Optical absorption of polarized light in InAs/GaSb quantum wells
Identifieur interne : 000193 ( Russie/Analysis ); précédent : 000192; suivant : 000194Optical absorption of polarized light in InAs/GaSb quantum wells
Auteurs : RBID : Pascal:09-0062564Descripteurs français
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Abstract
Using an eight-band k .p model Hamiltonian with the Burt-Foreman envelope function theory, we have investigated the optical absorption of both linearly and circularly polarized light, as well as related phenomena in InAs/GaSb broken-gap quantum wells grown along the [001] direction, with emphasis on the effects of electron-hole hybridization and the various symmetry-breaking mechanisms such as structural inversion asymmetry, bulk inversion asymmetry and interface Hamiltonian. The optical matrix elements exhibit unusual angular dependence in close connection with the spin-flip transitions which are originally forbidden. The spin split of the 2e subband results in two profound absorption peaks for the 1hh-2e transition for both linearly polarized and circularly polarized light. A large lateral optical anisotropy appears in the absorption coefficient of linearly polarized light, which can reach almost 100% with a reducing thickness of the quantum well. For the absorption of circularly polarized light, we found a large enhancement of electron spin polarization in the upper 2e subband, which was generally considered as forbidden if the polarization is along the direction perpendicular to the plane-of-light incidence.
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<author><name sortKey="Zakharova, A" uniqKey="Zakharova A">A. Zakharova</name>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Absorption spectra</term>
<term>Asymmetry</term>
<term>Circular polarization</term>
<term>Electron hole pair</term>
<term>Energy gap</term>
<term>Envelope function</term>
<term>Gallium antimonides</term>
<term>Hamiltonians</term>
<term>Hybridization</term>
<term>Indium arsenides</term>
<term>Linear polarization</term>
<term>Matrix elements</term>
<term>Quantum wells</term>
<term>Spin polarization</term>
<term>Symmetry breaking</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Spectre absorption</term>
<term>Paire électron trou</term>
<term>Polarisation spin</term>
<term>Hamiltonien</term>
<term>Fonction enveloppe</term>
<term>Polarisation rectiligne</term>
<term>Polarisation circulaire</term>
<term>Bande interdite</term>
<term>Hybridation</term>
<term>Brisure symétrie</term>
<term>Asymétrie</term>
<term>Elément matriciel</term>
<term>Arséniure d'indium</term>
<term>Antimoniure de gallium</term>
<term>Puits quantique</term>
<term>InAs</term>
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<front><div type="abstract" xml:lang="en">Using an eight-band k .p model Hamiltonian with the Burt-Foreman envelope function theory, we have investigated the optical absorption of both linearly and circularly polarized light, as well as related phenomena in InAs/GaSb broken-gap quantum wells grown along the [001] direction, with emphasis on the effects of electron-hole hybridization and the various symmetry-breaking mechanisms such as structural inversion asymmetry, bulk inversion asymmetry and interface Hamiltonian. The optical matrix elements exhibit unusual angular dependence in close connection with the spin-flip transitions which are originally forbidden. The spin split of the 2e subband results in two profound absorption peaks for the 1hh-2e transition for both linearly polarized and circularly polarized light. A large lateral optical anisotropy appears in the absorption coefficient of linearly polarized light, which can reach almost 100% with a reducing thickness of the quantum well. For the absorption of circularly polarized light, we found a large enhancement of electron spin polarization in the upper 2e subband, which was generally considered as forbidden if the polarization is along the direction perpendicular to the plane-of-light incidence.</div>
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<fA11 i1="02" i2="1"><s1>SEMENIKHIN (I.)</s1>
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<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
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<s2>22362 Lund</s2>
<s3>SWE</s3>
<sZ>3 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Department of Physics, Chemistry and Biology, Linköping University</s1>
<s2>58183 Linköping</s2>
<s3>SWE</s3>
<sZ>3 aut.</sZ>
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<fC01 i1="01" l="ENG"><s0>Using an eight-band k .p model Hamiltonian with the Burt-Foreman envelope function theory, we have investigated the optical absorption of both linearly and circularly polarized light, as well as related phenomena in InAs/GaSb broken-gap quantum wells grown along the [001] direction, with emphasis on the effects of electron-hole hybridization and the various symmetry-breaking mechanisms such as structural inversion asymmetry, bulk inversion asymmetry and interface Hamiltonian. The optical matrix elements exhibit unusual angular dependence in close connection with the spin-flip transitions which are originally forbidden. The spin split of the 2e subband results in two profound absorption peaks for the 1hh-2e transition for both linearly polarized and circularly polarized light. A large lateral optical anisotropy appears in the absorption coefficient of linearly polarized light, which can reach almost 100% with a reducing thickness of the quantum well. For the absorption of circularly polarized light, we found a large enhancement of electron spin polarization in the upper 2e subband, which was generally considered as forbidden if the polarization is along the direction perpendicular to the plane-of-light incidence.</s0>
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<fC03 i1="01" i2="3" l="FRE"><s0>Spectre absorption</s0>
<s5>02</s5>
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<fC03 i1="01" i2="3" l="ENG"><s0>Absorption spectra</s0>
<s5>02</s5>
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<fC03 i1="02" i2="X" l="FRE"><s0>Paire électron trou</s0>
<s5>03</s5>
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<fC03 i1="02" i2="X" l="ENG"><s0>Electron hole pair</s0>
<s5>03</s5>
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<fC03 i1="02" i2="X" l="SPA"><s0>Par electrón hueco</s0>
<s5>03</s5>
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<fC03 i1="03" i2="X" l="FRE"><s0>Polarisation spin</s0>
<s5>04</s5>
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<fC03 i1="03" i2="X" l="ENG"><s0>Spin polarization</s0>
<s5>04</s5>
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<fC03 i1="03" i2="X" l="SPA"><s0>Polarización spin</s0>
<s5>04</s5>
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<fC03 i1="04" i2="3" l="FRE"><s0>Hamiltonien</s0>
<s5>05</s5>
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<s5>05</s5>
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<s5>06</s5>
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<fC03 i1="05" i2="X" l="ENG"><s0>Envelope function</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Función envolviente</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Polarisation rectiligne</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Linear polarization</s0>
<s5>07</s5>
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<fC03 i1="07" i2="3" l="FRE"><s0>Polarisation circulaire</s0>
<s5>08</s5>
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<fC03 i1="07" i2="3" l="ENG"><s0>Circular polarization</s0>
<s5>08</s5>
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<s5>09</s5>
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<s5>09</s5>
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<s5>10</s5>
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<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Brisure symétrie</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Symmetry breaking</s0>
<s5>11</s5>
</fC03>
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<s5>12</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Asymmetry</s0>
<s5>12</s5>
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<fC03 i1="12" i2="3" l="FRE"><s0>Elément matriciel</s0>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Matrix elements</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Arséniure d'indium</s0>
<s2>NK</s2>
<s5>15</s5>
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<fC03 i1="13" i2="3" l="ENG"><s0>Indium arsenides</s0>
<s2>NK</s2>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Antimoniure de gallium</s0>
<s2>NK</s2>
<s5>16</s5>
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<fC03 i1="14" i2="3" l="ENG"><s0>Gallium antimonides</s0>
<s2>NK</s2>
<s5>16</s5>
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<fC03 i1="15" i2="3" l="FRE"><s0>Puits quantique</s0>
<s5>17</s5>
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<s5>17</s5>
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<fC03 i1="16" i2="3" l="FRE"><s0>InAs</s0>
<s4>INC</s4>
<s5>52</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>GaSb</s0>
<s4>INC</s4>
<s5>53</s5>
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<fN21><s1>047</s1>
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