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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 2861-2862 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We continue the study of a model non-Gaussian influence functional proposed by Allinger, Carmeli, and Chandler [J. Chem. Phys. 84, 1724 (1986)] to approximate the exact influence functional resulting from integrating out all quantum states but those of primary interest. The premise of this work is that the influence of many secondary states on a single primary state can be closely approximated by the influence of a degenerate level of states with equal coupling to the primary state. The degeneracy reflects the fluctuations possible among the secondary states and in fact can be associated with the partition function of the exact secondary states. The new calculations presented herein emphasize the importance of entropic-like effects properly described by this degeneracy, and for the models we examine, our basic premise is shown to be correct.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 114 (2001), S. 5313-5321 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We use a self-consistent field approximation to model the configurations of end-charged homopolymer and block copolymer brushes in response to an external electric field due to charges on the grafting surface. By varying the charge density on the grafting surface, we can cause the chains either to extend outward, greatly increasing the brush height, or to loop back to the grafting surface. We show that such a copolymer brush can present one block at the exposed surface in the extended state and present the other block in the retracted state. This occurs for both a solvated brush and a dry brush. We also compare these results to those of a modified Alexander–de Gennes model for the end-charged homopolymer brush. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 1520-6904
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 6387-6397 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Recent experiments, analytical theory, and simulations have raised and examined the possibility of entropically driven segregation effects in conformationally asymmetric polymer blends. We consider herein a model of surface segregation in a molten blend of two polymers with different flexibilities as characterized by the pure-component parameter β2=R2g/Vmol, where Rg is the radius of gyration and Vmol is the molecular volume of a polymer chain. Analytic solutions to the self-consistent field equations are presented for small deviations of the conformational asymmetry parameter ε=(βA/βB)2 from unity. Even in the absence of enthalpic interactions with the wall, we find an effective exchange surface potential of entropic origin, which can be understood in terms of an imperfect screening of the wall by the self-consistent potential. We find that the more flexible component segregates to the surface, in qualitative agreement with an earlier density functional calculation, but with a different parameterization of the surface potential. For weak conformational asymmetry, the magnitude of the segregation is found to be proportional to (ε−1), and inversely proportional to the bulk screening length of the total monomer density. Our analysis indicates that unlike single-component melts, where reflecting boundary conditions are appropriate, molten blends near a surface are described by an effective mixed boundary condition on the polymer Green's function G(z,z′;s,s′) of the form ∂zG∝UG, where U is the strength of the surface potential. In the perturbative limit, ||ε−1||(very-much-less-than)1, this proves equivalent to effective constant flux boundary conditions. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 96 (1992), S. 4077-4083 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of organic chemistry 47 (1982), S. 2661-2663 
    ISSN: 1520-6904
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 1990-2000 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Multicomponent nucleation analysis is reformulated to include all paths of nucleation. Starting with simple measurement theory, one is led to define a global nucleation rate that corresponds to what is observable experimentally. This rate can be calculated at steady state and estimated for arbitrary times, provided the rate matrix and the free energy obey certain constraints. When applied to the special case of a quadratic barrier, the global nucleation rate is smaller than the standard result based on the rate of saddle-point nucleation. Cases with more general barriers can also be treated by the same method.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 2644-2650 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The time lag in transient nucleation is solved exactly for both the simple monomer approximation and the more complicated multipath kinetics with detailed balancing. It is shown that only initial and steady-state quantities are required for its calculation. The time lag within the continuum approximation is also considered. By evaluating the exact expression approximately, a simple functional form is obtained. The controversy over the "prefactor'' in previous approximate time lags is resolved. It is shown that in general none of the approximate time lags are correct. The "relative time lag'' is introduced. It is useful when detailed balance is not obeyed and also when the lower cutoff cluster size is not known precisely.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 4444-4453 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have extended the reference interaction site model (RISM)-polaron theory of Chandler et al. [J. Chem. Phys. 81, 1975 (1984)] to treat self-trapping and localized states of excess electrons in polar fluids. The extension is based on a new closure of the RISM equation presented herein. The theory is applied to the hydrated electron employing a simple class of electron-water pseudopotentials. Included in this class are models coinciding with those already examined by others using computer simulations. In those cases, the results for both structural and energetic properties compare well with those of simulation. The work function, or equivalently, the excess chemical potential of the hydrated electron are also computed; the theoretical result agrees with experiment to about 1%. Most interesting, however, is that as the parameter characterizing the pseudopotentials is varied, a critical parameter is found where the electron behavior changes essentially discontinuously from a trapped state to a "super''-trapped state. This transition may have a direct bearing on theoretical efforts to explain the properties of solvated electrons.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 1922-1931 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The continuum approximation in nucleation theory is reconsidered. It is shown that a minor change in indexing the discrete flux leads naturally to an approximation which is both simple and accurate. More complicated schemes are introduced using the formalism of spectral density (weighting) functions. Optimization of these functions produces additional approximations that minimize the errors in either the rate equation or the nucleation current. These new continuum approximations are compared to the traditional Frenkel form [Kinetic Theory of Liquids (Oxford University, Oxford, 1946)] and to the alternatives proposed by Goodrich [Proc. R. Soc. London, Ser. A 227, 167 (1964)] and Shizgal and Barrett [J. Chem. Phys. 91, 6505 (1989)]. Results show that the new forms are more accurate. Generalization to multipath kinetics (clustering or association) is also discussed. Finally, it is shown that within the continuum approximation, nucleation is mathematically equivalent to position-dependent diffusion.
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