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A comparison of unrestricted Hartree-Fock- and restricted open-shell Hartree-Fock-based methods for determining the magnetic hyperfine parameters of NO (X2Π)
The magnetic hyperfine structure parameters of NO X 2Π have been determined through a variety of ab initio methods based on restricted and unrestricted Hartree–Fock zeroth order wave functions. Examples of the former include singles configuration interaction (CI), multireference CI, and averaged cou...
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Published in: | The Journal of chemical physics 1993-08, Vol.99 (4), p.2829-2840 |
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description | The magnetic hyperfine structure parameters of NO X 2Π have been determined through a variety of ab initio methods based on restricted and unrestricted Hartree–Fock zeroth order wave functions. Examples of the former include singles configuration interaction (CI), multireference CI, and averaged coupled pair functional theory. Examples of the latter include Mo/ller–Plesset perturbation theory (through fifth order, with estimates to infinite order), coupled cluster methods, and quadratic CI (with approximate inclusion of triple and quadruple excitations). The performance of the various methods in reproducing the difficult-to-describe 14N and 17O isotropic hyperfine interactions is judged in light of both experimental data, where available, and estimated full CI values. The full CI limit was approached through a systematic sequence of ever-more-extensive, selected multireference CI wave functions that would, in principle, include the full CI as its final element. While the isotropic coupling constants were found to converge very slowly along this sequence, at least in comparison to other one-electron properties, the selected CI approach was efficient enough in its recovery of correlation effects to be used with large basis sets. The biggest calculation in the sequence of CI wave functions included over two million configurations. Energies and properties exhibited sufficient regularity to allow fitting with simple functional forms. The error arising from the lack of basis set completeness is estimated by comparison to fully numerical, partial-wave self-consistent field (SCF) and singles CI results. Effects due to vibrational motion are accounted for by numerical integration of the one-dimensional Schrödinger equation. |
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D ; MCCULLOUGH, E. A ; MILLER, R. J</creator><creatorcontrib>FELLER, D ; GLENDENING, E. D ; MCCULLOUGH, E. A ; MILLER, R. J</creatorcontrib><description>The magnetic hyperfine structure parameters of NO X 2Π have been determined through a variety of ab initio methods based on restricted and unrestricted Hartree–Fock zeroth order wave functions. Examples of the former include singles configuration interaction (CI), multireference CI, and averaged coupled pair functional theory. Examples of the latter include Mo/ller–Plesset perturbation theory (through fifth order, with estimates to infinite order), coupled cluster methods, and quadratic CI (with approximate inclusion of triple and quadruple excitations). The performance of the various methods in reproducing the difficult-to-describe 14N and 17O isotropic hyperfine interactions is judged in light of both experimental data, where available, and estimated full CI values. The full CI limit was approached through a systematic sequence of ever-more-extensive, selected multireference CI wave functions that would, in principle, include the full CI as its final element. While the isotropic coupling constants were found to converge very slowly along this sequence, at least in comparison to other one-electron properties, the selected CI approach was efficient enough in its recovery of correlation effects to be used with large basis sets. The biggest calculation in the sequence of CI wave functions included over two million configurations. Energies and properties exhibited sufficient regularity to allow fitting with simple functional forms. The error arising from the lack of basis set completeness is estimated by comparison to fully numerical, partial-wave self-consistent field (SCF) and singles CI results. 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D</creatorcontrib><creatorcontrib>MCCULLOUGH, E. A</creatorcontrib><creatorcontrib>MILLER, R. J</creatorcontrib><title>A comparison of unrestricted Hartree-Fock- and restricted open-shell Hartree-Fock-based methods for determining the magnetic hyperfine parameters of NO (X2Π)</title><title>The Journal of chemical physics</title><description>The magnetic hyperfine structure parameters of NO X 2Π have been determined through a variety of ab initio methods based on restricted and unrestricted Hartree–Fock zeroth order wave functions. Examples of the former include singles configuration interaction (CI), multireference CI, and averaged coupled pair functional theory. Examples of the latter include Mo/ller–Plesset perturbation theory (through fifth order, with estimates to infinite order), coupled cluster methods, and quadratic CI (with approximate inclusion of triple and quadruple excitations). The performance of the various methods in reproducing the difficult-to-describe 14N and 17O isotropic hyperfine interactions is judged in light of both experimental data, where available, and estimated full CI values. The full CI limit was approached through a systematic sequence of ever-more-extensive, selected multireference CI wave functions that would, in principle, include the full CI as its final element. While the isotropic coupling constants were found to converge very slowly along this sequence, at least in comparison to other one-electron properties, the selected CI approach was efficient enough in its recovery of correlation effects to be used with large basis sets. The biggest calculation in the sequence of CI wave functions included over two million configurations. Energies and properties exhibited sufficient regularity to allow fitting with simple functional forms. The error arising from the lack of basis set completeness is estimated by comparison to fully numerical, partial-wave self-consistent field (SCF) and singles CI results. Effects due to vibrational motion are accounted for by numerical integration of the one-dimensional Schrödinger equation.</description><subject>664100 - Theory of Electronic Structure of Atoms & Molecules- (1992-)</subject><subject>ATOMIC AND MOLECULAR PHYSICS</subject><subject>CALCULATION METHODS</subject><subject>CHALCOGENIDES</subject><subject>COMPARATIVE EVALUATIONS</subject><subject>CONFIGURATION INTERACTION</subject><subject>CORRELATIONS</subject><subject>ELECTRON CORRELATION</subject><subject>Electron correlation calculations for atoms and molecules</subject><subject>Electronic structure of atoms, molecules and their ions: theory</subject><subject>EVALUATION</subject><subject>EVEN-ODD NUCLEI</subject><subject>Exact sciences and technology</subject><subject>FUNCTIONALS</subject><subject>FUNCTIONS</subject><subject>HARTREE-FOCK METHOD</subject><subject>HYPERFINE STRUCTURE</subject><subject>ISOTOPES</subject><subject>LIGHT NUCLEI</subject><subject>MAGNETIC PROPERTIES</subject><subject>MULTIPLETS</subject><subject>NITRIC OXIDE</subject><subject>NITROGEN 14</subject><subject>NITROGEN COMPOUNDS</subject><subject>NITROGEN ISOTOPES</subject><subject>NITROGEN OXIDES</subject><subject>NUCLEI</subject><subject>ODD-ODD NUCLEI</subject><subject>OXIDES</subject><subject>OXYGEN 17</subject><subject>OXYGEN COMPOUNDS</subject><subject>OXYGEN ISOTOPES</subject><subject>PERTURBATION THEORY</subject><subject>PHYSICAL PROPERTIES</subject><subject>Physics</subject><subject>STABLE ISOTOPES</subject><subject>TRIPLETS</subject><subject>WAVE FUNCTIONS</subject><issn>0021-9606</issn><issn>1089-7690</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1993</creationdate><recordtype>article</recordtype><recordid>eNpV0MFKxDAUBdAgCo6j4CcEcTEuqnlpmzbLYXBUGJyNgruSpq82Ok1KEhf-jPhFfpMdRkRXb3EPj8sl5BTYJTCRXsFlJnKQfI9MgJUyKYRk-2TCGIdECiYOyVEIL4wxKHg2IR9zql0_KG-Cs9S19M16DNEbHbGht8pHj5gsnX5NqLIN_RO6AW0SOtxs_rtahTHtMXauCbR1njYY0ffGGvtMY4e0V88Wo9G0ex_Qt8YiHRuofsvCtsT9ms6e-NfnxTE5aNUm4MnPnZLH5fXD4jZZrW_uFvNVokGKmKRlKTJoSlVoXeRZmXFZ1y0AFowLJjPdpEUmGwmc16BGIOo8A522IsecqzKdkrPdXxeiqYI2EXWnnbWoYyV4UUKRjmi2Q9q7EDy21eBNr_x7Bazajl9BtRt_pOc7Oqig1ab1ymoTfv3YkPEc0m__ZoRm</recordid><startdate>19930815</startdate><enddate>19930815</enddate><creator>FELLER, D</creator><creator>GLENDENING, E. D</creator><creator>MCCULLOUGH, E. A</creator><creator>MILLER, R. J</creator><general>American Institute of Physics</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>19930815</creationdate><title>A comparison of unrestricted Hartree-Fock- and restricted open-shell Hartree-Fock-based methods for determining the magnetic hyperfine parameters of NO (X2Π)</title><author>FELLER, D ; GLENDENING, E. D ; MCCULLOUGH, E. A ; MILLER, R. J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c196t-388641d8a7cc7548429bbf11e7026094cd3749d9122b1a5486b541c3f65e52a83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1993</creationdate><topic>664100 - Theory of Electronic Structure of Atoms & Molecules- (1992-)</topic><topic>ATOMIC AND MOLECULAR PHYSICS</topic><topic>CALCULATION METHODS</topic><topic>CHALCOGENIDES</topic><topic>COMPARATIVE EVALUATIONS</topic><topic>CONFIGURATION INTERACTION</topic><topic>CORRELATIONS</topic><topic>ELECTRON CORRELATION</topic><topic>Electron correlation calculations for atoms and molecules</topic><topic>Electronic structure of atoms, molecules and their ions: theory</topic><topic>EVALUATION</topic><topic>EVEN-ODD NUCLEI</topic><topic>Exact sciences and technology</topic><topic>FUNCTIONALS</topic><topic>FUNCTIONS</topic><topic>HARTREE-FOCK METHOD</topic><topic>HYPERFINE STRUCTURE</topic><topic>ISOTOPES</topic><topic>LIGHT NUCLEI</topic><topic>MAGNETIC PROPERTIES</topic><topic>MULTIPLETS</topic><topic>NITRIC OXIDE</topic><topic>NITROGEN 14</topic><topic>NITROGEN COMPOUNDS</topic><topic>NITROGEN ISOTOPES</topic><topic>NITROGEN OXIDES</topic><topic>NUCLEI</topic><topic>ODD-ODD NUCLEI</topic><topic>OXIDES</topic><topic>OXYGEN 17</topic><topic>OXYGEN COMPOUNDS</topic><topic>OXYGEN ISOTOPES</topic><topic>PERTURBATION THEORY</topic><topic>PHYSICAL PROPERTIES</topic><topic>Physics</topic><topic>STABLE ISOTOPES</topic><topic>TRIPLETS</topic><topic>WAVE FUNCTIONS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>FELLER, D</creatorcontrib><creatorcontrib>GLENDENING, E. D</creatorcontrib><creatorcontrib>MCCULLOUGH, E. A</creatorcontrib><creatorcontrib>MILLER, R. J</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>The Journal of chemical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>FELLER, D</au><au>GLENDENING, E. D</au><au>MCCULLOUGH, E. A</au><au>MILLER, R. J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A comparison of unrestricted Hartree-Fock- and restricted open-shell Hartree-Fock-based methods for determining the magnetic hyperfine parameters of NO (X2Π)</atitle><jtitle>The Journal of chemical physics</jtitle><date>1993-08-15</date><risdate>1993</risdate><volume>99</volume><issue>4</issue><spage>2829</spage><epage>2840</epage><pages>2829-2840</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><coden>JCPSA6</coden><abstract>The magnetic hyperfine structure parameters of NO X 2Π have been determined through a variety of ab initio methods based on restricted and unrestricted Hartree–Fock zeroth order wave functions. Examples of the former include singles configuration interaction (CI), multireference CI, and averaged coupled pair functional theory. Examples of the latter include Mo/ller–Plesset perturbation theory (through fifth order, with estimates to infinite order), coupled cluster methods, and quadratic CI (with approximate inclusion of triple and quadruple excitations). The performance of the various methods in reproducing the difficult-to-describe 14N and 17O isotropic hyperfine interactions is judged in light of both experimental data, where available, and estimated full CI values. The full CI limit was approached through a systematic sequence of ever-more-extensive, selected multireference CI wave functions that would, in principle, include the full CI as its final element. While the isotropic coupling constants were found to converge very slowly along this sequence, at least in comparison to other one-electron properties, the selected CI approach was efficient enough in its recovery of correlation effects to be used with large basis sets. The biggest calculation in the sequence of CI wave functions included over two million configurations. Energies and properties exhibited sufficient regularity to allow fitting with simple functional forms. The error arising from the lack of basis set completeness is estimated by comparison to fully numerical, partial-wave self-consistent field (SCF) and singles CI results. Effects due to vibrational motion are accounted for by numerical integration of the one-dimensional Schrödinger equation.</abstract><cop>Woodbury, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.465192</doi><tpages>12</tpages></addata></record> |
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subjects | 664100 - Theory of Electronic Structure of Atoms & Molecules- (1992-) ATOMIC AND MOLECULAR PHYSICS CALCULATION METHODS CHALCOGENIDES COMPARATIVE EVALUATIONS CONFIGURATION INTERACTION CORRELATIONS ELECTRON CORRELATION Electron correlation calculations for atoms and molecules Electronic structure of atoms, molecules and their ions: theory EVALUATION EVEN-ODD NUCLEI Exact sciences and technology FUNCTIONALS FUNCTIONS HARTREE-FOCK METHOD HYPERFINE STRUCTURE ISOTOPES LIGHT NUCLEI MAGNETIC PROPERTIES MULTIPLETS NITRIC OXIDE NITROGEN 14 NITROGEN COMPOUNDS NITROGEN ISOTOPES NITROGEN OXIDES NUCLEI ODD-ODD NUCLEI OXIDES OXYGEN 17 OXYGEN COMPOUNDS OXYGEN ISOTOPES PERTURBATION THEORY PHYSICAL PROPERTIES Physics STABLE ISOTOPES TRIPLETS WAVE FUNCTIONS |
title | A comparison of unrestricted Hartree-Fock- and restricted open-shell Hartree-Fock-based methods for determining the magnetic hyperfine parameters of NO (X2Π) |
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