Electronic structure of semiconductor nanostructures

In this thesis we have used a combination of theory and experiment to explore the electronic structure of two nanoscale semiconductor systems, namely porous silicon and the metal-semiconductor tunnel junction in a scanning tunneling microscope (STM). The experimental techniques used to study thes...

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Main Author: Patitsas, Steve N.
Format: Others
Language:English
Published: 2009
Online Access:http://hdl.handle.net/2429/6748
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description In this thesis we have used a combination of theory and experiment to explore the electronic structure of two nanoscale semiconductor systems, namely porous silicon and the metal-semiconductor tunnel junction in a scanning tunneling microscope (STM). The experimental techniques used to study these systems are complementary in the sense that STM provides atomic scale information on surface structure while X-ray absorption and fluorescence provide abundant information on electronic structure. STM provides a unique way to locally probe the electronic structure of a surface with atomic resolution. We have used a linear combination of atomic orbitals model to explain the features seen in X-ray absorption and fluorescence spectra of bulk silicon and porous silicon. We can explain why the band edges shift in porous Si relative to bulk Si using a quantum confinement model. These band shifts can also be modeled by effective mass theory. The linear combination of atomic orbitals model has also shown that X-ray fluorescence spectra are sensitive to the structure of porous Si on a nanometer length scale. We show that the observed spectra are in good agreement with the nanostructures being very thin <100> oriented Si sheets. In order to perform cross-sectional STM measurements on semiconductor heterostructures an ultra-high vacuum STM with a precise lateral sample motion capability was constructed as part of the thesis. This STM also has variable sample temperature capability from room temperature down to 120 K. As well as imaging, with atomic resolution, a GaAs/AlGaAs interface in cross-section we have imaged the following various heterostructures in cross-section for the first time; a CoSi₂layer buried in Si, an InGaAs quantum well and a ZnSe layer on GaAs. Spatially resolved STM spectroscopy of the CoSi₂layer distinguished between the metallic nature of the CoSi₂and the semiconductor nature of Si. From STM on Si(l 10) we have proposed a "sextet" model for the atomic structure of the clean reconstructed Si(110) surface. A GaAs/ZnSe interface was also imaged for the first time with atomic resolution. The conduction band offset of this interface was obtained by measuring the width of the depleted region on the ZnSe side of the interface. In order to gain information on the electronic structure of semiconductor surfaces we performed current-voltage measurements with our STM. We show that STM current-voltage measurements on clean (110) GaAs can give information about the presence of material on the end of the STM tip. The turn-on voltage of the current at positive tip-sample bias can be explained by assuming there is an insulating layer on the end of the STM tip. This contamination which has the effect of increasing the tunnel-junction resistance at negative tipsample bias but not at positive bias may be GaAs which is deposited on the tip from the sample during STM operation. A thin layer of GaAs is sufficient to fit the data. STM current-voltage measurements performed on clean n-type (110) GaAs also showed structure at both forward and negative bias which arises from tip-induced band-bending as well as the very low density of states at the bottom of the conduction band of GaAs and the transition to much higher density of states at the L6-point located 0.25 eV above the conduction band minimum. Variable temperature current-voltage characteristics show an exponential dependence from room temperature down to 125 K that cannot be explained by thermionic emission. The measured temperature dependence can be explained by assuming the affinity of the (110) GaAs surface is =0.2 eV smaller at 125 K than at room temperature. === Science, Faculty of === Physics and Astronomy, Department of === Graduate
author Patitsas, Steve N.
spellingShingle Patitsas, Steve N.
Electronic structure of semiconductor nanostructures
author_facet Patitsas, Steve N.
author_sort Patitsas, Steve N.
title Electronic structure of semiconductor nanostructures
title_short Electronic structure of semiconductor nanostructures
title_full Electronic structure of semiconductor nanostructures
title_fullStr Electronic structure of semiconductor nanostructures
title_full_unstemmed Electronic structure of semiconductor nanostructures
title_sort electronic structure of semiconductor nanostructures
publishDate 2009
url http://hdl.handle.net/2429/6748
work_keys_str_mv AT patitsassteven electronicstructureofsemiconductornanostructures
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spelling ndltd-UBC-oai-circle.library.ubc.ca-2429-67482018-01-05T17:33:22Z Electronic structure of semiconductor nanostructures Patitsas, Steve N. In this thesis we have used a combination of theory and experiment to explore the electronic structure of two nanoscale semiconductor systems, namely porous silicon and the metal-semiconductor tunnel junction in a scanning tunneling microscope (STM). The experimental techniques used to study these systems are complementary in the sense that STM provides atomic scale information on surface structure while X-ray absorption and fluorescence provide abundant information on electronic structure. STM provides a unique way to locally probe the electronic structure of a surface with atomic resolution. We have used a linear combination of atomic orbitals model to explain the features seen in X-ray absorption and fluorescence spectra of bulk silicon and porous silicon. We can explain why the band edges shift in porous Si relative to bulk Si using a quantum confinement model. These band shifts can also be modeled by effective mass theory. The linear combination of atomic orbitals model has also shown that X-ray fluorescence spectra are sensitive to the structure of porous Si on a nanometer length scale. We show that the observed spectra are in good agreement with the nanostructures being very thin <100> oriented Si sheets. In order to perform cross-sectional STM measurements on semiconductor heterostructures an ultra-high vacuum STM with a precise lateral sample motion capability was constructed as part of the thesis. This STM also has variable sample temperature capability from room temperature down to 120 K. As well as imaging, with atomic resolution, a GaAs/AlGaAs interface in cross-section we have imaged the following various heterostructures in cross-section for the first time; a CoSi₂layer buried in Si, an InGaAs quantum well and a ZnSe layer on GaAs. Spatially resolved STM spectroscopy of the CoSi₂layer distinguished between the metallic nature of the CoSi₂and the semiconductor nature of Si. From STM on Si(l 10) we have proposed a "sextet" model for the atomic structure of the clean reconstructed Si(110) surface. A GaAs/ZnSe interface was also imaged for the first time with atomic resolution. The conduction band offset of this interface was obtained by measuring the width of the depleted region on the ZnSe side of the interface. In order to gain information on the electronic structure of semiconductor surfaces we performed current-voltage measurements with our STM. We show that STM current-voltage measurements on clean (110) GaAs can give information about the presence of material on the end of the STM tip. The turn-on voltage of the current at positive tip-sample bias can be explained by assuming there is an insulating layer on the end of the STM tip. This contamination which has the effect of increasing the tunnel-junction resistance at negative tipsample bias but not at positive bias may be GaAs which is deposited on the tip from the sample during STM operation. A thin layer of GaAs is sufficient to fit the data. STM current-voltage measurements performed on clean n-type (110) GaAs also showed structure at both forward and negative bias which arises from tip-induced band-bending as well as the very low density of states at the bottom of the conduction band of GaAs and the transition to much higher density of states at the L6-point located 0.25 eV above the conduction band minimum. Variable temperature current-voltage characteristics show an exponential dependence from room temperature down to 125 K that cannot be explained by thermionic emission. The measured temperature dependence can be explained by assuming the affinity of the (110) GaAs surface is =0.2 eV smaller at 125 K than at room temperature. Science, Faculty of Physics and Astronomy, Department of Graduate 2009-04-02T23:57:29Z 2009-04-02T23:57:29Z 1996 1997-05 Text Thesis/Dissertation http://hdl.handle.net/2429/6748 eng For non-commercial purposes only, such as research, private study and education. Additional conditions apply, see Terms of Use https://open.library.ubc.ca/terms_of_use. 15664712 bytes application/pdf