91405 Orsay</s2>
<s3>FRA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
</fA14>
<fA20><s1>1374-1378</s1>
</fA20>
<fA21><s1>2008</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>11118</s2>
<s5>354000184267920170</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2009 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>27 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>09-0032391</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Solid state sciences</s0>
</fA64>
<fA66 i1="01"><s0>FRA</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>With all-optical means, the nuclear spin coherence lifetime is measured for the first time in a crystal doped with low-concentration thulium. A novel Raman echo scheme is demonstrated. The hyperfine splitting is varied over a 15 MHz-wide range with the help of an external magnetic field. Over this range the spin coherence lifetime remains close to 350 [is in the electronic ground state. Thulium-doped materials are proved to be interesting substitutes to other rare earth ion-doped crystals as quantum memory candidates, thanks to their convenient wavelength, their adjustable three-level system and their stable and long spin coherence lifetime.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B00C67L</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Spin nucléaire</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Nuclear spin</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Durée vie</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Lifetime</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Ordinateur quantique</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Quantum computer</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Spectrométrie Raman</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Raman spectroscopy</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE"><s0>Décomposition hyperfine</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG"><s0>Hyperfine splitting</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA"><s0>Descomposición hiperfina</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Champ extérieur</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>External fields</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Effet champ magnétique</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Magnetic field effects</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE"><s0>Etat électronique</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG"><s0>Electron state</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA"><s0>Estado electrónico</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Propriété électronique</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Electronic properties</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Propiedad electrónica</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Structure électronique</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Electronic structure</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Densité état électron</s0>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Electronic density of states</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Etat fondamental</s0>
<s5>14</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Ground states</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE"><s0>Oxyde d'aluminium</s0>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="X" l="ENG"><s0>Aluminium oxide</s0>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA"><s0>Aluminio óxido</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Grenat aluminium yttrium</s0>
<s5>16</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>YAG</s0>
<s5>16</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE"><s0>Oxyde d'yttrium</s0>
<s5>17</s5>
</fC03>
<fC03 i1="16" i2="X" l="ENG"><s0>Yttrium oxide</s0>
<s5>17</s5>
</fC03>
<fC03 i1="16" i2="X" l="SPA"><s0>Ytrio óxido</s0>
<s5>17</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Cristal quantique</s0>
<s5>18</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG"><s0>Quantum crystals</s0>
<s5>18</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>29</s5>
</fC03>
<fC03 i1="18" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>29</s5>
</fC03>
<fC03 i1="19" i2="X" l="FRE"><s0>Dopage</s0>
<s5>30</s5>
</fC03>
<fC03 i1="19" i2="X" l="ENG"><s0>Doping</s0>
<s5>30</s5>
</fC03>
<fC03 i1="19" i2="X" l="SPA"><s0>Doping</s0>
<s5>30</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>Addition lanthanide</s0>
<s5>31</s5>
</fC03>
<fC03 i1="20" i2="3" l="ENG"><s0>Rare earth additions</s0>
<s5>31</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>Système 3 niveaux</s0>
<s5>33</s5>
</fC03>
<fC03 i1="21" i2="3" l="ENG"><s0>Three-level systems</s0>
<s5>33</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE"><s0>Détection hétérodyne</s0>
<s5>34</s5>
</fC03>
<fC03 i1="22" i2="3" l="ENG"><s0>Heterodyne detection</s0>
<s5>34</s5>
</fC03>
<fC03 i1="23" i2="3" l="FRE"><s0>Tm</s0>
<s4>INC</s4>
<s5>46</s5>
</fC03>
<fC03 i1="24" i2="3" l="FRE"><s0>0367L</s0>
<s4>INC</s4>
<s5>65</s5>
</fC03>
<fN21><s1>022</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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Optical investigation of nuclear spin coherence in Tm:YAG

Optical investigation of nuclear spin coherence in Tm:YAG

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