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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 570-578 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Theoretical calculations are presented for the polarizability parameters through the fourth power of an applied static electric field for Ne and HF and through the second power in the field for the negative ions F− and OH−. Large Gaussian basis sets are employed and electron correlation is incorporated using the modified coupled pair functional (MCPF) method and for Ne and HF using coupled-cluster single- and double-excitation (CCSD) methods with two approaches of including the effect of triple excitations. The MCPF method is found to perform well in relation to the more rigorous CCSD method. Our theoretical values for Ne are in good accord with the recent experimental value of Shelton, as well as with recent theoretical studies. Our best results for the first and second hyperpolarizability of HF are in slightly better agreement with experiment than previous theoretical studies, but still show a very large disparity.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 89 (1988), S. 2985-2992 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The nitrogen atom isotropic hyperfine coupling constant Aiso is studied as a function of improvements in both the one-particle and n-particle basis sets. Our study underscores the importance of diffuse basis functions. For example, the (9s 5p) primitive set of Huzinaga augmented with an even-tempered diffuse s function yields values for Aiso that are virtually identical to an energy-optimized (23s 12p) even-tempered set. The Aiso constant is found to converge relatively quickly with increasing l quantum numbers: d, f, and g functions are estimated to contribute 2.5±0.2, 0.4±0.1, and 0.05±0.05 MHz, respectively. Full CI calibration calculations indicate that very high levels of correlation treatment are required for quantitative results. In addition, a strong coupling is observed between the one-particle and n-particle requirements. Our best result of 10.4 MHz is in excellent agreement with the accurate experimental value of 10.4509 MHz.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 3700-3706 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The magnetic hyperfine parameters of 17OH are studied as a function of the one- and n-particle spaces. All of the parameters, except the spin density on oxygen, bF(O), are well described by modest levels of theory. Thus, we have directed much of our effort to understanding the computational requirements for accurately determining bF(O). Full configuration-interaction (FCI) calculations in six Gaussian basis sets give unambiguous results for the effect of uncontracting the oxygen s and p basis sets, of adding diffuse s and p functions, and of adding polarization functions to oxygen. FCI calculations in a [6s 2p 1d/2s] contracted basis give a bF(O) value that is in good agreement with experiment. A critical factor in any n-particle treatment is a balanced treatment of core and valence correlation. The size-extensive modified coupled-pair functional method provides bF values in reasonably good agreement with the FCI. Methods that account quantitatively for the valence correlation, such as complete-active-space self-consistent-field/multireference configuration interaction, appear to introduce an imbalance between core and valence contributions to bF when the one-particle basis sets are flexibly contracted in the core.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 1352-1357 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using the demon density functional program, 104 points on the potential-energy surface for the ground electronic state of the HNSi molecule were calculated. An analytic function was fitted through these points and used in two different computer programs (called Morse oscillator–rigid bender internal dynamics and triatom) to calculate the vibration–rotational energies of the HNSi and DNSi molecules. Other analytic functions were fitted through the calculated dipole-moment data to compute the vibrational transition moments and the vibrationally averaged dipole moments. The computed fundamentals ν1, ν2, and ν3 for HNSi from the triatom program are 3466, 413, and 1172 cm−1, respectively, in reasonable agreement with the observed values of 3588, 523, and 1198 cm−1. Agreement is similar for the Morse oscillator–rigid bender internal dynamics program as well as for DNSi.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 8870-8876 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using the deMon density functional program, we calculated 150 points on the potential-energy surface for the ground electronic state (X˜ 1Σ+) of the HCP molecule. An analytical function was fitted through these points and used in two different computer programs (called triatom and dvr) to calculate the vibration-rotational energies of the HCP and DCP molecules. The computed vibrational fundamentals of ν1, ν2, and ν3 for HCP (DCP) are 3134 (2365), 654 (509), and 1269 (1227) cm−1, respectively, in good agreement with the observed values of 3217 (2419), 675 (525), and 1278 (1231) cm−1. The calculated vibrational energies of HCP show a pronounced regularity, in accordance with the observed harmonic-vibrational characteristic of the molecule concerned. The average energy deviation of the computed vibration-rotational energies of HCP up to 8200 cm−1 from the 58 corresponding observations is 90±32 cm−1, thus demonstrating the deMon potential-energy function to be of good quality.
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 4753-4765 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: This paper presents a comparison between density functional theory local density approximation (LDA) and Hartree–Fock approximation (HFA) calculations of dipole moments, polarizabilities, and first hyperpolarizabilities, using "comparable'' basis sets, in order to assess the relative quality of the LDA and the HFA for calculating these properties. Specifically, calculations were done using basis sets of roughly double or triple zeta plus polarization quality, with and without added field-induced polarization (FIP) functions, for the seven small molecules H2, N2, CO, CH4, NH3, H2O, and HF, using the HFA option in the program HONDO8 and the LDA options in the programs DMol and deMon. For the calculations without FIP functions, the results from HONDO8 HFA and deMon LDA, both of which use Gaussian basis sets, are very similar, while DMol, which uses a LDA numerical atomic orbital basis set, gives substantially better results. Adding FIP functions does much to alleviate these observed basis set artifacts and improves agreement with experiment. With FIP functions, the results from the two sets of LDA calculations (deMon and DMol) are very similar to each other, but differ markedly from the HFA results, and the LDA results are in significantly better agreement with experiment. This is particularly true for the hyperpolarizabilities. This appears to be the first detailed study of DFT calculations of molecular first hyperpolarizabilities. We note that closer attention to numerical details of the finite field calculation of β(two down arrows) is necessary than would usually be the case with traditional ab initio methods. A proof that the Hellmann–Feynman theorem holds for Kohn–Sham calculations is included in the Appendix.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 103 (1995), S. 1842-1845 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The unrestricted generalized transition-state model using B88/P86 functional with Dunning's cc-pV5Z basis set, found to be an excellent method of calculating core-electron binding energies (CEBEs), was further applied to many more molecules, some of which contain atoms from the third period. Estimation of relativistic corrections has also been refined. The average absolute deviation of over 50 calculated CEBEs from experiment is 0.30 eV before inclusion of approximate relativistic corrections (Crel), and 0.23 eV after adding Crel. Those molecules with observed CEBEs served to confirm our procedure, whereas the other cases provided our prediction of CEBEs. © 1995 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 102 (1995), S. 3312-3321 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Density functional theory (DFT) is a field enjoying a tremendous recent surge in popularity among theoretical and practical chemists alike because of its ability to more easily handle larger molecular systems than conventional ab initio methods. Until recently, however, assessment of the quality of the properties predicted (and therefore the charge density) from DFT had been limited mainly to dipole moments and their nuclear coordinate and electric field derivatives. This paper presents the calculated results for some of the one-electron properties of the eight small molecules (NH3, PH3, H2O, H2S, HF, HCl, CO, and N2). The properties chosen weight different regions of the charge density, from either very close in or at the nucleus (e.g., δ, the electron density at the nucleus) to regions farther out from the nucleus (e.g., the diamagnetic susceptibility 〈r2〉). It is found that properties which depend on an accurate knowledge of the electron density near to the nucleus are predicted poorly by the local density approximation (LDA), while others more dependent on the charge density farther out from the nucleus are predicted much more accurately, possibly due to cancellation of errors. Use of the LDA is therefore not recommended for "tight'' properties; use of a functional employing gradient corrections would be more suitable for this purpose. © 1995 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 15387-15395 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 68 (1964), S. 1793-1797 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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