529 research outputs found
Density of states near the Mott-Hubbard transition in the limit of large dimensions
The zero temperature Mott-Hubbard transition as a function of the Coulomb
repulsion U is investigated in the limit of large dimensions. The behavior of
the density of states near the transition at U=U_c is analyzed in all orders of
the skeleton expansion. It is shown that only two transition scenarios are
consistent with the skeleton expansion for U<U_c: (i) The Mott-Hubbard
transition is "discontinuous" in the sense that in the density of states finite
spectral weight is redistributed at U_c. (ii) The transition occurs via a point
at U=U_c where the system is neither a Fermi liquid nor an insulator.Comment: 4 pages, 1 figure; revised version accepted for publication in Phys.
Rev. Let
A Mean Field Analysis of One Dimensional Quantum Liquid with Long Range Interaction
Bi-local mean field theory is applied to one dimensional quantum liquid with
long range interaction, which has exact ground state wave function. We
obtain a mean field solution and an effective action which expresses a long
range dynamics. Based on them the ground state energy and correlation functions
are computed. The ground state energy agrees fairly well with the exact value
and exponents have weaker coupling constant dependence than that of partly
known exact value.Comment: EPHOU-93-002, 10 pages (LaTeX), 3 figures available upon request as
hard cop
Nuclear spin-orbit interaction from chiral pion-nucleon dynamics
Using the two-loop approximation of chiral perturbation theory, we calculate
the momentum and density dependent nuclear spin-orbit strength .
This quantity is derived from the spin-dependent part of the interaction energy
of a nucleon scattering off weakly inhomogeneous isospin
symmetric nuclear matter. We find that iterated -exchange generates at
saturation density, MeV, a spin-orbit strength at of
MeVfm in perfect agreement with the empirical
value used in the shell model. This novel spin-orbit strength is neither of
relativistic nor of short range origin. The potential underlying the
empirical spin-orbit strength becomes a
rather weak one, MeV, after the identification as suggested by the present calculation. We observe however a
strong -dependence of leading even to a sign change above
MeV. This and other features of the emerging spin-orbit Hamiltonian
which go beyond the usual shell model parametrization leave questions about the
ultimate relevance of the spin-orbit interaction generated by -exchange
for a finite nucleus. We also calculate the complex-valued isovector
single-particle potential in isospin asymmetric
nuclear matter proportional to . For the real part we find
reasonable agreement with empirical values and the imaginary part vanishes at
the Fermi-surface .Comment: 20 pages, 10 Figures, Accepted for publication in Nuclear Physics
Diagrammatic theory for Periodic Anderson Model: Stationary property of the thermodynamic potential
Diagrammatic theory for Periodic Anderson Model has been developed, supposing
the Coulomb repulsion of localized electrons as a main parameter of the
theory. electrons are strongly correlated and conduction electrons
are uncorrelated. Correlation function for and mass operator for
electrons are determined. The Dyson equation for and Dyson-type equation
for electrons are formulated for their propagators. The skeleton diagrams
are defined for correlation function and thermodynamic functional. The
stationary property of renormalized thermodynamic potential about the variation
of the mass operator is established. The result is appropriate as for normal
and as for superconducting state of the system.Comment: 12 pages, 10 figure
Conserving Gapless Mean-Field Theory for Bose-Einstein Condensates
We formulate a conserving gapless mean-field theory for Bose-Einstein
condensates on the basis of a Luttinger-Ward thermodynamic functional. It is
applied to a weakly interacting uniform gas with density and s-wave
scattering length to clarify its fundamental thermodynamic properties. It
is found that the condensation here occurs as a first-order transition. The
shift of the transition temperature from the ideal-gas result
is positive and given to the leading order by , in agreement with a couple of previous estimates. The theory is
expected to form a new theoretical basis for trapped Bose-Einstein condensates
at finite temperatures.Comment: Minor errors remove
Non-perturbative approach to Luttinger's theorem in one dimension
The Lieb-Schultz-Mattis theorem for spin chains is generalized to a wide
range of models of interacting electrons and localized spins in one-dimensional
lattice. The existence of a low-energy state is generally proved except for
special commensurate fillings where a gap may occur. Moreover, the crystal
momentum of the constructed low-energy state is , where is the
Fermi momentum of the non-interacting model, corresponding to Luttinger's
theorem. For the Kondo lattice model, our result implies that must be
calculated by regarding the localized spins as additional electrons.Comment: Note added on the rigorous proof given by H. Tasaki; also added some
references; 5 pages, REVTEX (no figure
Consistency of Wilsonian effective actions
Wilsonian effective actions are interpreted as free energies in ensembles
with prescribed field expectation values and prescribed connected two-point
functions. Since such free energies are directly obtained from
two-particle-irreducible functionals, it follows that Wilsonian effective
actions satisfy elementary perturbative consistency conditions, and
non-perturbative convexity conditions. In particular, the exact determination
of a Wilsonian action by other means (e.g. supersymmetry) allows one to extract
restrictions on the particular cutoff scheme and field reparametrization that
would lead to such a Wilsonian action from an underlying microscopic action.Comment: 3 pages, RevTe
Localized Wavefunctions and Magnetic Band Structure for Lateral Semiconductor Superlattices
In this paper we present calculations on the electronic band structure of a
two-dimensional lateral superlattice subject to a perpendicular magnetic field
by employing a projection operator technique based on the ray-group of
magnetotranslation operators. We construct a new basis of appropriately
symmetrized Bloch-like wavefunctions as linear combination of well-localized
magnetic-Wannier functions. The magnetic field was consistently included in the
Wannier functions defined in terms of free-electron eigenfunctions in the
presence of external magnetic field in the symmetric gauge. Using the above
basis, we calculate the magnetic energy spectrum of electrons in a lateral
superlattice with bi-directional weak electrostatic modulation. Both a square
lattice and a triangular one are considered as special cases. Our approach
based on group theory handles the cases of integer and rational magnetic fluxes
in a uniform way and the provided basis could be convenient for further both
analytic and numerical calculations.Comment: 19 pages, 5 figures. accepted to Int. J. Mod. Phys. B (April 2006
Uncertainty Principle and Off-Diagonal Long Range Order in the Fractional Quantum Hall Effect
A natural generalization of the Heisenberg uncertainty principle inequality
holding for non hermitian operators is presented and applied to the fractional
quantum Hall effect (FQHE). This inequality was used in a previous paper to
prove the absence of long range order in the ground state of several 1D systems
with continuous group symmetries. In this letter we use it to rule out the
occurrence of Bose-Einstein condensation in the bosonic representation of the
FQHE wave function proposed by Girvin and MacDonald. We show that the absence
of off-diagonal long range order in this 2D problem is directly connected with
the behavior of the static structure function at small momenta.Comment: 10 pages, plain TeX, UTF-09-9
The absence of finite-temperature phase transitions in low-dimensional many-body models: a survey and new results
After a brief discussion of the Bogoliubov inequality and possible
generalizations thereof, we present a complete review of results concerning the
Mermin-Wagner theorem for various many-body systems, geometries and order
parameters. We extend the method to cover magnetic phase transitions in the
periodic Anderson Model as well as certain superconducting pairing mechanisms
for Hubbard films. The relevance of the Mermin-Wagner theorem to approximations
in many-body physics is discussed on a conceptual level.Comment: 33 pages; accepted for publication as a Topical Review in Journal of
Physics: Condensed Matte
- …