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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8673-8679 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A master equation (ME) approximation describing the effect of vibrational/rotational (V/R) relaxation on unimolecular reactions in the gas phase is presented. It is demonstrated that some forms of ME can be transformed exactly to an effective two-dimensional Smoluchowsky type differential equation (SE) in the V/R energy variables, V and R. The SE allows interpretation in a unified way of both weak and strong collision limits. Analytical expressions for the unimolecular reaction rate coefficient ku(T) are derived for simple models of the energy dependence of the microscopic reaction rate k(V,R) and V/R density of states. For realistic k(V,R) (obtained from flexible transition state theory for the reaction CH4→ArCH3+H) the SE is solved numerically. Both numerical and analytical calculations show that the collisional rotational energy transfer can, in principle, affect the rate coefficient ku(T). However, for the particular reaction considered, ku is found to be less sensitive to changes in the average rotational energy transfer than to changes in the average vibrational energy transfer. Furthermore, the strong collision limit is achieved only for unrealistically large values of the average rotational energy transfer. This means that it is a good approximation in this case one can treat V/R energy transfer and dissociation by a one-dimensional master equation in total energy.
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  • 2
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    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8704-8709 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Ab initio molecular electronic structure theory has been used to study the AlOH–HAlO unimolecular isomerization reaction on the singlet ground state potential energy surface. Electron correlation effects were included via configuration interaction and coupled-cluster methods. Basis sets as complete as triple zeta plus two sets of polarization functions and a set of higher angular momentum functions [TZ(2df,2pd)] were employed. The classical barrier for hydrogen migration from X˜ HAlO to X˜ AlOH is predicted to be 38.4 kcal mol−1 using the TZ(2df,2pd) basis set with the coupled-cluster method including all single and double excitations with the effect of connected triple excitations included perturbatively [CCSD(T)]. After correction for zero-point vibrational energies (ZPVEs), an activation energy of 36.6 kcal mol−1 is obtained. The ΔE for isomerization is −42.2 (−40.5 with ZPVE correction) kcal mol−1 at the same level of theory. The dipole moments of HAlO and AlOH in their equilibrium geometries are 4.525 and 1.040 Debye, respectively, at the same level of theory. A comparison is also made between a theoretically predicted harmonic vibrational frequency and a recently determined experimental fundamental frequency for X˜ AlOH.
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  • 3
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8734-8741 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The theory of bonding in endohedral complexes is generalized to carbon clusters other than C60. Parameters that determine electronic properties of endohedral complexes, such as their complexation energies, shifts in ionization potentials, and dipole moments, are calculated for the C70, C76, C78 (2 isomers), C82 and C84 (2 isomers) host cages. In addition, conditions for the presence/absence of electron transfer in endohedral complexes of these carbon clusters are derived and orientational preferences of guests are determined. Trends in the calculated quantities associated with increasing host cage sizes are discussed.
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  • 4
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8749-8760 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The characteristics of the first and second derivatives of the canonical orbital energies for the closed shell self-consistent-field (SCF) wave function have been studied. The first derivatives of the orbital energies were determined analytically and the second derivatives by the finite difference method. These derivatives were transformed from the Cartesian coordinate system to the normal coordinate system for a variety of stationary points. It is demonstrated that the first and second derivatives of the orbital energies in terms of the normal coordinates provide very useful chemical information concerning the molecular structures and unimolecular reactions for a range of chemical species. Similarities and differences between the present approach and Mulliken–Walsh method are also discussed.
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  • 5
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8785-8789 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The lowest 5Π and 5Σ+ states of CO are characterized using very large one-particle basis sets and the internally contracted multireference configuration–interaction treatment of electron correlation. It is found that the (1)5Σ+ state is weakly bound (De=572 cm−1) with an re of 4.76 a0, in good agreement with earlier theoretical calculations by Rosenkrantz et al. [Theor. Chim. Acta 82, 153 (1992)]. The (1)5Π state (hereafter designated a‘ 5Π) has a weakly bound outer well (De=18 cm−1, re=5.80 a0) and a significantly bound inner well (De=6043 cm−1, re=2.76 a0). It is shown that the emission spectrum between about 360 and 520 nm observed by Bahrdt et al. [Chem. Phys. 144, 273 (1990)] can be assigned to the a‘ 5Π−a' 3Σ+ and a‘ 5Π−d 3Δ transitions. Franck–Condon factors are presented to aid in the experimental identification of the a‘ 5Π state by absorption from the low-lying triplet states of CO.
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  • 6
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8810-8818 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The insertion of a nickel atom in the CH bond of CH4 is calculated using density functional theory by determining the transition state and the dissociated state of HNiCH3. A barrier for nickel insertion of 40.7 kJ/mol is found and its origin is discussed. The insertion is exothermic by 34.0 kJ/mol. From the potential energy surface at the transition state and the dissociated state vibrational and rotational frequencies are obtained. Unimolecular and bimolecular transition state theory is used for the calculation of rate constants, sticking coefficients, and activation energies for the nickel insertion reaction as well as the nickel elimination reaction. Activation energies for nickel insertion in both CH4 and CD4 are small compared with other theoretical work. A moderate kinetic isotope effect for the insertion reaction is found when all hydrogens are substituted by deuterium, whereas no significant kinetic isotope effect is found for nickel elimination. Hydrogen tunneling corrections on rate coefficients are also evaluated, but their effect is negligible. Sticking coefficients are small, which is consistent with experimental sticking coefficients of CH4 on nickel surfaces.
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  • 7
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The first order dimer model made by Stiles and Buckingham for predicting optical activity has been extended up to an infinite order N-mer model within the framework of the Fano–DeVoe type dipole approximation. The present formalism involves four mechanisms (1) the Kirkwood–Moffitt coupled oscillator mechanism through the Coulombic interactions; (2) the local asymmetric mechanism due to the intrinsic monomer optical activity; (3) the indirect electric–magnetic coupling mechanism through the Coulombic interactions; (4) the Condon, Alter, Eyring (CAE) direct electric–magnetic coupling mechanism through the electrostatic interactions between the upper to upper state transition moments on a certain site and the permanent dipole moments on the other sites. However, mechanism (4) must be excluded if we follow the Fano–DeVoe approximation, whereas it is indispensable for circular dichroism (CD) calculations of polypeptides to incorporate the CAE electric–magnetic coupling mechanism. This requirement is attained by assuming the intra-amide monomer intensity borrowing of the very weak 210 nm region nπ* state from the strong 190 nm region ππ* state through the CAE electrostatic interactions on the basis of the Schellman–Oriel perturbation equation and the Bayley–Nielsen–Schellman secular matrix theory. The present theory has particularly well predicted the CD band shapes of α-polypeptides even with the dipole approximation. The contributions due to the asymmetric fields have been found to become specifically large, while the coupled oscillator mechanism has been calculated to be a leading term.
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  • 8
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8888-8891 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The mobilities of the ions SF2+, SF3+, SF4+, SF5+, and S2F7+ in SF6 gas have been measured using an electrical shutter method with an electron ionization ion source. Measurements were made at gas temperatures of 22–36 °C over a range of E/N, the ratio of electric field strength to gas number density, from 55–550 Td (1 Townsend (Td)=10−17 V cm2) and over the pressure range 0.1–0.7 Torr. The zero-field reduced mobilities of SF2+, SF3+, SF4+, SF5+, and S2F7+ were determined to be 0.64, 0.61, 0.64, 0.65,and 0.48 cm2 V−1 s−1, respectively.
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  • 9
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8910-8918 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: It is customary in the physicochemical literature to define the static transverse dielectric function of a polar fluid according to the relation εT(k) = 1 + 4πβST(k), where β=(kBT)−1 and ST(k) is a measure of the static fluctuations of the Fourier components of the transverse part of the electric polarization field in the fluid. In this work we evaluate εT(k) for models of two classes. (1) In a DS model each molecule is a hard sphere with a point dipole at its center. It is the simplest representative of models in which the long range intermolecular interactions are generated by a set of point multipoles located at a single point in the molecule. In this case ST(k) is SM,T(k), the static correlation function of the transverse part of the dipole polarization density Mˆ(k). (2) In a ζDS model fluid, comprising nonideal dipolar hard spheres, the long range interactions are accounted for by two opposite partial charges on either side of the sphere's center and separated by a distance l. The ζDS model is the simplest interaction site model (ISM) of a polar fluid. For an ISM the relevant structure factor ST(k) is SPμ ,T(k), the static correlation of the transverse part of the full electric polarization density vector Pˆμ(k). Here we compare εT(k) for DS and ζDS models with the help of the mean spherical approximation for the required structure functions. The ζDS–DS difference in εT(k) at large k is found to parallel the behavior of the static longitudinal dielectric function εL(k). However, εT(k), unlike εL(k), is a damped oscillatory function of k with no poles on the real k axis.
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  • 10
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8963-8969 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The Fokker–Planck equation for a thermalized ensemble of Brownian particles is exactly solved by a method of (nontruncated) moments, using the expansion of the velocity distribution in Hermite polynomial eigenfunctions. We explicitly studied only the cases of linear and quadratic external potentials bounded by a reflecting wall. The double Laplace transforms (with respect to position and time) of the moments of the velocity distribution were obtained from the generating function, which was found to be a functional only of the density of particles. The closed equation for the density can be derived for the thermalized system. The solution of this equation (obtained by means of a Laplace transform in time) is analyzed in the long and short time limits. The (truncated) moment solution for a nonthermalized problem is also discussed. In the long time limit, the solutions for both thermalized and nonthermalized systems approach the Smoluchowski diffusive approximation.
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  • 11
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8994-9013 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We develop a new density functional treatment for the liquid–liquid interface of phase separated binary polymer blends. In contrast to previous density functional theory studies of these interfaces, we incorporate the compressibility (i.e., "equation of state effects'') of the system through use of a compressible version of Flory–Huggins theory. The introduction of compressibility is demonstrated to severely complicate the mathematical description. The coupled, nonlinear Euler–Lagrange equations for the interfacial profile and tension are shown to become numerically unstable and permit analytic solution in the asymptotic profile wings. Our computations are limited to symmetric binary blends because this restriction enables us to compute numerically the central portion of the interfacial profile and thereby test more general variational methods (applicable also to unsymmetric blends) that we develop for computing the full interfacial profile and the interfacial tension. The total density of the symmetric blend is found to be reduced in the profile center relative to the bulk density by 0.4%–1.5%. While this total density fluctuation costs free energy, it reduces unfavorable polymer–polymer contacts, thereby diminishing the total interfacial tension. The applicability of our approximate scheme is tested.
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  • 12
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 9018-9029 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The chemisorption properties of carbon monoxide on two vicinal Ni(100) surfaces have been studied with surface infrared reflection–absorption spectroscopy and low energy electron diffraction. For coverages ≤0.50 monolayer, equilibrium adlayers are formed in which CO populates atop sites on the low-index (100) terrace, as well as twofold bridging sites along both the highly-kinked and close-packed step edges of the Ni[(100)-1.4°(01¯0)] and Ni[(100)-9°(01¯1¯)] surfaces investigated. Low energy electron diffraction (LEED) measurements confirm that all three long-range structures established on the (100) surface—c(2×2) at 0.50 ML, hexagonal at 0.61 ML, and compressed-hexagonal at 0.69 ML—are also formed on the Ni [(100)-1.4°(01¯0)] surface. On the Ni [(100)-9°(01¯1¯)] surface, however, only the ordered c(2×2) structure appears. A simple Arrhenius analysis of the relative population of step and terrace sites estimates a small binding energy preference for populating step sites. This weak preference is of comparable magnitude to the CO–CO interactions that produce long range structures. To evaluate quantitatively the binding energy difference between adsorption at step and terrace sites, step adsorption isotherms are measured as a function of total coverage at select temperatures over the 90–300 K window. The isotherms are modeled with simple Monte Carlo simulations of adsorption on stepped surfaces, which include a 1.0 kcal/mol binding energy preference for step sites. The data and simulations indicate that the primary role played by the steps in the chemisorption of CO is to serve as nucleation centers for island growth.
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  • 13
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8031-8036 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The availability of the easily implemented Gaussian-2 (G2) methodology has made it possible for the nonspecialist to calculate accurate heats of formation for many molecules on workstations. In order to quantify its performance for transition state structures, we have used G2 and a modified G2 on several transition states whose structures and energies have been well characterized either by experiment or multireference configuration interaction studies. The G2 method performs well in predicting energies of transition states (even for nonisogyric reactions), with an absolute average deviation of 1.5 kcal/mole in the classical barrier height for the cases studied, while it is less successful in predicting geometries and frequencies. We investigated modifying the G2 method for use with transition states by using QCISD/6-311G(d,p) geometries and frequencies instead of MP2/6-31G(d) geometries and scaled HF/6-31G(d) frequencies. The QCISD geometries and frequencies agree well with values from the literature, and this modified G2 procedure offers improved performance in predicting transition state energies.
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  • 14
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8051-8056 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using sophisticated ab initio methods, the equilibrium structure of the ClF2 radical has been predicted to be bent, confirming previous experimental and theoretical work. The single, double and perturbative triple excitation coupled cluster level of theory along with a triple-ζ plus double polarization basis set gives the geometrical parameters re=1.756 A(ring) and θe=151.8°. At the same level of theory, harmonic vibrational frequencies were predicted to be 536, 243, and 568 cm−1 for the symmetric stretch, bend and asymmetric stretch, respectively. In addition to this high level study of the harmonic vibrational frequencies, theoretical analyses of anharmonic terms have been included in order to help settle the controversy surrounding experimental assignments of the fundamental vibrational frequencies. This research supports Mamantov's experimental assignment of the bending and symmetric stretching fundamental, over the experimental objections of Prochaska. The vibrational frequency splitting due to 37ClF2 was also studied indicating that only the splitting of the bending and asymmetric stretching modes should be readily observable experimentally. Dipole moments and infrared (IR) intensities were also predicted.
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  • 15
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    The Journal of Chemical Physics 98 (1993), S. 8080-8095 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The hypernetted chain (HNC) integral equation is solved for a variety of systems including the simple fluid of hard spheres with attractive Yukawa tail, the symmetrical and highly asymmetrical mixtures of charged particles, and the mixtures of hard spheres with positively nonadditive diameters. All these systems exhibit a liquid–gas or fluid–fluid phase separation. We are concerned with the behavior of the HNC solution near the two-phase region in the phase diagram. In all cases, the HNC equation does not have solutions inside a certain region whose boundary line is not a spinodal line. As the boundary is approached, the isothermal compressibility deduced from the compressibility route does not diverge, but tends to finite values. The isotherms and isochores terminate at the boundary line in square root branch points. This behavior is directly correlated to the existence of multiple HNC solutions. Physical and nonphysical solutions coincide on the boundary line. This universal HNC behavior is compared with that of the mean spherical approximation and Percus–Yevick integral equations.
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  • 16
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8119-8125 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We present computer simulation results of the pair-connectedness function and the two-point cluster function for random media, consisted of equisized particles of adhesive sphere model. The pair-connectedness function P(r1,r2) is defined as that the quantity ρ2 P(r1,r2)dr1 dr2 represents the probability of finding two particles centered in the volume elements dr1 and dr2 about r1 and r2, respectively, and are physically connected. On the other hand, the two-point cluster function C2(r1,r2) gives the probability of finding two points at positions r1 and r2, in the same cluster of one of the phases. Data are compared with the analytical results from the Percus–Yevick (PY) approximation. In low densities, Monte Carlo data reasonably agree with the PY approximation results, while in high densities near percolation thresholds, data significantly deviate from the analytical results.
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  • 17
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    The Journal of Chemical Physics 98 (1993), S. 8186-8193 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We study the time-dependent intermediate scattering function of a semidilute colloidal suspension of hard spheres with neglect of hydrodynamic interactions. The dynamics of the suspension is assumed to be governed by the generalized Smoluchowski equation. The Laplace transform of the scattering function involves the static structure factor and an irreducible memory kernel. The latter is approximated by the first term of its expansion in powers of volume fraction. The time-dependent scattering function is found by integration over the spectrum of relaxation rates.
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  • 18
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    The Journal of Chemical Physics 98 (1993), S. 8194-8198 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We describe a new gradient technique to determine the coexistence curve of partially miscible liquid mixtures. The method allows this determination to be done using a single sample and gives the proper slice (temperature-order parameter) of the coexistence surface, in contrast to the conventional methods. We employed this technique to determine the coexistence curve of a ternary microemulsion, consisting of water, benzene, and benzyldimethyl-n-hexadecyl ammonium chloride (BHDC), in a narrow temperature range close to the critical point. The value of the exponent β describing the coexistence curve was found to be 0.34±0.08.
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  • 19
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    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 8236-8243 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The crystal structure of deuterated benzene has been investigated over the complete temperature range 4–280 K. Our results are in excellent agreement with previous studies, recorded at a limited number of temperatures, and display a smooth variation of the lattice parameters over the complete temperature range. No evidence of the suggested low-temperature phase transitions, or marked premelting effects have been found. Detailed measurements of the lattice parameters close to the melting point display an anomalous behavior of the b lattice parameter and the orientation of the molecules which is believed to be evidence of a disordering transition at temperatures above the melting point.
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  • 20
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    The Journal of Chemical Physics 98 (1993), S. 8308-8323 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A combination of experimental methods has been employed for the study of Cl2 adsorption and reaction on Si(100)–(2×1). At 100 K, Cl2 adsorption occurs rapidly to a coverage of ∼0.7 Cl/Si. This is followed by slower adsorption kinetics with further Cl2 exposure. Two Cl adsorption states are observed experimentally. One of the adsorption states is terminally bonded Cl on the inclined dangling bond of the symmetric Si2 dimer sites, with a vibrational frequency, ν(SiCl) of 550∼600 cm−1. These bonded Cl atoms give four off-normal Cl+ ESDIAD emission beams from the orthogonal domains of silicon dimer sites. The Si–Cl bond angle for this adsorption configuration is estimated to be inclined 25°±4° off-normal. The second Cl adsorption state, a minority species, is bridge bonded Cl with ν(Si2Cl) of ∼295 cm−1 which produces Cl+ ion emission along the surface normal direction. Both adsorption states are present at low temperatures. Irreversible conversion from bridge bonded Cl to terminally bonded Cl begins to occur near 300 K; the conversion is complete near ∼673 K. LEED studies indicate that the (2×1) reconstruction for the substrate is preserved for all Cl coverages. The most probable Cl+ kinetic energy in electron stimulated desorption, ESD, is 1.1−+0.30.6 eV. A significant adsorbate-adsorbate quenching effect reducing the Cl+ ion yield in ESD occurs above a Cl(a) coverage of ∼0.5 ML (monolayer) due to interadsorbate interactions. The maximum Cl+ yield is about 4×10−7 Cl+/e at an electron energy of 120 eV. Temperature programmed desorption results show that SiCl2 is the major etching product which desorbs at about 840 K.
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  • 21
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    The Journal of Chemical Physics 98 (1993), S. 399-408 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The nature of the C7H7+ ion created through resonant dissociative multiphotoionization of para-chlorotoluene by an ultraviolet (UV) laser was investigated thanks to its interaction with a second laser beam. The dissociation pattern corresponding to one or several photon absorption could be observed. Cross section for the one-photon absorption in the 265/530 nm range revealed the presence of the tropylium and benzyl isomers and suggested they possessed substantial internal energy. This was confirmed by the study of the C7H7++hν(large-closed-square)C5H5++C2H2 reaction, and more precisely of its rate and of the kinetic energy released. A ladder switch mechanism for the three-photon dissociative ionization of para-chlorotoluene leading to C7H7+ is shown to agree with our results.
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  • 22
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    The Journal of Chemical Physics 98 (1993), S. 420-426 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Analytical rate coefficient expressions are derived at low temperatures for the fast reactions of a 2Π molecule with each of a structureless ion, a 2Π molecule, and a 1Σ molecule. The procedure, based on classical capture theory, involves perturbation theory and simple long-range electrostatic potential terms for the various interactions. The open-shell nature of the reactant molecules is fully considered. The predictions made are contrasted with those quoted previously for the equivalent reactions involving 1Σ molecules and interesting differences in the temperature dependencies of the rate coefficient are highlighted.
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  • 23
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    The Journal of Chemical Physics 98 (1993), S. 437-443 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: High level ab initio calculations have been carried out to assess the pairwise additivity of potentials in the attractive or well regions of the potential surfaces of clusters of helium atoms. A large basis set was employed and calculations were done at the Brueckner orbital coupled cluster level. Differences between calculated potentials for several interacting atoms and the corresponding summed pair potentials reveal the three-body and certain higher order contributions to the interaction strengths. Attraction between rare gas atoms develops from dispersion, and so helium clusters provide the most workable systems for analyzing nonadditivity of dispersion. The results indicate that the many-body or nonpairwise contributions tend to be less than a few percent of the attractive interaction across regions around the minima of the potential energy surfaces of small clusters. Dipole–dipole–dipole dispersion and dipole–dipole–quadrupole dispersion are noticeable parts of the small three-body terms.
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  • 24
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    The Journal of Chemical Physics 98 (1993), S. 9094-9106 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The problem of simultaneous phase separation and ordering kinetics in mixtures containing a nematic component is addressed through the introduction of a time-dependent Landau–Ginzburg model. Dynamic equations for the time evolution of orientation and concentration fluctuations are given; the solution to these equations leads to explicit expressions for the structure factors for concentration and orientation. It is shown that the theory shares some salient features with the Cahn theory of spinodal decomposition. A simulation of a quenching experiment is performed and the time evolution of the structure factors during spinodal decomposition is calculated. Relevant small angle light scattering experiments which could be used to test the model are discussed.
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  • 25
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    The Journal of Chemical Physics 98 (1993), S. 9080-9093 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The thermodynamics of symmetric polymer blends is investigated using the polymer reference interaction site model integral equation theory with the new molecular closures presented in the previous paper. In contrast to the atomic mean spherical approximation reported earlier by Schweizer and Curro [J. Chem. Phys. 91, 5059 (1989); Chem. Phys. 149, 105 (1990)] (in which the critical temperature is proportional to the square root of the degree of polymerization), the molecular closures predict a linear dependence of the critical temperature on the degree of polymerization, in agreement with classical mean field theory. Detailed numerical calculations using the reference molecular mean spherical approximation (R-MMSA) and the reference molecular Percus–Yevick (R-MPY) closures are presented for the intermolecular structure and effective chi parameter in symmetric blends of semiflexible chains. For the symmetric blend, the R-MMSA closure is almost an integral equation realization of mean field theory, consistent with the analytical results presented in the previous paper. With the R-MPY closure, at low densities, the effective chi parameter is significantly renormalized down from its mean field value and displays a strong composition dependence. As the density is increased, both the renormalization of the effective chi parameter and its composition dependence become weaker. These trends are consistent with recent computer simulations. The influence of chain aspect ratio and the precise choice of intermolecular potentials on blend thermodynamics and phase separation are also explored. With the exception of the composition dependence of the effective chi parameter in the R-MPY theory, the analytical thread calculations are shown to be in qualitative, and sometimes quantitative, agreement with all the numerical results for symmetric blends.
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  • 26
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    The Journal of Chemical Physics 98 (1993), S. 9126-9133 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The thermodynamics of monodisperse solutions of polymers in the neighborhood of the phase separation temperature is studied by means of Wilson's recursion relation approach, starting from an effective φ4 Hamiltonian derived from a continuum model of a many-chain system in poor solvents. Details of the chain statistics are contained in the coefficients of the field variables φ, so that the parameter space of the Hamiltonian includes the temperature, coupling constant, molecular weight, and excluded volume interaction. The recursion relations are solved under a series of simplifying assumptions, providing the scaling forms of the relevant parameters, which are then used to determine the scaling form of the free energy. The free energy, in turn, is used to calculate the other singular thermodynamic properties of the solution. These are characteristically power laws in the reduced temperature and molecular weight, with the temperature exponents being the same as those of the 3d Ising model. The molecular weight exponents are unique to polymer solutions, and the calculated values compare well with the available experimental data.
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  • 27
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    The Journal of Chemical Physics 98 (1993), S. 9167-9176 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The interaction of oxygen with the Cu(111) surface in ultrahigh vacuum (UHV) has been studied in the temperature range 400〈T〈800 K using second-harmonic generation (SHG) and x-ray photoelectron spectroscopy (XPS). When the clean surface is exposed to oxygen at pressures between 5×10−8 and 10−5 Torr and for T〈500 K, the SHG intensity decreases monotonically with exposure by more than one order of magnitude to a value which has no measurable temperature dependence. For T(approximately-greater-than)500 K, the SHG intensity passes through a minimum before achieving this constant value. The observation of this minimum is interpreted in terms of an outward relaxation of the Cu(111) surface as oxygen penetrates the subsurface region. When UHV conditions are restored for T(approximately-greater-than)600 K, the SHG intensity reverses its temporal dependence. These observations are consistent with initial incorporation of atomic oxygen into the subsurface region at a rate which is dependent on surface temperature and oxygen pressure and subsequent backdiffusion in UHV, driven by the oxygen concentration gradient near the surface. From experiments performed at different oxygen pressures and sample temperatures we establish rate constants for oxygen incorporation and surface outward relaxation as a function of temperature. The kinetics of oxygen incorporation determined from changes in the SHG intensity are compared with those derived elsewhere from ellipsometry studies. Differences yielded by the two experimental techniques are related to differences in monitored depths. Complementary XPS experiments suggest that sites occupied by the subsurface oxygen are characterized by tetrahedral symmetry.
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  • 28
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    The Journal of Chemical Physics 98 (1993), S. 9218-9219 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Gaseous benzene and benzene-d6 have been photolyzed with a 158 nm laser. Transient species have been found to have decay rate constants (2.2±0.2)×107 s−1 and (0.7±0.2)×107 s−1, respectively. These rates are explained in terms of the C–H/C–D dissociation by the hot molecule mechanism.
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  • 29
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    The Journal of Chemical Physics 98 (1993), S. 9222-9222 
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  • 30
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    The Journal of Chemical Physics 98 (1993), S. 9223-9223 
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  • 31
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    The Journal of Chemical Physics 98 (1993), S. 7699-7710 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The method of two-dimensional exchange spectroscopy under condition of magic angle sample spinning (MAS) and synchronization of the mixing time with the rotor period is extended to spin I=1 nuclei. Theoretical equations are derived for the cross peak intensities as a function of the magnetic and kinetic parameters of the system and the method is demonstrated on a number of deuterated compounds. Dimethylmalonic acid–d6 is first used to illustrate the effect of rotor synchronization by the complete absence of cross peaks when no exchange takes place. The method is then applied to two dynamic systems, viz. dimethylsulfone–d6 and thiourea–C6D12 inclusion compound. The experimental results are compared with simulations as well as with analogous experiments on nonspinning samples. Since chemical shift effects are often negligible in deuterium NMR the time domain sampling can in principle be reduced to the number of the desired spinning sidebands, resulting in considerable time savings. The main advantage of the method is the gain in sensitivity at the expense of the characteristic ridge pattern of static two-dimensional exchange experiments. The gain in sensitivity may be sufficient for performing such experiments on deuterium in isotopically normal compounds. The feasibility of such experiments is demonstrated by the recording of a one-dimensional deuterium MAS spectrum of a nonenriched sample.
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  • 32
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    The Journal of Chemical Physics 98 (1993), S. 7730-7742 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The 488 and 514 nm negative ion photoelectron spectra of FeCO−, obtained at an instrumental resolution of 5 meV (40 cm−1), show vibrationally resolved transitions from the anion ground state to the ground state and a low-lying excited state of the neutral molecule. The ground state of FeCO is assigned as the 3Σ− state and the excited state, lying 1135±25 cm−1 higher in energy, as the 5Σ− state. The fundamental vibrational frequencies are νCO=1950±10, νFeC=530±10, and νbend=330±50 cm−1 in the 3Σ− state, and νCO=1990±15, νFeC=460±15, and νbend=180±60 cm−1 in the 5Σ− state. Principal force constants are estimated from these results. Based on a Franck–Condon analysis of the spectrum and other considerations, the Fe–C bond is determined to be 0.15±0.04 A(ring) shorter, and the C–O bond 0.05±0.02 A(ring) longer, in the 3Σ− state than in the 5Σ− state. These results demonstrate the importance of sdσ hybridization in reducing the σ repulsion between the metal 4s electron and the CO 5σ lone pair, a mechanism that is available only when the electrons in the singly occupied 3dσ and 4s orbitals are singlet coupled as in the 3Σ− state. The FeCO− anion displays a high Fe–C stretching frequency (465±10 cm−1), as well as an asymptotic Fe–CO bond energy, a bending frequency (230±40 cm−1) and equilibrium bond lengths intermediate between those in the 3Σ− and 5Σ− states. Since the FeCO− ground state is assigned as a 4Σ− state in which the extra electron occupies a σ orbital, these results indicate that the increased σ repulsion is partially offset by stronger metal–CO π bonding in the anion. The electron affinity of FeCO is measured to be 1.157±0.005 eV.
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    The Journal of Chemical Physics 98 (1993), S. 7763-7772 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The two-color (1+1') threshold photoelectron spectra of naphthalene in a supersonic free jet have been recorded via nine vibronic levels of the S1 electronic state up to about 1420 cm−1 above the S1 band origin. The threshold photoelectron spectra recorded via the S1 band origin and via totally symmetric ag vibronic levels show significant intensity in Δν=+1 transitions in nontotally symmetric vibrations having b1g symmetry indicating that the ionization transition gains significant intensity through a vibronic coupling mechanism between the two lowest doublet cationic states. The strongest departure from the expected Δν=0 propensity in the threshold photoelectron spectra occurs through excitation of the totally symmetric 8 mode having ag symmetry indicating that a considerable displacement occurs along the normal coordinate of this 8 mode upon ionization from the S1 state. The superior resolution of the threshold photoelectron technique over conventional photoelectron methods has allowed accurate values for the fundamental vibrational frequencies of naphthalene in its ground cationic state to be determined and it has also allowed a more rigorous investigation of the vibronic coupling mechanism that occurs between the two lowest doublet cationic states. Moreover, an improved value for the adiabatic ionization energy of naphthalene of 65 687±7 cm−1 (8.1442±0.0009 eV) has been determined.
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    Notes: The ground state geometries of small neutral Agn(n=2–9) and cationic Agn+ (n=2–9) clusters have been determined in the framework of the Hartree–Fock and complete active space self-consistent field (CASSCF) procedure employing a relativistic effective core potential (RECP) accounting for core–valence correlation effects (CVC). Similarities and differences between topologies of neutral and charged structures have been found. Large scale configuration interaction (CI) calculations for 5s electrons only have been carried out for determining stabilities and ionization potentials (IP). A comparison between predicted and measured observables allows tentative geometrical assignments. Structural and electronic properties of small Ia and Ib clusters are compared.
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    The Journal of Chemical Physics 98 (1993), S. 8154-8159 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Many important issues in the field of crystal growth and surface science can be interpreted satisfactorily on the basis of the surface free energy of solid–fluid interfaces. However, the values of energies are not always available either from theory or from experiment. In this paper, starting from the grand canonical partition function, a general expression of the surface free energy is derived within the framework of an inhomogeneous cell model. The results are applied to estimate surface free energies of metal-melt systems, which are compared with the experimental results of Turnbull. Our estimated results agree well in almost every case with Turnbull's results. Based on our model, various factors which may affect the surface free energy are discussed.
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    The Journal of Chemical Physics 98 (1993), S. 8262-8270 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Dynamics of amorphous cis-1,4-polybutadiene was studied by incoherent inelastic and quasielastic neutron scattering below 10 meV in a wide temperature range covering the glass transition temperature Tg. The spectra at low temperatures below Tg show a broad excitation peak at about 2–3 meV, which is the so-called low-energy excitation and believed to be an origin of anomalous thermal properties of amorphous materials at low temperatures. It was found that the temperature dependence of the low-energy excitation intensity can be normalized by the Bose factor at temperatures low enough below Tg. With increasing temperature, a very fast motion appears in the energy range below ∼4 meV at around the Vogel–Fulcher temperature T0, which is ∼50 K below Tg. This fast motion is often interpreted as the β process predicted by the mode coupling theory. In this paper, both the low-energy excitation and the fast motion were analyzed in terms of a common microscopic picture, i.e., an asymmetric double well potential. The natures of the two motions are discussed focusing on the relation between the two motions as well as the glass transition dynamics.
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    The Journal of Chemical Physics 98 (1993), S. 8330-8336 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The reactions O(1D)+HCl→OH+Cl (1a) and OCl+H (1b), O(1D)+DCl→OD+Cl (2a) and OCl+D (2b), and O(1D)+Cl2→OCl+Cl (3) are studied at an average collision energy of 7.6, 7.7, and 8.8 kcal/mol for (1), (2), and (3), respectively. H, D, and Cl atoms are detected by the resonance-enhanced multiphoton ionization technique. The average kinetic energies released to the products are estimated from Doppler profile measurements of the product atoms. The relative yields [OCl+H]/[OH+Cl] and [OCl+D]/[OD+Cl] are directly measured, and a strong isotope effect (H/D) on the relative yields is found. The fine-structure branding ratios [Cl(2P1/2]/[Cl(2P3/2)] of the reaction products are also measured. The results suggest that nonadiabatic couplings take place at the exit channels of the reactions (1a) and (2a), while the reaction (3) is totally adiabatic.
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    The Journal of Chemical Physics 98 (1993), S. 427-436 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A hybrid quantum/semiclassical method is proposed and applied to study realistically the dynamics of the three-fragment photodissociation process Ar...HCl+hν→Ar+H+Cl. In the method the hydrogen motion is treated by exact quantum mechanics, while the heavy atoms are described by semiclassical Gaussian wave packets. This treatment is expected to reproduce the main quantum features of the dynamics. Part of the wave packet is found to describe resonance events in which the light particle is temporarily trapped inside the Ar...Cl cage and oscillates periodically between the heavy atoms before it dissociates. Interference between frequency components of the H wave function that populate different resonance levels give rise to interesting quantum effects. Such effects appear in the angular distribution of the hydrogen fragment, which shows some diffraction oscillations, and scattering into classically forbidden regions. Quantum interferences between the resonances are also the cause of a pronounced structure of peaks in the H photofragment kinetic energy distribution (KED). Time-correlation functions of the wave functions involved are computed, and the implications for the absorption spectrum and its relation to the KED of the H atom are discussed. The results demonstrate the power and applicability of quantum/semiclassical time-dependent self-consistent-field (TDSCF) as a tool for studying the dynamics and spectroscopy of realistic molecular systems.
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    The Journal of Chemical Physics 98 (1993), S. 331-335 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A theoretical study is presented on the photodissociation dynamics of Cl2 in crystalline xenon at 100 K, and within a range of pressure between 0 and 100 kbar. Temperature/pressure ensemble molecular dynamics simulations were carried out. The potentials used were accurate enough to reproduce the experimental equation of state of solid xenon. The results show that the photodissociation quantum yield varies strongly with pressure, falling from 30% at zero pressure, to 2% at 12.5 kbar, and 0% at higher pressures. These yields are in good agreement with experimental measurements. This behavior is found to be due to the strong effect of pressure on the librational (rotational) amplitudes of the Cl2 molecule and to the sharp dependence of the photodissociation yield on the molecular orientation in the reagent cage.
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    The Journal of Chemical Physics 98 (1993), S. 336-341 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The mechanism of the resonance-enhanced two-photon ionization (RE2PI) and the dissociation of ammonia clusters has been investigated by using the two-color ionization technique and the reflectron time-of-flight mass spectrometer. The clusters are firstly excited to the intermediate state corresponding to the A˜ 1A2 state of an ammonia molecule. The lifetime of the intermediate species is found to be 〈10 ns for the production of NH4+ and (NH3)2+, and longer than 1 μs for (NH3)nNH4+ (1≤n≤6). This result implies that NH4+ is produced by the ionization of the dimer followed by the dissociation of NH2 , whereas the higher protonated cluster ions are produced by the second photon ionization of the (NH3)nNH4 radicals produced by the dissociation of the parent clusters in the intermediate state. The appearance potentials of (NH3)2+ and (NH3)nNH4+ (0≤n≤4) are also determined by two-color RE2PI technique. Those values are discussed in connection with the two possible mechanisms for the observed ion production, which confirms the scheme obtained from the lifetime measurement.
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    The Journal of Chemical Physics 98 (1993), S. 8660-8666 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A selected ion flow tube study has been carried out at 300 K of the reactions of some atomic and molecular positive and negative halogen ions with Cl2 and Br2 from which the rate coefficients k and ion product distributions have been determined. For the energetic F+ ion reactions, dissociative charge transfer is the dominant process, while for the Cl+ ions, only nondissociative charge transfer occurs. For the less energetic Br+ and I+ reactions, dihalogen molecular ions are important products. All these positive ion reactions proceed quite efficiently, i.e., the k are appreciable fractions of kc, their respective collisional rate coefficients, except for the reactions of Cl2 with the lower energy ions of the spin–orbit triplet of I+, i.e., I+(3P1,0), for which k∼0.07kc, this being due to the endothermicities of the reactions. The molecular ion Cl2+ undergoes rapid nondissociative charge transfer with Br2, a process which is, of course, endothermic for the reaction of Br2+ with Cl2 and so no reaction is observed. The less-energetic atomic negative ion reactions proceed—via atom exchange—in which the atomic negative ion of the reactant molecular species and a dihalogen molecule are produced. For those reactions that are exothermic, the k are, within error, equal to (2/3)kc, implying that they proceed via complexes which separate statistically back to reactants (1/3) and forward to products (2/3). Both the Br−+Cl2 and Cl−+Br2 reactions are somewhat less efficient (i.e., k〈2/3kc), a result of the slight endothermicities of the reactions. Of the molecular negative ion reactions, electron transfer is the major process in the Cl2− reaction with Br2, whereas the reaction of Br2− with Cl2 proceeds relatively slowly producing the triatomic ion BrCl2−.
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    The Journal of Chemical Physics 98 (1993), S. 7819-7825 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The distribution of the widths of N quasidegenerate metastable states decaying into a large number K of dissociation continua is studied in the framework of the random matrix theory. For strong overlap, the distribution of the imaginary parts of the eigenvalues of the effective Hamiltonian H−iΓ/2 is that of the eigenvalues of the width matrix Γ. The latter is found to belong to a model of random matrices proposed by Wigner and developed by Dyson. The analytical expression of the asymptotic density ρ(γ) for equal partial widths and N=K→∞ is a semicircular law centered at twice the mean width γ¯ times a function 1/γ. It predicts extensive fluctuations around the mean with a high density of small widths. As a result, the average survival probability of the metastable states lying within a narrow energy range decays more slowly than the exponential law which is assumed in the RRKM theory.
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    The Journal of Chemical Physics 98 (1993), S. 7855-7867 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Absolute cross sections are measured for the reactions of O2+(X 2Πg) with H2 , D2 , and HD from thermal energies to over 4 eV. The OH++OH, HO2++H, O++H2O, and H2O++O product channels (and the corresponding isotopic analogs) are observed, although H2++O2 is not. While the first three products appear at their thermodynamic thresholds, formation of H2O++O, the least endothermic channel, exhibits a barrier to reaction. In the HD system, the DO2+ product ion is strongly favored over the HO2+ product. Results for internally excited O2+ reactants, probably the a 4Πu state, are also presented. Analysis of the excitation functions, molecular orbital arguments, and statistical kinetic theories are used to understand the mechanisms and dynamics of this reaction. It is shown that the inefficiency of the O+ product channel is due to spin and symmetry constraints. The other three product channels proceed through a long-lived intermediate, but formation of this intermediate from reactants requires surmounting a barrier measured to be 1.1±0.1 eV. The intramolecular isotope effects are shown to be due to statistical and dynamic effects.
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    The Journal of Chemical Physics 98 (1993), S. 7898-7902 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Recrossings of the transition state are normally thought of as modifying the dynamical prefactor (transmission coefficient) which corrects the Rice–Ramsperger–Kassel–Marcus (RRKM) theory. Here, a semiclassical path analysis is used to show that recurrences to parts of phase space from which reactive transitions can occur also lead to fluctuations of the reaction rate about its microcanonical average. This result leads to a simple formula for the power spectrum of the rates.
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    The Journal of Chemical Physics 98 (1993), S. 7951-7957 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The protonation of N2O and the intramolecular proton transfer in N2OH+ have been studied using large basis sets in conjunction with second-order many-body perturbation theory (MP2), singles and doubles coupled cluster (CCSD), the augmented coupled cluster method [CCSD(T)], and complete active space self-consistent field (CASSCF) methods. It is shown that MP2 is inadequate even for HNNO+, which has a minor nondynamical correlation effect; for the transition state only CCSD(T) produces a reliable geometry due to serious nondynamical correlation effects. Harmonic frequencies accurate to 50 cm−1 or better are predicted for both protonated species. The proton affinity at 298.15 K is found to be 137.6 kcal/mol, in excellent agreement with the recent experimental redetermination of 137.3±1 kcal/mol; the HNNO+ isomer is found to be 4.4 kcal/mol above the HONN+ isomer, with an interconversion barrier of ∼89 kcal/mol, herewith confirming recent experimental evidence that both species occur together with an energy difference of 6±1.5 kcal/mol. Comparison of the traditional double-zeta plus polarization (DZP) basis and the newer correlation consistent polarized valence double zeta (cc-pVDZ) basis set appears to indicate that the latter might lead to more accurate geometries and harmonic frequencies, although a more detailed investigation would be needed before any definitive conclusions.
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    The Journal of Chemical Physics 98 (1993), S. 7958-7968 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A novel generalized valence bond wave function expressed in terms of local nonorthogonal orbitals is shown to attain nearly all of the correlation energy of a corresponding complete-active-space self-consistent-field (CASSCF) wave function. This new wave function allows for the local orbitals to variationally respond to different spin couplings. The result is a very compact description of correlation effects contained in complex CASSCF expansions. The CASSCF expansion is also shown to contain a description of resonance among nonorthogonal valence bond structures.
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    The Journal of Chemical Physics 98 (1993), S. 8347-8347 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A comment on recombination rate constant in liquid and gaseous krypton is presented.The problem is addressed from the point of re− encounter theory. (AIP) E
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    The Journal of Chemical Physics 98 (1993), S. 119-125 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Results of classical Monte Carlo simulations of Li atom doped fcc Ne solids are presented. Li atom trapping sites based on four-atom and six-atom vacancies required only minor relaxation of the matrix surroundings to reach equilibrium. Trapping sites based on one-atom and two-atom vacancies were unstable and rearranged to yield crowded versions of the relaxed four-atom trapping site. The lattice strain associated with the crowded trapping sites could be relieved by the incorporation of nearby additional vacancies. These results are all consistent with the intuitive concept of a minimum volume trapping site in a van der Waals guest/host system; for the Li/Ne system apparently at least four Ne atoms must be removed to accommodate a Li atom. In all cases, the energies of the trapped Li atoms were at least ≈0.25 eV above the energy of a Li atom separated from close-packed solid Ne, indicating that Li atoms are indeed unwelcome in solid Ne.
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    The Journal of Chemical Physics 98 (1993), S. 140-149 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Oscillatory bound→continuum emission from vibrational levels v'=0–6 of the B(2Σ+) state of InAr onto the repulsive walls of the X1(2Π1/2), X2(2Π3/2), and A(2Σ+) electronic states, has been measured. In the B(2Σ+)→X1(2Π1/2) spectrum, the intensity extrema have been associated with particular extrema and nodes of the radial wave functions of the emitting levels, and the resulting phase vs energy information directly inverted to yield a pointwise potential for the X1(2Π1/2) state. Analysis of the observed peak heights then showed that on the range 2.9–3.8 A(ring) the associated transition moment function is constant. The overlapping of the B(2Σ+)→X2(2Π3/2) and B(2Σ+)→A(2Σ+) spectra prevents application of the above inversion procedure, but reliable estimates of these two final-state potentials were obtained by matching quantum mechanical simulated spectra with experiment. The simulations also showed that the transition moment functions associated with all three transitions are of approximately equal strength.
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    The Journal of Chemical Physics 98 (1993), S. 158-163 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: In contrast to the CH4/argon system, methane and krypton form homogeneous solutions. Inelastic neutron scattering (INS) has been used to observe the concentration dependence of the rotational spectra of CH4 in krypton. The methane concentrations (0.3%, 3.2%, and 6.5%) were chosen such that the INS spectra are dominated by scattering from isolated defects and methane dimers. A model based on a Gaussian distribution of local orientational potentials reproduces the measured intensities well and enables the separation of the contributions of the different configurations to the scattering. It is demonstrated that the substitution of one krypton atom on the nearest-neighbor shell by a methane molecule reduces the energy of the J=1 level by about 5%.
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  • 52
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    The Journal of Chemical Physics 98 (1993), S. 186-200 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The photoionization and dissociation characteristics of (C2H2)n (n=2, 3, and 4) have been studied by the threshold photoelectron–photoion coincidence technique applied to a molecular beam. For photon energies between 10.20 and 11.27 eV, only dissociative ionization pathways were observed for the clusters; no direct ionization of (C2H2)2, (C2H2)3, and (C2H2)4 to the stable ions C4H4+, C6H6+, and C8H8+ was observed. The shape of the time of flight peaks is consistent with statistical dissociation dynamics, and statistical analysis of the fragment peak shapes suggests that the dimer, trimer, and tetramer produce the fragments C4H2+/C4H3+, C4H4+, and C6H6+, respectively. Consistent with these observations, ab initio calculations are presented which indicate that the neutral T-shaped dimer and triangular trimer geometries are unstable on the ionic potential energy surface, and indeed have vertical ionization energies well above the dissociation limits of many of their possible product channels. The statistical modeling of the C4H4+ peak width is consistent with a process in which the trimer neutral produces a C4H4+–C2H2 complex, which then dissociates via monomer evaporation without exploring any of the covalent C6H6+ potential energy surface, i.e., benzene ion is not formed. The heat of formation of the observed C4H4+ daughter is estimated to be 1240±15 kJ/mol, indicating that it is cyclobutadiene, butatriene, or vinylacetylene ion. The peak width of C6H6+ is also analyzed, and suggests a process whereby the tetramer produces a C6H6+–C2H2 complex, which dissociates via monomer evaporation without exploring any of the covalent C8H8+ potential energy surface. The heat of formation of the C6H6+ daughter fragment is estimated as 1160±15 kJ/mol, which is consistent with the formation of benzvalene ion.
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  • 53
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    The Journal of Chemical Physics 98 (1993), S. 201-205 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A three-dimensional quantum mechanical study of the control of a branching photochemical reaction H+OD←DOH→D+OH is presented. It is shown that with two laser pulses, one pulse used to generate a superposition of the (0,2,0) and the (1,0,0) states, and the other, a VUV pulse, used to dissociate the molecule by exciting it to the B continuum, it is possible to control which of two chemical channels is preferred. The control parameters used are the center frequency of the excitation laser and the time delay between the two pulses. For the above superposition state, a combination of a 200 fs excitation pulse and a 50 fs dissociation pulse is found to yield the widest (10% to 90% yield in the H+OD channel) range of control, essentially irrespective of the photolysis wavelength.
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  • 54
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    The Journal of Chemical Physics 98 (1993), S. 231-235 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Time-of-flight mass spectrometry is used to investigate (TiN)n+ clusters produced by a laser-induced plasma reactor source. The mass spectral abundance patterns indicate that the clusters have cubic structures resembling subunits of the fcc lattice of solid TiN. The primary stoichiometries observed are (TiN)n+ (n=1–126), except for TinNn−1+ (n=14, 63). The most stable structures of the clusters are cuboids, in some cases containing a completed terrace. Even at the very early stages of crystal growth, the gas-phase clusters prefer a cubic crystalline atomic arrangement with a highly symmetric structure.
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  • 55
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    The Journal of Chemical Physics 98 (1993), S. 257-268 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Using the N2–N2 interaction potential of van der Avoird et al. [J. Chem. Phys. 84, 1629 (1986)] rotationally inelastic collision cross sections have been computed within the infinite order sudden (IOS) approximation, assuming the molecules are distinguishable. Methods for enforcing detailed balance and correcting for effects of inelasticity, which are ignored in the IOS approximation, are considered, including the energy corrected sudden (ECS) method. Suitably averaged cross sections are compared with experimental Raman Q-branch linewidths for temperatures from 295 to 1500 K and with recently measured room temperature state-to-state rates. Agreement is rather good, especially if ECS corrections are applied.
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  • 56
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    The Journal of Chemical Physics 98 (1993), S. 280-289 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Multiple product channels are observed for the reaction of 13CO++ with each of the rare gases (Rg) at Elab=49±1 eV. A beam of 13CO++ is produced by electron impact ionization and is mass selected using a quadrupole mass spectrometer. The ion beam is focused into a collision region and the reaction products are monitored using time-of-flight mass spectrometry. Relative yields for the production of 13C+, O+, and 13CO+ are measured directly. Absolute charge transfer reaction cross sections for collisions of 13CO++ with He, Ne, Ar, and Kr are estimated by comparing the Rg+ production with that for the charge transfer reactions of doubly charged rare gas ions with neutral rare gas atoms. The cross sections are found to range from 0.9−0.9+1.5 A(ring)2 for collisions of 13CO++ with He to 37.5±19.6 A(ring)2 for collisions with Kr. The reaction of 13CO++ with He proceeds almost exclusively into the collision-induced dissociation channel. The branching fraction for collision-induced dissociation is smaller for reactions with Ne and almost disappears for Ar, Kr, and Xe. As the relative importance of the collision-induced dissociation process decreases, branching into the charge transfer channel increases. The charge transfer reactions of 13CO++ with Ar, Kr, and Xe are shown to populate excited, dissociative electronic states of 13CO+ selectively. These effects are modeled successfully using Landau–Zener theory in conjunction with reaction window theory.
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  • 57
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    The Journal of Chemical Physics 98 (1993), S. 308-315 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Diabatic potential-energy functions for the two lowest excited states of the doublet HeH2+ system which fit published ab initio data [McLaughlin and Thompson, J. Chem. Phys. 70, 2748 (1979)] at a quantitative level have been obtained, similar to that obtained previously for the ground state (root-mean-square error about 1 kcal/mol), and without any quantity of ad hoc character, preserving the accuracy of the ab initio points. The corresponding adiabatic potential-energy functions are obtained by solving a 2×2 determinant that uses the diabatic energies and an interaction term fitted to the lowest eigenvalue to obtain a global root mean square as low as possible (0.93 kcal/mol). The lowest adiabatic potential-energy function satisfies the criteria needed to be used in full three-dimensional scattering calculations for the collisionally-induced predissociation charge-exchange reaction He++H2→He+H++H and, using the ground-state potential-energy surface also, the collision-induced dissociation reaction H2+(v)+He→He+H++H and the exoergic reaction He++H2→HeH++H.
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    The Journal of Chemical Physics 98 (1993), S. 316-320 
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    Notes: Infrared laser kinetic spectroscopy was extended to the study of formation and decomposition processes in a hollow cathode discharge. The processes responsible for the disappearance of the CN radical in different vibrational states (v=0–7) were investigated. From the time evolution of the signal, information on the reaction rates of vibrationally excited CN molecules with C2N2 and on their vibrational relaxation could be obtained. The measured first order reaction rate constants lie between 350–800 s−1 and the rate constants for the deactivation, which is thought to be due to V–V relaxation in collisions with C2N2, between 520–900 s−1 for the v=0–7 states of CN.
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  • 59
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    The Journal of Chemical Physics 98 (1993), S. 363-372 
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    Notes: Experiments performed on moderately dense gases indicate that the absorption of photons with energies in excess of the dissociation energy of I2 often fails to cause dissociation and, instead, results in the direct production of iodine molecules in the ground electronic state. To account for this, Otto, Schroeder, and Troe (OST) proposed that the photons are absorbed by I2–solvent complexes from which the solvent subsequently is ejected and the I2 simultaneously deposited in the electronic ground state. Our earlier calculations (for solvent ethane) already have established that the concentrations of I2–solvent complexes are, indeed, large enough to satisfy the requirements of the OST model. What we now propose is a dynamic mechanism that accounts for the photoabsorptive dissociation of the complex into a solvent fragment and a vibrationally excited I2 molecule in the ground electronic state. The occurrence of such an event is surprising because, at first glance, it appears to violate commonly accepted notions about the interconversion of electronic and nuclear, kinetic energy.
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    The Journal of Chemical Physics 98 (1993), S. 383-389 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Using pulse radiolysis techniques, rates of recombination of Ar2+ ions with electrons in bulk argon were measured over a wide pressure range (150 to 1065 torr) at bulk gas temperatures of 295, 335, and 375 K. No pressure dependence for the total recombination rate constant was observed at any temperature studied. This observation is consistent with the model, whereby the encounter pair is stabilized by electron energy loss while in the Coulomb field of the cation. The presence of a Ramsauer minimum in the electron/argon atom momentum-transfer cross section versus energy profile means that, at low energies, energy loss is very slow. The neutral-assisted three-body recombination mechanism in argon does not significantly enhance the total rate of recombination above the two-body rate.
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    The Journal of Chemical Physics 99 (1993), S. 6865-6875 
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    Notes: Into the classical Lifson–Roig model of the helix–coil transition in homo(poly)amino acids, we introduce a simple long-range interaction which models hydrophobic contacts between secondary structure elements, yet at the same time, retains its essentially 1D character. Although its properties cannot be determined analytically anymore, the model can be studied readily by Monte Carlo computer simulations. We show that our model assumptions lead to a markedly changed behavior in the transition from random coil to "folded'' states. Remarkably, even in a homopolymer, the additional long-range interactions stabilize structures resembling secondary structure elements of globular proteins in number and average size. We present results from our simulations which demonstrate a glasslike transition behavior of the homopolymer model as well as an on-site construction mechanism for the formation of α helices.
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    The Journal of Chemical Physics 99 (1993), S. 6253-6263 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We calculate the absorption spectrum of a cluster using a computational method in which classical-like degrees of freedom for the nuclei are described by Gaussian wave packets while the valence electrons are treated quantum mechanically. We examine the spectral features in comparison to an even simpler mixed quantum-classical model in which the nuclear motion is treated by purely classical mechanics. Anomalous features (such as negative absorption) in the absorption spectrum which can arise from mixed quantum-classical methods are examined and the Gaussian wave packet nuclear dynamics is found to substantially reduce these anomalous features. This method is applied to a two-coordinate model problem in which exact numerical results can be obtained and we find that the method works fairly well. We also apply the method to the valence electronic absorption spectrum for a KXe6 cluster. The method does not suffer from the dramatic failure seen when Xe motion is treated classically. The method is used to calculate the vibrational width and the vibrational structure of the electronic absorption spectrum.
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    The Journal of Chemical Physics 99 (1993), S. 6245-6252 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Relative Raman scattering cross sections of totally symmetric vibrational modes of liquid methanol, ethanol, and ethylene glycol are measured as a function of excitation wavelength in the preresonant spectral region 37 593–47 393 cm−1. Raman spectra are also obtained with 50 043 and 54 198 cm−1 excitation, the latter energy being directly resonant with the first excited state of the alcohols. The data indicate that the first three excited electronic states (with transition energies of approximately 54 600, 62 500, and 66 000 cm−1, respectively) make no significant contribution to the Raman scattered intensities and are nearly entirely Rydberg in character. The low-lying electronic structure of ethylene glycol appears to be primarily Rydberg in character as well. The dominant C–H and O–H stretching modes gain intensity largely from valence state(s) with transition energies near 70 000 cm−1, while the C–O stretching and CH2,3 bending modes gain intensity from even higher energy states (∼85 000 cm−1).
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    The Journal of Chemical Physics 99 (1993), S. 6264-6277 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A quantum mechanical relaxation theory is developed to enable approximate computation of electronic absorption line shapes of condensed phase systems where nonadiabatic coupling effects are important. At the simplest level, these computations require a time kernel (termed a memory kernel) which can be obtained from a sequence of wave packet propagations, each carried out on a single Born–Oppenheimer potential surface. Complications associated with the need to evolve wave packets on several nonadiabatically coupled surfaces are thereby avoided. Moreover, for many condensed phase problems the memory kernel can be computed via semiclassical techniques which rely on classical trajectories and simple Monte Carlo methods. The promise of the theory is demonstrated by numerical applications to the spectroscopic spin boson model [R. D. Coalson, J. Chem. Phys. 86, 995 (1987)], a nontrivial multimode model of electronic absorption lineshapes involving two nonadiabatically coupled excited state surfaces. The relevant quantum dynamics for the spectroscopic spin boson model can be computed exactly via path integration techniques. In this way, the accuracy of the proposed relaxation theory can be benchmarked, and the applicability of various semiclassical prescriptions for computing the memory kernel ascertained.
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    The Journal of Chemical Physics 99 (1993), S. 6278-6286 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Delayed pulsed field threshold ionization of clusters excited to high long-lived Rydberg states is used to study their dissociation behavior. Benzene–Ar and benzene–Kr dimers are excited by resonance enhanced two-photon ionization to Rydberg levels close to various ionization thresholds. The field ionized threshold ions are monitored and separated from the non-energy-selected ions in a reflecting field mass spectrometer with high mass resolution. The appearance of threshold ions at the daughter ion mass indicates the onset of a dissociation process. Daughter ions are first observed for the 16161(3/2) level of the two investigated dimers. This leads to an upper limit of the dissociation energy of benzene–Ar of 340 cm−1 which is probably higher than the true dissociation energy. For the first time threshold ions are observed for large internal energies of some 5 eV in the core indicating that high Rydberg states maintain their long lifetime even if the core is electronically or vibrationally excited by several eV.
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    The Journal of Chemical Physics 99 (1993), S. 6941-6949 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: An amorphous sediment of charged colloidal particles in a nonaqueous solvent was prepared by centrifugation. The evolution of sediment height and volume fraction profile to equilibrium were studied with light scattering. A simple sedimentation–diffusion equation allows the experimental data to be modeled quantitatively. The top of the sediment crystallizes within a week, whereas the lower part of the sediment does not show any sign of crystallization after several months, indicating a strong concentration dependence of crystallization rate.
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    The Journal of Chemical Physics 99 (1993), S. 6971-6976 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Dielectric properties of the local mode of motions (the β relaxation process) in two D-sorbitol glasses are presented as a function of temperature and pressure. The glasses were vitrified from the liquid by isobaric cooling at a rate of −0.2 K/min under 0.1 and 78.5 MPa. The following results are different from those observed in molecular and polymer glasses: the relaxation magnitude of the higher-density glass vitrified under 78.5 MPa is larger than that of the lower-density glass vitrified under the atmospheric pressure; the distribution of the relaxation time of the higher-density glass is narrower than that of the lower-density glass; and the relaxation magnitude of each glass appears to increase slightly with pressure. The results are interpreted by the difference in the distribution of intermolecular hydrogen bonds frozen-in at the vitrification points. It is also suggested that the hydrogen bonds in the glasses may be slightly decomposed and/or weakened by external pressure.
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    The Journal of Chemical Physics 99 (1993), S. 6302-6307 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We have performed polarized resonance coherent anti-Stokes Raman experiments on the permanganate ion doped in potassium perchlorate single crystals at temperature T=15 K. At this temperature the m (Cs) site splitting of the excited degenerate 1T2-electronic level of the permanganate ion and the vibronic structure are well resolved. We report on the A'-ν1 coherent anti-Stokes Raman excitation profile which shows a strong dependence on the frequency of the pump laser. The simulation of the experimental results is performed by using the transform theory, which enables one to calculate the resonance Raman excitation profile solely from the measured absorption spectrum. According to the well known relation between the third-order nonlinear susceptibility and the Raman polarizability the coherent anti-Stokes excitation profile is given by a simple product of two Raman excitation profiles which are shifted relative to each other. The linear and the quadratic electron-phonon coupling as well as the influence of non-Condon terms were taken into account. Since the transform theory is mode selective in case there are no mode mixing effects the results derived from the description of the Raman excitation profiles and the coherent anti-Stokes excitation profiles are more definite. For this purpose one only needs the model parameters of the mode of interest. The simulation of the A'-ν1 coherent anti-Stokes profile shows that a small amount of non-Condon coupling yields to a better agreement with the experiment.
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    The Journal of Chemical Physics 99 (1993), S. 7056-7075 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We explore collisions of Ne, CH4, NH3, and D2O with glycerol, a hydrogen bonding liquid, and with squalane, a liquid hydrocarbon. The experiments are carried out by directing a molecular beam at a continuously renewed liquid surface in vacuum and monitoring the identity and velocity of the scattered products with mass spectroscopy. We observe both direct inelastic scattering and trapping desorption when the gases strike the liquids. The polyatomic gases thermalize readily at low collision energies but rebound more frequently as the incident energy increases. We find that impulsive energy transfer is extensive and depends only weakly on the type of gas or liquid; for encounters leading to direct scattering, the gases appear to undergo hard spherelike collisions with the CH2 and CH3 groups of squalane and the OH and CH2 groups of glycerol. The gases accommodate differently on the two liquids, however: Neon and methane equilibrate more efficiently on squalane, ammonia thermalizes equally well on each liquid, and water is trapped more frequently by glycerol. The differences in trapping probabilities are smaller than expected from their solubilities, but they roughly follow trends in the free energies and enthalpies of solvation. Our results suggest that thermal accommodation in gas–liquid collisions reflects both the mechanical roughness and softness of hydrocarbons and the strong attractive forces between protic gases and the OH groups of glycerol.
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    The Journal of Chemical Physics 99 (1993), S. 7098-7107 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The experimental electron-spin resonance (ESR) line shapes of the micellar (L1) and lamellar (Lα) phases of the binary system 1-oleoyl-sn-glycero-3-phosphocholine (OlLPC)/water have been interpreted quantitatively using a two-dynamic (TD) model. This dynamic model comprises the local dynamics of Freed's model [J. Chem. Phys. 55, 5270 (1971); 58, 3185 (1973); 77, 3915 (1982)] and a second Brownian motion referring to the combined effect of the micellar reorientation and the translational motion of the amphiphile molecule along the micellar surface. With this model, we focus our attention on a comparison of the local dynamics between the L1 and Lα phases. It is found from the TD model that the local ordering (λ) and dynamics (τ⊥) of the L1 phase change compared with those of the Lα phase according to λ(L1)(approximately-greater-than)λ(Lα) and τ⊥(L1)〈τ⊥(Lα). The observed lower local ordering in the lamellar phase compared with that in the micellar phase may be interpreted in terms of the different packing constraints of the OlLPC molecule in the two phases.
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    The Journal of Chemical Physics 99 (1993), S. 7124-7149 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A statistical thermodynamic theory is developed to study curvature elastic properties of self-assembled monolayer films formed by nonionic surfactants at the interface between water and oil domains in microemulsions. A mean-field approximation to the conformational entropy is obtained by sequential placement of chain segments on a lattice, such that bond-correlated excluded volume effects are properly incorporated. The resulting free energy is minimized at zero lateral (osmotic) pressure with respect to a set of layer- and orientation-dependent statistical weights, from which the splay and Gaussian bending elastic moduli, spontaneous curvature, molecular area, and chain segment distributions are predicted. Calculations are reported for monolayers comprised of a single surfactant and for mixtures of surfactants of different lengths and stiffness. We examine the origins of the significant differences between our predictions and those of Szleifer et al. In particular, for self-assembled monolayers, we find that the bending moduli of mixtures of chains of different lengths are not lower than those of a single-component monolayer with a surfactant of corresponding number-average length. The approach to long-chain behavior of the elastic moduli is predicted to occur for chains much longer than those normally used experimentally as nonionic surfactants. However, extrapolation of our predictions to this limit yields power-law exponents very similar to those predicted by Wang and Safran.
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    The Journal of Chemical Physics 99 (1993), S. 7209-7213 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We used a Monte Carlo computer simulation to determine the behavior of proteins near and within a bilayer. The bilayer is represented by a hydrophobic slab, which is bounded above and below by hydrophilic regions. The protein is modeled as a neutral, self-avoiding chain, which contains both hydrophobic and hydrophilic sites. Through these simulations, we examined the effect of sequence distribution and the strength of the interaction energies on the interfacial activity of the proteins. The findings reveal both structural and energetic conditions under which proteins will remain localized at the surface of the bilayer or, penetrate and traverse the membrane. The results provide design criteria for fabricating proteins or biopolymers that display the desired interactions with bilayers.
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    The Journal of Chemical Physics 99 (1993), S. 7179-7189 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The potential energy of interaction between two deformed particles, having the shape of spherical segments and separated by a planar film, is considered. An exact explicit expression for the van der Waals interaction energy between such deformed particles of arbitrary size and deformation is derived by using the microscopic approach of Hamaker [Physica 4, 1058 (1937)]. By means of Derjaguin's approximation [Kolloid Z. 69, 155 (1934)] explicit expressions for the electrostatic, steric, depletion, and other types of interaction are derived. The relative contributions of the interaction across the planar film and between the spherical surfaces surrounding the film, are analyzed for different cases. The surface deformation energy caused by an increase of the interfacial area during the particle deformation is also considered. The implication of the obtained formulas for treatment of the particle interactions in some particular systems like emulsions, microemulsions, and vesicles, as well as for the adhesion of such particles to a solid wall is briefly discussed.
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    The Journal of Chemical Physics 99 (1993), S. 7232-7239 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A model of the stochastic behavior of the electrochemical interface is presented when electrochemical reactions limited by diffusion of the reacting species occur on the electrode surface. The random fluctuations of the state variables (concentrations and voltage) are supposed to come from Poisson elementary noise sources which are directly acting on the elementary fluxes, either reactive or diffusive, of the particles. The evolution of the state variables is governed by Langevin equations obtained from the linearization of the nonlinear electrochemical equations deduced from the heterogeneous electrochemical kinetics. The Langevin noise sources are derived from the Poisson elementary noise sources. Their first and second order moments are calculated and appear to be coherent with the master equation approach. Finally, the control and observation variables are defined for the electrochemical interface and the power spectral density of the observable quantity (current or potential) are derived from the Poisson elementary noise sources.
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    The Journal of Chemical Physics 99 (1993), S. 7271-7272 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A novel computer simulation technique for studying fluids in confined geometries has been developed and used to replicate Pfeffer's experiment on osmosis in semipermeable membranes in 1877. Our results confirm the validity of van't Hoff's famous relationship for osmotic pressure over a wide range of concentrations, and also clearly establish its validity even for molecular systems. We believe this is the first theoretical validation of this result for such a wide range of concentrations, where no explicit assumption of ideality is made for the interactions of the solute molecules.
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    The Journal of Chemical Physics 99 (1993), S. 7277-7278 
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    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The multitrajectory semiclassical method combined with the fixed rotor approximation is used to investigate the differential state-to-state scattering in H++H2 collisions at Ec.m.=20 eV. Little differences are found with respect to previous quantal infinite order calculations of Baer et al. [J. Chem. Phys. 91, 4169 (1989)] when similar DIM (diatomics in molecules) potential energy surfaces are used. Adjustment of the ground state DIM potential energy surface to ab initio data considerably improves the comparison with the experiment of Niedner et al. [J. Chem. Phys. 87, 2685 (1987)].
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  • 77
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    The Journal of Chemical Physics 99 (1993), S. 5668-5676 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The kinetics of NH3D+ rotation in ammonium sulfate and ammonium thiocyanate are measured at low temperature (8–60 K). Infrared hole burning of the N–D stretching bands causes reorientation of the ions among distinct positions relative to the crystal lattice, producing nonequilibrium population distributions. The slow relaxation (time scale of minutes to hours) is monitored with a Fourier-transform infrared spectrometer as the ions tunnel back to their equilibrium distributions. Kinetic models are used to extract rate constants for rotation between orientations. The rate constants range from 0.01 h−1 at 8 K, to about 10 h−1 above 50 K. The higher temperature data is described by barrier transmission calculations with barrier heights of 1000 to 1600 cm−1. The low temperature data agrees with rates calculated from a phonon-assisted tunneling model for transitions between the ground states of the orientations, with energy differences between ground states on the order of 10 cm−1. Calculations of the tunneling rates between quantum states in a potential for the rotation of the NH3D+ ion in ammonium sulfate generated by a point-charge model are also performed and compared to the experimental results.
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  • 78
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    The Journal of Chemical Physics 99 (1993), S. 5701-5711 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The Rydberg states L 1Π(v=0), L' 1Π(v=1), K 1Σ+(v=0), W 1Π(v=0), and W' 1Π(v=2) have been studied in a 2+1 double-resonance detection scheme with a resolution of 0.005 cm−1. Accurate molecular constants have been derived for these states. From the observed linewidths of individual rotational transitions, predissociation rates for the Rydberg states have been deduced. For the first time a clear J and e/f dependence for the predissociation of CO has been observed. One of the states causing the observed predissociation could be identified as the D' 1Σ+ state.
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  • 79
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    The Journal of Chemical Physics 99 (1993), S. 5712-5717 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We report on the optical response of size selected Ag2, Ag3, Au2, and Au3 embedded in argon matrices. Cluster samples were investigated in situ by excitation, fluorescence, and absorption spectroscopy. The spectra for the dimers are in agreement with previous measurements made on conventionally prepared matrices. Our previously reported spectra of trimers in krypton are confirmed by the argon results. The influence of the matrix gas will briefly be discussed.
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  • 80
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    The Journal of Chemical Physics 99 (1993), S. 6409-6415 
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    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Resonant two-photon ionization spectroscopy has been used to interrogate diatomic AlNi produced by laser vaporization of a 1:1 alloy target in a supersonic molecular beam of helium. Although a large density of states in this molecule prohibits a concise elucidation of its electronic structure, the presence of discrete transitions has allowed several bands to be rotationally resolved. From the analysis of these bands the ground state has been determined as X 2Δ5/2, originating from the 3sAl23dNi9σ2 configuration, and the bond length has been measured as 2.3211±0.0007 A(ring). The dissociation energy and ionization potential of AlNi have also been determined as D0(open circle)(AlNi)=2.29±0.05 eV and I.P.(AlNi)=6.95±0.09 eV, respectively.
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  • 81
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    The Journal of Chemical Physics 99 (1993), S. 6384-6393 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have examined the onset and evolution of multiple scattering of light on a series of latex dispersions as a function of increasing volume concentration φ of particles. We have shown that using vertically polarized incident light, the static scattered intensity becomes progressively depolarized, with increasing φ. The polarization of scattered light is completely random in the limit of strong multiple scattering. The spectra of decay times of dynamic light scattering display a region of oligo scattering at intermediate φ where both the single and multiple scattering components can be dynamically identified. For φ(approximately-greater-than)0.03 the limit of diffusive transport of light is attained. The obtained results confirm that our earlier measurements of dynamic light scattering on systems exhibiting critical opalescence are not influenced by multiple light scattering.
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  • 82
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    The Journal of Chemical Physics 99 (1993), S. 6416-6420 
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    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Gas phase electron diffraction data have been successfully recorded for zinc phthalocyanine. Molecular structure parameters have been determined by least square fitting a geometrically consistent model of C4v symmetry to the data. The results agree well with previous x-ray diffraction studies of crystals. However, the zinc atom was found to be slightly out the plane of the molecule in contrast with the x-ray results.
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  • 83
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    The Journal of Chemical Physics 99 (1993), S. 6449-6460 
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    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The relationships between dipole-induced dipole (DID) light scattering spectra and other dynamical properties of a fluid close to the glass transition were studied in a computer simulation of a highly supercooled binary atomic fluid. The predictions of the mode coupling theory (MCT) of the glass transition, which relates spectral features in the DID spectra to the relaxation of Fourier components of the density, were examined in detail. The MCT account of the origin of the α and β peaks in the spectra was confirmed, thereby corroborating recent experimental findings. Other issues examined included the role played by compositional fluctuations, the coupling of the DID polarizability to shear waves, and the influence of the range of the intermolecular polarizability on interaction-induced spectra near to the glass transition.
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  • 84
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    The Journal of Chemical Physics 99 (1993), S. 6436-6448 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We have measured the terminal rovibrational distribution of Na2 in a molecular beam produced by a supersonic expansion of pure sodium at source pressure × nozzle diameter products p0d=0.02 and 0.32 Torr cm. The rovibrational distribution was determined by the laser-induced fluorescence technique and covers the 550–1200 and 550–2700 cm−1 internal energy ranges, respectively. The highest vibrational state for which molecules were detected is v‘=15. For the lower stagnation pressure, the internal energy distribution is well relaxed and can be described by a temperature of about 350–400 K. For the p0d=0.32 Torr cm experiment, the distribution is nonthermal with a large population excess for the levels with a high internal energy. The local temperature exceeds 460 K at 2000 cm−1. A striking result is that the rovibrational distribution depends almost exclusively on the internal energy (i.e., it does not depend much on the partitioning of this energy between vibration and rotation). This new result does not seem to be in contradiction with previous experiments which tested only a small set of levels. We discuss the mechanisms of the rovibrational relaxation during the sodium beam expansion. Recent experiments have shown that this relaxation is a very efficient process and we believe that it can explain our observations. We attribute the population excess of the rovibrational levels with a high internal energy to the process of dimerization in the expansion. Finally, a nonstatistical behavior of the Na2 ortho/para population was observed for the vibrational levels v‘=10–15. Such an effect for hydrogen molecules formed by three-body recombination has been predicted by Roberts within the resonance complex theory of this process [R. E. Roberts, J. Chem. Phys. 54, 1423 (1971)].
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    The Journal of Chemical Physics 99 (1993), S. 6429-6435 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The b˜ 1B1→a˜ 1A1 emission spectrum of the CH2 radical has been studied in the 13 330–18 180 cm−1 region. Methylene (a˜ 1A1) is produced by photolysis of ketene at 308 nm and excited to single rovibrational levels of the b˜ 1B1 state by a tunable pulsed dye laser. The emission from the b˜ 1B1 state is spectrally dispersed with a resolution of 0.25 A(ring). Term values and transitions are reported for new levels of the b˜ 1B1(0,v2,0) (v2=14 and 15) and a˜ 1A1(0,0,0) states with J≥6 and 0≤Ka≤6. Unusually intense ΔKa=3 transitions and several ΔKa=5 transitions are observed. Analysis of the emission spectra gives the relative intensities of transitions from a selected rovibrational level in the upper b˜ 1B1 state to rovibrational levels in the a˜ 1A1 state. These relative intensities together with the fluorescence lifetimes of the b˜ 1B1 levels determine the absolute Einstein emission coefficients for rovibronic transitions in the visible spectrum of methylene. These data permit accurate measurement of rovibrational state populations for CH2(a˜ 1A1) by laser-induced fluorescence spectroscopy.
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  • 86
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    The Journal of Chemical Physics 99 (1993), S. 5910-5916 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We report the observation of the A 2Πu electronically excited state of the isolated, gas phase O2− superoxide anion by photofragmentation in the range of 4.5 eV, well above the onset of the electron detachment continuum at 0.45 eV. The action spectrum of O− photoproducts displays an abrupt onset in the vicinity of the known O2− dissociation energy. Quantum yield studies indicate that the dissociative pathway is about 3% relative to the direct electron photodetachment channel. The angular distribution of the ejected O− ions reveals a primarily parallel electronic transition (β=+1.2±0.1), allowing the 2Πu identification of the excited electronic state. This state has been observed previously in fluorescence from O2− in alkali crystals at low temperature, and appears to be the same excited state invoked to account for dissociative attachment of electrons onto neutral O2..
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    The Journal of Chemical Physics 99 (1993), S. 5944-5950 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We observe the photodissociation of SiH4 in a pulsed molecular beam after excitation with 125.1 nm vacuum ultraviolet light generated via resonant four-wave mixing in mercury vapor. Ultraviolet radiation from a Nd:YAG/dye laser combination ionizes the neutral photodissociation fragments and a time-of-flight mass spectrometer detects the ions. The photodissociation signal consists entirely of silicon atoms and silylidyne (SiH) in its first electronically excited state. We see no silylene (SiH2) or silyl radicals (SiH3). Thus, the photodissociation cleaves almost all of the silicon–hydrogen bonds, but the energetics of the dissociation require the production of at least one hydrogen molecule per dissociation event. These results imply that the high energy content of the initially excited Rydberg state prevents formation of the silylene and silyl radicals in stable vibronic states and that dissociation pathways exist that connect the Rydberg state directly to the corresponding silicon atom and silylidyne asymptotes. These pathways are likely to exist because of Jahn–Teller distortion from the initial Td symmetry. Very little of the available energy appears as kinetic energy of the fragments but rather as electronic excitation of the products. Our results differ from those of earlier studies that concluded silylene and silyl are the principle products.
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  • 88
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    The Journal of Chemical Physics 99 (1993), S. 6071-6077 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: An algorithm based on allowing the form of the intermolecular potential to fluctuate is introduced into molecular dynamics and Monte Carlo simulations. It is shown that this method accelerates the approach to equilibrium in frustrated systems. It provides a very useful method for determining all of the local minima in complex systems. Examples are mixing in dense binary liquids and folding of long polymer chains. When this method is combined with umbrella sampling techniques it accelerates the simulations of a wide class of chemically important systems.
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    The Journal of Chemical Physics 99 (1993), S. 6201-6204 
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    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A charge transfer (CT) excited state has been identified in the photoelectron spectrum of Cl−NH3. A narrow band at 4.0 eV binding energy (BE) is assigned to ionization of Cl−, and a broad band peaking at 6.45±0.15 eV BE corresponds to a CT state, Cl−NH+3. The assignments are confirmed by ab initio calculations, yielding binding energies of 3.88 and 6.36 eV.
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    The Journal of Chemical Physics 99 (1993), S. 6215-6216 
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    Topics: Physics , Chemistry and Pharmacology
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    The Journal of Chemical Physics 99 (1993), S. 6098-6113 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Interactions between charged surfaces immersed in aqueous calcium solutions were measured using the surface force apparatus and the atomic force microscope. With the surface force apparatus, good agreement with previously reported measurements was found for mica surfaces in dilute solutions up to 0.1 M. However, at higher concentrations large discrepancies were observed. Compared to the earlier work, the strength of the force was lower by two or three orders of magnitude and the range was diminished. Experiments using the atomic force microscope indicated similar force-distance profiles for the interaction between silicon nitride and mica. With this technique concentrations as high as 5 M can be investigated, and owing to the small radius of curvature much higher pressures can be recorded. Results obtained by both methods confirm that the force is strongly attractive at very small surface separations, in agreement with the theoretical predictions based on calculations of ion correlations. Just outside of that interval the interaction is repulsive, and it can be quantitatively explained by taking into account the adsorption of hydrated ions onto the surface (sign reversal of the effective surface charge) and the layering of co- and counterions. At larger surface separations, the behavior indicates a balance between the double layer repulsion and the van der Waals attraction (the presence of a secondary minimum).
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    The Journal of Chemical Physics 99 (1993), S. 4894-4907 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The infrared spectrum of the water–formamide complex in argon matrices has been recorded from 10 to 4000 cm−1. The interaction energy of the complex forming molecules has been calculated from a theoretical potential. One global and three different local minima have been found for this potential. Intermolecular vibration frequencies have been calculated for each minimum. The results are compared with the experimentally observed far infrared spectrum. In agreement with microwave measurements and ab initio calculations, the global minimum of the complex is found, both from calculations and experiment, to have a cyclic structure with water forming a hydrogen bond to the amide oxygen and receiving a hydrogen bond from an amide hydrogen. In addition to the cyclic complex, we observe one of the local minimum structures of the complex, where water accepts a hydrogen bond from the amide NH on the CH side of the amide.
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  • 93
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    The Journal of Chemical Physics 99 (1993), S. 6205-6207 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We apply three different spherical reference theories to the isotropic phase of the hard spheroid fluid. Of these three, the theory due to Barker and Henderson [J. Chem. Phys. 47, 4714 (1967)] gives the best equation of state. It would not seem, however, to predict an isotropic–nematic phase transition.
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    The Journal of Chemical Physics 99 (1993), S. 6517-6530 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: A theory is presented for the rate constant k for electron transfer between a metal electrode and a redox couple solute in solution, in or near the electronically adiabatic regime. The departure of k from its electronically adiabatic transition state theory limit kTST is described via Grote–Hynes theory, and includes two sources of friction. The electronic friction arises from excitation of electron hole pairs in the metal, i.e., electronic nonadiabaticity effects. The solvent friction arises from solvent dynamical effects. Both features can result in significant reduction of k below kTST, and their interplay can lead to interesting nonmonotonic variations with reaction overpotential.
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    The Journal of Chemical Physics 99 (1993), S. 6506-6516 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The kinetic energy dependence of the collision-induced dissociation (CID) of Crn+ (n=2–21) with xenon is studied by using a guided ion beam mass spectrometer. Examination of the general dissociation behavior over a broad collision energy range shows that chromium cluster ions dissociate primarily by sequential atom loss with a few exceptions, most notably Cr5+. Bond energies of chromium cluster ions D(Crn−1+–Cr) are determined from measurements of the CID thresholds. The cluster size dependence of chromium cluster bond energies shows that odd-sized clusters are more stable than even clusters for smaller clusters (n≤9) and local maxima at n=13, 14, and 20 for larger clusters. The even–odd alternation in the stability of small chromium clusters suggests that these cluster cations are bound mainly by the 4s electrons. The pattern of stability for the larger clusters, in particular, the observation that the 14- and 20-atom clusters are relatively stable, is consistent with clusters built around a dimer core.
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    The Journal of Chemical Physics 99 (1993), S. 6531-6536 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We investigate the plausible mechanism of fast decomposition of acetyl chloride upon 1nπ* (CO) excitation through the selective C–Cl bond-fission on the lowest excited singlet state surface using ab initio quantum chemical methods. Effects of zero point energy corrections and of electron correlation have been considered. The pathway involves dissociation, via a φClφ*CO and a φClφ*C–Cl configurations where φ's stand for wave functions of σ-molecular orbitals.
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    The Journal of Chemical Physics 99 (1993), S. 6537-6544 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: The direct photoionization process NO A 2Σ+ (v=0, N=13)→NO+ X 1Σ+ (v+=0, N+)+e− is studied by energy- and angle-resolved photoelectron spectroscopy by employing two-color resonance-enhanced multiphoton ionization (REMPI) via excitation of the NO A–X(0–0) R21(11.5) transition. The photoelectron angular distributions (PADs) associated with individual rotational levels N+ of the ion are determined. Combined analysis of the newly obtained PADs and those reported earlier for the processes NO A 2Σ+ (v=0, N≥20)→NO+ X 1Σ+ (v+=0, N+)+e− via P21+Q1 branch excitation shows that the photoionization dynamics is independent of the rotational quantum number of state to be ionized and of the spin state of the photoelectron. Quantitative comparison of our results with threshold photoelectron measurements provides strong evidence that ionization in the pulsed-electric-field threshold technique is not via direct photoionization.
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    The Journal of Chemical Physics 99 (1993), S. 6545-6552 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Reactions of photolytically prepared hot deuterium atoms with OCS have been investigated: (i) under gas phase, single collision, arrested relaxation (i.e., bulk) conditions; and (ii) by photoinitiating reactions within weakly bound OCS–DI complexes. Nascent SD(X 2Π, v=0) rotational, spin–orbit, and Λ-doublet populations were obtained for the photolysis wavelengths 250, 225, and 223 nm by using A 2Σ←X 2Π laser induced fluorescence (LIF). The reason for using deuterium is strictly experimental: A 2Σ predissociation rates are considerably smaller for SD than for SH. The SD (v=0) rotational distribution was found to be very cold and essentially the same for both bulk and complexed conditions; the most probable rotational energy is ∼180 cm−1. No bias in Λ-doublet populations was detected. Spin–orbit excitation for bulk conditions was estimated to be [2Π1/2]/[2Π3/2]∼0.25, where 2Π1/2 is the upper spin–orbit component. This ratio could not be obtained with complexes because of limited S/N. The complete set of present and past experimental findings, combined with recent theoretical results of Rice, Cartland, and Chabalowski suggest a mechanism in which SD derives from a very short lived HSCO precursor. This can result from direct hydrogen attack at the sulfur and/or the transfer of hydrogen from carbon to sulfur via the HCOS intermediate.
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    The Journal of Chemical Physics 99 (1993), S. 6579-6582 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: We have reexamined whether N2(v=1) transfers its vibrational quantum to NO+(v=0). In light of recent results that show that CH3I does not charge transfer rapidly with NO+(v=1), we show that previous measurements could not have detected vibrational–vibrational (V–V) energy transfer from N2(v=1) to NO+(v=0). We have made measurements to examine this process by using C2H5I as the monitor for NO+(v=1). Our results show that NO+(v(approximately-greater-than)0) is indeed produced from reaction of NO+(v=0) with N2(v) but these results cannot be used to distinguish between resonant V–V energy transfer from N2(v=1) to NO+(v=0) and V–V, T energy transfer from higher levels of N2(v).
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    The Journal of Chemical Physics 99 (1993), S. 6553-6561 
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    Topics: Physics , Chemistry and Pharmacology
    Notes: Time resolved studies of the title reaction have been carried out by photodissociating the HI moiety within weakly bound CO2–HI complexes. The HOCO° intermediate decomposes via a unimolecular decomposition mechanism, and the emerging hydroxyl radicals are monitored with subpicosecond temporal resolution by using laser-induced fluorescence. The measured rates are in good agreement with several theoretical predictions: Rice, Ramsperger, Kassel, and Marcus (RRKM) calculations; classical trajectory simulations on the best available potential energy surface; and recent quantum scattering calculations.
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