MYPAPERS.bib

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@ARTICLE{correia2001lpm,
  AUTHOR = {S. Correia},
  TITLE = {Corrections to the Boltzmann mean free path in
                  disordered systems with finite size scatterers},
  JOURNAL = {J. Phys. A: Math. Gen.},
  YEAR = {2001},
  VOLUME = {34},
  NUMBER = {44},
  PAGES = {9349-9356},
  MONTH = {November},
  URL = {http://xxx.lpthe.jussieu.fr/abs/cond-mat/0103131},
  PDF = {/sci_docs/physics/papers/JPhysA/correia2001lpm.pdf},
  ROPSECTIONS = {MYPAPERS},
  ABSTRACT = {The mean free path is an essential characteristic
                  length in disordered systems. In microscopic
                  calculations, it is usually approximated by the
                  classical value of the elastic mean free path. It
                  corresponds to the Boltzmann mean free path when
                  only isotropic scattering is considered, but it is
                  different for anisotropic scattering. In this paper,
                  we work out the corrections to the so called
                  Boltzmann mean free path due to multiple scattering
                  effects on finite size scatterers, in the $s$-wave
                  approximation, i.e. when the elastic mean free path
                  is equivalent to the Boltzmann mean free path. The
                  main result is the expression for the mean free path
                  expanded in powers of the perturbative parameter
                  given by the scatterer density.}
}


@MISC{correia2000modelling,
  AUTHOR = {Sebastiao Correia and Janos Polonyi and Jean
                  Richert},
  TITLE = {Modelling static impurities},
  URL = {http://fr.arxiv.org/abs/cond-mat/0010370},
  PS = {/sci_docs/physics/papers/arxiv/correia2000modelling.ps.gz},
  ROPSECTIONS = {MYPAPERS},
  ABSTRACT = {A simple model is presented for the calculation of
                  the quenched average over impurities which are
                  rendered static by setting their mass equal to
                  infinity. The path integral formalism of the second
                  quantized theory contains annealed averages
                  only. The similarity with the Gaussian quenched
                  potential model is discussed. }
}


@MISC{correia2000effective,
  AUTHOR = {Sebastiao Correia and Janos Polonyi and Jean
                  Richert},
  TITLE = {An effective theory for conductance by symmetry
                  breaking},
  HOWPUBLISHED = {\textnormal{\texttt{cond-mat/0001053}}},
  YEAR = {2000},
  URL = {http://fr.arxiv.org/abs/cond-mat/0001053},
  PS = {/sci_docs/physics/papers/arxiv/correia2000effective.ps.gz},
  ROPSECTIONS = {MYPAPERS},
  ABSTRACT = {An effective theory is suggested for the
                  particle-anti particle and the particle-particle
                  modes of strongly disordered electron systems. The
                  effective theory is studied in the framework of the
                  saddle point expansion and found to support a vacuum
                  which is not invariant under translations in
                  imaginary time. The Goldstone bosons of this
                  symmetry breaking generate a pole in the
                  density-density correlation function. The condensate
                  of the auxiliary field corresponding to the
                  particle-particle channel produces conductivity
                  without relying on the long range fluctuations. The
                  results are obtained for d>1. }
}


@ARTICLE{correia2002functional,
  AUTHOR = {Sebastiao Correia and Janos Polonyi and Jean
                  Richert},
  TITLE = {The Functional Callan-Symanzik Equation for the
                  Coulomb Gas},
  JOURNAL = {Annals of Physics},
  YEAR = {2002},
  VOLUME = {296},
  NUMBER = {2},
  PAGES = {214-234},
  MONTH = {March},
  PDF = {/sci_docs/physics/papers/AnnPhys/correia2002functional.pdf},
  URL = {http://fr.arxiv.org/abs/cond-mat/0108048},
  ROPSECTIONS = {MYPAPERS},
  ABSTRACT = {A non-perturbative scheme, based on the functional
                  generalization of the Callan-Symanzik equation is
                  developed to treat the Coulomb interaction in an
                  electron gas. The one-particle irreducible vertex
                  functions are shown to satisfy an evolution equation
                  whose initial condition is given by means of the
                  classical action and the final point corresponds to
                  the physical system. This equation is truncated by
                  expanding it in momenta and excitation energies,
                  leaving the electric charge as an arbitrary, not
                  necessarily small parameter. Exact coupled partial
                  differential equations up to first order in the
                  frequencies and excitation energies are derived. The
                  numerical integration of these equations is left to
                  a later stage. Nevertheless, in order to demonstrate
                  the relation with the perturbation expansion the
                  one-loop Lindhard function and screening are
                  reproduced in the independent mode approximation of
                  the evolution equation.}
}


@ARTICLE{scjpjr,
  AUTHOR = {S. Correia and J. Polonyi and J. Richert},
  TITLE = {An effective theory for conductance by symmetry breaking},
  JOURNAL = {\textnormal{\texttt{cond-mat/0001053}}},
  YEAR = {2000},
  ROPSECTIONS = {MYPAPERS},
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}