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  • 101
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    The Journal of Chemical Physics 117 (2002), S. 3848-3855 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The multimode Brownian oscillator (MBO) model with Ohmic dissipation has frequently been used to interpret photon echo and spectral data on solvation dynamics of chromophores in liquids at room temperature. We report on the applicability of this model to high-resolution linear electronic absorption spectra of chromophores in solid hosts at low temperatures, where the zero-phonon line (ZPL) is resolved from phonon sideband structure. The results are also relevant to frequency and time domain nonlinear spectra. In the MBO model, active BOs (phonons) are linearly coupled to bath modes. This coupling endows the bath modes with absorption intensity which, with Ohmic dissipation (white light spectrum for the bath modes), results in the bath modes contributing to absorption in the region of the ZPL. Experimental results for a multitude of molecular systems indicate that the ZPL profile is determined by electronic dephasing, which is not accounted for in the MBO model. Thus, it is important to assess the contribution of the MBO bath modes to the ZPL profile. To this end, closed-form, finite temperature expressions for the underdamped MBO (UMBO) model are derived for the linear response function, linear absorption spectrum, and width and Franck–Condon factor of the ZPL. It is proven formally that the UMBO ZPL width is zero at T=0 K. Results of calculations for model systems whose parameter values (BO damping constant, frequency and Huang–Rhys factor) are typical of real systems are presented. It is concluded that Ohmic dissipation leads to unphysically large ZPL widths as well as asymmetric ZPL profiles that appear not to have been observed. Moreover, the ZPL width adds to those of the multi-BO (phonon) transitions. Thus, use of the UMBO model with Ohmic dissipation to interpret data on relaxation dynamics of nuclear modes may result in erroneous conclusions. It is shown that Franck–Condon factors of the ZPL obtained with the UMBO model can differ significantly from those calculated with the conventional formula. © 2002 American Institute of Physics.
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  • 102
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    The Journal of Chemical Physics 117 (2002), S. 3856-3873 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Molecular dynamics simulation is used to study the relaxation of the polarizability anisotropy in liquid ethanol at temperatures of 298 and 348 K. Ethanol molecules are represented by a four-site semi-flexible model in which the internal degree of freedom, corresponding to the torsional motion around the C–O bond, is taken into consideration. The molecular polarizability is calculated using an interaction-site model, based on the modified dipole-induced dipole model developed by Thole. The collective polarizability induced by intermolecular interactions is included using first-order perturbation theory and calculated considering both center–center and site–site models. Results are analyzed in terms of projected variables that allow the decomposition of the total relaxation into orientational and collision-induced components, both of which are influenced by molecular flexibility. We compare our data with the results of low-frequency depolarized Rayleigh light scattering experiments, examining the possibility of separating different relaxation processes from spectroscopic signals in the time and frequency domains. We find that even though the largest contributor to polarizability anisotropy dynamics is orientational relaxation, collision-induced contributions are important, especially at shorter times. Moreover, we show that torsional motion also plays a significant role in the fast decay of the polarizability anisotropy of the system. Although liquid ethanol is strongly associated and its dipolar relaxation is highly collective, we find orientational pair correlation effects on polarizability relaxation to be negligible. A comparison with simulation data previously obtained for methanol suggests that increasing the alcohol chain length decreases the relative importance of OH dynamics in polarizability relaxation. We further show that, as expected for such a structured liquid composed of strongly asymmetric molecules, polarizability and dipole relaxation processes exhibit marked differences. © 2002 American Institute of Physics.
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  • 103
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    The Journal of Chemical Physics 116 (2002), S. 3410-3419 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The crystal-melt interfaces of a binary hard-sphere fluid mixture in coexistence with a single-component hard-sphere crystal is investigated using molecular-dynamics simulation. In the system under study, the fluid phase consists of a two-component mixture of hard spheres of differing size, with a size ratio α=0.414. At low pressures this fluid coexists with a pure fcc crystal of the larger particles in which the small particles are immiscible. For two interfacial orientations, [100] and [111], the structure and dynamics within the interfacial region is studied and compared with previous simulations on single component hard-sphere interfaces. Among a variety of novel properties, it is observed that as the interface is traversed from fluid to crystal the diffusion constant of the larger particle vanishes before that of the small particle, defining a region of the interface where the large particles are frozen in their crystal lattice, but the small particles exhibit significant mobility. This behavior was not seen in previous binary hard-sphere interface simulations with less asymmetric diameters. © 2002 American Institute of Physics.
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  • 104
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    The Journal of Chemical Physics 116 (2002), S. 3430-3448 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A computationally efficient method was developed for calculating Coulomb interactions in three-dimensional (3D) systems with two-dimensional (2D) periodicity; the 2D particle-mesh Ewald (2D-PME) method we previously developed was extended. The formulation and numerical algorithms are described in detail for calculating the Coulomb potential energy, the Coulomb force, and the Coulomb component of the pressure tensor. Computational efficiency and accuracy of the 2D-PME method were evaluated for two water systems with 2D periodicity in the x and y directions and with non-periodicity in the z direction. Compared with exact results calculated by using the original 2D Ewald summations, the 2D-PME method yielded significantly accurate calculations, similar to the computationally efficient method we previously developed for calculating 2D Ewald summations (2D-EW method). For a given accuracy, the 2D-PME method was faster than the 2D-EW method for the water systems we examined. The computational effort of the 2D-PME method decreases as the computationally efficiency of the Fourier transforms used in the 2D-PME method increases. The 2D-PME method is therefore promising for accelerating molecular dynamics and Monte Carlo simulations for 3D systems with 2D periodicity. © 2002 American Institute of Physics.
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  • 105
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    The Journal of Chemical Physics 116 (2002), S. 3484-3492 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We investigate vapor–liquid equilibria of dendrimer/solvent (benzyl ether dendrimer/toluene) systems by the combination of incompressible lattice cluster theory and atomistic simulation technique. We also examine the structure effect of dendritic polymer and the specific interaction due to the difference of interaction energies of endgroup at the periphery of dendrimer molecules. The interaction energy parameters are obtained by the pairs method including Monte Carlo simulation technique with excluded volume constraint. In the pairs method, we do not simulate the whole molecule as in molecular dynamics or molecular mechanics, but only monomer segments interacting with solvent molecules. In general, those parameters are determined by fitting experimental data. Our results show that the specific interactions between the endgroup and the solvent molecule play an important role in determining phase behaviors of the given systems. © 2002 American Institute of Physics.
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  • 106
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    The Journal of Chemical Physics 116 (2002), S. 3493-3501 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The hypernetted-chain integral equations are solved on a three-dimensional cubic grid to calculate the spatial distribution of the depletion potential between a big solute of arbitrary geometry and a big sphere immersed in small spheres forming the solvent. By analyzing the potential along a specific trajectory of the big sphere, effects due to the geometric feature of the big solute (step edges, trenches, corners, changing curvature, etc.) can be examined in detail. As an illustration, effects of the step edge on the lateral depletion potential along a wall surface are analyzed. Along the trajectory considered, the big sphere moves at constant height, starting on the center of the wall surface and moving horizontally past the edge. The big sphere is repelled from the edge into the wall surface, and to escape to the bulk it must overcome a significantly high free-energy barrier. As another illustration, simple model calculations are performed for the lock and key steric interaction between macromolecules. The potential at contact (i.e., the stabilization free energy) for the key that exactly fits the lock is far larger than for smaller and larger keys and considerably in excess of the value predicted by the Asakura–Oosawa theory. © 2002 American Institute of Physics.
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  • 107
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    The Journal of Chemical Physics 116 (2002), S. 2675-2679 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The reaction of ground-state atomic oxygen (O(3P)) with allyl radical (C3H5) was investigated in the crossed beam configuration. O(3P) and C3H5 were generated by the photodissociation of NO2 and the supersonic flash pyrolysis of allyl iodide, respectively. The nascent internal distributions of the OH(X2Π : v″=0,1) reaction product from the newly observed channel of O(3P)+C3H5→C3H4+OH were probed by laser induced fluorescence (LIF) spectroscopy. The distributions showed significant excitations with an unusual bimodal feature: the low and high rotational components without spin-orbit and Λ-doublet propensities in the ground and first excited vibrational states. On the basis of population analysis and comparison with the ab initio and statistical calculations, the experimental distributions are estimated to be totally non-statistical and suggest that the dynamics of the reaction might be described by two competing mechanisms: a major direct abstraction process and an indirect short-lived addition-complex forming process. © 2002 American Institute of Physics.
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  • 108
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    The Journal of Chemical Physics 116 (2002), S. 2705-2717 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Fourth-order quantum master equations (FQMEs) are derived in both time nonlocal and local forms for a general system Hamiltonian, with new detailed expressions for the fourth-order kernel, where the bath correlation functions are explicitly decoupled from the system superoperators. Further simplifications can be made for the model of linearly coupled harmonic oscillator bath. Consideration of the high temperature Ohmic bath limit leads to a general Markovian FQME with compact forms of time independent superoperators. Two examples of this equation are then considered. For the system of a quantum particle in a continuous potential field, the equation reduces to a known form of the quantum Fokker–Planck equation, except for a fourth-order potential renormalization term that can be neglected only in the weak system-bath interaction regime. For a two-level system with off-diagonal coupling to the bath, fourth-order corrections do not alter the relaxation characteristics of the second-order equation and introduce additional coherence terms in the equations for the off-diagonal elements. © 2002 American Institute of Physics.
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  • 109
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    The Journal of Chemical Physics 116 (2002), S. 2757-2762 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Kinetic properties of the single rotational states 2≤N≤8 of the electronically excited CH(A2Δ,v=0) radical have been studied in the gas phase at room temperature in the presence of CO. Rate constants of the state-to-state relaxation are presented. Further, rate constants were determined for the electronic quenching of single N states and compared with data recently reported by Cerezo and Martin [J. Photochem. Photobiol., A 134, 127 (2000)]. The radiative lifetimes of the rotational levels are given, too. © 2002 American Institute of Physics.
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  • 110
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    The Journal of Chemical Physics 116 (2002), S. 2728-2747 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Accurate estimates of the magnetic coupling in binuclear complexes can be obtained from ab initio configuration interaction (CI) calculations using the difference dedicated CI technique. The present paper shows that the same technique also provides a way to analyze the various physical contributions to the coupling and performs numerical analysis of their respective roles on four binuclear complexes of Cu (d9) ions. The bare valence-only description (including direct and kinetic exchange) does not result in meaningful values. The spin-polarization phenomenon cannot be neglected, its sign and amplitude depend on the system. The two leading dynamical correlation effects have an antiferromagnetic character. The first one goes through the dynamical polarization of the environment in the ionic valence bond forms (i.e., the M+(centered ellipsis)M− structures). The second one is due to the double excitations involving simultaneously single excitations between the bridging ligand and the magnetic orbitals and single excitations of the environment. This dispersive effect results in an increase of the effective hopping integral between the magnetic orbitals. Moreover, it is demonstrated to be responsible for the previously observed larger metal-ligand delocalization occurring in natural orbitals with respect to the Hartree–Fock ones. © 2002 American Institute of Physics.
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  • 111
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    The Journal of Chemical Physics 116 (2002), S. 2794-2802 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Minimal Electron Nuclear Dynamics theory is applied to D2+NH3+ reaction at collision energies from 6 to 16 eV in the center-of-mass frame. This method for direct nonadiabatic dynamics describes the electrons with a family of complex determinantal wave functions in terms of nonorthogonal spin orbitals and treats the nuclei as classical particles. There are no geometrical constraints imposed on this six-atom system. Emphasis is put on the details of the abstraction and exchange reaction mechanisms for ground-state reactants. Comparisons are made to recent molecular-beam experiments. © 2002 American Institute of Physics.
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  • 112
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: When the spin–orbit interaction is included, the character of a conical intersection in a molecule with an odd number of electrons differs dramatically from that of its nonrelativistic counterpart. In contrast to the two-dimensional branching space (η=2) in the nonrelativistic case, for these conical intersections the branching space is five-dimensional (η=5) in general, or three-dimensional (η=3) when Cs symmetry is present. Recently we have introduced an algorithm, based on analytic gradient techniques, to locate such conical intersections and used related techniques to efficiently construct and study the properties of the vectors defining the branching space. Here we extend this analysis. A perturbative description of the η=3 case is reported and used to determine the energy, derivative couplings, and a "rigorous" diabatic basis in the vicinity of a conical intersection. The perturbative results are compared with those of exact numerical calculations employing model Hamiltonians. The implications for the nuclear motion problem are discussed. © 2002 American Institute of Physics.
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  • 113
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    The Journal of Chemical Physics 116 (2002), S. 2863-2869 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Accurate quantum mechanical results for the thermal rate constant of the prototypical six atom reaction, CH4+H→CH3+H2, are reported in this article. Previous k(T) results for temperature values below 500 K are extended up to 1000 K. This is achieved employing a combined iterative diagonalization and statistical sampling approach for the evaluation of the flux correlation function. The accurate reaction rate data obtained for the extended temperature range is used to test several approximations related to the transition state theory. The study especially focuses on the contribution of vibrationally excited states of the activated complex to the thermal rate constant. © 2002 American Institute of Physics.
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  • 114
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    The Journal of Chemical Physics 116 (2002), S. 2870-2878 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rotationally resolved spectra of h2- and d1-formic acid embedded in liquid helium droplets have been recorded in the spectral region of the O–H (ν1) and C–H (ν2) stretch vibrations. Accidental resonant mixing between the ν1-band of h2-formic acid and the combination bands (ν2+ν7) and (ν2+ν9) has been observed. The fundamental ν1 band can interact via Fermi resonance with the (ν2+ν7), and the (ν2+ν7) via Coriolis coupling with the (ν2+ν9) band. Examination of the resonance induced line-broadening effects suggests that the helium environment modifies vibrational relaxation dynamics. The 2ν3 C(Double Bond)O stretch overtone is also observed and was assigned by a density functional theory (DFT) ab initio calculation. The spectroscopic constants are determined by fitting all spectra with a standard gas phase Hamiltonian. © 2002 American Institute of Physics.
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  • 115
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    The Journal of Chemical Physics 116 (2002), S. 2907-2921 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A recently developed microscopic model for associating fluids that accurately captures the thermodynamics of liquid water [Truskett et al., J. Chem. Phys. 111, 2647 (1999)] is extended to aqueous solutions with nonpolar species. The underlying association model incorporates the highly directional and open nature of water's hydrogen-bond network, and, as a result, captures a number of the distinguishing properties of liquid water, such as the density anomaly. The model for aqueous mixtures developed herein predicts many of the thermodynamic signatures of hydrophobic hydration without resorting to empirical temperature-dependent parameters. The predicted solubility of nonpolar species is slight over a wide range of temperatures, and exhibits a minimum as a function of temperature, in accord with experiment. Hydration is opposed by a dominant entropy and favored by the enthalpy at low temperatures. At elevated temperatures these roles are reversed. Furthermore, the hydration entropies for hydrophobes of varying size converge over a very narrow temperature range. Comparison with experimental and simulation data for nonpolar solutes in water shows that the theory tends to exaggerate the solute's transfer heat capacity at low temperature, and hence solubility minima and entropy convergence are predicted to occur at lower temperatures than observed. Our results support the emerging view that hydrophobic effects can be attributed in large part to the equation of state for pure water. © 2002 American Institute of Physics.
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  • 116
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    The Journal of Chemical Physics 116 (2002), S. 2983-2990 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using computer simulations, we have investigated the kinetics of a two-dimensional, two-component fluid mixture on a lattice in the presence of a field which drives the different species in opposite directions. A kinetic instability arises when the field strength and fluid density are sufficiently large. The nonuniform state which emerges has zero flux and consists of layers of particles, essentially close-packed and perpendicular to the field direction. The layers each contain particles of essentially a single species, but the layer composition alternates between the different species with periodicity depending on the fluid density and the field strength. A mean-field analysis suggests this is a first-order dynamic phase transition, which is consistent with the computer simulations. © 2002 American Institute of Physics.
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  • 117
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    The Journal of Chemical Physics 116 (2002), S. 2991-2996 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The structure of solutions of lithium in ammonia has been studied at 0, 2, 8, and 22 mol % metal (MPM) and 200 K by wide-angle x-ray diffraction. The principal diffraction peak shifts from 2.14(2) Å−1 at 0 MPM to 1.93(3) Å−1 at 22 MPM, reflecting the 30% decrease in overall density as the solution expands to accommodate the excess electrons. We find that the solvent is significantly perturbed over both the short- and intermediate-length scales. The nearest neighbor (N–N) coordination number decreases from 11.8(10) at 0 MPM to 7.6(10) at 22 MPM. In addition, electrostriction around the fourfold coordinated lithium ions causes N–N correlations to become progressively shorter as concentration is increased. At 22 MPM a strong diffraction prepeak is located at 1.05(3) Å−1. Upon dilution to 2 MPM, our experiments find that this feature shifts to 1.29(5) Å−1. We conclude that the prepeak observed in our experiments is a signature of polaronic solvent cavities of approximate radius 2.6 Å. The first solvation shell of an excess electron then contains about 7 ammonia molecules, the second shell about 30 ammonia molecules. This picture is in excellent agreement with interpretation of magnetic resonance data. © 2002 American Institute of Physics.
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  • 118
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    The Journal of Chemical Physics 116 (2002), S. 2967-2972 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Monte Carlo simulations have been conducted to investigate the phase behavior of 2:1 hard-core electrolyte models. Two distinct cases have been considered: In the first, both bivalent cations and monovalent anions are spherical. In the second, bivalent cations are modeled as rigid dimers composed of two tangent hard spheres, each carrying a positive charge at the center. Critical temperatures and densities have been calculated as a function of the size asymmetry between positive and negative ions. The simulated critical temperature and critical density are strongly influenced by size asymmetry and by the shape of the ions. Changes in the critical constants are traced back to ground-state energy configurations of small ionic clusters. The trends observed in simulations for the critical temperature and density as a function of size asymmetry are shown to contradict the predictions of available theoretical formalisms. © 2002 American Institute of Physics.
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  • 119
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    The Journal of Chemical Physics 116 (2002), S. 3027-3041 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Atomistic computer simulation models are used to interpret the results of recent high resolution transmission electron microscopy (HRTEM) experiments which have studied the filling of carbon nanotubes by liquid KI. In the HRTEM experiments, the liquid KI fills narrow width nanotubes to form low-dimensional crystallites which display specific distortions in comparison with the idealized bulk fragments. The atomistic origin of these distortions are discussed. Molecular dynamics simulations are then used to directly model the filling of these tubes and an understanding of the filling mechanisms is developed. The dependence of the filling structure on the pore radius and morphology of the carbon nanotube is discussed. Novel crystalline structures, often incorporating specific twisting, is observed for the smaller diameter nanotubes. The physical origins of the observed filling mechanisms are discussed. © 2002 American Institute of Physics.
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  • 120
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    The Journal of Chemical Physics 116 (2002), S. 2879-2887 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An ab initio adiabatic and diabatic study of the KH molecule is performed for all states below the ionic limit [i.e., K (4s, 4p, 5s, 3d, 5p, 4d, 6s, and 4f)+H(1s)] in 1Σ+ and 3Σ+ symmetries. Adiabatic results are also reported for 1Π, 3Π, 1Δ, and 3Δ symmetries. The ab initio calculations rely on pseudopotential, operatorial core valence correlation, and full valence CI approaches, combined to an efficient diabatization procedure. For the low-lying states, our vibrational level spacings and spectroscopic constants are in very good agreement with the available experimental data. Diabatic potentials and dipoles moments are analyzed, revealing the strong imprint of the ionic state in the 1Σ+ adiabatic states while improving the results. The undulations of the diabatic curves and of the triplet–singlet diabatic energy difference which we found positive, as in Hund's rule, are related to the Rydberg functions. As for LiH, the vibrational spacing of the A state is bracketed by our results with and without the improvement taking into account the diabatic representation. Experimental suggestions are also given. © 2002 American Institute of Physics.
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  • 121
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    The Journal of Chemical Physics 116 (2002), S. 2896-2906 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We present the photodissociation spectroscopy of the complexes of Mg+ with di- and tri-ethylamine in the spectral range of 230–440 nm. Mass spectrometry of the two parent complexes exhibits the persistent product Mg+ from nonreactive quenching throughout the whole wavelength range. As for the reactive channels, C3H7•-elimination products are dominant when the complexes are excited to 3Px,y. Furthermore, photoexcitation of Mg+–NH(C2H5)2 to 3Px,y yields a minor MgH-elimination fragment. On the other hand, photodissociation of Mg+–N(C2H5)3 produces charge-transfer fragments N+(C2H5)3 and (C2H5)2N+CH2. The action spectra of the two complexes consist of two pronounced peaks on the red and blue side of the Mg+ 3 2P←3 2S atomic transition. The calculated absorption spectra of the two complexes using the optimized structures of their ground states agree nicely with the observed action spectra. Photofragment branching fractions of the products are shown to be nearly independent of the photon energy for the 3Px,y excitation, indicating the importance of exit channel effects. A photoreaction mechanism is proposed for C3H7•-elimination, which entails Mg+ insertion into one C–N bond, followed by a nonadiabatic transition to the ground-state surface through a conical intersection. However, for the MgH-elimination channel in the photodissociation of Mg+–NH(C2H5)2, Mg+ rather inserts into the α-C–H bond. Finally, photoexcitation of Mg+–N(C2H5)3 leads to a prominent charge-transfer product [N+(C2H5)3]*, which dissociates further to (C2H5)2N+CH2 by a loss of CH3•. © 2002 American Institute of Physics.
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  • 122
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    The Journal of Chemical Physics 116 (2002), S. 2945-2954 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Computer simulations of bubble oscillations in aqueous methanol solution are performed under conditions of sonoluminescence (SL) in order to study the mechanism of SL quenching by methanol reported by Ashokkumar et al. [J. Phys. Chem. B 101, 10849 (1997); J. Phys. Chem. A 104, 8462 (2000)]. It is shown that methanol molecules evaporate into the bubble at the bubble expansion and almost all of them are dissociated inside a heated bubble at the collapse. The bubble temperature at the collapse decreases by the endothermal heat of the dissociation of methanol and by the increase of the molar heat of the gases inside a bubble, which results in the SL quenching. It is shown that SL from argon bubbles is more effectively quenched by methanol compared to SL from air bubbles. © 2002 American Institute of Physics.
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  • 123
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    The Journal of Chemical Physics 116 (2002), S. 2973-2982 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Acoustical absorption spectra between 10 kHz and 2 GHz are reported for various monosaccharides in water. With the exception of solutions of methyl-β-D-arabinopyranoside (0.5 mol/l) the spectra reveal absorption with relaxation characteristics in excess to the asymptotic high frequency absorption term. Up to three relaxation terms per spectrum emerge within the measuring frequency range. Regression analysis of the measured spectra in terms of a suitable analytical spectral function yields five relaxation regimes with relaxation times on the order of 1 μs, 100 ns, 10 ns, 1 ns, or 100 ps, respectively. These relaxation regimes are assigned to the chair–chair ring inversion, two modes of pseudorotation, an exocyclic side group isomerization and a molecular association mechanism. Particular emphasis is given to the ring inversion which is additionally verified by time resolved measurements of nonequilibrium tautomer systems, utilizing the coupling of the inversion to the carbohydrate mutarotation. Further evidence is derived from measurements of solutions of D-fructose in mixtures of ethanol and water. © 2002 American Institute of Physics.
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  • 124
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    The Journal of Chemical Physics 116 (2002), S. 3018-3026 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The electrical conductivity of molten salt has been theoretically investigated starting from the linear response theory in view of a microscopic point. The velocity correlation functions in molten salt are expressed in terms of pair potentials and pair distribution functions in detail. Using these functions and generalized Langevin equations for the cation and anion of molten salt, the unified relations among the conductivity coefficients are obtained. In particular, it is shown that the ratio of partial conductivities, σ+/σ−, is equal to the inverse mass ratio, m−/m+. The friction constant of this molten salt is also expressed in terms of the pair potential and pair distribution function, by using the fluctuation dissipation theorem for random fluctuating force. Numerical results for molten alkali halides are presented and they are, more or less, the same order as the experimental results and computational ones. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2425-2432 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The SAC-CI method was applied to the electronic excitation spectra of Cl2O, ClOOCl, and F2O. The ensuing theoretical spectra have well reproduced the experimental spectra for Cl2O and Cl2O2 and detailed characterizations of the peaks and structures were given by calculating the oscillator strength, second moment, and dipole moment for each state. For the UV region of Cl2O, the observed peaks were assigned to the valence excited states in agreement with the previous theoretical studies. For the VUV region, in the present study we have proposed the first theoretical assignments. Both valence and Rydberg excited states were calculated in this energy region, some of which resulted different from the experimental assignments. For Cl2O2, the broad band of the experimental spectrum was mainly attributed to one intense peak due to the 3B state. The theoretical spectrum above 6 eV was proposed, which so far has not been addressed and clarified before. The excitation spectrum of F2O up to about 13.0 eV was calculated and compared with the previous theoretical study. The shape and main features of the calculated spectrum was found to be very similar to that of Cl2O, and the valence and Rydberg excited states were clearly discriminated. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2447-2455 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Fluorescence of transition A˜ 1Au−X˜ 1Ag of trans-glyoxal in a supersonic jet is recorded with laser excitation in the wavelength region 393–417 nm. Full rotational analysis is performed for nine bands in a region 395–410 nm. Fluorescence decays with quantum beats from several rovibrational levels in A˜ 1Au of glyoxal are detected. As lines in Fourier-transform spectra of those decay curves split on application of an external magnetic field, this oscillatory behavior results from coherent excitation of mixed S1 and T1 states. On excitation with high energy, those lines become broadened as the lifetime of the T1 state decreases because of coupling to a dissociation continuum. An abrupt increase of linewidth in transformed spectra at 25 350 cm−1 (394.5 nm) indicates that this position corresponds to a threshold for dissociation. For excitation energy greater than 25 450 cm−1, most observed decay curves of fluorescence emission display biexponential behavior. The decay of the fast component of the biexponential curve corresponds to intersystem crossing and the slow component to decay of those eigenstates. For energies exceeding 25 550 cm−1, the slow component diminishes, to yield nearly single exponential decay, indicating that the rate of dissociation is greater than that of intersystem crossing. Results of these quantum-beat experiments imply a new dissociation pathway from the triplet surface. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2464-2471 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The CP/MAS spectra of spins-1/2 directly bonded to a quadrupolar nucleus (for example, 13C coupled to 14N) often show fine structure, due to dipolar coupling. As the magnetic field is increased, splittings decrease and disappear. For the 13C–14N system, spectra appear as doublets with an intensity ration of 1:2. The mechanism for this is well-understood. Internuclear dipolar coupling, normally averaged out by spinning, appears because the 14N nucleus is not quantized exactly along the static magnetic field—the molecule-fixed quadrupolar interaction is not negligible compared to the lab-frame Zeeman interaction. Sample spinning cannot remove dipolar coupling if the quantization direction depends on molecular orientation. While the principle is clear, a fully detailed theory is lacking. Perturbation theory or average Hamiltonian theory work well if the quadrupolar interaction is small, or is very large, with respect to Zeeman term. However, there is little available that permits the calculation of the full spinning sideband spectra for all strengths of the quadrupolar interaction. In this paper, the spin system is solved exactly, by full matrix diagonalization, for a given orientation. This involves a careful analysis of the definition of quantization. Floquet theory is adopted to handle sample spinning—the time-dependent Hamiltonian is replaced by an expanded time-independent "Floquet" Hamiltonian. Due to the time-dependent quantization direction resulting from quadrupolar coupling, off-diagonal blocks must be computed by numerical Fourier transformation. Once the Floquet matrix is set up, and dephasing of coherences accounted, the result is a comprehensive means of simulating spectra, valid for all ranges of parameters. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2480-2486 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We use long molecular dynamics simulations of methane molecules in explicit water at three different temperatures at pressures of 1 and 4000 atm to calculate entropic and enthalpic contributions to the free energy of methane–methane association. In agreement with previous simulation studies, we find that the contact minimum is dominated by entropy whereas the solvent-separated minimum is stabilized by favorable enthalpy of association. Both the entropy and enthalpy at the contact minimum change negligibly with increasing pressure leading to the relative pressure insensitivity of the contact minimum configurations. In contrast, we find that the solvent-separated configurations are increasingly stabilized at higher pressures by enthalpic contributions that prevail over the slightly unfavorable entropic contributions to the free energy. The desolvation barrier is dominated by unfavorable enthalpy of maintaining a dry volume between methanes. However, the increasing height of the desolvation barrier with increasing pressures results from entropy changes at the barrier configurations. Further resolution of the enthalpy of association shows that major contributions to the enthalpy arise from changes in water–water interactions and the mechanical work (PΔV) expended in bringing the methanes to a separation of r. A connection of these thermodynamic features with the underlying changes in water structure is made by calculating methane–methane–water oxygen triplet correlation functions. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2487-2492 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Solving integral equations is an effective approach to obtain the radial distribution function (RDF) of multicomponent mixtures. In this work, by extending Gillan's approach [M. J. Gillan, Mol. Phys. 38(6), 1781 (1979)], the integral equation was solved by numerical method and was applied to both binary and ternary mixtures. The Lennard-Jones (LJ) potential function was used to express the pair molecular interactions in calculating the RDF and chemical potential. This allowed a comparison with available simulation data, on the RDF and the chemical potential, since the simulation data have been reported for the LJ potential function. The RDF and the chemical potential results indicated good agreement with the simulation data. The calculations were extended to the ternary system and the RDFs for carbon dioxide–octane–naphthalene were obtained. The numerical method used in solving integral equation was rapidly convergent and not sensitive to the first estimation. The method proposed in this work can be easily extended to more than the three-component systems. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 2317-2323 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The dielectric spectrum of the organic glass former 1,1′-bis (p-methoxyphenyl) cyclohexane was measured over a range of temperatures and pressures, corresponding to a variation of the structural relaxation time, τα, by 8 decades. The temperature dependence of τα corresponded to a fragility equal to 72, which is consistent with the correlation of same with the shape (breadth) of the relaxation function. The dependence on pressure of τα could be described as a simple activated process, with a pressure-independent activation volume equal to ∼230 cm3/mol, varying inversely with temperature. The pressure coefficient of the glass temperature, Tg, was 240 K/GPa. At frequencies beyond the structural relaxation peak, there is a second, thermally activated process, having an activation energy=74.2 kJ/mol. The relaxation times for this process were invariant to pressure. Extrapolation of these relaxation times (measured below the Tg) intersects the ambient pressure structural relaxation data at a temperature, Tβ=268 K. This is about equal to the temperature, TB, at which the structural relaxation times deviated from a single Vogel–Fulcher–Tamman curve. In this respect, the secondary process exhibits the properties of a Johari–Goldstein relaxation. However, since Tβ varies with pressure, it remains to be seen whether its equivalence to TB is maintained at elevated pressure. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2536-2541 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Using the Z-scan technique, we study the nonlinear interaction of a dilute methanolic solution of chloro-aluminum phthalyocyanine with a ∼70 ns long train of laser pulses, each of 18 ps duration. The observations are explained by taking into account, in addition to the photoexcitation of a ground state molecule by a single pulse, thermal lensing and photoabsorption by an excited molecule (singlet or triplet) produced by previous pulses. A microscopic picture of the heating process in the solution is provided. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 2377-2388 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Brownian dynamics simulations have been carried out to model attractive polymers in solution. Bead–spring polymer chains with attractions between the end beads were modeled over a wide concentration range on either side of the overlap concentration, ρ*, for the corresponding random coil polymers. The polymers were treated as beads linked by finitely extensible nonlinear elastic springs and the excluded volume repulsion between unlinked beads was represented by a pair potential with a Gaussian analytic form. For the sticky end-beads the potential has an attractive tail of Gaussian form. In addition to chains with purely repulsive bead–bead nonbonded interactions, three different systems with attactive end beads were modeled. There were those with (a) head–head (H–H) attractions, (b) with both H–H and tail–tail (T–T) attractions, and (c) with head–tail (H–T) attractions. The dimensions of the chains, the bead–bead radial distribution functions, as well as the dynamic properties such as stress tensor time-correlation functions, infinity frequency elastic modulus, and specific viscosity of the solution were calculated as functions of solution density and end-bead attraction class. We show that with the three classes of attractive end-bead functionality, the model polymers all depart from random coil statistics and show evidence of enhanced association, even in the dilute regime, especially for the H–T systems, which can form necklacelike structures at low dilution and micellelike states with increasing concentration. (Not all of the polymer statistics measures show major differences though.) However, only the rheology if the H–T system is markedly different from the random coil case. The rheology of the H–T system is quite different in qualitative and quantitative behavior to the other classes studied. There is a progressive retardation and increasingly near-exponential decay in the shear stress relaxation function. The viscosity of the H–T class of polymers is typically at least an order of magnitude higher than that of the others, even at concentrations far below the overlap concentration ρ* for such polymers. The infinite frequency elastic modulus is also typically about five times larger for the H–T class across the density range when compared with the other three types modeled. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 2425-2434 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We investigate the Rubinstein–Duke model for polymer reptation by means of density-matrix renormalization group techniques both in the absence and presence of a driving field. In the former case the renewal time τ and the diffusion coefficient D are calculated for chains up to N=150 reptons and their scaling behavior in N is analyzed. Both quantities scale as powers of N:τ∼Nz and D∼1/Nx with the asymptotic exponents z=3 and x=2, in agreement with the reptation theory. For an intermediate range of lengths, however, the data are well fitted by some effective exponents whose values are quite sensitive to the dynamics of the end reptons. We find 2.7〈z〈3.3 and 1.8〈x〈2.1 for the range of parameters considered and we suggest how to influence the end reptons dynamics in order to bring out such a behavior. At finite and not too small driving field, we observe the onset of the so-called band inversion phenomenon according to which long polymers migrate faster than shorter ones as opposed to the small field dynamics. For chains in the range of 20 reptons we present detailed shapes of the reptating chain as function of the driving field and the end-repton dynamics. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1405-1408 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We apply a Monte Carlo technique specialized for the simulation of rare events to study the activated counterions motions in the aluminosilicate Na+-mordenite. Mean activation barriers are obtained from minimum energy paths calculated on realistic potential energy surfaces by using a Metropolis algorithm. Energy barriers for Na+ hops calculated for lattices with various Si/Al ratio are found in good agreement with the Na+ detrapping energies measured by thermally stimulated current spectroscopy. One shows that the dielectric activated motions of Na+ proceed between degenerated many-body ground states with different dipolar moment by either sequential or collective hopping motions. This provides a first microscopic description of dielectric relaxation measured in zeolites. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1441-1449 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We have investigated the performance of the new optimized exchange functional (OPTX) developed by Handy and Cohen [Mol. Phys. 99, 403 (2001)] for predicting geometries, heats of reaction, and barrier heights for twelve organic reactions (six closed-shell and six radical). OPTX has been used in conjunction with, among others, the well-known Lee–Yang–Parr (LYP) correlational functional to form two new functionals, OLYP and O3LYP. These are similar to the well-established BLYP and B3LYP functionals, respectively, with OPTX replacing the standard Becke exchange functional, B88. Our results strongly support claims made by their developers that OLYP is superior to BLYP, and essentially renders it obsolete. The computed OLYP heats of reaction, barrier heights, and even molecular geometries (with larger basis sets), are comparable with, if not better than, the corresponding B3LYP values. The O3LYP functional is overall better than B3LYP, albeit not by much. Both OLYP and O3LYP are among the best functionals currently available; the performance of OLYP in particular is noteworthy given that this functional includes no exact exchange. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1479-1481 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Variational transition state theory with multidimensional tunneling contributions (VTST/MT) is tested against quantum mechanical rate constants for the reaction H+CH4→H2+CH3 at temperatures up to 1000 K. The VTST/MT method can be and has been applied to many reactions that cannot be treated by rigorous quantum dynamics methods. Studying the accuracy of VTST/MT by comparison with accurate quantal results that are becoming available for systems of increasing size is important for validating the theory. In the present study, covering a factor of five in temperature, the VTST/MT method is found to have a mean deviation from accurate quantal rate constants for a six-body reaction of only 13% and maximum deviation of only 23%. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1529-1535 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The equilibrium structure and potential energy surface of magnesium monohydroxide in its ground doublet state, X 2Σ+ MgOH, have been determined from large-scale ab initio calculations using the spin-restricted coupled-cluster method, RCCSD(T), with basis sets of double-through quintuple-zeta quality. The effects of core-electron correlation on the calculated molecular parameters were investigated. The vibrational-rotational energy levels of various MgOH isotopomers were calculated using the variational method. The spectroscopic constants determined are found to be in remarkably good agreement with experimental data. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1567-1574 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Fluorescence decay of the rotationally cooled oxalylfluoride excited to the different single rotational levels of the A˜ 1Au(81) state was measured as a function of an external magnetic field. On excitation to this level, the dynamics in both zero and nonzero fields may be described using the intermediate-molecule limit, with the fluorescence exhibiting biexponential decay. The fast component decay rate constant is the field-independent parameter, while that of the slow component depends on the magnetic field strength. The results obtained were explained by the indirect (electronic and nuclear-spin-decoupling) mechanism, proposed earlier. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1660-1672 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We present a quantum-mechanical model for termolecular association reactions XY+Z+M→XYZ+M involving the formation of a long-lived complex XYZ*. The rotation of the molecule XYZ is treated in the infinite order sudden approximation (IOS) and its vibrations are treated by the coupled-channel method (VCC). Resonances featuring the XYZ* long-lived complex formation are first computed by means of the stabilization method and are then included in the vibrational basis functions used for the inelastic VCC-IOS scattering calculation. The method yields rate constants for the association process selected in resonance and bound states of XYZ. We apply the method to the formation of ozone and investigate isotope effects. Calculations of energy transfer and collision-induced recombination of O+O2 in collision with Ar are reported for a range of ozone isotopomers. The bending mode of O3 is not treated explicitly in these computations. The results establish a strong selectivity in vibrational state-to-state cross sections for the deactivation of O3 during the collisional energy transfer process with Ar. The present calculations also account for the high sensitivity of rate constants with respect to the isotopic composition of ozone molecules but not in the same proportion as experiments. The energy transfer from selected initial vibrational states is also calculated as a function of the initial relative kinetic energy. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1686-1691 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We investigate the effects of the long-range dipolar interaction on the formation of the stripe patterns in two-dimensional (2D) spin systems with competing short- and long-range interactions by using the continuous time Monte Carlo technique. We find that there exists an optimal temperature region at which the best stripe patterns are prone to be formed, and the stability and the orientational ordering of striped structures mainly depend on the temperature T, while the width of the striped domains is determined by the strength of the long-range dipolar interaction g. Furthermore, a complete T-g phase diagram is obtained. The results provide a simple and universal picture to account for striking and substantial physics revealed in the prevalent striped morphologies of 2D spin systems. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1714-1722 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The dielectric permittivity and loss spectra of the glassy state of 5-methyl-2-hexanol obtained by quenching it from the liquid state has been studied. In one experiment, the spectra were studied at different temperatures as the quenched sample was heated at 0.1 K/min from 105.3 to 160.5 K. In the second experiment, the quenched sample was heated from 77 to 131.6 K and kept at that temperature for 14.6 ks. The relaxation rate, fm,β, the dielectric relaxation strength, Δεβ, and the distribution of relaxation time parameters, α and β, for the Johari–Goldstein process were determined. The parameter β was found to be equal to 1 and independent of both the temperature and time, Δεβ initially decreased on increasing the temperature, reached a minimum value at ∼145.6 K, and then increased. The plot of fm,β against the reciprocal temperature decreased in slope and at ∼140 K became linear. This indicates that fm,β increases on structural relaxation. In the course of the annealing at 131.6 K, Δεβ of the quenched sample decreased with time, approaching a plateau value. It is described by an equation, Δεβ(t)=Δεβ(t→∞)+[Δεβ(t=0)−Δεβ(t→∞)]exp[−(t/τ)], where t is the time, and τ (=3.5 ks) is the characteristic time. It is pointed out that contrary to the earlier finding, o-terphenyl shows a β relaxation in the equilibrium liquid state. A consideration of dielectric permittivity arising from small-angle motions of all molecules, which has been suggested as an alternative mechanism for the localized motions seen as β relaxation, indicates that this mechanism is inconsistent with the known increase in the equilibrium permittivity on cooling. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1750-1758 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The nonlinear dielectric relaxation of an assembly of polar molecules submitted to the action of a dc field superimposed on an ac electric field is studied theoretically in the framework of the noninertial rotational diffusion model. It is also assumed that the permanent dipole moment vector makes an arbitrary angle with respect to the long molecular axis of each rodlike molecule. By calculating the ensemble averages of two Wigner rotation matrix elements 〈D0,01(Ω)〈(t) and 〈D0,11(Ω)〉(t), it is possible to express the first three harmonic components of the electric polarization varying in ω, 2ω and 3ω in analytic form, together with the steady-state frequency-dependent component. Three-dimensional dispersion and absorption plots are presented in order to show the influence of the diffusion anisotropy parameter Δ. Cole–Cole diagrams of the second and third harmonic components are also presented allowing one to distinguish two relaxation processes along the short and the long molecular axes, respectively. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2284-2288 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The localized electronic structure of single-walled carbon nanotubes (SWNTs) is qualitatively and quantitatively described by use of the first-principles calculations, and the localized molecular orbitals are distilled and the corresponding work functions are calculated within the framework of linear combination of atomic orbitals for molecular orbital. We find that the localized molecular orbital and localized work function are sensitive to the morphology of carbon nanotubes as like local density of states. With the localized electronic structures (i.e., localized work function, localized molecular orbital, and local density of states) of carbon nanotubes with various morphologies, we cannot only easily clarify the field emission characteristics of SWNTs, but also successfully interpret why open-ended SWNTs have higher chemical reactivity than capped ones. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2330-2330 
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    The Journal of Chemical Physics 116 (2002), S. 1215-1227 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We present a complex-symmetric version of the preconditioned inexact spectral transform (PIST) method, for calculating resonance energies and widths. The PIST method uses an iterative linear solver to compute inexact Lanczos vectors for (EI−H)−1, and then diagonalizes the Hamiltonian in the inexact Lanczos representation. Our new version requires complex-symmetric variants of: (1) the Lanczos algorithm, (2) the linear solver, (3) the preconditioner we introduced in a previous paper [J. Chem. Phys. 114, 9254 (2001)]. The new method works extremely well for HCO, enabling us to calculate the first 17 dissociative resonances in less then 90 second of CPU time. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1269-1276 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The finite-basis-set optimized effective potential (OEP) method is presented from an integral equation point of view. It is shown that the projection method for solving the OEP integral equation provides a consistent and convenient approach for including orbital-dependent functionals and potentials in the finite-basis-set implementations of the Kohn–Sham theory. Different finite-basis-set realizations of the OEP method are introduced and tested within the exchange-only approximation. An exact condition involving the local multiplicative exchange potential and the nonlocal Hartree–Fock exchange potential built from Kohn–Sham orbitals is incorporated in our schemes. Numerical results are presented. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1325-1329 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Focusing and selecting the HBr–N2O cluster beam was performed by using a 2 m long electrostatic hexapole field. The observed focusing curve shows a clear evidence that the linear type HBr–N2O isomer which has symmetry of symmetric top was preferentially detected in the cluster beam formed under the experimental condition used here, even though our previous ab initio calculations predict that the bent type isomer is theoretically possible. The best fit simulation for the experimental focusing curve was achieved only if we assume vibrational excitation in the van der Waals mode of the linear type HBr–N2O. The permanent dipole moment is determined to be 0.50±0.05 D. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1343-1349 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Global optimization of the geometry of small Ni clusters interacting with benzene molecules yields equilibrium structures where the Ni atoms find themselves caged between the benzene molecules. This leads to quenching of the Ni magnetic moment in most of the complexes even though the structure of the caged Ni clusters remain relatively unchanged from their otherwise free gas phase geometry. The accuracy of these predictions, based on density functional theory with generalized gradient approximation for exchange and correlation, is established by the good agreement achieved between the calculated and available experimental dissociation energies and ionization potentials. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1380-1387 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We report calculated cross sections for elastic and inelastic collisions of low-energy electrons with tetrafluoroethene, C2F4. The elastic cross section shows a number of resonance features, which we classify according to symmetry and analyze in relation to available experimental data. Electron-impact excitation cross sections are obtained for the 1 3B1u (T) and 1 1B1u (V) states arising from the π→π* transition, as well as for eight other low-lying excited states arising from excitations out of the highest occupied molecular orbital. As expected, the T and V states make the largest individual contributions to electron-impact excitation at low energies; however, the other states are shown to contribute significantly to the total excitation cross section at impact energies from 10 to 25 eV. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1417-1423 
    ISSN: 1089-7690
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Single vibronic level emission spectra have been obtained by pumping individual vibronic bands in the B˜1B2–X˜1A1 electronic transitions of jet-cooled H2CGe and D2CGe. Analysis of the spectra gave for the first time the frequencies of the following ground state fundamentals: for H2CGe, ν2=1238 cm−1, ν3=782 cm−1, ν4=673 cm−1, ν6=351 cm−1, and for D2CGe, ν1=2089 cm−1, ν2=1000 cm−1, ν3=694 cm−1, ν4=520 cm−1, and ν6=282 cm−1. The vibrational data have been combined with our previously determined molecular structures to obtain approximate harmonic force fields for the ground and excited states. Franck–Condon simulations of the emission spectra in the harmonic approximation show reasonable agreement with experiment, except for unexpected activity in the out-of-plane bending mode. This is attributed to a very anharmonic out-of-plane bending potential in the S2 excited state. Germylidene also has a very low ground state CH2 rocking frequency (ν6) which is along the normal coordinate leading to isomerization to the less stable trans-bent germyne isomer, H–C(Triple Bond)Ge–H. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1443-1456 
    ISSN: 1089-7690
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The energetics and ultrafast dynamics in the H atom transfer configuration of ammonia dimer and trimer clusters have been studied. The clusters are first excited to the electronic A˜ state with a 208 nm femtosecond laser pump pulse. This state is allowed to relax for about 1 ps during which the H-transfer state is formed which is then electronically excited by a time-delayed infrared control pulse at 832 nm and finally ionized with a third femtosecond probe pulse at 416 nm. We have also performed complementary theoretical studies elucidating the experimental findings. For the dimer in the excited NH4(3p)(centered ellipsis)NH2(X˜) state the time-dependent ion signals reveal an isotope-independent short lifetime of about τ6=(130±60) fs which can be explained by a curve crossing with the repulsive NH4(3s)(centered ellipsis)NH2(A˜) state, whereas the trimer signal persists on a time scale being more than one order of magnitude longer and exhibits a very large isotope effect. This is interpreted as being due to internal conversion from the excited state NH3NH4(3p)(centered ellipsis)NH2(X˜) back to the NH3NH4(3s)(centered ellipsis)NH2(X˜) ground state. The analysis of the corresponding photoelectron spectra also confirms the transition energies between the electronic states involved, e.g., ΔE[NH4(3s→3p)(centered ellipsis)NH2]=1.5 eV and ΔE[NH3NH4(3s→3p)(centered ellipsis)NH2]=1.2 eV, as determined by our ab initio calculations. © 2002 American Institute of Physics.
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  • 152
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    The Journal of Chemical Physics 116 (2002), S. 1493-1499 
    ISSN: 1089-7690
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We report accurate energetics for the water trimer through pentamer global ring minima and four low-lying hexamer isomers (cage, prism, book, cyclic S6) from first principles electronic structure calculations. The family of augmented correlation-consistent orbital basis sets of double through quintuple zeta quality was used in order to estimate complete basis set (CBS) limits for the cluster total association energies at the second order perturbation (MP2) level of theory. These are −15.8 kcal/mol (trimer), −27.6 kcal/mol (tetramer), −36.3 kcal/mol (pentamer), −45.9 kcal/mol (prism hexamer), −45.8 kcal/mol (cage hexamer), −45.6 kcal/mol (book hexamer), and −44.8 kcal/mol (ring S6 hexamer). Effects of higher correlation, estimated at the coupled cluster plus single and double with a perturbative estimate of the triple excitations [CCSD(T)] level of theory, as well as inclusion of estimates for core–valence correlation suggest that these estimates are accurate to within 0.2 kcal/mol. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2184-2193 
    ISSN: 1089-7690
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    Topics: Physics , Chemistry and Pharmacology
    Notes: One- and two-dimensional 2H- and 13C-NMR (nuclear magnetic resonance) echo spectroscopy and 1H static field gradient NMR self-diffusion experiments have been used to study the reorientational and translational dynamics of benzene molecules adsorbed on zeolite NaY as a function of loading. Comparison of the data with model calculations establish that the elementary motional process of the guest molecules is consistently identified as a jump process among well defined adsorption sites inside a supercage and/or a jump between nearby supercages. In cases where the zeolite cavities contain high loadings of guest molecules, each molecular jump is accompanied by concomitant relaxation of the local environment. Molecular jump events between adsorption sites correspond to the elementary processes from which long range translational diffusion evolves. © 2002 American Institute of Physics.
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  • 154
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    The Journal of Chemical Physics 116 (2002), S. 2219-2228 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: To describe the polypeptide helix–coil transition, while the Ising-based theory has been playing the principal role for 40 years, we can now make use of computer simulation using the so-called "all-atom model" that is far more precise than the Ising-based model. In this study, by conducting molecular dynamics (MD) simulations of helix–coil transition exhibited by a short polyalanine chain, we investigated how the MD simulation results and the Ising-based theoretical values coincide with each other, placing a focus on their equilibrium statistical mechanical properties. Several important physical properties, such as temperature-dependent helix ratio, distribution of the helix-residue number, position-dependent helix ratio, and pair-correlation between residue states were taken up as the proving grounds on which we made a comparison between the all-atom model simulation and the Ising-based theory. As an overall trend, we realized that the Ising-based theoretical results agreed with the all-atom simulation results at least qualitatively, suggesting that the Ising-based model, though very simple, extracts the essence of the phenomenon with respect to the equilibrium properties. On the other hand we found some quantitative disagreements between them. The origins of the observed disagreements are discussed by going into details of the all-atom model. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2261-2268 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Self-avoiding lattice walks are often used as minimalist models of proteins. Typically, the polypeptide chain is represented as a lattice walk with each amino acid residue lying on a lattice point, and the Hamiltonian being a sum of interactions between pairs of sequentially nonadjacent residues on adjacent points. Interactions depend on the types of the two residues, and there are usually two or more types. A sequence is said to fold to a particular "native" conformation if the ground state is nondegenerate, i.e., that native conformation is the unique global energy minimum conformation. However, real proteins have some flexibility in the folded state. If this is permitted in a lattice model, the most stably and cooperatively folding sequences have very disordered native states unless the Hamiltonian either favors only a few specific interactions or includes a solvation term. The result points the way toward qualitatively more realistic lattice models for protein folding. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2289-2300 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We study the structure and thermodynamics of the critical nuclei in metastable binary polymer blends using the self-consistent field method. At the mean-field level, our results are valid throughout the entire metastable region and provide a smooth crossover from the classical capillary-theory predictions near the coexistence curve to the density functional predictions of Cahn and Hilliard (properly transcribed into expressions involving the parameters of the binary polymer blends) near the spinodal. An estimate of the free energy barrier provides a quantitative criterion (the Ginzburg criterion) for the validity of the (mean-field) self-consistent approach. The region where mean-field theory is valid and where there can be a measurable nucleation rate is shown to be poorly described by the existing limiting theories; our predictions are therefore most relevant in this region. We discuss our results in connection with recent experimental observations by Balsara and co-workers. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 2269-2276 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The high packing density of residues in proteins ought to be manifested in some order; to date this packing order has not been thoroughly characterized. The packing regularity in proteins is important because the internal organization of proteins can have a dominant effect on functional dynamics, and it can aid in the design, simulation and evaluation of structures. Packing metrics could also inform us about normal sequence variability, an issue that, with the accumulating genome data, becomes increasingly important. Other studies, indicating a possible correlation between packing density, sequence conservation, and folding nucleation [O. B. Ptitsyn, J. Mol. Biol. 278, 655 (1998)], have emphasized the importance of packing. Here, residue clusters from protein databank structures, each comprised of a central residue and all neighbors located within the first coordination shell, have been rigidly re-oriented and superimposed in a self-consistent optimization. About two-thirds of residues are found to follow approximately the relative orientation preferences of face-centered-cubic packing, when examined on a coarse-grained scale (one site per residue), while the remaining one-third occupy random positions. The observed regularity, which becomes more pronounced after optimal superimposition of core residues, appears to be the result of uniform sampling of the coordination space around each residue on a coarse-grained scale with hydrophobic clustering and volume exclusion, to achieve packing densities close to that of the universal closest packing of identical spheres. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1211-1214 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Infrared spectra of CH stretches have been investigated on the surfaces of synthetic diamond crystallites (5, 100, and 700 nm in diameter) to provide insights into the mid-infrared emission bands of stardusts in interstellar media. While the spectrum of 5-nm diamonds fails to display the distinct 2835 cm−1 (or 3.53 μm) band, a remarkably good match of the absorption bands of larger diamond grains with the emission observed for the stars Elias 1 and HD 97048 is obtained. Suggested by this study, the nanodiamonds that can display such characteristic emission bands at 3.53 μm in these two interstellar systems have a size significantly larger than 5 nm. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1239-1249 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The power method for solving N-particle eigenvalue equations is contracted onto the two-particle space to produce a reduced "variational" method for solving the contracted Schrödinger equation (CSE), also known as the density equation. In contrast to the methods which solve a system of approximate nonlinear equations to determine the two-particle reduced density matrix (2-RDM) nonvariationally, the contracted power method updates the 2-RDM iteratively through a "gradient" of the N-particle energy. After each power iteration we modify the 2-RDM to satisfy certain N-representability conditions through an extension of purification to correlated RDMs. The contracted power method is illustrated with a variety of molecules. Significant features of the present calculations include (i) accurate results for both first- and second-order functionals for building the 3- and the 4-RDM's from the 2-RDM's; (ii) the first molecular implementation of the Mazziotti correction within the CSE [Mazziotti, Phys. Rev. A 60, 3618 (1999)]; (iii) a spin–orbital formulation; (iv) the treatment of both core and valence orbitals as active; and; (v) a reduction of the CSE computational scaling through fast summation and the natural-orbital transformation. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1313-1317 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: High-resolution laser-induced fluorescence spectroscopy has been used to investigate the 18 163 cm−1 band of Pt2 in a supersonically cooled molecular beam. Rotational constants of the ground and excited states were extracted from the rotationally resolved spectrum and determined to be B0″=0.031 754(12) cm−1 and B0′=0.028 672(11) cm−1, respectively. These values correspond to ground- and excited-state bond lengths of r0″=2.33297(44) Å and r0′=2.455 16(47) Å, respectively. Nuclear spin statistics that are observed in the spectrum demonstrate that the ground state is of either 0g+ or 0u− symmetry. Of these, 0g+ is by far the more probable. Comparisons with Au2 are made, suggesting that it may be appropriate to consider Pt2 as having a double bond. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1303-1312 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The potential energy surface of a model propane dimer was systematically mapped with quantum chemical calculations. The calculations included approximately 12 separation distances between the monomers for each of 121 different relative geometries, or 1487 different configurations. The generated potential energy map reveals that the most attractive interactions are those having a maximum number of close contacts between carbon and hydrogen. The potential well depth of the most attractive orientation found was −1.625 kcal mol−1. The complete ab initio energy surface was fitted to a simple model consisting of pairwise-additive interatomic potentials, each modeled with a modified Morse function of interatomic distance. The resultant model accurately represents the entire propane dimer ab initio energy surface. The efficacy of the generated parameter set was tested with previously published ethane dimer energies and propane routes not included in fitting. The new parameter set is consistent with these results indicating a high level of transferability for the interatomic C–H, C–C, and H–H potentials obtained. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1296-1302 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: An accurate calculation of the energy differences between stationary points on the torsional potential energy surface of n-pentane is performed using ab initio Hartree–Fock theory, advanced many-body methods such as MP2, MP3, CCSD, and CCSD(T), as well as density functional theory, together with basis sets of increasing size. This study focuses on the four conformers of this compound, namely, the all staggered trans–trans (TT), trans–gauche (TG), gauche–gauche (G+G+), and gauche–gauche (G+G−) structures, belonging to the C2v, C1, C2, and C1 symmetry point groups, respectively. A focal point analysis up to 635 basis functions is carried out to determine when the series of relative energies of the four conformers approach convergence. It is found that relative to the minimum energy TT conformer, the energy differences of the TG, G+G+, and G+G− conformers obtained from ab initio methods are 0.621, 1.065, and 2.917 kcal mol−1, respectively. Converged energy differences obtained with three density functionals, B3PW91, B3LYP, and MPW1K, are found to be considerably higher than those computed ab initio. Mole fractions of the various conformers are evaluated at different temperatures from thermostatistical data accounting for vibrational and rotational entropies, as well as zero-point vibrational energies in the rigid rotor-harmonic oscillator approximation. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1330-1338 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The electronic and molecular structure of a series of nonstoichiometric pentaatomic species, Al3X2−(X=C,Si,Ge) and their corresponding neutrals, have been studied by photoelectron spectroscopy and ab initio calculations. Well-resolved photodetachment transitions were observed for all three species and were compared with the calculations. Al3C2− was found to have a C2v(1A1) global minimum with an Al− ion coordinated to the CC triple bond in a quasi-linear AlCCAl molecule. Al3Si2− and Al3Ge2− were found to be different from the isoelectronic Al3C2− anion. They each have an almost planar trapezium global minimum structure with several low-lying isomers. The quasi-planarity of Al3Si2− and Al3Ge2− was understood by comparison with the previously known SiAl4− planar molecule. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1361-1369 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The electronic energy transfer pathways that occur following collisions between I2 in the E ion-pair electronic state (v=0, J=55) and He and Ar atoms have been determined. The nearby D, D′, and β ion-pair states are populated, but with relative branching ratios that vary with the rare gas collision partner. In He/I2 collisions, the D state is preferentially populated, while Ar/I2 collisions preferentially populate the β electronic state. Bimolecular rate constants and effective hard sphere collision cross sections have been determined for each channel; the cross sections range from 7.0±1.0 Å2 for populating the β state with Ar collisions to 0.9±0.2 Å2 for populating the D′ state with He collisions. For both rare gas collision partners, and all three final electronic states, low vibrational levels are populated, in rough accord with the relevant Franck–Condon factors. There is little propensity observed for population of vibrational levels that are in near resonance with the initially prepared level in the E state. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 1351-1362 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Liquid-state integral equation methods are employed to study the thermodynamic and structural properties of ideal and repelling rigid rods mixed with hard spheres in the limits when one of the species is dilute. The role of rod aspect ratio and sphere/rod size asymmetry is explored over a wide range of system parameters encompassing the colloid, nanoparticle, and crossover regimes. Novel predictions are found for the polymer (sphere) mediated depletion potentials and second virial coefficients of particles (rods) in dense polymer (sphere) suspensions. The adequacy of the closure approximations employed is tested by comparison with available numerical calculations and more rigorous theories in special limits. The liquid-state theory appears to be accurate for all properties in the nanoparticle regime and for the insertion chemical potential of needles and spherocylinders. However, it significantly underestimates depletion attractions effects in the colloidal regime of short rods and large spheres due to nonlocal entropic repulsion effects between polymers and particles not captured by the classic Percus–Yevick approximation. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 117 (2002), S. 961-964 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Interaction between HKrCl and N2 is investigated in a low temperature Kr matrix and by using ab initio calculations. Two configurations of the HKrCl(centered ellipsis)N2 complex are found both computationally and experimentally. The complexes show large monomer-to-complex blueshifts (+112.9 and +32.4 cm−1 experimentally) of the H–Kr stretching vibration mode. The large blueshifts are attributed to the enhanced (HKr)+Cl− ion-pair character of complexed HKrCl resulting in stronger H–Kr covalent bonding. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1204-1205 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: An undocumented approximation has been found in the discussion of the effects of molecular diffusion in the CRAZED experiment, as presented in the reference quoted in the title. A detailed discussion shows the subtle origin of the problem. Reference is given to discussions which avoid this approximation by using the extended Bloch equation. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 865-868 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We examine the thermodynamics of supercooled liquids focusing on the immediate vicinity of an onset temperature, TA, where system dynamics just begin to experience caging effects. Simulation data from a polymer model and from small molecule mixtures show, in agreement with experiment, that the configurational entropy becomes strongly temperature dependent below TA. Since the diffusion coefficient follows the Adam-Gibbs relationship, our results clearly establish a thermodynamic connection to the localized dynamics of glass-forming liquids. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 869-877 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The nuclear magnetic shielding polarizabilities of N2, F2, CO, HF, HCl, HCN, HNC, and C2H2 have been computed at the coupled-cluster singles and doubles (CCSD) level augmented by a perturbative treatment of triple excitations [CCSD(T)] using gauge-including atomic orbitals and a mixed analytical-numerical approach based on the numerical differentiation of analytically evaluated shieldings. Extended basis sets have been employed to ensure results close to the basis set limit, and convergence of the electron-correlation treatment is investigated. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 928-935 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The interactions of Cu(2S:3d104s1, 2D:3d94s2, and 2P:3d104p1) with SiH4 and GeH4 were studied by means of Hartree–Fock–SCF and multiconfigurational-SCF followed by variational and multireference second order Möller–Plesset perturbational configuration interaction (CIPSI) calculations, using relativistic effective core potentials. The Cu atom in its 2P(3d104p1) state is inserted in the Si–H and Ge–H bonds. In both interactions their corresponding 5 2A′ potential energy surfaces are initially attractive and become repulsive only after having encountered the avoided crossing region with the initially repulsive 4 2A′ surface adiabatically linked with the Cu(2D:3d94s2)–SiH4(GeH4) fragments. The three 2A′ curves derived from the interaction of the Cu(2D:3d94s2) atom with silicon (or germane) molecule are initially repulsive. Each one of them shows two avoided crossings and its lowest lying 2 2A′ curve goes sharply down until it meets the X 2A′ curve adiabatically linked with the Cu(2S:3d104s1)+SiH4(GeH4) asymptotes. The 2 2A′ curve becomes repulsive after the avoided crossing with the X 2A′ curve. The lowest-lying X 2A′ potential leads to the HCuZH3 X 2A1 (Z=Si, Ge) intermediate molecule. This intermediate molecule, diabatically correlated with the Cu(2P:3d104p1)+ZH4 fragments which lie 5.8 and 1.6 kcal/mol, respectively, above the ground state reactants, have been carefully characterized as well as the dissociation channels leading to the CuH+ZH3 and H+CuZH3 products. These products are reached from the HCuZH3 intermediates without activation barriers. This work suggests that the simultaneous photoexcitation of the Cu atom in presence of silane and germane molecules in the gas phase could be used to produce better quality a-SiGe:H thin films. © 2002 American Institute of Physics.
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    Notes: We applied a quantum mechanics/molecular mechanics method that makes use of the mean field approximation to study the polarization of several alcohols in the liquid phase. The method is based on the calculation of the averaged solvent electrostatic potential from molecular dynamics data. Because of the reduced number of quantum calculations that our approximation involves, it permits the use of flexible basis sets, the consideration of the electron correlation and the solvent and solute polarization. We found that the molecules studied undergo strong polarization when they pass from the gas to the liquid phase. From this point of view, the polarization methanol displays a behavior lightly different from ethanol and propanol. The vaporization energies are very well reproduced especially when the correlation energy is included. The differences with the experimental values are less than 3% in the three systems studied. Finally, we consider the effect on the thermodynamics and the structure of the solution of the choice of the Lennard-Jones parameters. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1658-1670 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Electron transfer (ET) interactions of a series of 7-aminocoumarin dyes with aliphatic amine donors have been investigated using steady-state (SS) and time-resolved (TR) fluorescence quenching, picosecond laser flash photolysis (LFP) and pulse radiolysis (PR) techniques. For different coumarin–amine pairs, the estimated quenching constants (kq) from SS and TR fluorescence measurements are found to be similar within the experimental error. That ET from amine donors to excited (S1) coumarin dyes takes place has been established from the LFP and the PR results. For different coumarin–amine pairs, the kq values are seen to correlate well with the free energy changes (ΔG0) for the ET reactions following Marcus' outer-sphere ET theory. The total reorganization energy (λ) estimated from this correlation is seen to be just similar to the solvent reorganization energy (λs). The leveled-off kq value under diffusion-controlled condition (kqDC) appears to be much lower (∼2.5 times) for the present systems compared to the corresponding value obtained for the ET reactions in coumarin–aromatic amine systems. The large difference in the kqDC values with aliphatic and aromatic amines as the electron donors has been rationalized on the basis of the shapes of the highest occupied molecular orbitals (HOMO) of the amine donors. For aliphatic amines, since their HOMOs are largely localized on the amino group, a large orientation factor is involved in the encounter complexes for the ET reaction to take place. With π like HOMOs, such orientational restriction is just nominal with the aromatic amines as the electron donors. Present ET results under diffusive conditions have also been discussed with a comparison to the ET rates observed under nondiffusive conditions, where the amines are directly used as the solvent donors. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1707-1712 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Monochromatic UV light in the spectral interval between 4.0 and 5.5 eV is used in order to selectively excite 3- and 4-coordinated oxygen anion sites on the surface of MgO nanoparticles exposed to O2 gas. As a result, two different paramagnetic O− surface species and also ozonide anions O3− are observed by electron paramagnetic resonance (EPR) spectroscopy. The relative abundance of each of the O− species exhibits a specific dependence on the energy of the exciting photons. EPR data together with the results of theoretical modeling suggest that both O− species are located at 3-coordinated sites having different local environments. At sufficiently high O2 pressures molecular oxygen does not only act as an electron trap, favoring the O− formation, but it also contributes to UV induced O3− formation with a maximum efficiency at 4.2 eV. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1725-1730 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We report an observation of strong emission of CN− ions during heating of a nitrogen ion-irradiated graphite surface. An activation energy of 5.0±0.2 eV for thermionic CN− emission is derived from its temperature dependence. From the results of thermal desorption of neutral molecules and thermionic electron emission, it is proposed that the thermally induced CN− ions may originate from the dissociative negative ionization of desorbing C2N2 molecules on the surface via a thermionic electron attachment mechanism. This mechanism is supported by the dissociative negative ionization of the desorbed C2N2 molecules in the gas phase, as observed by negative ion RGA measurement. The large negative ionization cross section of C2N2 molecules at an electron energy of 0.8–0.9 eV, which also leads to the formation of CN− ions, is believed to be responsible for the CN− emission during heating of the nitrogen ion irradiated graphite. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1737-1743 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We report pressure (0–28 kbar) and temperature (1.1–4.3 K) dependent photon echo results for tetra-tert-butyl-terrylene (TBT) in a polyisobutylene (PIB) host. Increased pressure is found to increase the homogeneous dephasing rate over the temperature range of this study, in contrast to pressure dependent hole burning results reported for other polymer systems at somewhat higher temperatures (≥4.2 K). A relatively small pressure increase (0 to 9 kbar) resulted in a change in the temperature dependence of the dephasing characterized by a lowering of the temperature power law exponent from ∼1.3 to ∼0.9. Further pressure increase above 9 kbar was characterized by an additional increase in the homogeneous dephasing rate without further change in the temperature exponent. The results are compared to high pressure photon echo studies of other polymer systems, and discussed in terms of the TLS (two-level-systems) model. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1063-1071 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: This is a joint effort of an experimental and a theoretical group to understand neutron scattering linewidths of almost free quantum rotors. In the first part we introduce a new method for simulating the dynamics of small quantum systems at finite temperatures. Thermal fluctuations are implemented through a stochastic perturbation potential, which drives the system to thermal equilibrium. It is modeled in analogy to the classical Langevin equation. In the second part we present neutron scattering data for the NH3-rotor in Ni–Ni–2C12H10 Hofmann clathrates. By comparison of the experimental with the simulated data we find a classical behavior for the coupling strength of the phonons to the rotor. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1085-1091 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A quantum-mechanical model description of a molecular photoswitch is developed. It takes into account (i) the electronic curve crossing arising from the cis-trans twisting of a double bond, resulting in an ultrafast internal-conversion process of the system and (ii) the coupling of the initially excited chromophore (the "system") to the remaining degrees of freedom (the "bath"), affecting a vibrational cooling of the hot photoproducts. The latter mechanism is responsible for the localization of the molecule in the cis and trans configuration, respectively, thus determining the quantum yield of the photoreaction. Following a discussion of the validity and the numerical implementation of the Redfield formulation employed, detailed numerical studies of the time-dependent dissipative photoisomerization dynamics are presented. While the short-time dynamics ((approximately-less-than)1 ps) is dominated by the coherent wave-packet motion of the system, the time evolution at larger times mainly reflects the interaction between system and bath. The quantum yield of the cis-trans forward reaction (Yc→t) and the trans-cis backward reaction (Yt→c) is shown to depend on the energy storage of the photoreaction and, in particular, on the form of the system–bath coupling. On the other hand, it is found that Yt→c=1−Yc→t, that is the population probabilities of the cis and trans configuration at long times do not depend on the initial preparation of the system. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1128-1136 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The kinetics of molecular nitrogen desorption from Rh(111) single-crystal surfaces covered with atomic nitrogen were characterized by both isothermal and temperature-programmed experiments. A complex kinetic behavior was observed for this system not describable by typical Arrhenius expressions even if coverage-dependent activation energies are considered. In fact, the possibility of developing an analytical expression for those desorption rates is voided by the fact that they depend not only on surface temperature and nitrogen coverage but also on the mode of preparation of the system. Isotope labeling experiments support the idea of the formation of surface nitrogen islands and of preferential recombination and desorption at their edges. Coadsorbed oxygen, a typical by-product in NO reduction catalysis, behaves kinetically in a way similar to surface nitrogen as far as N2 desorption is concerned. The recombination of two surface nitrogen atoms is typically slower than the reaction between one nitrogen and one adsorbed NO molecule, and therefore the catalytic reduction of NO most likely occurs via the latter pathway.© 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1171-1184 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We modify Larson's lattice model [J. Chem. Phys. 83, 2411 (1985)] and use it to study self-assembly of surfactants in a supercritical solvent by large-scale Monte Carlo simulations. Carbon dioxide and perfluoroalkylpoly(ethylene oxide) serve as prototypes for the solvent and surfactant, respectively. Larson-model type parameters for carbon dioxide and perfluoroalkylpoly(ethylene oxide) are obtained using experimental values of critical parameters and solubility along with a modified Berthelot combining rule. We perform canonical Monte Carlo simulations at a supercritical temperature, varying the number of surfactant head and tail segments, the solvent density and the surfactant concentration. Various properties such as the critical micelle concentration, the aggregate size distribution, and the size and shape of the micelles are evaluated and pseudophase diagrams are constructed. We further investigate the ability of the surfactant solutions to dissolve more solute than solutions without surfactants by calculating the partition coefficient. Water serves as a prototype for the solute and Larson-model type parameters for water are obtained in the same way as for carbon dioxide and perfluoroalkylpoly(ethylene oxide). © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 1193-1200 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We report on dynamic properties of carbon monoxy myoglobin (MbCO) embedded in trehalose matrices of different water content, studied by FTIR spectroscopy and CO rebinding after flash-photolysis. FTIR spectroscopy was used to study the thermal behavior of the bound CO stretching and of the adjacent bands arising from trehalose and residual water, as a function of the sample water content. These measurements enabled us to get information on the relation between the interconversion among A substates (as evidenced by the thermal behavior of the CO stretching band) and the dynamics of the trehalose-water matrix. Under condition of drought, the protein internal dynamics is tightly coupled to the dynamics of the external matrix and is modulated by traces of residual water. Under such condition, substates interconversion is hindered due to extreme increase of energy barriers. At variance sizeable substates interconversion takes place following a small water uptake, obtained by exposure of the dry sample to a nondry surrounding atmosphere. FTIR results were in full agreement with flash-photolysis data. In particular, the heme pocket dynamics, which regulates the migration of the flashed off CO molecule within the protein matrix, can be well described on the basis of the information obtained by FTIR measurements. Under condition of drought, in which vanishing temperature dependence of the CO stretching band is observed, the rebinding kinetics is governed by quasi-static rate constant distributions. At variance, stretched exponentials describe geminate rebinding following slight water uptake by the sample, which, as shown by FTIR, brings about interconversion among conformational A substates. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 906-912 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The fragmentation dynamics of allene and propyne molecules following photoexcitation at 203.3, 209.0 and 213.3 nm have been investigated by H (Rydberg) atom photofragment translational spectroscopy methods. Contrary to conclusions reached in previous photochemical studies of these molecules, at a photolysis wavelength of 193 nm, we find the translational energy spectra associated with the H atom product forming channel in both molecules to be essentially identical, and to have a form that is reproduced well by an approximate statistical model that assumes population of all possible vibrational states of the H2CCCH partner. Such behavior can be most readily accommodated by assuming that, for both molecules, at the excitation energies used in the present work, internal conversion to, and isomerization on, the ground state potential energy surface precedes fragmentation. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 897-905 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We present a method to predict products, transition states, and reaction paths of unimolecular chemical reactions such as dissociation or rearrangement reactions of small to medium sized molecules. The method thus provides the necessary input for established procedures to compute barrier heights and reaction rates, which conventionally have to be assumed heuristically. The method is an extension of the force field based conformational flooding procedure, but here aims at an accelerated barrier crossing of chemical reactions rather than conformational motions. Accordingly, it is now coupled to density functional molecular dynamics, such that the chemical reaction under study takes place at the picoseconds time scale set by todays computer technology. Barrier crossings are accelerated by means of an additional energy term (flooding potential) that locally destabilizes the educt conformation without affecting possible transition states or product states. The method is applied to two test systems, bicyclopropylidene and methylenecyclopropane, for which the reaction paths are predicted correctly. New details of reaction pathways are found, such as a transient concerted, but asynchronous rotation of the two methylene groups for the bicyclopropylidene→methylenespiropentane reaction. Our method can be applied to simulations in the gas phase as well as in solution and can be combined with force field simulations, e.g., in hybrid density functional/force field (QM/MM) computations. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 936-945 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The kinetic energy dependencies of the reactions of Vn+ (n=2–13) with D2 are studied in a guided ion beam tandem mass spectrometer. Products observed are VnD+ for all clusters and VnD2+ for n=4–13. All reactions are observed to exhibit thresholds, except for formation of VnD2+ for n=4,5,7,9,11–13. The enhanced reactivity of the odd-sized clusters towards D2 chemisorption is nicely correlated with the D0(Vn+–V) bond energies. The odd-number clusters are less stable and more reactive, suggesting that they are open shell, whereas the even-number clusters, which are more stable and less reactive, appear to be closed shell. Threshold analyses of the endothermic reactions lead to Vn+–D binding energies (n=1–13), which reach values comparable to the bulk phase for larger clusters. The Vn+–D bond energies show odd–even oscillations anticorrelated with D0(Vn+–V) for n〈5, but roughly parallel with D0(Vn+–V) for n〉5. Magnitude differences in the two series of bond energies suggest that the metal–metal bonding has appreciable 3d–3d contributions. The variation in the Vn+–D bond energies with cluster size is explained using promotion energy arguments. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 964-973 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Four theoretical methods, using continuous transformation of the origin of the current density (CTOCD) to annihilate either the diamagnetic or the paramagnetic contribution, have been employed at the coupled Hartree–Fock level of accuracy to evaluate magnetic susceptibility and nuclear magnetic shielding of five planar molecules with the chemical formula C6H6. The results have been compared with corresponding estimates from basis sets of London orbitals, showing the near Hartree–Fock quality of calculated values and the practicality of CTOCD approaches. Maps of streamlines and intensity of the current density induced in the π-electrons by a stationary magnetic- field perpendicular to the molecular plane are shown to interpret the different magnetic response properties of benzene isomers by means of the Ring–Current model. The plots show delocalized flow in benzene, determining its enhanced diamagnetism. Diamagnetic loops, localized in the region of carbon–carbon bonds, and a paramagnetic vortex in the vicinity of electronic centroid, are found in 3,4-dimethylenecyclobutene and trimethylenecyclopropane. This pattern is typical of conjugated nonaromatic molecules. Delocalized diamagnetic circulation observed in fulvene explains its exalted magnetic susceptibility. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 455-459 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Organic dendrimers are a fascinating new class of materials for opto-electronic applications. We present coupled electronic oscillator calculations on novel nanoscale conjugated dendrimers for use in organic light-emitting diodes. Strong confinement of excitations at the center of the dendrimers is observed, which accounts for the dependence of intermolecular interactions and charge transport on the degree of branching of the dendrimer. The calculated absorption spectra are in excellent agreement with the measured data and show that benzene rings are shared between excitations on the linear segments of the hyperbranched molecules. The coupled electronic oscillator approach is ideally suited to treat large dendritic molecules. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 784-790 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We have studied the adsorption of sulfur (S(Double Bond)), mercapto (HS–), and methylthiolate (CH3S–) on Au(111). The three adsorbates are found to form strong bonds to the gold surface through the S-end. While the sulfur atom adsorbs in the high coordinated fcc site, the mercapto and methylthiolate molecules adsorb in bridge or bridgelike sites. The bending of the sulfur–hydrogen and sulfur–methyl bonds away from the surface normal plays a key role in this sites preference. We show that the back bonded sulfur species prefer the bridge sites because of lower steric repulsion at these sites between the gold surface and the hydrogen and methyl groups, respectively. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 825-831 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We have studied the optical absorptions of a series of point defects in SiO2 by means of time-dependent density functional response theory (TD-DFT). The structure of the defects has been described with cluster models and atomic orbital basis functions. For each center the lowest singlet→singlet and singlet→triplet (for diamagnetic defects) and doublet→doublet (for paramagnetic defects) transitions have been considered. The results have been compared with accurate ab initio calculations based on explicit treatment of correlation effects and, when possible, with experimental data. Defects with localized wave functions and low excitation energies (〈5 eV) are well described by TD-DFT and the predicted transition energies are within a few tenths of an eV from the experimental or ab initio values. For defects which give rise to transition energies higher than 5 eV the TD-DFT values are 10%–20% too low. The comparison of various exchange-correlation functionals show that the hybrid B3LYP method provides more accurate answers than other gradient-corrected DFT approaches. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 854-859 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We present Monte Carlo simulations of the formation and structure of polysilanes and polysilyne networks. The simulation technique allows for the investigation of large systems, containing up to 10 000 monomers. Our results show that ring formation is an important factor for both types of materials. For polysilyne networks, a random structure is found incorporating cyclic substructures, linear chains, and branching points. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 8247-8250 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The geometry of the internal space of porous media determines transport properties at all scales. We demonstrate an experimental scheme to quantify the body-to-throat ratio and the shape of the pores through direct measurements of geometrical quantities. We used a constant-rate mercury injection measurement to obtain the throat size and the pore-body volume, and an NMR method (DDIF) to obtain the pore size distribution in a Berea sandstone. This approach uniquely identifies the pore throats and bodies and enables a quantification of their sizes. Our results show that the pore bodies in Berea sandstone is likely to be described by a very much elongated cavity. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 8270-8275 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Highly accurate relativistic Gaussian basis sets with a finite-nucleus model are developed for the 103 elements from H (Z=1) to Lr (Z=103). The present GTO sets augment the relativistic basis sets with a point-charge model proposed in the first paper of this series. The relativistic third-order Douglas–Kroll approach is adopted in optimizing the orbital exponents of a basis set by minimizing the atomic self-consistent field (SCF) energy. The basis sets are designed to have equal quality and to be appropriate for the incorporation of relativistic effects. The performance of the present basis sets is tested by calculations on a prototypical molecule, gold dimer using SCF and the singles and doubles coupled-cluster model with perturbative triples [CCSD(T)]. Several spectroscopic constants are calculated for the ground state of Au2. At the basis set superposition error (BSSE) corrected CCSD(T) level, the deviation from experiment is ΔRe=0.018 Å, Δωe=−3 cm−1, and ΔDe=−0.17 eV. The finite-size nucleus effect makes Re, ωe, and De smaller by 0.004 Å, 1 cm−1, and 0.05 eV, respectively. The application shows that the present relativistic Gaussian-type orbitals (GTO) basis sets with a finite-nucleus model are accurate and reliable. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 8307-8317 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We examine in detail the causes of the structural transitions that occur for those small Lennard-Jones clusters that have a nonicosahedral global minima. Based on the principles learned from these examples, we develop a method to construct structural phase diagrams that show in a coarse-grained manner how the equilibrium structure of large clusters depends on both size and temperature. The method can be augmented to account for anharmonicity and quantum effects. Our results illustrate that the vibrational entropy can play a crucial role in determining the equilibrium structure of a cluster. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 8343-8352 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The vinyl radical (C2H3)A˜ 2A″←X˜ 2A′ spectrum has been measured between 530 and 385 nm using cavity-ringdown spectroscopy. The active vibrational progressions involve C–C stretching and alpha H–C–C bending vibrations. Optimal rotational constants and linewidths were determined for the first four vibrational bands by modeling the spectrum as an asymmetric top. The best-fit rotational constants obtained for the excited electronic state are consistent with the molecular geometry predicted by ab initio calculations. The lifetime of the vibrationless level in the excited electronic state is estimated to be a few picoseconds, and increasing vibrational excitation leads to a decrease in the lifetime, based upon an increasing linewidth. Various possibilities for the predissociation mechanism are discussed. The most likely is judged to be a conical intersection or seam of intersections. A preliminary CASSCF calculation has found the point on the relevant potential energy surfaces at which the ground and electronically excited states are closest. While the geometry and other properties of this crossing point are in accord with the experimental results, the calculated position of the point of closest approach of the two electronic states lies considerably (〉1 eV, including zero-point energy) above the already predissociative A˜ 2A″ state origin. Other mechanisms are also discussed to account for the observed rapid predissociation. Clearly there is a need for a higher level theoretical work on this problem. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 8353-8366 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We present high-level ab initio calculations for the global adiabatic potential energy surfaces of the ground state (X˜ 2A′) and several excited states (A˜ 2A′, B˜ 2A″, C˜ 2A′, D˜ 2A′, and E˜ 2A″) of LiFH, including the valleys leading to Li+HF and LiF+H. The ab initio calculations were carried out using the multireference singles and doubles configuration interaction method with 99 reference configuration state functions (CSFs) for the 2A′ states and 39 reference CSFs for the 2A″ states. The basis set consisted of 140 contracted Gaussian functions, including specifically optimized diffuse functions, and calculations were performed on a dense grid of ∼3500 nuclear geometries which allowed us to construct an accurate analytic representation of the two lowest-energy LiFH potential energy surfaces. An analytic 2×2 quasidiabatic potential energy matrix was obtained by fitting physically motivated functional forms to the ab initio data for the two lowest-energy adiabatic states and explicitly including long-range interactions. The newly presented LiFH fit is compared to several ground-state LiFH fits and one excited-state LiFH fit that have appeared in the literature. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 8439-8446 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: In this article we extend previous studies of the dynamical instabilities to incorporate the roles of the tipping angle, the overall shape of the sample, (optional) pulsed field gradients in various directions, and radiation damping. The linear stability for small perturbations is discussed analytically in detail, and numerical simulations are used to have a glimpse at the turbulent spin motion for large perturbations. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 8455-8462 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: In this paper we calculate the contribution Ds to the self-diffusion coefficient D0 from the coupling of solute motion to solvent density fluctuations in an infinitely dilute near-critical binary mixture using the methods of fully renormalized kinetic theory in the disconnected approximation. The expression for Ds is found to be similar to mode-coupling expressions for diffusion coefficients in dense or supercooled liquids. As a function of the solvent density ρ, and along the critical isotherm, D0 exhibits an anomalous decrease in the vicinity of the critical point that originates in the vanishing of Ds according to the scaling relation Ds∼(ρ−ρc)2, where ρc is the critical density. An analogous decrease in D0 has recently been observed in the simulations of Drozdov and Tucker [J. Chem. Phys. 114, 4912 (2001)] on a neat liquid of Lennard-Jones particles, and has been ascribed to local density inhomogeneities in the medium. © 2002 American Institute of Physics.
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    The Journal of Chemical Physics 116 (2002), S. 8504-8508 
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    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Large-scale molecular dynamics simulations are performed to predict the structural and thermodynamic properties of liquid krypton using a potential energy function based on the two-body potential of Aziz and Slaman plus the triple-dipole Axilrod–Teller (AT) potential. By varying the strength of the AT potential we study the influence of three-body contribution beyond the triple-dipole dispersion. It is seen that the AT potential gives an overall good description of liquid Kr, though other contributions such as higher order three-body dispersion and exchange terms cannot be ignored. © 2002 American Institute of Physics.
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  • 197
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    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 116 (2002), S. 8523-8532 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We observed high N contents inside BN fullerenelike multilayered nanocages (ca. 30–100 nm) formed by reacting CNx nanotubes (x≤0.1) and B2O3 in a N2 atmosphere at 1985–2113 K. High-resolution transmission electron microscopy (HRTEM), electron energy loss spectroscopy, energy dispersion x-ray spectroscopy, electron diffraction analysis, spatially resolved energy-filtered TEM, and in situ TEM electron irradiation studies suggest that super-high pressures (of several GPa) are generated inside nanocages, responsible of crystallizing gaseous nitrogen trapped within the BN shells. In addition, high-pressure-induced phase transformation of graphiticlike BN into diamondlike cubic BN occurs inside the nanocages. Thus, BN nanocages play an unusual role of super-high-pressure nanocells. © 2002 American Institute of Physics.
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  • 198
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    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 116 (2002), S. 8588-8595 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The mean spherical approximation (MSA) was used to investigate the phase behavior of charged colloidal systems with and without added salt. The competition between cohesive Coulomb interactions and stabilizing entropic and hard-core interactions controls the stability of the system and under certain circumstances, a liquid–gas-type phase transition can occur. The critical parameters and phase diagrams in the MSA obtained via the internal energy path, are compared with two-component Monte Carlo simulations and other theoretical approaches. © 2002 American Institute of Physics.
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  • 199
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    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 116 (2002), S. 845-853 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: In this paper the microscopic dynamics of methyl side groups in polyisoprene is studied by means of inelastic neutron scattering. By combining time-of-flight and backscattering technique a range of four decades can be obtained (0.2 ps–2 ns). The two experimental results were combined in the time domain by using an inverse Fourier transform. Multiple scattering effects were treated by a novel procedure acting on the time-dependent intermediate scattering function S(Q,t). In the description of the data incoherent and coherent scattering from "fixed" atoms was taken into account, i.e., atoms in the main chain that move too slow to be observed in the dynamical window of the experiment. In this way good agreement with the rotation rate distribution model of a threefold jump could be obtained. Seeming discrepancies of the elastic incoherent structure factor vanish after the corrections mentioned above. The distribution of activation energies can be expressed as a Gaussian with an average of 9.7 kJ/mol and a width of 30%. It turns out that the width calculated by the model fit of the data depends on the use of the multiple scattering correction while the average activation energy can also be obtained reliably without that correction from high Q spectra. © 2002 American Institute of Physics.
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  • 200
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 116 (2002), S. 8255-8261 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A direct inversion iterative subspace version of the relaxed constrained algorithm is found to be a very powerful convergence acceleration technique for the solution of the self-consistent field equations found in the Hartree–Fock method and Kohn–Sham-based density functional theory (KS-DFT). The present algorithm, abbreviated EDIIS, is benchmarked against the direct inversion iterative subspace method based on the commutator of the density and Fock matrices developed by Pulay (DIIS). Our findings indicate that while EDIIS is able to rapidly bring the density matrix from any initial guess to a solution region, the DIIS method is faster when the density matrix is close to convergence. Consequently, we propose a combination of EDIIS and DIIS methods, which is both very robust and highly efficient. We also show how EDIIS can detect the presence and determine the value of fractional occupations in KS-DFT. © 2002 American Institute of Physics.
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