29 research outputs found
Quantitative Estimates on the Binding Energy for Hydrogen in Non-Relativistic QED. II. The spin case
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
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 .Comment: 14 pages, Latex. Final version, accepted for publication in J. Math.
Phy
Binding threshold for the Pauli-Fierz operator
For the Pauli-Fierz operator with a short range potential we study the
binding threshold as a function of the fine structure constant and
show that it converges to the binding threshold for the Schr\"odinger operator
in the small limit
Surface segregation of conformationally asymmetric polymer blends
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
but different statistical segment lengths and 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
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
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
We study the energy distribution function for interfaces in a
random field environment at zero temperature by summing the leading terms in
the perturbation expansion of 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 behave as,
, , while the distribution
function of the energy tends for large 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
In this paper, we determine the exact expression for the hydrogen binding
energy in the Pauli-Fierz model up to the order ,
where denotes the finestructure constant, and prove rigorous bounds on
the remainder term of the order . As a consequence,
we prove that the binding energy is not a real analytic function of ,
and verify the existence of logarithmic corrections to the expansion of the
ground state energy in powers of , as conjectured in the recent
literature.Comment: AMS Latex, 51 page
Weakly coupled bound states of Pauli operators
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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