Optical Studies and Transmission Electron Microscopy of HgCdTe Quantum Well Heterostructures for Very Long Wavelength Lasers

HgTe/CdHgTe quantum well (QW) heterostructures have attracted a lot of interest recently due to insights they provided towards the physics of topological insulators and massless Dirac fermions. Our work focuses on HgCdTe QWs with the energy spectrum close to the graphene-like relativistic dispersion...

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Vydáno v:	Nanomaterials (Basel, Switzerland) Ročník 11; číslo 7; s. 1855
Hlavní autoři:	Rumyantsev, Vladimir V., Razova, Anna A., Bovkun, Leonid S., Tatarskiy, Dmitriy A., Mikhailovskii, Vladimir Y., Zholudev, Maksim S., Ikonnikov, Anton V., Uaman Svetikova, Tatyana A., Maremyanin, Kirill V., Utochkin, Vladimir V., Fadeev, Mikhail A., Remesnik, Vladimir G., Aleshkin, Vladimir Y., Mikhailov, Nikolay N., Dvoretsky, Sergey A., Potemski, Marek, Orlita, Milan, Gavrilenko, Vladimir I., Morozov, Sergey V.
Médium:	Journal Article
Jazyk:	angličtina
Vydáno:	Basel MDPI AG 19.07.2021 MDPI
Edice:	Semiconductor Hetero-Nanostructures for Opto-Electronics Applications
Témata:	Augers Energy spectra Experiments Fermions Graphene Heterostructures HgCdTe Lasers Mercury cadmium tellurides Molecular beam epitaxy Operating temperature Optical measurement Photoconductivity Photoluminescence Photons Physics Quantum wells Radiation Recombination Retrofitting Sensors Spectrum analysis stimulated emission Topological insulators Transmission electron microscopy Waveguides Wavelengths Germany HgCdTe heterostructures stimulated emission
ISSN:	2079-4991, 2079-4991
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Abstract	HgTe/CdHgTe quantum well (QW) heterostructures have attracted a lot of interest recently due to insights they provided towards the physics of topological insulators and massless Dirac fermions. Our work focuses on HgCdTe QWs with the energy spectrum close to the graphene-like relativistic dispersion that is supposed to suppress the non-radiative Auger recombination. We combine various methods such as photoconductivity, photoluminescence and magneto-optical measurements as well as transmission electron microscopy to retrofit growth parameters in multi-QW waveguide structures, designed for long wavelengths lasing in the range of 10–22 μm. The results reveal that the attainable operating temperatures and wavelengths are strongly dependent on Cd content in the QW, since it alters the dominating recombination mechanism of the carriers.
AbstractList	HgTe/CdHgTe quantum well (QW) heterostructures have attracted a lot of interest recently due to insights they provided towards the physics of topological insulators and massless Dirac fermions. Our work focuses on HgCdTe QWs with the energy spectrum close to the graphene-like relativistic dispersion that is supposed to suppress the non-radiative Auger recombination. We combine various methods such as photoconductivity, photoluminescence and magneto-optical measurements as well as transmission electron microscopy to retrofit growth parameters in multi-QW waveguide structures, designed for long wavelengths lasing in the range of 10–22 μm. The results reveal that the attainable operating temperatures and wavelengths are strongly dependent on Cd content in the QW, since it alters the dominating recombination mechanism of the carriers. HgTe/CdHgTe quantum well (QW) heterostructures have attracted a lot of interest recently due to insights they provided towards the physics of topological insulators and massless Dirac fermions. Our work focuses on HgCdTe QWs with the energy spectrum close to the graphenelike relativistic dispersion that is supposed to suppress the non-radiative Auger recombination. We combine various methods such as photoconductivity, photoluminescence and magneto-optical measurements as well as transmission electron microscopy to retrofit growth parameters in multi-QW waveguide structures, designed for long wavelengths lasing in the range of 10–22 \mum. The results reveal that the attainable operating temperatures and wavelengths are strongly dependent on Cd content in the QW, since it alters the dominating recombination mechanism of the carriers. HgTe/CdHgTe quantum well (QW) heterostructures have attracted a lot of interest recently due to insights they provided towards the physics of topological insulators and massless Dirac fermions. Our work focuses on HgCdTe QWs with the energy spectrum close to the graphene-like relativistic dispersion that is supposed to suppress the non-radiative Auger recombination. We combine various methods such as photoconductivity, photoluminescence and magneto-optical measurements as well as transmission electron microscopy to retrofit growth parameters in multi-QW waveguide structures, designed for long wavelengths lasing in the range of 10-22 μm. The results reveal that the attainable operating temperatures and wavelengths are strongly dependent on Cd content in the QW, since it alters the dominating recombination mechanism of the carriers.HgTe/CdHgTe quantum well (QW) heterostructures have attracted a lot of interest recently due to insights they provided towards the physics of topological insulators and massless Dirac fermions. Our work focuses on HgCdTe QWs with the energy spectrum close to the graphene-like relativistic dispersion that is supposed to suppress the non-radiative Auger recombination. We combine various methods such as photoconductivity, photoluminescence and magneto-optical measurements as well as transmission electron microscopy to retrofit growth parameters in multi-QW waveguide structures, designed for long wavelengths lasing in the range of 10-22 μm. The results reveal that the attainable operating temperatures and wavelengths are strongly dependent on Cd content in the QW, since it alters the dominating recombination mechanism of the carriers.
Author	Aleshkin, Vladimir Y. Potemski, Marek Bovkun, Leonid S. Utochkin, Vladimir V. Orlita, Milan Mikhailov, Nikolay N. Tatarskiy, Dmitriy A. Mikhailovskii, Vladimir Y. Uaman Svetikova, Tatyana A. Maremyanin, Kirill V. Remesnik, Vladimir G. Rumyantsev, Vladimir V. Zholudev, Maksim S. Gavrilenko, Vladimir I. Dvoretsky, Sergey A. Ikonnikov, Anton V. Fadeev, Mikhail A. Razova, Anna A. Morozov, Sergey V.
AuthorAffiliation	3 LNCMI-EMFL, CNRS UPR3228, University Grenoble Alpes, University Toulouse, University Toulouse 3, INSA-T, 38042 Grenoble, France; evilra66it@gmail.com (L.S.B.); marek.potemski@lncmi.cnrs.fr (M.P.); milan.orlita@lncmi.cnrs.fr (M.O.) 2 Faculty of Radiophysics, Lobachevsky State University, 603950 Nizhny Novgorod, Russia 6 Faculty of Physics, Lomonosov Moscow State University, 119991 Moscow, Russia; antikon@physics.msu.ru (A.V.I.); aurelia8002@gmail.com (T.A.U.S.) 9 Faculty of Mathematics and Physics, Institute of Physics, Charles University, KeKarlovu 5, 121 16 Prague 2, Czech Republic 1 Institute for Physics of Microstructures of RAS, 603950 Nizhny Novgorod, Russia; annara@ipmras.ru (A.A.R.); tatarsky@ipmras.ru (D.A.T.); zholudev@ipmras.ru (M.S.Z.); kirillm@ipm.sci-nnov.ru (K.V.M.); utvlvas@ipmras.ru (V.V.U.); fadeev@ipmras.ru (M.A.F.); aleshkin@ipmras.ru (V.Y.A.); gavr@ipmras.ru (V.I.G.); more@ipmras.ru (S.V.M.) 7 Rzhanov Institute of Semiconductor Physics, Siberian Branch, Russian Academy
AuthorAffiliation_xml	– name: 6 Faculty of Physics, Lomonosov Moscow State University, 119991 Moscow, Russia; antikon@physics.msu.ru (A.V.I.); aurelia8002@gmail.com (T.A.U.S.) – name: 2 Faculty of Radiophysics, Lobachevsky State University, 603950 Nizhny Novgorod, Russia – name: 1 Institute for Physics of Microstructures of RAS, 603950 Nizhny Novgorod, Russia; annara@ipmras.ru (A.A.R.); tatarsky@ipmras.ru (D.A.T.); zholudev@ipmras.ru (M.S.Z.); kirillm@ipm.sci-nnov.ru (K.V.M.); utvlvas@ipmras.ru (V.V.U.); fadeev@ipmras.ru (M.A.F.); aleshkin@ipmras.ru (V.Y.A.); gavr@ipmras.ru (V.I.G.); more@ipmras.ru (S.V.M.) – name: 5 Resource Center for Nanotechnology, Saint-Petersburg University, 199034 Saint-Petersburg, Russia; zihertge@gmail.com – name: 4 Faculty of Physics, Lobachevsky State University, 603950 Nizhny Novgorod, Russia – name: 8 Advanced School of General and Applied Physics, Lobachevsky State University, 603950 Nizhny Novgorod, Russia – name: 9 Faculty of Mathematics and Physics, Institute of Physics, Charles University, KeKarlovu 5, 121 16 Prague 2, Czech Republic – name: 7 Rzhanov Institute of Semiconductor Physics, Siberian Branch, Russian Academy of Sciences, 630090 Novosibirsk, Russia; remesnik@isp.nsc.ru (V.G.R.); mikhailov@isp.nsc.ru (N.N.M.); dvor@isp.nsc.ru (S.A.D.) – name: 3 LNCMI-EMFL, CNRS UPR3228, University Grenoble Alpes, University Toulouse, University Toulouse 3, INSA-T, 38042 Grenoble, France; evilra66it@gmail.com (L.S.B.); marek.potemski@lncmi.cnrs.fr (M.P.); milan.orlita@lncmi.cnrs.fr (M.O.)
Author_xml	– sequence: 1 givenname: Vladimir V. orcidid: 0000-0003-0739-2214 surname: Rumyantsev fullname: Rumyantsev, Vladimir V. – sequence: 2 givenname: Anna A. surname: Razova fullname: Razova, Anna A. – sequence: 3 givenname: Leonid S. orcidid: 0000-0003-2748-5792 surname: Bovkun fullname: Bovkun, Leonid S. – sequence: 4 givenname: Dmitriy A. orcidid: 0000-0001-8973-0939 surname: Tatarskiy fullname: Tatarskiy, Dmitriy A. – sequence: 5 givenname: Vladimir Y. surname: Mikhailovskii fullname: Mikhailovskii, Vladimir Y. – sequence: 6 givenname: Maksim S. surname: Zholudev fullname: Zholudev, Maksim S. – sequence: 7 givenname: Anton V. orcidid: 0000-0001-8557-2566 surname: Ikonnikov fullname: Ikonnikov, Anton V. – sequence: 8 givenname: Tatyana A. surname: Uaman Svetikova fullname: Uaman Svetikova, Tatyana A. – sequence: 9 givenname: Kirill V. surname: Maremyanin fullname: Maremyanin, Kirill V. – sequence: 10 givenname: Vladimir V. surname: Utochkin fullname: Utochkin, Vladimir V. – sequence: 11 givenname: Mikhail A. orcidid: 0000-0002-2203-264X surname: Fadeev fullname: Fadeev, Mikhail A. – sequence: 12 givenname: Vladimir G. surname: Remesnik fullname: Remesnik, Vladimir G. – sequence: 13 givenname: Vladimir Y. surname: Aleshkin fullname: Aleshkin, Vladimir Y. – sequence: 14 givenname: Nikolay N. surname: Mikhailov fullname: Mikhailov, Nikolay N. – sequence: 15 givenname: Sergey A. orcidid: 0000-0002-1295-5598 surname: Dvoretsky fullname: Dvoretsky, Sergey A. – sequence: 16 givenname: Marek surname: Potemski fullname: Potemski, Marek – sequence: 17 givenname: Milan surname: Orlita fullname: Orlita, Milan – sequence: 18 givenname: Vladimir I. surname: Gavrilenko fullname: Gavrilenko, Vladimir I. – sequence: 19 givenname: Sergey V. surname: Morozov fullname: Morozov, Sergey V.
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Snippet	HgTe/CdHgTe quantum well (QW) heterostructures have attracted a lot of interest recently due to insights they provided towards the physics of topological...
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SubjectTerms	Augers Energy spectra Experiments Fermions Graphene Heterostructures HgCdTe Lasers Mercury cadmium tellurides Molecular beam epitaxy Operating temperature Optical measurement Photoconductivity Photoluminescence Photons Physics Quantum wells Radiation Recombination Retrofitting Sensors Spectrum analysis stimulated emission Topological insulators Transmission electron microscopy Waveguides Wavelengths
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Title	Optical Studies and Transmission Electron Microscopy of HgCdTe Quantum Well Heterostructures for Very Long Wavelength Lasers
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