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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 7489-7498 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Full three-dimensional quantum variational calculations have been carried out using model potentials to investigate the effect of barrier height to linearity on bending vibrational levels for zero total angular momentum states (J=0) in a bent symmetric triatomic molecule AB2. Contrary to the results of a previous study of one-dimensional bending vibration only, the precise spectral pattern is found to depend on not only the height of the potential barrier, but also detailed features of the potential energy surface and various coupling terms in the kinetic energy operator. The results for some real bent triatomic molecules are analyzed and compared with the results for model potentials. Both results indicate that there is no simple formula to compute the barrier height from the analysis of the spectral pattern of the molecule. A possible explanation is presented with the focus on mode mixing in high vibrational states and it is well manifested by the isotopic substitution of hydrogen (1H) with deuterium (2H) atom in an AH2 type molecule.
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  • 2
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 59 (1991), S. 1767-1769 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A low-energy ion-beam-assisted deposition (IBAD) technique has been developed to fabricate W-Si-N Schottky contacts of enhanced thermal stabilities on n-GaAs. By implementing remote sputtering and glancing angle low-energy N+ ion irradiation, the thermal stabilities of the W-Si-N/n-GaAs Schottky contacts were enhanced to be stable up to 850 °C, while keeping the Schottky barrier heights to the best values obtained with conventional sputtering. Thermal stabilities of the IBAD refractory metals/n-GaAs interfaces were investigated also for various W-Si-N compositions by examining the microstructure and Schottky diode characteristics. WSi0.3N0.4 showed the most stable Schottky contacts on n-GaAs of which the barrier height changed only 20 meV after thermal annealing between 700 and 850 °C, and that is proposed to be due to the stable metallurgical microstructure compared to the element tungsten and tungsten nitride.
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 92 (1988), S. 1821-1830 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 106 (1997), S. 4022-4027 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A systematic ab initio investigation has been carried out to examine the effects of a basis set and correlation method on barrier height to linearity of bent triatomic CH2 and H2O in their ground electronic states. The theoretical models employed varied from Hartree–Fock with minimal STO-3G to highly correlated quadratic configuration interaction method QCISD(T) with Dunning's correlation-consistent aug-cc-pVQZ basis set. It is shown that the barrier height to linearity is very sensitive to the choice of the model and it is necessary to employ a proper theoretical model with large enough basis set to be assured of the convergence of the calculated barrier height. We found that calculated barrier height to linearity tends to be higher than experimentally determined barrier height in most cases, which is caused by the slower convergence of energy at linear saddle point geometry than at bent equilibrium geometry. The effect of frozen core approximation in correlated calculations is shown to always increase the barrier height to linearity slightly (less than 3% of total amount) from the value with the full activation of orbitals, regardless of the basis set or correlation method used in the study. © 1997 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 112 (2000), S. 230-237 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The equilibrium and saddle point structures of the ammonia dimer were investigated employing a series of correlation-consistent basis sets, cc-pVXZ and aug-cc-pVXZ(X=D,T,Q) at the Hartree–Fock (HF), second order and fourth order Møller–Plesset perturbation theory (MP2, MP4) levels. It is shown that the energies and geometries of the stationary structures are sensitive to the basis set and electron correlation, and the proper combination of electron correlation treatment (MP2 or better) and basis set requirement (aug-cc-pVTZ or better) is necessary to determine the equilibrium structure and ordering of the stationary structures. The equilibrium structure of the ammonia dimer is found to be an asymmetric cyclic (eclipsed) structure with Cs symmetry. Although this is generally consistent with the equilibrium structure predicted from the model potential by Olthof et al. [J. Chem. Phys. 101, 8430 (1994)], it appears to be more shifted toward the linear structure than the centrosymmetric cyclic structure, which signifies a certain degree of hydrogen bonding in this dimer. The MP2 barrier height to proton donor–acceptor interchange at MP2/aug-cc-pVQZ//MP2/aug-cc-pVTZ is 7.6 cm−1, which is in excellent agreement with the value predicted from the model potential by Olthof et al. While the barrier height to rotation of one monomer (hydrogen-bond acceptor) about its C3 axis is relatively low, ∼20 cm−1, the corresponding value of the other monomer (hydrogen-bond donor) is shown to be rather high, probably more than 450 cm−1 at the equilibrium structure. The binding energies of the ammonia dimer are computed with and without counterpoise correction for basis set superposition error. The MP2 complete basis set (CBS) limit electronic binding energy of (NH3)2 is estimated to be within 13.2±0.3 kJ/mol. © 2000 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 112 (2000), S. 10746-10753 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The convergence behavior of the total and correlation energies of He, H2, and He2 with the increase of basis quality in the correlation-consistent basis sets, cc-pVXZ and aug-cc-pVXZ(X=D,T,Q,5,6), was studied to search for a proper extrapolation scheme to predict the accurate complete basis set (CBS) limits at the MP2, CCSD, and CCSD(T) level. The functional form employed for extrapolation is a simple polynomial including inverse cubic power and higher-order terms of the cardinal number X in the correlation-consistent basis set as well as exponential function. It is found that a simple extrapolation of two successive correlation-consistent basis set energies (total or correlation energies) using (X+k)−3 [k=0 for MP2 and k=−1 for CCSD and CCSD(T) level] gives in general the most reliable (and accurate in case of total energy) estimates to the CBS limit energies. It is also shown that the choice of proper basis set, which can represent the electronic motions in the fragment and complex equally well, appears necessary for reliable estimate of the relative energies such as the binding energy of the complex. From the extrapolation of aug-cc-pV5Z and aug-cc-pV6Z energies with (X+k)−3, we obtained 21.3(21.4), 28.4(29.0) and 33.2(33.8) microhartrees as the CBS limit binding energy of He2 at the internuclear separation of 5.6 a.u. at the MP2, CCSD, and CCSD(T) level, respectively, with the values in parentheses representing the exact CBS limit binding energies. © 2000 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 110 (1999), S. 4413-4418 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An ab initio investigation employing highly correlated electronic methods and large basis sets has been carried out to determine the equilibrium geometries and binding energies of He2H+ and Ne2H+. The theoretical methods employed include the Moller–Plesset Perturbation Theory (MP2, MP4), and coupled cluster with single and double substitution with noniterative triple excitation [CCSD(T)] ab initio methods with two different type of basis sets, the segmented contracted 6-311++G basis sets with multiple polarization functions, and the correlation consistent aug-cc-pVxZ (x=D,T,Q,5) basis sets. It is found that both species have in common linear symmetric XHX+ equilibrium geometries with dissociation energies of more than 4000 cm−1 to X+XH+ (X=He, Ne). A convergence study comparing the uncorrected and counterpoise (CP) corrected dissociation energies with respect to the complete basis set (CBS) limiting values shows that the CP method generally yields less accurate dissociation energies than the uncorrected ones in both ionic species; a possible explanation is given in terms of differences in geometries between the dissociated and complex state. The dissociation energies for He2H+ to He+HeH+ at MP4/aug-cc-pV5Z and CCSD(T)/aug-cc-pV5Z levels are, in cm−1, 4622.2(4621.7) and 4631.1(4631.7), respectively, with the values in parentheses representing the dissociation energies at the CBS limit. The corresponding dissociation energies for Ne2H+ at MP4/aug-cc-pVQZ and CCSD(T)/aug-cc-pVQZ levels are 5846.9(5746.3) and 5807.1(5703.9), though the estimated CBS limit in this case is less reliable than in the case of He2H+. © 1999 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 116 (2002), S. 5389-5394 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The basis set limit electronic binding energies of He2, (HF)2, and (H2O)2 at the MP2 and CCSD(T) level (coupled cluster single and double excitations with perturbative triples correction) were estimated through the extrapolation of two successive energies of the dimer with correlation-consistent aug-cc-pVXZ (X=D(2),T(3),Q(4),5,6) basis sets by 1/Xp, where the convergence power p was derived from the basis set convergence behavior of the monomer (He, HF, and H2O) energies toward the known corresponding basis set limits. It is shown that the convergence behaviors of the correlation energy of the monomer and dimer with correlation-consistent basis sets closely resemble each other in these weakly bound systems, which is well demonstrated by the excellent agreement of the estimated basis set limit binding energies on this premise with the reference values in all cases. By contrast, the accuracy of a simple two-point 1/X3 extrapolation scheme in estimating the binding energies of these complexes is shown to depend on the correlation level, basis set quality, and kind of interatomic or molecular interactions present in the system. For the extrapolation of correlation energies of the dimer with aug-cc-pVDZ and aug-cc-pVTZ basis set by 1/Xp with the convergence power p determined from the basis set convergence behavior of the monomer correlation energies, the estimated MP2 binding energies for He2, (HF)2, and (H2O)2 are 19.5 μEh(21.4), 7.00 mEh(7.04), and 7.79 mEh(7.82), with the values in parentheses representing the exact basis set limit binding energies. The corresponding CCSD(T) binding energies for He2, (HF)2, and (H2O)2 are 30.8 μEh(33.8), 7.19 mEh(7.21), and 7.86 mEh(7.88), respectively. © 2002 American Institute of Physics.
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  • 9
    Publication Date: 2010-07-22
    Print ISSN: 1089-5639
    Electronic ISSN: 1520-5215
    Topics: Chemistry and Pharmacology , Physics
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  • 10
    Publication Date: 2005-12-01
    Print ISSN: 1089-5639
    Electronic ISSN: 1520-5215
    Topics: Chemistry and Pharmacology , Physics
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