Exploring two-dimensional electron gases with two-dimensional Fourier transform spectroscopy
The dephasing of the Fermi edge singularity excitations in two modulation doped single quantum wells of 12 nm and 18 nm thickness and in-well carrier concentration of ∼4 × 10(11) cm(-2) was carefully measured using spectrally resolved four-wave mixing (FWM) and two-dimensional Fourier transform (2DF...
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Veröffentlicht in: | The Journal of chemical physics 2014-10, Vol.141 (13), p.134505-134505 |
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creator | Paul, J Dey, P Tokumoto, T Reno, J L Hilton, D J Karaiskaj, D |
description | The dephasing of the Fermi edge singularity excitations in two modulation doped single quantum wells of 12 nm and 18 nm thickness and in-well carrier concentration of ∼4 × 10(11) cm(-2) was carefully measured using spectrally resolved four-wave mixing (FWM) and two-dimensional Fourier transform (2DFT) spectroscopy. Although the absorption at the Fermi edge is broad at this doping level, the spectrally resolved FWM shows narrow resonances. Two peaks are observed separated by the heavy hole/light hole energy splitting. Temperature dependent "rephasing" (S1) 2DFT spectra show a rapid linear increase of the homogeneous linewidth with temperature. The dephasing rate increases faster with temperature in the narrower 12 nm quantum well, likely due to an increased carrier-phonon scattering rate. The S1 2DFT spectra were measured using co-linear, cross-linear, and co-circular polarizations. Distinct 2DFT lineshapes were observed for co-linear and cross-linear polarizations, suggesting the existence of polarization dependent contributions. The "two-quantum coherence" (S3) 2DFT spectra for the 12 nm quantum well show a single peak for both co-linear and co-circular polarizations. |
doi_str_mv | 10.1063/1.4896777 |
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(SNL-NM), Albuquerque, NM (United States)</creatorcontrib><description>The dephasing of the Fermi edge singularity excitations in two modulation doped single quantum wells of 12 nm and 18 nm thickness and in-well carrier concentration of ∼4 × 10(11) cm(-2) was carefully measured using spectrally resolved four-wave mixing (FWM) and two-dimensional Fourier transform (2DFT) spectroscopy. Although the absorption at the Fermi edge is broad at this doping level, the spectrally resolved FWM shows narrow resonances. Two peaks are observed separated by the heavy hole/light hole energy splitting. Temperature dependent "rephasing" (S1) 2DFT spectra show a rapid linear increase of the homogeneous linewidth with temperature. The dephasing rate increases faster with temperature in the narrower 12 nm quantum well, likely due to an increased carrier-phonon scattering rate. The S1 2DFT spectra were measured using co-linear, cross-linear, and co-circular polarizations. Distinct 2DFT lineshapes were observed for co-linear and cross-linear polarizations, suggesting the existence of polarization dependent contributions. The "two-quantum coherence" (S3) 2DFT spectra for the 12 nm quantum well show a single peak for both co-linear and co-circular polarizations.</description><identifier>ISSN: 0021-9606</identifier><identifier>EISSN: 1089-7690</identifier><identifier>DOI: 10.1063/1.4896777</identifier><identifier>PMID: 25296819</identifier><language>eng</language><publisher>United States: American Institute of Physics</publisher><subject>Carrier density ; Coherence ; dephasing ; doping ; Four-wave mixing ; Fourier transforms ; NANOSCIENCE AND NANOTECHNOLOGY ; polarization ; Quantum phenomena ; Quantum wells ; Spectra ; Spectroscopy ; Spectrum analysis ; Temperature dependence</subject><ispartof>The Journal of chemical physics, 2014-10, Vol.141 (13), p.134505-134505</ispartof><rights>2014 AIP Publishing LLC.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c375t-4445e06ada6439b71404c4be334778752fafcdffc7d5782c462ea262963eacb23</citedby><cites>FETCH-LOGICAL-c375t-4445e06ada6439b71404c4be334778752fafcdffc7d5782c462ea262963eacb23</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,777,781,882,27905,27906</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/25296819$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/servlets/purl/1083698$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Paul, J</creatorcontrib><creatorcontrib>Dey, P</creatorcontrib><creatorcontrib>Tokumoto, T</creatorcontrib><creatorcontrib>Reno, J L</creatorcontrib><creatorcontrib>Hilton, D J</creatorcontrib><creatorcontrib>Karaiskaj, D</creatorcontrib><creatorcontrib>Sandia National Lab. (SNL-NM), Albuquerque, NM (United States)</creatorcontrib><title>Exploring two-dimensional electron gases with two-dimensional Fourier transform spectroscopy</title><title>The Journal of chemical physics</title><addtitle>J Chem Phys</addtitle><description>The dephasing of the Fermi edge singularity excitations in two modulation doped single quantum wells of 12 nm and 18 nm thickness and in-well carrier concentration of ∼4 × 10(11) cm(-2) was carefully measured using spectrally resolved four-wave mixing (FWM) and two-dimensional Fourier transform (2DFT) spectroscopy. Although the absorption at the Fermi edge is broad at this doping level, the spectrally resolved FWM shows narrow resonances. Two peaks are observed separated by the heavy hole/light hole energy splitting. Temperature dependent "rephasing" (S1) 2DFT spectra show a rapid linear increase of the homogeneous linewidth with temperature. The dephasing rate increases faster with temperature in the narrower 12 nm quantum well, likely due to an increased carrier-phonon scattering rate. The S1 2DFT spectra were measured using co-linear, cross-linear, and co-circular polarizations. Distinct 2DFT lineshapes were observed for co-linear and cross-linear polarizations, suggesting the existence of polarization dependent contributions. The "two-quantum coherence" (S3) 2DFT spectra for the 12 nm quantum well show a single peak for both co-linear and co-circular polarizations.</description><subject>Carrier density</subject><subject>Coherence</subject><subject>dephasing</subject><subject>doping</subject><subject>Four-wave mixing</subject><subject>Fourier transforms</subject><subject>NANOSCIENCE AND NANOTECHNOLOGY</subject><subject>polarization</subject><subject>Quantum phenomena</subject><subject>Quantum wells</subject><subject>Spectra</subject><subject>Spectroscopy</subject><subject>Spectrum analysis</subject><subject>Temperature dependence</subject><issn>0021-9606</issn><issn>1089-7690</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNplkb1OwzAURi0EoqUw8AIoggWGFP_FTkZUtYBUiQU2JMt1nNZVYgc7Uenb49LCAJOX4-_ecz8ALhEcI8jIPRrTvGCc8yMwRDAvUs4KeAyGEGKUFgyyATgLYQ0hRBzTUzDAGS5YjooheJ9-trXzxi6TbuPS0jTaBuOsrBNda9V5Z5OlDDokG9Ot_jEz13ujfdJ5aUPlfJOE9vtXUK7dnoOTStZBXxzeEXibTV8nT-n85fF58jBPFeFZl1JKMw2ZLCWjpFhwRCFVdKEJoZznPMOVrFRZVYqXGc-xogxriVlUIFqqBSYjcL3PdaEzIijTabVSztq4iogHIazII3S7h1rvPnodOtGYoHRdS6tdHwRiCHJGWL7Lu_mDrqNn9A0CI0xyRjPOI3W3p1TUDV5XovWmkX4bR4pdLwKJQy-RvTok9otGl7_kTxHkC5Akh9o</recordid><startdate>20141007</startdate><enddate>20141007</enddate><creator>Paul, J</creator><creator>Dey, P</creator><creator>Tokumoto, T</creator><creator>Reno, J L</creator><creator>Hilton, D J</creator><creator>Karaiskaj, D</creator><general>American Institute of Physics</general><general>American Institute of Physics (AIP)</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope><scope>OIOZB</scope><scope>OTOTI</scope></search><sort><creationdate>20141007</creationdate><title>Exploring two-dimensional electron gases with two-dimensional Fourier transform spectroscopy</title><author>Paul, J ; Dey, P ; Tokumoto, T ; Reno, J L ; Hilton, D J ; Karaiskaj, D</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c375t-4445e06ada6439b71404c4be334778752fafcdffc7d5782c462ea262963eacb23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Carrier density</topic><topic>Coherence</topic><topic>dephasing</topic><topic>doping</topic><topic>Four-wave mixing</topic><topic>Fourier transforms</topic><topic>NANOSCIENCE AND NANOTECHNOLOGY</topic><topic>polarization</topic><topic>Quantum phenomena</topic><topic>Quantum wells</topic><topic>Spectra</topic><topic>Spectroscopy</topic><topic>Spectrum analysis</topic><topic>Temperature dependence</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Paul, J</creatorcontrib><creatorcontrib>Dey, P</creatorcontrib><creatorcontrib>Tokumoto, T</creatorcontrib><creatorcontrib>Reno, J L</creatorcontrib><creatorcontrib>Hilton, D J</creatorcontrib><creatorcontrib>Karaiskaj, D</creatorcontrib><creatorcontrib>Sandia National Lab. (SNL-NM), Albuquerque, NM (United States)</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>The Journal of chemical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Paul, J</au><au>Dey, P</au><au>Tokumoto, T</au><au>Reno, J L</au><au>Hilton, D J</au><au>Karaiskaj, D</au><aucorp>Sandia National Lab. (SNL-NM), Albuquerque, NM (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Exploring two-dimensional electron gases with two-dimensional Fourier transform spectroscopy</atitle><jtitle>The Journal of chemical physics</jtitle><addtitle>J Chem Phys</addtitle><date>2014-10-07</date><risdate>2014</risdate><volume>141</volume><issue>13</issue><spage>134505</spage><epage>134505</epage><pages>134505-134505</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><abstract>The dephasing of the Fermi edge singularity excitations in two modulation doped single quantum wells of 12 nm and 18 nm thickness and in-well carrier concentration of ∼4 × 10(11) cm(-2) was carefully measured using spectrally resolved four-wave mixing (FWM) and two-dimensional Fourier transform (2DFT) spectroscopy. Although the absorption at the Fermi edge is broad at this doping level, the spectrally resolved FWM shows narrow resonances. Two peaks are observed separated by the heavy hole/light hole energy splitting. Temperature dependent "rephasing" (S1) 2DFT spectra show a rapid linear increase of the homogeneous linewidth with temperature. The dephasing rate increases faster with temperature in the narrower 12 nm quantum well, likely due to an increased carrier-phonon scattering rate. The S1 2DFT spectra were measured using co-linear, cross-linear, and co-circular polarizations. Distinct 2DFT lineshapes were observed for co-linear and cross-linear polarizations, suggesting the existence of polarization dependent contributions. The "two-quantum coherence" (S3) 2DFT spectra for the 12 nm quantum well show a single peak for both co-linear and co-circular polarizations.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><pmid>25296819</pmid><doi>10.1063/1.4896777</doi><tpages>1</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Carrier density Coherence dephasing doping Four-wave mixing Fourier transforms NANOSCIENCE AND NANOTECHNOLOGY polarization Quantum phenomena Quantum wells Spectra Spectroscopy Spectrum analysis Temperature dependence |
title | Exploring two-dimensional electron gases with two-dimensional Fourier transform spectroscopy |
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