29 research outputs found

    Quantitative Estimates on the Binding Energy for Hydrogen in Non-Relativistic QED. II. The spin case

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    The hydrogen binding energy in the Pauli-Fierz model with the spin Zeeman term is determined up to the order alpha cube, where alpha denotes the fine-structure constant

    The increase of Binding Energy and Enhanced Binding in Non-Relativistic QED

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    We consider a Pauli-Fierz Hamiltonian for a particle coupled to a photon field. We discuss the effects of the increase of the binding energy and enhanced binding through coupling to a photon field, and prove that both effects are the results of the existence of the ground state of the self-energy operator with total momentum P=0P = 0.Comment: 14 pages, Latex. Final version, accepted for publication in J. Math. Phy

    Binding threshold for the Pauli-Fierz operator

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    For the Pauli-Fierz operator with a short range potential we study the binding threshold as a function of the fine structure constant α\alpha and show that it converges to the binding threshold for the Schr\"odinger operator in the small α\alpha limit

    Surface segregation of conformationally asymmetric polymer blends

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    We have generalized the Edwards' method of collective description of dense polymer systems in terms of effective potentials to polymer blends in the presence of a surface. With this method we have studied conformationally asymmetric athermic polymer blends in the presence of a hard wall to the first order in effective potentials. For polymers with the same gyration radius RgR_g but different statistical segment lengths lAl_{A} and lBl_{B} the excess concentration of stiffer polymers at the surface is derived as % \delta \rho _{A}(z=0)\sim (l_{B}^{-2}-l_{A}^{-2}){\ln (}R_{g}^{2}/l_{c}^{2}{)%}, where lcl_{c} is a local length below of which the incompressibility of the polymer blend is violated. For polymer blends differing only in degrees of polymerization the shorter polymer enriches the wall.Comment: 11 pages, 7 figures, revtex

    Localization transition of random copolymers at interfaces

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    We consider adsorption of random copolymer chains onto an interface within the model of Garel et al. Europhysics Letters 8, 9 (1989). By using the replica method the adsorption of the copolymer at the interface is mapped onto the problem of finding the ground state of a quantum mechanical Hamiltonian. To study this ground state we introduce a novel variational principle for the Green's function, which generalizes the well-known Rayleigh-Ritz method of Quantum Mechanics to nonstationary states. Minimization with an appropriate trial Green's function enables us to find the phase diagram for the localization-delocalization transition for an ideal random copolymer at the interface.Comment: 5 page

    Universal energy distribution for interfaces in a random field environment

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    We study the energy distribution function ρ(E)\rho (E) for interfaces in a random field environment at zero temperature by summing the leading terms in the perturbation expansion of ρ(E)\rho (E) in powers of the disorder strength, and by taking into account the non perturbational effects of the disorder using the functional renormalization group. We have found that the average and the variance of the energy for one-dimensional interface of length LL behave as, R∝Lln⁥L_{R}\propto L\ln L, ΔER∝L\Delta E_{R}\propto L, while the distribution function of the energy tends for large LL to the Gumbel distribution of the extreme value statistics.Comment: 4 pages, 2 figures, revtex4; the distribution function of the total and the disorder energy is include

    Quantitative estimates on the Hydrogen ground state energy in non-relativistic QED

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    In this paper, we determine the exact expression for the hydrogen binding energy in the Pauli-Fierz model up to the order O(α5logâĄÎ±âˆ’1)O(\alpha^5\log\alpha^{-1}), where α\alpha denotes the finestructure constant, and prove rigorous bounds on the remainder term of the order o(α5logâĄÎ±âˆ’1)o(\alpha^5\log\alpha^{-1}). As a consequence, we prove that the binding energy is not a real analytic function of α\alpha, and verify the existence of logarithmic corrections to the expansion of the ground state energy in powers of α\alpha, as conjectured in the recent literature.Comment: AMS Latex, 51 page

    Weakly coupled bound states of Pauli operators

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    We consider the two-dimensional Pauli operator perturbed by a weakly coupled, attractive potential. We show that besides the eigenvalues arising from the Aharonov-Casher zero modes there are two or one (depending on whether the flux of the magnetic field is integer or not) additional eigenvalues for arbitrarily small coupling and we calculate their asymptotics in the weak coupling limit.Comment: 19 page
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