Surface Nanostructuring during Selective Area Epitaxy of Heterostructures with InGaAs QWs in the Ultra-Wide Windows

Selective area epitaxy (SAE) is widely used in photonic integrated circuits, but there is little information on the use of this technique for the growth of heterostructures in ultra-wide windows. Samples of heterostructures with InGaAs quantum wells (QWs) on GaAs (100) substrates with a pattern of a...

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Main Authors: Viktor Shamakhov, Dmitriy Nikolaev, Sergey Slipchenko, Evgenii Fomin, Alexander Smirnov, Ilya Eliseyev, Nikita Pikhtin, Peter Kop`ev
Format: Article
Language:English
Published: MDPI AG 2020-12-01
Series:Nanomaterials
Subjects:
Online Access:https://www.mdpi.com/2079-4991/11/1/11
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author Viktor Shamakhov
Dmitriy Nikolaev
Sergey Slipchenko
Evgenii Fomin
Alexander Smirnov
Ilya Eliseyev
Nikita Pikhtin
Peter Kop`ev
author_facet Viktor Shamakhov
Dmitriy Nikolaev
Sergey Slipchenko
Evgenii Fomin
Alexander Smirnov
Ilya Eliseyev
Nikita Pikhtin
Peter Kop`ev
author_sort Viktor Shamakhov
collection DOAJ
description Selective area epitaxy (SAE) is widely used in photonic integrated circuits, but there is little information on the use of this technique for the growth of heterostructures in ultra-wide windows. Samples of heterostructures with InGaAs quantum wells (QWs) on GaAs (100) substrates with a pattern of alternating stripes (100-μm-wide SiO<sub>2</sub> mask/100-μm-wide window) were grown using metalorganic chemical vapour deposition (MOCVD). It was found that due to a local change in the growth rate of InGaAs QW in the window, the photoluminescence (PL) spectra measured from the edge to the center of the window exhibited maximum blueshifts of 14 and 19 meV at temperatures of 80 K and 300 K, respectively. Using atomic force microscopy, we have demonstrated that the surface morphologies of structures grown using standard epitaxy or SAE under identical MOCVD growth conditions correspond to a step flow growth with a step height of ~1.5 ML or a step bunching growth mode, respectively. In the structures grown with the use of SAE, a strong variation in the surface morphology in an ultra-wide window from its center to the edge was revealed, which is explained by a change in the local misorientation of the layer due to a local change in the growth rate over the width of the window.
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spelling doaj.art-eda89ea5d45e49edb27208d293db507a2023-11-21T02:12:27ZengMDPI AGNanomaterials2079-49912020-12-011111110.3390/nano11010011Surface Nanostructuring during Selective Area Epitaxy of Heterostructures with InGaAs QWs in the Ultra-Wide WindowsViktor Shamakhov0Dmitriy Nikolaev1Sergey Slipchenko2Evgenii Fomin3Alexander Smirnov4Ilya Eliseyev5Nikita Pikhtin6Peter Kop`ev7Ioffe Institute, 26 Politekhnicheskaya, St Petersburg 194021, RussiaIoffe Institute, 26 Politekhnicheskaya, St Petersburg 194021, RussiaIoffe Institute, 26 Politekhnicheskaya, St Petersburg 194021, RussiaElfolum Ltd., 26 Politekhnicheskaya, St Petersburg 194021, RussiaIoffe Institute, 26 Politekhnicheskaya, St Petersburg 194021, RussiaIoffe Institute, 26 Politekhnicheskaya, St Petersburg 194021, RussiaIoffe Institute, 26 Politekhnicheskaya, St Petersburg 194021, RussiaIoffe Institute, 26 Politekhnicheskaya, St Petersburg 194021, RussiaSelective area epitaxy (SAE) is widely used in photonic integrated circuits, but there is little information on the use of this technique for the growth of heterostructures in ultra-wide windows. Samples of heterostructures with InGaAs quantum wells (QWs) on GaAs (100) substrates with a pattern of alternating stripes (100-μm-wide SiO<sub>2</sub> mask/100-μm-wide window) were grown using metalorganic chemical vapour deposition (MOCVD). It was found that due to a local change in the growth rate of InGaAs QW in the window, the photoluminescence (PL) spectra measured from the edge to the center of the window exhibited maximum blueshifts of 14 and 19 meV at temperatures of 80 K and 300 K, respectively. Using atomic force microscopy, we have demonstrated that the surface morphologies of structures grown using standard epitaxy or SAE under identical MOCVD growth conditions correspond to a step flow growth with a step height of ~1.5 ML or a step bunching growth mode, respectively. In the structures grown with the use of SAE, a strong variation in the surface morphology in an ultra-wide window from its center to the edge was revealed, which is explained by a change in the local misorientation of the layer due to a local change in the growth rate over the width of the window.https://www.mdpi.com/2079-4991/11/1/11MOCVDselective area epitaxyselective area growthphotoluminescenceatomic force microscopysemiconductors
spellingShingle Viktor Shamakhov
Dmitriy Nikolaev
Sergey Slipchenko
Evgenii Fomin
Alexander Smirnov
Ilya Eliseyev
Nikita Pikhtin
Peter Kop`ev
Surface Nanostructuring during Selective Area Epitaxy of Heterostructures with InGaAs QWs in the Ultra-Wide Windows
Nanomaterials
MOCVD
selective area epitaxy
selective area growth
photoluminescence
atomic force microscopy
semiconductors
title Surface Nanostructuring during Selective Area Epitaxy of Heterostructures with InGaAs QWs in the Ultra-Wide Windows
title_full Surface Nanostructuring during Selective Area Epitaxy of Heterostructures with InGaAs QWs in the Ultra-Wide Windows
title_fullStr Surface Nanostructuring during Selective Area Epitaxy of Heterostructures with InGaAs QWs in the Ultra-Wide Windows
title_full_unstemmed Surface Nanostructuring during Selective Area Epitaxy of Heterostructures with InGaAs QWs in the Ultra-Wide Windows
title_short Surface Nanostructuring during Selective Area Epitaxy of Heterostructures with InGaAs QWs in the Ultra-Wide Windows
title_sort surface nanostructuring during selective area epitaxy of heterostructures with ingaas qws in the ultra wide windows
topic MOCVD
selective area epitaxy
selective area growth
photoluminescence
atomic force microscopy
semiconductors
url https://www.mdpi.com/2079-4991/11/1/11
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