Analyzing Electronic Correlation Effects in Molecules and Semiconductor Point Defects from First Principles Beyond Density Functional Theory

dc.contributor.authorKaranovich, Anrien
dc.contributor.committeechairPark, Kyungwhaen
dc.contributor.committeememberMayhall, Nicholasen
dc.contributor.committeememberScarola, Vito W.en
dc.contributor.committeememberSoghomonian, Victoria Garabeden
dc.contributor.departmentPhysicsen
dc.date.accessioned2025-01-04T09:01:36Zen
dc.date.available2025-01-04T09:01:36Zen
dc.date.issued2025-01-03en
dc.description.abstractTransition-metal based molecules and point defects in wide-bandgap semiconductors have been of particular interest lately due to their potential quantum information science applications. To accurately calculate the electronic properties of these systems from first principles, it is important to appropriately account for electronic correlation effects. Density functional theory (DFT) has been one of the most popular methods to perform calculations on correlated systems, due to the combination of numerical efficiency and precision in many applications. However, traditional DFT methods fail to accurately calculate the important electronic and magnetic properties, such as bandgaps in semiconductors or magnetic ordering in defects, to name a few. This dissertation focuses on two areas in which traditional DFT methods are likely to produce inaccurate predictions. The first area is connected to an error that is intrinsic to most DFT formulations due to the approximate nature of the exchange-correlation functional, known as the self-interaction error (SIE). It is known to cause the underestimation of bandgaps in solids, underestimated reaction barriers in molecules, and incorrect dissociation curves. The second area is the case where the ground and/or excited states are described by multiconfigurational wavefunctions rather than a single Slater determinant. Chapter 1 of the thesis provides a brief overview of various electronic-structure methods, as well as the Fermi-Löwdin Orbital Self-Interaction Correction method (FLOSIC) which is used to remedy the SIE in DFT. Chapter 2 reports on the application of the FLOSIC-DFT on a Cu-based molecule, and its effects on the predicted electronic properties. Chapter 3 describes the application of the FLOSIC-DFT to the computation of the hyperfine coupling terms, which are crucial for the realization of spin qubits and for interpreting electron paramagnetic resonance experiments. Chapter 4 turns to the application of a multiconfigurational method to describe the electronic properties of a silicon vacancy in silicon carbide, a potential point-defect qubit.en
dc.description.abstractgeneralComputational electronic structure methods, which attempt to predict optical, electronic, and other properties of molecules and materials just by solving the Schrödinger equation for the wavefunction of the electrons in them, have been instrumental in many areas of research, including the design of semiconductors, drug discovery, improved solar panel design, and discovering systems that can work as qubits for quantum-computing purposes, to name a few. One of the most successful sets of these methods, known as Density Functional Theory (DFT) methods, makes solving for electronic wavefunctions (and from them, other materials properties) computationally efficient, while maintaining the accuracy of such predictions by accounting for the complex quantum-mechanical interactions between the particles. For this, DFT was the subject of the 1998 Nobel Prize in chemistry. However, there are several areas where DFT is typically not successful in producing accurate predictions. One of the areas is connected to the approximated term in all DFT methods that often erroneously accounts for electrons interacting on themselves (an effect known as the self-interaction error). The other area is related to systems that must be described with superposition of several electronic configurations. Chapter 1 of the thesis provides a brief overview of various electronic-structure methods, as well as the Fermi-Löwdin Orbital Self-Interaction Correction method (FLOSIC) which suggests a modification to the standard DFT methods that aims to remove the self-interaction error. Chapter 2 reports on the application of the FLOSIC-DFT on a Cu-based molecule, and its effects on the predicted electronic properties. Chapter 3 describes the application of the FLOSIC-DFT to describe the interaction between the magnetic moments of electrons and nuclei, known as the hyperfine coupling, which is crucial for the realization of spin qubits and for interpreting some experimental results. Chapter 4 turns to the application of a multiconfigurational method to describe the electronic properties of a silicon vacancy in silicon carbide, a potential point-defect qubit.en
dc.description.degreeDoctor of Philosophyen
dc.format.mediumETDen
dc.identifier.othervt_gsexam:42442en
dc.identifier.urihttps://hdl.handle.net/10919/123904en
dc.language.isoenen
dc.publisherVirginia Techen
dc.rightsIn Copyrighten
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/en
dc.subjectDensity Functional Theoryen
dc.subjectElectronic Structureen
dc.subjectElectronic Correlationen
dc.subjectSelf-Interaction Correctionen
dc.subjectSelf-Interaction Erroren
dc.subjectMultireference Methodsen
dc.subjectFLOSICen
dc.subjectCASSCFen
dc.subjectCASPT2en
dc.subjectPoint Defectsen
dc.titleAnalyzing Electronic Correlation Effects in Molecules and Semiconductor Point Defects from First Principles Beyond Density Functional Theoryen
dc.typeDissertationen
thesis.degree.disciplinePhysicsen
thesis.degree.grantorVirginia Polytechnic Institute and State Universityen
thesis.degree.leveldoctoralen
thesis.degree.nameDoctor of Philosophyen

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