AustralieFrV1, PascalFrancis, Curation, bibRecord, 003A76

Optical decoherence and persistent spectral hole burning in Tm3+:LiNbO3

Identifieur interne : 003A76 ( PascalFrancis/Curation ); précédent : 003A75; suivant : 003A77

Optical decoherence and persistent spectral hole burning in Tm3+:LiNbO3

Auteurs : C. W. Thiel [États-Unis] ; Y. Sun [États-Unis] ; T. Böttger [États-Unis] ; W. R. Babbitt [États-Unis] ; R. L. Cone [États-Unis]

Source :

Journal of luminescence [ 0022-2313 ] ; 2010.

RBID : Pascal:10-0351220

Descripteurs français

Pascal (Inist)
- Hole burning, Transition optique, Dopage, Addition thulium, Etat excité, Durée vie porteur charge, Décomposition quadripolaire, Effet Stark, Effet champ électrique, Niobate de lithium, LiNbO3.
Wicri :
- topic : Dopage.

English descriptors

KwdEn :
- Carrier lifetime, Doping, Electric field effects, Excited states, Hole burning, Lithium niobates, Optical transition, Quadrupolar splitting, Stark effect, Thulium additions.

Abstract

We report studies of decoherence and spectral hole burning for the 794 nm optical transition of thulium-doped lithium niobate. In addition to transient spectral holes due to the ³H₄ and ³F₄ excited states of Tm³⁺, persistent spectral holes with lifetimes of up to minutes were observed when a magnetic field of a few hundred Gauss was applied. The observed anti-hole structure identified the hole burning mechanism as population storage in the ¹⁶⁹Tm nuclear hyperfine levels. In addition, the magnetic field was effective in suppressing spectral diffusion, increasing the phase memory lifetime from 11 μs at zero field to 23 μs in a field of 320 Gauss applied along the crystal's c-axis. Coupling between Tm³⁺ and the ⁷Li and ⁹³Nb spins in the host lattice was also observed and a quadrupole shift of 22 kHz was measured for ⁷Li at 1.7 K. A Stark shift of 18 kHz cm/V was measured for the optical transition with the electric field applied parallel to the c-axis.

A01	`01`	`1`		`@0 0022-2313`
A02	`01`			`@0 JLUMA8`
A03		`1`		`@0 J. lumin.`
A05				`@2 130`
A06				`@2 9`
A08	`01`	`1`	`ENG`	`@1 Optical decoherence and persistent spectral hole burning in Tm³⁺:LiNbO₃`
A09	`01`	`1`	`ENG`	`@1 Special Issue based on the Proceedings of the Tenth International Meeting on Hole Burning, Single Molecule, and Related Spectroscopies: Science and Applications (HBSM 2009), Palm cove, Australia, June 22-27, 2009. Issue dedicated to Ivan Lorgeré and Oliver Guillot-Noël`
A11	`01`	`1`		`@1 THIEL (C. W.)`
A11	`02`	`1`		`@1 SUN (Y.)`
A11	`03`	`1`		`@1 BÖTTGER (T.)`
A11	`04`	`1`		`@1 BABBITT (W. R.)`
A11	`05`	`1`		`@1 CONE (R. L.)`
A12	`01`	`1`		`@1 CHANELIERE (Thierry) @9 ed.`
A12	`02`	`1`		`@1 SELLARS (Matt J.) @9 ed.`
A12	`03`	`1`		`@1 MANSON (Neil B.) @9 ed.`
A14	`01`			`@1 Department of Physics, Montana State University, EPS 264 @2 Bozeman, MT 59717 @3 USA @Z 1 aut. @Z 4 aut. @Z 5 aut.`
A14	`02`			`@1 Spectrum Lab, Montana State University @2 Bozeman, MT 59717 @3 USA @Z 1 aut. @Z 4 aut.`
A14	`03`			`@1 Department of Physics, University of South Dakota @2 Vermillion, SD 57069 @3 USA @Z 2 aut.`
A14	`04`			`@1 Department of Physics, University of San Francisco @2 San Francisco, CA 94117 @3 USA @Z 3 aut.`
A15	`01`			`@1 Laboratoire Aimé Cotton, CNRS-UPR 3321, Univ. Paris-Sud, Bât. 505 @2 91405 Orsay @3 FRA @Z 1 aut.`
A15	`02`			`@1 Laser Physics Centre, Research School of Physics and Engineering, The Australian National University @2 Canberra, ACT 0200 @3 AUS @Z 2 aut. @Z 3 aut.`
A20				`@1 1598-1602`
A21				`@1 2010`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 14666 @5 354000193752120070`
A44				`@0 0000 @1 © 2010 INIST-CNRS. All rights reserved.`
A45				`@0 39 ref.`
A47	`01`	`1`		`@0 10-0351220`
A60				`@1 P @2 C`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of luminescence`
A66	`01`			`@0 NLD`
C01	`01`		`ENG`	@0 We report studies of decoherence and spectral hole burning for the 794 nm optical transition of thulium-doped lithium niobate. In addition to transient spectral holes due to the ³H₄ and ³F₄ excited states of Tm³⁺, persistent spectral holes with lifetimes of up to minutes were observed when a magnetic field of a few hundred Gauss was applied. The observed anti-hole structure identified the hole burning mechanism as population storage in the ¹⁶⁹Tm nuclear hyperfine levels. In addition, the magnetic field was effective in suppressing spectral diffusion, increasing the phase memory lifetime from 11 μs at zero field to 23 μs in a field of 320 Gauss applied along the crystal's c-axis. Coupling between Tm³⁺ and the ⁷Li and ⁹³Nb spins in the host lattice was also observed and a quadrupole shift of 22 kHz was measured for ⁷Li at 1.7 K. A Stark shift of 18 kHz cm/V was measured for the optical transition with the electric field applied parallel to the c-axis.
C02	`01`	`3`		`@0 001B70H47`
C03	`01`	`3`	`FRE`	`@0 Hole burning @5 02`
C03	`01`	`3`	`ENG`	`@0 Hole burning @5 02`
C03	`02`	`X`	`FRE`	`@0 Transition optique @5 03`
C03	`02`	`X`	`ENG`	`@0 Optical transition @5 03`
C03	`02`	`X`	`SPA`	`@0 Transición óptica @5 03`
C03	`03`	`X`	`FRE`	`@0 Dopage @5 04`
C03	`03`	`X`	`ENG`	`@0 Doping @5 04`
C03	`03`	`X`	`SPA`	`@0 Doping @5 04`
C03	`04`	`3`	`FRE`	`@0 Addition thulium @5 05`
C03	`04`	`3`	`ENG`	`@0 Thulium additions @5 05`
C03	`05`	`3`	`FRE`	`@0 Etat excité @5 06`
C03	`05`	`3`	`ENG`	`@0 Excited states @5 06`
C03	`06`	`3`	`FRE`	`@0 Durée vie porteur charge @5 07`
C03	`06`	`3`	`ENG`	`@0 Carrier lifetime @5 07`
C03	`07`	`X`	`FRE`	`@0 Décomposition quadripolaire @5 08`
C03	`07`	`X`	`ENG`	`@0 Quadrupolar splitting @5 08`
C03	`07`	`X`	`SPA`	`@0 Descomposición cuadripolar @5 08`
C03	`08`	`3`	`FRE`	`@0 Effet Stark @5 13`
C03	`08`	`3`	`ENG`	`@0 Stark effect @5 13`
C03	`09`	`3`	`FRE`	`@0 Effet champ électrique @5 14`
C03	`09`	`3`	`ENG`	`@0 Electric field effects @5 14`
C03	`10`	`3`	`FRE`	`@0 Niobate de lithium @2 NK @5 15`
C03	`10`	`3`	`ENG`	`@0 Lithium niobates @2 NK @5 15`
C03	`11`	`3`	`FRE`	`@0 LiNbO3 @4 INC @5 52`
N21				`@1 221`

A30	`01`	`1`	`ENG`	`@1 International Conference on Hole Burning, Single Molecule, and Related Spectroscopies: Science and Applications (HBSM 2009) @2 10 @3 Palm Cove AUS @4 2009-06-22`

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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Optical decoherence and persistent spectral hole burning in Tm<sup>3+</sup>
:LiNbO<sub>3</sub>
</title>
<author><name sortKey="Thiel, C W" sort="Thiel, C W" uniqKey="Thiel C" first="C. W." last="Thiel">C. W. Thiel</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, Montana State University, EPS 264</s1>
<s2>Bozeman, MT 59717</s2>
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<sZ>1 aut.</sZ>
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<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Spectrum Lab, Montana State University</s1>
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<author><name sortKey="Sun, Y" sort="Sun, Y" uniqKey="Sun Y" first="Y." last="Sun">Y. Sun</name>
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<s2>Vermillion, SD 57069</s2>
<s3>USA</s3>
<sZ>2 aut.</sZ>
</inist:fA14>
<country>États-Unis</country>
</affiliation>
</author>
<author><name sortKey="Bottger, T" sort="Bottger, T" uniqKey="Bottger T" first="T." last="Böttger">T. Böttger</name>
<affiliation wicri:level="1"><inist:fA14 i1="04"><s1>Department of Physics, University of San Francisco</s1>
<s2>San Francisco, CA 94117</s2>
<s3>USA</s3>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>États-Unis</country>
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<author><name sortKey="Babbitt, W R" sort="Babbitt, W R" uniqKey="Babbitt W" first="W. R." last="Babbitt">W. R. Babbitt</name>
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<s2>Bozeman, MT 59717</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
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<country>États-Unis</country>
</affiliation>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Spectrum Lab, Montana State University</s1>
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<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
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<author><name sortKey="Cone, R L" sort="Cone, R L" uniqKey="Cone R" first="R. L." last="Cone">R. L. Cone</name>
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<series><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
<idno type="ISSN">0022-2313</idno>
<imprint><date when="2010">2010</date>
</imprint>
</series>
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<seriesStmt><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
<idno type="ISSN">0022-2313</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Carrier lifetime</term>
<term>Doping</term>
<term>Electric field effects</term>
<term>Excited states</term>
<term>Hole burning</term>
<term>Lithium niobates</term>
<term>Optical transition</term>
<term>Quadrupolar splitting</term>
<term>Stark effect</term>
<term>Thulium additions</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Hole burning</term>
<term>Transition optique</term>
<term>Dopage</term>
<term>Addition thulium</term>
<term>Etat excité</term>
<term>Durée vie porteur charge</term>
<term>Décomposition quadripolaire</term>
<term>Effet Stark</term>
<term>Effet champ électrique</term>
<term>Niobate de lithium</term>
<term>LiNbO3</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">We report studies of decoherence and spectral hole burning for the 794 nm optical transition of thulium-doped lithium niobate. In addition to transient spectral holes due to the <sup>3</sup>
H<sub>4</sub>
 and <sup>3</sup>
F<sub>4</sub>
 excited states of Tm<sup>3+</sup>
, persistent spectral holes with lifetimes of up to minutes were observed when a magnetic field of a few hundred Gauss was applied. The observed anti-hole structure identified the hole burning mechanism as population storage in the <sup>169</sup>
Tm nuclear hyperfine levels. In addition, the magnetic field was effective in suppressing spectral diffusion, increasing the phase memory lifetime from 11 μs at zero field to 23 μs in a field of 320 Gauss applied along the crystal's c-axis. Coupling between Tm<sup>3+</sup>
 and the <sup>7</sup>
Li and <sup>93</sup>
Nb spins in the host lattice was also observed and a quadrupole shift of 22 kHz was measured for <sup>7</sup>
Li at 1.7 K. A Stark shift of 18 kHz cm/V was measured for the optical transition with the electric field applied parallel to the c-axis.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0022-2313</s0>
</fA01>
<fA02 i1="01"><s0>JLUMA8</s0>
</fA02>
<fA03 i2="1"><s0>J. lumin.</s0>
</fA03>
<fA05><s2>130</s2>
</fA05>
<fA06><s2>9</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Optical decoherence and persistent spectral hole burning in Tm<sup>3+</sup>
:LiNbO<sub>3</sub>
</s1>
</fA08>
<fA09 i1="01" i2="1" l="ENG"><s1>Special Issue based on the Proceedings of the Tenth International Meeting on Hole Burning, Single Molecule, and Related Spectroscopies: Science and Applications (HBSM 2009), Palm cove, Australia, June 22-27, 2009. Issue dedicated to Ivan Lorgeré and Oliver Guillot-Noël</s1>
</fA09>
<fA11 i1="01" i2="1"><s1>THIEL (C. W.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>SUN (Y.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>BÖTTGER (T.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>BABBITT (W. R.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>CONE (R. L.)</s1>
</fA11>
<fA12 i1="01" i2="1"><s1>CHANELIERE (Thierry)</s1>
<s9>ed.</s9>
</fA12>
<fA12 i1="02" i2="1"><s1>SELLARS (Matt J.)</s1>
<s9>ed.</s9>
</fA12>
<fA12 i1="03" i2="1"><s1>MANSON (Neil B.)</s1>
<s9>ed.</s9>
</fA12>
<fA14 i1="01"><s1>Department of Physics, Montana State University, EPS 264</s1>
<s2>Bozeman, MT 59717</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Spectrum Lab, Montana State University</s1>
<s2>Bozeman, MT 59717</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Department of Physics, University of South Dakota</s1>
<s2>Vermillion, SD 57069</s2>
<s3>USA</s3>
<sZ>2 aut.</sZ>
</fA14>
<fA14 i1="04"><s1>Department of Physics, University of San Francisco</s1>
<s2>San Francisco, CA 94117</s2>
<s3>USA</s3>
<sZ>3 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>1598-1602</s1>
</fA20>
<fA21><s1>2010</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>14666</s2>
<s5>354000193752120070</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2010 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>39 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>10-0351220</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 report studies of decoherence and spectral hole burning for the 794 nm optical transition of thulium-doped lithium niobate. In addition to transient spectral holes due to the <sup>3</sup>
H<sub>4</sub>
 and <sup>3</sup>
F<sub>4</sub>
 excited states of Tm<sup>3+</sup>
, persistent spectral holes with lifetimes of up to minutes were observed when a magnetic field of a few hundred Gauss was applied. The observed anti-hole structure identified the hole burning mechanism as population storage in the <sup>169</sup>
Tm nuclear hyperfine levels. In addition, the magnetic field was effective in suppressing spectral diffusion, increasing the phase memory lifetime from 11 μs at zero field to 23 μs in a field of 320 Gauss applied along the crystal's c-axis. Coupling between Tm<sup>3+</sup>
 and the <sup>7</sup>
Li and <sup>93</sup>
Nb spins in the host lattice was also observed and a quadrupole shift of 22 kHz was measured for <sup>7</sup>
Li at 1.7 K. A Stark shift of 18 kHz cm/V was measured for the optical transition with the electric field applied parallel to the c-axis.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70H47</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Hole burning</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Hole burning</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE"><s0>Transition optique</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="X" l="ENG"><s0>Optical transition</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA"><s0>Transición óptica</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="X" l="FRE"><s0>Dopage</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="X" l="ENG"><s0>Doping</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="X" l="SPA"><s0>Doping</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Etat excité</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Excited states</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Durée vie porteur charge</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Carrier lifetime</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE"><s0>Décomposition quadripolaire</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Quadrupolar splitting</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Descomposición cuadripolar</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Effet Stark</s0>
<s5>13</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Stark effect</s0>
<s5>13</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Effet champ électrique</s0>
<s5>14</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Electric field effects</s0>
<s5>14</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Niobate de lithium</s0>
<s2>NK</s2>
<s5>15</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Lithium niobates</s0>
<s2>NK</s2>
<s5>15</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>LiNbO3</s0>
<s4>INC</s4>
<s5>52</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>
</record>

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Optical decoherence and persistent spectral hole burning in Tm3+:LiNbO3

Optical decoherence and persistent spectral hole burning in Tm3+:LiNbO3

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