{"id":{"repo_id":"uiuc","oai_identifier":"oai:www.ideals.illinois.edu:2142/30942"},"canonical_url":"https://search.dev.ndltd.org/etd/uiuc/oai:www.ideals.illinois.edu:2142/30942","repository":{"repo_id":"uiuc","name":"University of Illinois - Urbana-Champaign","base_url":"https://www.ideals.illinois.edu/oai-pmh"},"display":{"title":"Vibrational many-body methods for molecules and extended systems","abstract":"\"Vibrational many-body methods for molecules and extended systems have been developed that can account for the effects of anharmonicity in the potential energy surfaces (PESs) on energies and other observable properties. For molecules, we present a general scheme to calculate anharmonic vibrational frequencies and vibrationally-averaged structures along with applications to some key species in hydrocarbon combustion chemistry: HCO$^+$, HCO, HNO, HOO, HOO$^-$, CH$_3^+$, and CH$_3$. We propose a hybrid, compact representation of PESs that combines the merits of two existing representations, which are a quartic force field (QFF) and numerical values on a rectilinear grid. We employed a combination of coupled-cluster singles and doubles (CCSD), CCSD with a second-order perturbation correction in the space of triples [CCSD(2)$_\\textit{T}$] and in the space of triples and quadruples [CCSD(2)$_\\textit{TQ}$], and a correlation-consistent basis set series to achieve the complete-correlation, complete-basis-set limits of the potential energy surfaces. The mean absolute deviation between the predicted and the observed frequencies is 11 cm$^{-1}$. For extended systems, we generalized the formulations of the vibrational self-consistent field (VSCF), vibrational M\\o ller--Plesset perturbation (VMP), and vibrational coupled-cluster (VCC) methods on the basis of a QFF in normal coordinates. We have identified algebraically and eliminated several terms in the formalisms of VSCF that have nonphysical size dependence, leading to compact and strictly size-extensive equations. This size-extensive VSCF method (XVSCF) thus defined has no contributions from cubic force constants and alters only the transition energies of the underlying harmonic-oscillator reference from a subset of quartic force constants. The mean-field potential of XVSCF felt by each mode is shown to be effectively harmonic, making the XVSCF equations subject to a self-consistent analytical solution without a basis-set expansion and matrix diagonalization, which are necessary in VSCF. We implemented the XVSCF method for finite systems, and applied it to molecules including polyacenes up to tetracene as well as to a model system of a linear chain of masses interacting through a quartic force field. We showed that the results of XVSCF and VSCF approach each other as the size of the system is increased, implicating the inclusion of unnecessary, nonphysical terms in VSCF. We have also shown that apart from reducing the scaling of the VSCF calculation from quartic to quadratic, XVSCF is nearly three orders of magnitude faster than VSCF implemented with a reduced set of force constants. The second-order VMP and VCC methods based on the XVSCF reference are shown to account for anharmonic effects due to all cubic and quartic force constants in a size-extensive fashion. We also presented the $\\Gamma$ approximation for extended systems, which amounts to including only in-phase phonons throughout the generation of PES and solution of the vibrational Schr\\\"\"{o}dinger equation. We computed the frequencies of the infrared- and/or Raman-active vibrations of polyethylene and polyacetylene using this approximation and we have shown that accounting for both electron correlation and anharmonicity is essential in achieving good agreement between computed and observed frequencies.\"","abstract_html":"&quot;Vibrational many-body methods for molecules and extended systems have been developed that can account for the effects of anharmonicity in the potential energy surfaces (PESs) on energies and other observable properties. For molecules, we present a general scheme to calculate anharmonic vibrational frequencies and vibrationally-averaged structures along with applications to some key species in hydrocarbon combustion chemistry: HCO<span class=\"etd-inline-math\"><sup>+</sup></span>, HCO, HNO, HOO, HOO<span class=\"etd-inline-math\"><sup>-</sup></span>, CH<span class=\"etd-inline-math\"><sub>3</sub><sup>+</sup></span>, and CH<span class=\"etd-inline-math\"><sub>3</sub></span>. We propose a hybrid, compact representation of PESs that combines the merits of two existing representations, which are a quartic force field (QFF) and numerical values on a rectilinear grid. We employed a combination of coupled-cluster singles and doubles (CCSD), CCSD with a second-order perturbation correction in the space of triples [CCSD(2)<span class=\"etd-inline-math\"><sub>\\</sub>textit{T}</span>] and in the space of triples and quadruples [CCSD(2)<span class=\"etd-inline-math\"><sub>\\</sub>textit{TQ}</span>], and a correlation-consistent basis set series to achieve the complete-correlation, complete-basis-set limits of the potential energy surfaces. The mean absolute deviation between the predicted and the observed frequencies is 11 cm<span class=\"etd-inline-math\"><sup>-1</sup></span>. For extended systems, we generalized the formulations of the vibrational self-consistent field (VSCF), vibrational M\\o ller--Plesset perturbation (VMP), and vibrational coupled-cluster (VCC) methods on the basis of a QFF in normal coordinates. We have identified algebraically and eliminated several terms in the formalisms of VSCF that have nonphysical size dependence, leading to compact and strictly size-extensive equations. This size-extensive VSCF method (XVSCF) thus defined has no contributions from cubic force constants and alters only the transition energies of the underlying harmonic-oscillator reference from a subset of quartic force constants. The mean-field potential of XVSCF felt by each mode is shown to be effectively harmonic, making the XVSCF equations subject to a self-consistent analytical solution without a basis-set expansion and matrix diagonalization, which are necessary in VSCF. We implemented the XVSCF method for finite systems, and applied it to molecules including polyacenes up to tetracene as well as to a model system of a linear chain of masses interacting through a quartic force field. We showed that the results of XVSCF and VSCF approach each other as the size of the system is increased, implicating the inclusion of unnecessary, nonphysical terms in VSCF. We have also shown that apart from reducing the scaling of the VSCF calculation from quartic to quadratic, XVSCF is nearly three orders of magnitude faster than VSCF implemented with a reduced set of force constants. The second-order VMP and VCC methods based on the XVSCF reference are shown to account for anharmonic effects due to all cubic and quartic force constants in a size-extensive fashion. We also presented the $\\Gamma$ approximation for extended systems, which amounts to including only in-phase phonons throughout the generation of PES and solution of the vibrational Schr\\&quot;&quot;{o}dinger equation. We computed the frequencies of the infrared- and/or Raman-active vibrations of polyethylene and polyacetylene using this approximation and we have shown that accounting for both electron correlation and anharmonicity is essential in achieving good agreement between computed and observed frequencies.&quot;","abstract_has_math":true,"creators":["Keceli, Murat"],"institution":"University of Illinois at Urbana-Champaign","degree_name":"Ph.D.","degree_level":"Dissertation","degree_discipline":"Chemical Physics","degree_department":null,"school":null,"contributors":["Hirata, So","Scheeline, Alexander","McCall, Benjamin J.","Girolami, Gregory S."],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2012,"date_issued":"2012-05-22T00:17:23Z","date_published":"2012-05-22T00:17:23Z","updated_at":"2026-07-22T22:25:29Z","subjects":["Anharmonic vibrations","anharmonicity","normal modes","phonons","Fermi resonance","many-body methods","self-consistent field","mean-field","Moller-Plesset perturbation","coupled-cluster","configuration interaction","size-consistency","size-extensive","gamma approximation","hybrid potential energy surface","quartic force field","size-extensive VSCF method (XVSCF)","vibrational self-consistent field (VSCF)","vibrational configuration-interaction (VCI)","vibrational Møller–Plesset perturbation (VMP)","normal coordinates","Watson Hamiltonian","polymer vibrations","polyethylene","polyacetylene","combustion chemistry","Formyl Radical (HCO)","Nitroxyl (HNO)","Hydroperoxyl (HOO)","Methyl groups (CH3)","chain model"],"languages":["en"],"rights":["Copyright 2012 Murat Keceli"],"rights_urls":[],"identifier_entries":[]},"links":{"outbound_url":"http://hdl.handle.net/2142/30942","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Hirata, So","Scheeline, Alexander","McCall, Benjamin J.","Girolami, Gregory S."]},{"key":"dc:creator","label":"Author","values":["Keceli, Murat"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["2012-05-22T00:17:23Z","2012-05"]},{"key":"dc:type","label":"Dc Type","values":["text"]},{"key":"thesis:degree_discipline","label":"Discipline","values":["Chemical Physics"]},{"key":"thesis:degree_level","label":"Degree Level","values":["Dissertation"]},{"key":"thesis:degree_name","label":"Degree Name","values":["Ph.D."]},{"key":"thesis:institution_name","label":"Thesis Institution Name","values":["University of Illinois at Urbana-Champaign"]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["Anharmonic vibrations","anharmonicity","normal modes","phonons","Fermi resonance","many-body methods","self-consistent field","mean-field","Moller-Plesset perturbation","coupled-cluster","configuration interaction","size-consistency","size-extensive","gamma approximation","hybrid potential energy surface","quartic force field","size-extensive VSCF method (XVSCF)","vibrational self-consistent field (VSCF)","vibrational configuration-interaction (VCI)","vibrational Møller–Plesset perturbation (VMP)","normal coordinates","Watson Hamiltonian","polymer vibrations","polyethylene","polyacetylene","combustion chemistry","Formyl Radical (HCO)","Nitroxyl (HNO)","Hydroperoxyl (HOO)","Methyl groups (CH3)","chain model"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:language","label":"Dc Language","values":["en"]},{"key":"dc:rights","label":"Dc Rights","values":["Copyright 2012 Murat Keceli"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["http://hdl.handle.net/2142/30942"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["\"Vibrational many-body methods for molecules and extended systems have been developed that can account for the effects of anharmonicity in the potential energy surfaces (PESs) on energies and other observable properties. For molecules, we present a general scheme to calculate anharmonic vibrational frequencies and vibrationally-averaged structures along with applications to some key species in hydrocarbon combustion chemistry: HCO$^+$, HCO, HNO, HOO, HOO$^-$, CH$_3^+$, and CH$_3$. We propose a hybrid, compact representation of PESs that combines the merits of two existing representations, which are a quartic force field (QFF) and numerical values on a rectilinear grid. We employed a combination of coupled-cluster singles and doubles (CCSD), CCSD with a second-order perturbation correction in the space of triples [CCSD(2)$_\\textit{T}$] and in the space of triples and quadruples [CCSD(2)$_\\textit{TQ}$], and a correlation-consistent basis set series to achieve the complete-correlation, complete-basis-set limits of the potential energy surfaces. The mean absolute deviation between the predicted and the observed frequencies is 11 cm$^{-1}$. For extended systems, we generalized the formulations of the vibrational self-consistent field (VSCF), vibrational M\\o ller--Plesset perturbation (VMP), and vibrational coupled-cluster (VCC) methods on the basis of a QFF in normal coordinates. We have identified algebraically and eliminated several terms in the formalisms of VSCF that have nonphysical size dependence, leading to compact and strictly size-extensive equations. This size-extensive VSCF method (XVSCF) thus defined has no contributions from cubic force constants and alters only the transition energies of the underlying harmonic-oscillator reference from a subset of quartic force constants. The mean-field potential of XVSCF felt by each mode is shown to be effectively harmonic, making the XVSCF equations subject to a self-consistent analytical solution without a basis-set expansion and matrix diagonalization, which are necessary in VSCF. We implemented the XVSCF method for finite systems, and applied it to molecules including polyacenes up to tetracene as well as to a model system of a linear chain of masses interacting through a quartic force field. We showed that the results of XVSCF and VSCF approach each other as the size of the system is increased, implicating the inclusion of unnecessary, nonphysical terms in VSCF. We have also shown that apart from reducing the scaling of the VSCF calculation from quartic to quadratic, XVSCF is nearly three orders of magnitude faster than VSCF implemented with a reduced set of force constants. The second-order VMP and VCC methods based on the XVSCF reference are shown to account for anharmonic effects due to all cubic and quartic force constants in a size-extensive fashion. We also presented the $\\Gamma$ approximation for extended systems, which amounts to including only in-phase phonons throughout the generation of PES and solution of the vibrational Schr\\\"\"{o}dinger equation. We computed the frequencies of the infrared- and/or Raman-active vibrations of polyethylene and polyacetylene using this approximation and we have shown that accounting for both electron correlation and anharmonicity is essential in achieving good agreement between computed and observed frequencies.\"","Item withdrawn by Mark Zulauf (zulauf@illinois.edu) on 2012-04-11T13:56:31Z Item was in collections: University of Illinois Theses & Dissertations (ID: 1) No. of bitstreams: 2 keceli_tez.tex: 306422 bytes, checksum: ce6573f924e94d64efb3a89500c77d78 (MD5) Keceli_Murat.pdf: 453645 bytes, checksum: 74e6ebd27f18d0cee34f113572c79ac2 (MD5)","Made available in DSpace on 2012-05-22T00:17:23Z (GMT). No. of bitstreams: 3 Keceli_Murat.pdf: 517774 bytes, checksum: 96166ec828e4436efc3a31313012fa24 (MD5) keceli_tez.tex: 306422 bytes, checksum: ce6573f924e94d64efb3a89500c77d78 (MD5) license.txt: 4061 bytes, checksum: 6df4e4c5c3c3b7476fff445406b0c5b8 (MD5)"]},{"key":"dc:title","label":"Title","values":["Vibrational many-body methods for molecules and extended systems"]}]}],"canonical_facts":{"dc:contributor":["Hirata, So","Scheeline, Alexander","McCall, Benjamin J.","Girolami, Gregory S."],"dc:creator":["Keceli, Murat"],"dc:date":["2012-05-22T00:17:23Z","2012-05"],"dc:description":["\"Vibrational many-body methods for molecules and extended systems have been developed that can account for the effects of anharmonicity in the potential energy surfaces (PESs) on energies and other observable properties. For molecules, we present a general scheme to calculate anharmonic vibrational frequencies and vibrationally-averaged structures along with applications to some key species in hydrocarbon combustion chemistry: HCO$^+$, HCO, HNO, HOO, HOO$^-$, CH$_3^+$, and CH$_3$. We propose a hybrid, compact representation of PESs that combines the merits of two existing representations, which are a quartic force field (QFF) and numerical values on a rectilinear grid. We employed a combination of coupled-cluster singles and doubles (CCSD), CCSD with a second-order perturbation correction in the space of triples [CCSD(2)$_\\textit{T}$] and in the space of triples and quadruples [CCSD(2)$_\\textit{TQ}$], and a correlation-consistent basis set series to achieve the complete-correlation, complete-basis-set limits of the potential energy surfaces. The mean absolute deviation between the predicted and the observed frequencies is 11 cm$^{-1}$. For extended systems, we generalized the formulations of the vibrational self-consistent field (VSCF), vibrational M\\o ller--Plesset perturbation (VMP), and vibrational coupled-cluster (VCC) methods on the basis of a QFF in normal coordinates. We have identified algebraically and eliminated several terms in the formalisms of VSCF that have nonphysical size dependence, leading to compact and strictly size-extensive equations. This size-extensive VSCF method (XVSCF) thus defined has no contributions from cubic force constants and alters only the transition energies of the underlying harmonic-oscillator reference from a subset of quartic force constants. The mean-field potential of XVSCF felt by each mode is shown to be effectively harmonic, making the XVSCF equations subject to a self-consistent analytical solution without a basis-set expansion and matrix diagonalization, which are necessary in VSCF. We implemented the XVSCF method for finite systems, and applied it to molecules including polyacenes up to tetracene as well as to a model system of a linear chain of masses interacting through a quartic force field. We showed that the results of XVSCF and VSCF approach each other as the size of the system is increased, implicating the inclusion of unnecessary, nonphysical terms in VSCF. We have also shown that apart from reducing the scaling of the VSCF calculation from quartic to quadratic, XVSCF is nearly three orders of magnitude faster than VSCF implemented with a reduced set of force constants. The second-order VMP and VCC methods based on the XVSCF reference are shown to account for anharmonic effects due to all cubic and quartic force constants in a size-extensive fashion. We also presented the $\\Gamma$ approximation for extended systems, which amounts to including only in-phase phonons throughout the generation of PES and solution of the vibrational Schr\\\"\"{o}dinger equation. We computed the frequencies of the infrared- and/or Raman-active vibrations of polyethylene and polyacetylene using this approximation and we have shown that accounting for both electron correlation and anharmonicity is essential in achieving good agreement between computed and observed frequencies.\"","Item withdrawn by Mark Zulauf (zulauf@illinois.edu) on 2012-04-11T13:56:31Z Item was in collections: University of Illinois Theses & Dissertations (ID: 1) No. of bitstreams: 2 keceli_tez.tex: 306422 bytes, checksum: ce6573f924e94d64efb3a89500c77d78 (MD5) Keceli_Murat.pdf: 453645 bytes, checksum: 74e6ebd27f18d0cee34f113572c79ac2 (MD5)","Made available in DSpace on 2012-05-22T00:17:23Z (GMT). No. of bitstreams: 3 Keceli_Murat.pdf: 517774 bytes, checksum: 96166ec828e4436efc3a31313012fa24 (MD5) keceli_tez.tex: 306422 bytes, checksum: ce6573f924e94d64efb3a89500c77d78 (MD5) license.txt: 4061 bytes, checksum: 6df4e4c5c3c3b7476fff445406b0c5b8 (MD5)"],"dc:identifier":["http://hdl.handle.net/2142/30942"],"dc:language":["en"],"dc:rights":["Copyright 2012 Murat Keceli"],"dc:subject":["Anharmonic vibrations","anharmonicity","normal modes","phonons","Fermi resonance","many-body methods","self-consistent field","mean-field","Moller-Plesset perturbation","coupled-cluster","configuration interaction","size-consistency","size-extensive","gamma approximation","hybrid potential energy surface","quartic force field","size-extensive VSCF method (XVSCF)","vibrational self-consistent field (VSCF)","vibrational configuration-interaction (VCI)","vibrational Møller–Plesset perturbation (VMP)","normal coordinates","Watson Hamiltonian","polymer vibrations","polyethylene","polyacetylene","combustion chemistry","Formyl Radical (HCO)","Nitroxyl (HNO)","Hydroperoxyl (HOO)","Methyl groups (CH3)","chain model"],"dc:title":["Vibrational many-body methods for molecules and extended systems"],"dc:type":["text"],"thesis:degree_discipline":["Chemical Physics"],"thesis:degree_level":["Dissertation"],"thesis:degree_name":["Ph.D."],"thesis:institution_name":["University of Illinois at Urbana-Champaign"]},"updated_at":"2026-07-22T22:25:29Z"}