Structure Determination and Defect Analysis n-Si<Lu>, p-Si<Lu> Raman Spectrometer Methods

In this work, lutetium-doped silicon samples were studied using the Raman scattering method. Registration and identification of both crystalline and amorphous phase components in the samples was carried out. There is some violation in the spectra of Raman scattering of light samples of silicon dope...

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Main Authors: Khodjakbar S. Daliev, Sharifa B. Utamuradova, Zavkiddin E. Bahronkulov, Alisher Kh. Khaitbaev, Jonibek J. Hamdamov
Format: Article
Language:English
Published: V.N. Karazin Kharkiv National University Publishing 2023-12-01
Series:East European Journal of Physics
Subjects:
Online Access:https://periodicals.karazin.ua/eejp/article/view/22143
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author Khodjakbar S. Daliev
Sharifa B. Utamuradova
Zavkiddin E. Bahronkulov
Alisher Kh. Khaitbaev
Jonibek J. Hamdamov
author_facet Khodjakbar S. Daliev
Sharifa B. Utamuradova
Zavkiddin E. Bahronkulov
Alisher Kh. Khaitbaev
Jonibek J. Hamdamov
author_sort Khodjakbar S. Daliev
collection DOAJ
description In this work, lutetium-doped silicon samples were studied using the Raman scattering method. Registration and identification of both crystalline and amorphous phase components in the samples was carried out. There is some violation in the spectra of Raman scattering of light samples of silicon doped with lutetium in comparison with the original sample. It was found that the intensity of Raman scattering of doped samples is 2-3 times higher than the scattering from silicon. The comparison is carried out for the intensities associated with the intensities of the single-phonon line of the silicon substrate. This effect of the Raman spectra in the range 930 cm‑1 – 1030 cm–1 appearing in this range is similar to the data reduction for multiphonon propagation on silicon. For the obtained images (n-Si<Lu> and p-Si<Lu>), the bands in the atomic range of combinatorial scattering have a mixed broad and oval background in the range from 623 cm-1 to 1400 cm-1. This background can change the shape of the observed bands.
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spelling doaj.art-a3224a406734426781b7415631497d5b2023-12-02T13:52:24ZengV.N. Karazin Kharkiv National University PublishingEast European Journal of Physics2312-43342312-45392023-12-01410.26565/2312-4334-2023-4-23Structure Determination and Defect Analysis n-Si<Lu>, p-Si<Lu> Raman Spectrometer MethodsKhodjakbar S. Daliev0Sharifa B. Utamuradova1Zavkiddin E. Bahronkulov2Alisher Kh. Khaitbaev3Jonibek J. Hamdamov4Branch of the Federal State Budgetary Educational Institution of Higher Education “National Research University MPEI”, Tashkent, UzbekistanInstitute of Semiconductor Physics and Microelectronics at the National University of Uzbekistan, Tashkent, UzbekistanInstitute of Semiconductor Physics and Microelectronics at the National University of Uzbekistan, Tashkent, UzbekistanNational University of Uzbekistan, Tashkent, UzbekistanInstitute of Semiconductor Physics and Microelectronics at the National University of Uzbekistan, Tashkent, Uzbekistan In this work, lutetium-doped silicon samples were studied using the Raman scattering method. Registration and identification of both crystalline and amorphous phase components in the samples was carried out. There is some violation in the spectra of Raman scattering of light samples of silicon doped with lutetium in comparison with the original sample. It was found that the intensity of Raman scattering of doped samples is 2-3 times higher than the scattering from silicon. The comparison is carried out for the intensities associated with the intensities of the single-phonon line of the silicon substrate. This effect of the Raman spectra in the range 930 cm‑1 – 1030 cm–1 appearing in this range is similar to the data reduction for multiphonon propagation on silicon. For the obtained images (n-Si<Lu> and p-Si<Lu>), the bands in the atomic range of combinatorial scattering have a mixed broad and oval background in the range from 623 cm-1 to 1400 cm-1. This background can change the shape of the observed bands. https://periodicals.karazin.ua/eejp/article/view/22143SiliconLutetiumRaman spectroscopyDiffusionDopingTemperature
spellingShingle Khodjakbar S. Daliev
Sharifa B. Utamuradova
Zavkiddin E. Bahronkulov
Alisher Kh. Khaitbaev
Jonibek J. Hamdamov
Structure Determination and Defect Analysis n-Si<Lu>, p-Si<Lu> Raman Spectrometer Methods
East European Journal of Physics
Silicon
Lutetium
Raman spectroscopy
Diffusion
Doping
Temperature
title Structure Determination and Defect Analysis n-Si<Lu>, p-Si<Lu> Raman Spectrometer Methods
title_full Structure Determination and Defect Analysis n-Si<Lu>, p-Si<Lu> Raman Spectrometer Methods
title_fullStr Structure Determination and Defect Analysis n-Si<Lu>, p-Si<Lu> Raman Spectrometer Methods
title_full_unstemmed Structure Determination and Defect Analysis n-Si<Lu>, p-Si<Lu> Raman Spectrometer Methods
title_short Structure Determination and Defect Analysis n-Si<Lu>, p-Si<Lu> Raman Spectrometer Methods
title_sort structure determination and defect analysis n si lu p si lu raman spectrometer methods
topic Silicon
Lutetium
Raman spectroscopy
Diffusion
Doping
Temperature
url https://periodicals.karazin.ua/eejp/article/view/22143
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AT zavkiddinebahronkulov structuredeterminationanddefectanalysisnsilupsiluramanspectrometermethods
AT alisherkhkhaitbaev structuredeterminationanddefectanalysisnsilupsiluramanspectrometermethods
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