IndiumV3, France, Analysis, bibRecord, 001D42

Quantum wells with zero valence-band offset: Drastic enhancement of forbidden excitonic transitions

Identifieur interne : 001D42 ( France/Analysis ); précédent : 001D41; suivant : 001D43

Quantum wells with zero valence-band offset: Drastic enhancement of forbidden excitonic transitions

Auteurs : RBID : Pascal:97-0112251

Descripteurs français

Pascal (Inist)
- 7135J, 7550P, 7866F, 7866H, Etude expérimentale, Etude théorique.

English descriptors

KwdEn :
- Experimental study, Theoretical study.

Abstract

Forbidden e1hh3 and e1lh3 exciton transitions (where hh and lh are heavy-hole and light-hole, respectively) appear in magnetooptical spectra of quantum wells that undergo a type-I-type-II band-alignment transition, here for ordinary (In,Ga)As/GaAs multiple quantum wells and a single CdTe quantum well with a (Cd,Mn)Te semimagnetic barrier exhibiting a giant Zeeman effect. The oscillator strength becomes so strong in a field of 11.25 T that vacuum-field Rabi splitting is clearly seen in reflection spectra when the e1lh3 exciton transition couples to the two-dimensional optical mode in a microcavity. © 1996 The American Physical Society.

Links toward previous steps (curation, corpus...)

to stream Main, to step Corpus: 018999
to stream Main, to step Repository: 019821
to stream France, to step Extraction: 001D42

Links to Exploration step

Pascal:97-0112251

Le document en format XML

<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Quantum wells with zero valence-band offset: Drastic enhancement of forbidden excitonic transitions</title>
<author><name sortKey="Kavokin, A V" uniqKey="Kavokin A">A. V. Kavokin</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>A. F. Ioffe Physico-Technical Institute, 26 Politechnicheskaya, St. Petersburg 194021, Russia</s1>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">Russie</country>
<wicri:regionArea>A. F. Ioffe Physico-Technical Institute, 26 Politechnicheskaya, St. Petersburg 194021</wicri:regionArea>
<wicri:noRegion>St. Petersburg 194021</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Kaliteevski, M A" uniqKey="Kaliteevski M">M. A. Kaliteevski</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>A. F. Ioffe Physico-Technical Institute, 26 Politechnicheskaya, St. Petersburg 194021, Russia</s1>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">Russie</country>
<wicri:regionArea>A. F. Ioffe Physico-Technical Institute, 26 Politechnicheskaya, St. Petersburg 194021</wicri:regionArea>
<wicri:noRegion>St. Petersburg 194021</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Goupalov, S V" uniqKey="Goupalov S">S. V. Goupalov</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>A. F. Ioffe Physico-Technical Institute, 26 Politechnicheskaya, St. Petersburg 194021, Russia</s1>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">Russie</country>
<wicri:regionArea>A. F. Ioffe Physico-Technical Institute, 26 Politechnicheskaya, St. Petersburg 194021</wicri:regionArea>
<wicri:noRegion>St. Petersburg 194021</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Berger, J D" uniqKey="Berger J">J. D. Berger</name>
<affiliation wicri:level="2"><inist:fA14 i1="02"><s1>Optical Sciences Center, University of Arizona, Tucson, Arizona 85721</s1>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">États-Unis</country>
<placeName><region type="state">Arizona</region>
</placeName>
<wicri:cityArea>Optical Sciences Center, University of Arizona, Tucson</wicri:cityArea>
</affiliation>
</author>
<author><name sortKey="Lyngnes, O" uniqKey="Lyngnes O">O. Lyngnes</name>
<affiliation wicri:level="2"><inist:fA14 i1="02"><s1>Optical Sciences Center, University of Arizona, Tucson, Arizona 85721</s1>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">États-Unis</country>
<placeName><region type="state">Arizona</region>
</placeName>
<wicri:cityArea>Optical Sciences Center, University of Arizona, Tucson</wicri:cityArea>
</affiliation>
</author>
<author><name sortKey="Gibbs, H M" uniqKey="Gibbs H">H. M. Gibbs</name>
<affiliation wicri:level="2"><inist:fA14 i1="02"><s1>Optical Sciences Center, University of Arizona, Tucson, Arizona 85721</s1>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">États-Unis</country>
<placeName><region type="state">Arizona</region>
</placeName>
<wicri:cityArea>Optical Sciences Center, University of Arizona, Tucson</wicri:cityArea>
</affiliation>
</author>
<author><name sortKey="Khitrova, G" uniqKey="Khitrova G">G. Khitrova</name>
<affiliation wicri:level="2"><inist:fA14 i1="02"><s1>Optical Sciences Center, University of Arizona, Tucson, Arizona 85721</s1>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">États-Unis</country>
<placeName><region type="state">Arizona</region>
</placeName>
<wicri:cityArea>Optical Sciences Center, University of Arizona, Tucson</wicri:cityArea>
</affiliation>
</author>
<author><name sortKey="Ribayrol, A" uniqKey="Ribayrol A">A. Ribayrol</name>
<affiliation wicri:level="4"><inist:fA14 i1="03"><s1>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5, France</s1>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
<sZ>11 aut.</sZ>
<sZ>12 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">France</country>
<wicri:regionArea>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5</wicri:regionArea>
<placeName><region type="region" nuts="2">Languedoc-Roussillon</region>
<settlement type="city">Montpellier</settlement>
</placeName>
<orgName type="university">Université Montpellier 2</orgName>
</affiliation>
</author>
<author><name sortKey="Bellabchara, A" uniqKey="Bellabchara A">A. Bellabchara</name>
<affiliation wicri:level="4"><inist:fA14 i1="03"><s1>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5, France</s1>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
<sZ>11 aut.</sZ>
<sZ>12 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">France</country>
<wicri:regionArea>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5</wicri:regionArea>
<placeName><region type="region" nuts="2">Languedoc-Roussillon</region>
<settlement type="city">Montpellier</settlement>
</placeName>
<orgName type="university">Université Montpellier 2</orgName>
</affiliation>
</author>
<author><name sortKey="Lefebvre, P" uniqKey="Lefebvre P">P. Lefebvre</name>
<affiliation wicri:level="4"><inist:fA14 i1="03"><s1>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5, France</s1>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
<sZ>11 aut.</sZ>
<sZ>12 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">France</country>
<wicri:regionArea>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5</wicri:regionArea>
<placeName><region type="region" nuts="2">Languedoc-Roussillon</region>
<settlement type="city">Montpellier</settlement>
</placeName>
<orgName type="university">Université Montpellier 2</orgName>
</affiliation>
</author>
<author><name sortKey="Coquillat, D" uniqKey="Coquillat D">D. Coquillat</name>
<affiliation wicri:level="4"><inist:fA14 i1="03"><s1>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5, France</s1>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
<sZ>11 aut.</sZ>
<sZ>12 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">France</country>
<wicri:regionArea>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5</wicri:regionArea>
<placeName><region type="region" nuts="2">Languedoc-Roussillon</region>
<settlement type="city">Montpellier</settlement>
</placeName>
<orgName type="university">Université Montpellier 2</orgName>
</affiliation>
</author>
<author><name sortKey="Lascaray, J P" uniqKey="Lascaray J">J. P. Lascaray</name>
<affiliation wicri:level="4"><inist:fA14 i1="03"><s1>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5, France</s1>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
<sZ>11 aut.</sZ>
<sZ>12 aut.</sZ>
</inist:fA14>
<country xml:lang="fr">France</country>
<wicri:regionArea>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5</wicri:regionArea>
<placeName><region type="region" nuts="2">Languedoc-Roussillon</region>
<settlement type="city">Montpellier</settlement>
</placeName>
<orgName type="university">Université Montpellier 2</orgName>
</affiliation>
</author>
</titleStmt>
<publicationStmt><idno type="inist">97-0112251</idno>
<date when="1996-10-15">1996-10-15</date>
<idno type="stanalyst">PASCAL 97-0112251 AIP</idno>
<idno type="RBID">Pascal:97-0112251</idno>
<idno type="wicri:Area/Main/Corpus">018999</idno>
<idno type="wicri:Area/Main/Repository">019821</idno>
<idno type="wicri:Area/France/Extraction">001D42</idno>
</publicationStmt>
<seriesStmt><idno type="ISSN">0163-1829</idno>
<title level="j" type="abbreviated">Phys. rev., B, Condens. matter</title>
<title level="j" type="main">Physical review. B, Condensed matter</title>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Experimental study</term>
<term>Theoretical study</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>7135J</term>
<term>7550P</term>
<term>7866F</term>
<term>7866H</term>
<term>Etude expérimentale</term>
<term>Etude théorique</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">Forbidden e1hh3 and e1lh3 exciton transitions (where hh and lh are heavy-hole and light-hole, respectively) appear in magnetooptical spectra of quantum wells that undergo a type-I-type-II band-alignment transition, here for ordinary (In,Ga)As/GaAs multiple quantum wells and a single CdTe quantum well with a (Cd,Mn)Te semimagnetic barrier exhibiting a giant Zeeman effect. The oscillator strength becomes so strong in a field of 11.25 T that vacuum-field Rabi splitting is clearly seen in reflection spectra when the e1lh3 exciton transition couples to the two-dimensional optical mode in a microcavity. © 1996 The American Physical Society.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0163-1829</s0>
</fA01>
<fA02 i1="01"><s0>PRBMDO</s0>
</fA02>
<fA03 i2="1"><s0>Phys. rev., B, Condens. matter</s0>
</fA03>
<fA05><s2>54</s2>
</fA05>
<fA06><s2>16</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Quantum wells with zero valence-band offset: Drastic enhancement of forbidden excitonic transitions</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>KAVOKIN (A. V.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>KALITEEVSKI (M. A.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>GOUPALOV (S. V.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>BERGER (J. D.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>LYNGNES (O.)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>GIBBS (H. M.)</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>KHITROVA (G.)</s1>
</fA11>
<fA11 i1="08" i2="1"><s1>RIBAYROL (A.)</s1>
</fA11>
<fA11 i1="09" i2="1"><s1>BELLABCHARA (A.)</s1>
</fA11>
<fA11 i1="10" i2="1"><s1>LEFEBVRE (P.)</s1>
</fA11>
<fA11 i1="11" i2="1"><s1>COQUILLAT (D.)</s1>
</fA11>
<fA11 i1="12" i2="1"><s1>LASCARAY (J. P.)</s1>
</fA11>
<fA14 i1="01"><s1>A. F. Ioffe Physico-Technical Institute, 26 Politechnicheskaya, St. Petersburg 194021, Russia</s1>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Optical Sciences Center, University of Arizona, Tucson, Arizona 85721</s1>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Groupe d'Etude des Semiconducteurs, CNRS, Université Montpellier II, CC074, Place E. Bataillon, 34095 Montpellier Cedex 5, France</s1>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
<sZ>11 aut.</sZ>
<sZ>12 aut.</sZ>
</fA14>
<fA20><s2>R11078-R11081</s2>
</fA20>
<fA21><s1>1996-10-15</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>144 B</s2>
</fA43>
<fA44><s0>8100</s0>
<s1>© 1997 American Institute of Physics. All rights reserved.</s1>
</fA44>
<fA47 i1="01" i2="1"><s0>97-0112251</s0>
</fA47>
<fA60><s1>P</s1>
<s3>CR</s3>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Physical review. B, Condensed matter</s0>
</fA64>
<fA66 i1="01"><s0>USA</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>Forbidden e1hh3 and e1lh3 exciton transitions (where hh and lh are heavy-hole and light-hole, respectively) appear in magnetooptical spectra of quantum wells that undergo a type-I-type-II band-alignment transition, here for ordinary (In,Ga)As/GaAs multiple quantum wells and a single CdTe quantum well with a (Cd,Mn)Te semimagnetic barrier exhibiting a giant Zeeman effect. The oscillator strength becomes so strong in a field of 11.25 T that vacuum-field Rabi splitting is clearly seen in reflection spectra when the e1lh3 exciton transition couples to the two-dimensional optical mode in a microcavity. © 1996 The American Physical Society.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70A35</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B70E50P</s0>
</fC02>
<fC02 i1="03" i2="3"><s0>001B70H66F</s0>
</fC02>
<fC02 i1="04" i2="3"><s0>001B70H66H</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>7135J</s0>
<s2>PAC</s2>
<s4>INC</s4>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>7550P</s0>
<s2>PAC</s2>
<s4>INC</s4>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>7866F</s0>
<s2>PAC</s2>
<s4>INC</s4>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>7866H</s0>
<s2>PAC</s2>
<s4>INC</s4>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Etude expérimentale</s0>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Experimental study</s0>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Etude théorique</s0>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Theoretical study</s0>
</fC03>
<fC07 i1="01" i2="3" l="FRE"><s0>Hétérostructure</s0>
</fC07>
<fC07 i1="01" i2="3" l="ENG"><s0>Heterostructures</s0>
</fC07>
<fC07 i1="02" i2="3" l="FRE"><s0>Puits quantique</s0>
</fC07>
<fC07 i1="02" i2="3" l="ENG"><s0>Quantum wells</s0>
</fC07>
<fC07 i1="03" i2="3" l="FRE"><s0>Indium arséniure</s0>
<s2>NK</s2>
</fC07>
<fC07 i1="03" i2="3" l="ENG"><s0>Indium arsenides</s0>
<s2>NK</s2>
</fC07>
<fC07 i1="04" i2="3" l="FRE"><s0>Gallium arséniure</s0>
<s2>NK</s2>
</fC07>
<fC07 i1="04" i2="3" l="ENG"><s0>Gallium arsenides</s0>
<s2>NK</s2>
</fC07>
<fC07 i1="05" i2="3" l="FRE"><s0>Cadmium tellurure</s0>
<s2>NK</s2>
</fC07>
<fC07 i1="05" i2="3" l="ENG"><s0>Cadmium tellurides</s0>
<s2>NK</s2>
</fC07>
<fC07 i1="06" i2="3" l="FRE"><s0>Manganèse tellurure</s0>
<s2>NK</s2>
</fC07>
<fC07 i1="06" i2="3" l="ENG"><s0>Manganese tellurides</s0>
<s2>NK</s2>
</fC07>
<fC07 i1="07" i2="3" l="FRE"><s0>Effet magnétooptique</s0>
</fC07>
<fC07 i1="07" i2="3" l="ENG"><s0>Magneto-optical effects</s0>
</fC07>
<fC07 i1="08" i2="3" l="FRE"><s0>Spectre absorption</s0>
</fC07>
<fC07 i1="08" i2="3" l="ENG"><s0>Absorption spectra</s0>
</fC07>
<fC07 i1="09" i2="3" l="FRE"><s0>Facteur réflexion</s0>
</fC07>
<fC07 i1="09" i2="3" l="ENG"><s0>Reflectivity</s0>
</fC07>
<fC07 i1="10" i2="3" l="FRE"><s0>Transition niveau énergie</s0>
</fC07>
<fC07 i1="10" i2="3" l="ENG"><s0>Energy-level transitions</s0>
</fC07>
<fC07 i1="11" i2="3" l="FRE"><s0>Force oscillateur</s0>
</fC07>
<fC07 i1="11" i2="3" l="ENG"><s0>Oscillator strengths</s0>
</fC07>
<fC07 i1="12" i2="3" l="FRE"><s0>Exciton</s0>
</fC07>
<fC07 i1="12" i2="3" l="ENG"><s0>Excitons</s0>
</fC07>
<fC07 i1="13" i2="3" l="FRE"><s0>Bande valence</s0>
</fC07>
<fC07 i1="13" i2="3" l="ENG"><s0>Valence bands</s0>
</fC07>
<fC07 i1="14" i2="3" l="FRE"><s0>Domaine température 0-13 K</s0>
</fC07>
<fC07 i1="14" i2="3" l="ENG"><s0>Temperature range 0-13 K</s0>
</fC07>
<fN21><s1>229</s1>
</fN21>
<fN47 i1="01" i2="1"><s0>9720M01706</s0>
</fN47>
</pA>
</standard>
</inist>
</record>

Pour manipuler ce document sous Unix (Dilib)

EXPLOR_STEP=IndiumV3/Data/France/Analysis

HfdSelect -h $EXPLOR_STEP/biblio.hfd -nk 001D42 | SxmlIndent | more

HfdSelect -h $EXPLOR_AREA/Data/France/Analysis/biblio.hfd -nk 001D42 | SxmlIndent | more

Pour mettre un lien sur cette page dans le réseau Wicri

{{Explor lien
   |wiki=   *** parameter Area/wikiCode missing *** 
   |area=    IndiumV3
   |flux=    France
   |étape=   Analysis
   |type=    RBID
   |clé=     Pascal:97-0112251
   |texte=   Quantum wells with zero valence-band offset: Drastic enhancement of forbidden excitonic transitions
}}

This area was generated with Dilib version V0.5.77.
Data generation: Mon Jun 9 10:27:54 2014. Site generation: Thu Mar 7 16:19:59 2024

	Serveur d'exploration sur l'Indium
	Attention, ce site est en cours de développement ! Attention, site généré par des moyens informatiques à partir de corpus bruts. Les informations ne sont donc pas validées.

Serveur d'exploration sur l'Indium

Quantum wells with zero valence-band offset: Drastic enhancement of forbidden excitonic transitions

Quantum wells with zero valence-band offset: Drastic enhancement of forbidden excitonic transitions

Descripteurs français

English descriptors

Abstract

Links toward previous steps (curation, corpus...)

Links to Exploration step

Le document en format XML

Pour manipuler ce document sous Unix (Dilib)

Pour mettre un lien sur cette page dans le réseau Wicri