DISORDER.bib

@COMMENT{{This file has been generated by bib2bib 1.46}}

@COMMENT{{Command line: bib2bib -ob DISORDER.bib -c " ropsections:'DISORDER' " bigBiblioFile.bib}}

@COMMENT{{ bigBiblioFile.bib generated by makebib.sh version }}

@COMMENT{{ concatenation of journals_ref.bib withpyblio.bib optimization.bib mypapers.bib other.bib refvulg.bib these_ref.bib philo.bib ../math/journals_ref.bib ../math/citeseer.bib ../math/books.bib }}

@COMMENT{{ date: Thu Nov 2 00:20:16 CET 2006 }}


@MISC{parisi1998replica,
  AUTHOR = {Giorgio Parisi},
  TITLE = {On the replica method for glassy systems},
  OPTHOWPUBLISHED = {},
  OPTMONTH = {},
  YEAR = {1998},
  NOTE = {Contribution to the Conference in Honour of Giovanni
                  Paladin, Rome September 1997. 10 pages and 2
                  figures},
  ROPSECTIONS = {DISORDER REPLICA PHYSX},
  PS = {/sci_docs/physics/papers/arxiv/parisi1998replica.ps.gz},
  ABSTRACT = {In this talk we review our theoretical understanding
                  of spin glasses paying a particular attention to the
                  basic physical ideas. We introduce the replica
                  method and we describe its probabilistic
                  consequences (we stress the recently discovered
                  importance of stochastic stability). We show that
                  the replica method is not restricted to systems with
                  quenched disorder. We present the consequences on
                  the dynamics of the system when it slows approaches
                  equilibrium are presented: they are confirmed by
                  large scale simulations, while we are still awaiting
                  for a direct experimental verification.}
}


@MISC{parisi1999replica,
  AUTHOR = {Giorgio Parisi},
  TITLE = {Replica and Glasses},
  YEAR = {1999},
  NOTE = {Contribution to the NATO-ASI school on Liquid State
                  Theory (Patti 1998). 25 pages and 6 figures},
  URL = {http://fr.arxiv.org/abs/cond-mat/9907052},
  PS = {/sci_docs/physics/papers/arxiv/parisi1999replica.ps.gz},
  ROPSECTIONS = {PHYSX DISORDER REPLICA},
  ABSTRACT = {In these two lectures I review our theoretical
                  understanding of spin glasses paying a particular
                  attention to the basic physical ideas. We introduce
                  the replica method and we describe its probabilistic
                  consequences (we stress the recently discovered
                  importance of stochastic stability). We show that
                  the replica method is not restricted to systems with
                  quenched disorder. We present the consequences on
                  the dynamics of the system when it slows approaches
                  equilibrium are presented: they are confirmed by
                  large scale simulations, while we are still awaiting
                  for a direct experimental}
}


@MISC{polonyi2002internal,
  AUTHOR = {Janos Polonyi},
  TITLE = {Internal Space Renormalization Group Methods for
                  Atomic and Condensed Matter Physics},
  HOWPUBLISHED = {Talk presented at the Conference "Renormalization
                  Group 2002 (RG-2002)" Strba, Slovakia,},
  MONTH = {March},
  YEAR = {2002},
  ROPSECTIONS = {QFT DISORDER},
  URL = {http://fr.arxiv.org/abs/cond-mat/0205040},
  PS = {/sci_docs/physics/papers/arxiv/polonyi2002internal.ps.gz},
  ABSTRACT = {The functional renormalization group method is used
                  to take into account the vacuum polarization around
                  localized bound states generated by external
                  potential. The application to Atomic Physics leads
                  to improved Hartree-Fock and Kohn-Sham equations in
                  a systematic manner within the framework of the
                  Density Functional Theory. Another application to
                  Condensed Matter Physics consists of an algorithm to
                  compute quenched averages with or without Coulomb
                  interaction in a non-perturbative manner.}
}


@MISC{polonyi2002current,
  AUTHOR = {Janos Polonyi},
  TITLE = {Current-density functional for disordered systems},
  HOWPUBLISHED = {cond-mat/0203090},
  YEAR = {2002},
  URL = {http://fr.arxiv.org/abs/cond-mat/0203090},
  PS = {/sci_docs/physics/papers/arxiv/polonyi2002current.ps.gz},
  ROPSECTIONS = {QFT DISORDER},
  ABSTRACT = { The effective action for the current and density is
                  shown to satisfy an evolution equation, constructed
                  by the analogy of the functional renormalization
                  group, which describes the dependence of the
                  one-particle irreducible vertex functions on the
                  strength of the disorder and the Coulomb
                  interaction. No small parameter is assumed in
                  deriving the evolution equation. The case of the
                  non-interacting electron gas is discussed in more
                  details. The effective action is constructed in the
                  initial condition for weakly fluctuating impurity
                  field in the framework of the gradient expansion. It
                  is conjectured that non-linearities should drive the
                  transport coefficients to zero at finite strength of
                  the disorder in a manner analogous to a formal
                  diffusion process and the quartic order terms of the
                  gradient expansion would be the key to the localized
                  phase.}
}


@ARTICLE{0959-7174-12-3-308,
  AUTHOR = {Knut S\o{}lna},
  TITLE = {Focusing of time-reversed reflections},
  JOURNAL = {Waves in Random Media},
  VOLUME = {12},
  NUMBER = {3},
  PAGES = {365-385},
  YEAR = {2002},
  ROPSECTIONS = {LOCALIZATION DISORDER MULTISCATT},
  PDF = {/sci_docs/physics/papers/WavesRandomMedia/solna2002focusing.pdf},
  ABSTRACT = {Recently time-reversal techniques have emerged as a
                  new, important and fascinating discipline within
                  wave propagation. Many of the problems involved can
                  best be understood, analysed and optimized based on
                  a random field model for the medium. Here we discuss
                  stable refocusing of second-order time-reversed
                  reflections. This phenomenon may appear as
                  surprising at first. However, we show how it can be
                  understood in very simple terms viewing the
                  wavefield as a stochastic process. We give
                  sufficient conditions on Green's function of the
                  propagation problem for the phenomenon to happen. In
                  particular we discuss acoustic wave propagation in
                  the regime of weak random medium fluctuations and
                  explicitly give the derivation of stable refocusing
                  in this case, illustrating it with numerical
                  examples.}
}


@ARTICLE{kuzovkov2002exact,
  AUTHOR = {V N Kuzovkov and W von Niessen and V Kashcheyevs and O Hein},
  TITLE = {Exact analytic solution for the generalized Lyapunov exponent of the two-dimensional Anderson localization},
  JOURNAL = {Journal of Physics: Condensed Matter},
  VOLUME = {14},
  NUMBER = {50},
  PAGES = {13777-13797},
  YEAR = {2002},
  ROPSECTIONS = {LOCALIZATION DISORDER PHASE_T},
  PDF = {/sci_docs/physics/papers/JPhysCondMat/kuzovkov2002exact.pdf},
  ABSTRACT = {The Anderson localization problem in one and two
  dimensions is solved analytically via the calculation of the
  generalized Lyapunov exponents. This is achieved by making use of
  signal theory. The phase diagram can be analysed in this way. In the
  one-dimensional case all states are localized for arbitrarily small
  disorder in agreement with existing theories. In the two-dimensional
  case for larger energies and large disorder all states are localized
  but for certain energies and small disorder extended and localized
  states coexist. The phase of delocalized states is marginally
  stable. We demonstrate that the metal\–insulator transition
  should be interpreted as a first-order phase
  transition. Consequences for perturbation approaches, the problem of
  self-averaging quantities and numerical scaling are discussed. }
}


@ARTICLE{mae2003energy,
  AUTHOR = {Naohiro Mae and Shinji Iida},
  TITLE = {Energy level statistics in weakly disordered systems: from quantum to diffusive regime},
  JOURNAL = {Journal of Physics A: Mathematical and General},
  VOLUME = {36},
  NUMBER = {4},
  PAGES = {999-1011},
  ROPSECTIONS = {DISORDER},
  PDF = {/sci_docs/physics/papers/JPhysA/mae2003energy.pdf},
  YEAR = {2003},
  ABSTRACT = {We calculate two-point energy level correlation function
  in weakly disordered metallic grain by taking account of
  localization corrections to the universal random matrix
  result. Using supersymmetric nonlinear \σ model and exactly
  integrating spatially homogeneous modes, we derive the expression
  valid for arbitrary energy differences from quantum to diffusive
  regime for the system with broken time reversal symmetry. Our result
  coincides with that obtained by Andreev and Altshuler (1995
  Phys. Rev. Lett . 72 902) where homogeneous modes are perturbatively
  treated. }
}


@ARTICLE{0305-4470-36-49-003,
  AUTHOR = {W Kirsch and O Lenoble and L Pastur},
  TITLE = {On the Mott formula for the ac conductivity and binary correlators in the strong localization regime of disordered systems},
  JOURNAL = {Journal of Physics A: Mathematical and General},
  VOLUME = {36},
  NUMBER = {49},
  PAGES = {12157-12180},
  YEAR = {2003},
  ROPSECTIONS = {LOCALIZATION DISORDER},
  PDF = {/sci_docs/physics/papers/JPhysA/kirsch2003mott.pdf},
  ABSTRACT = {We present a method that allows us to find the asymptotic form of various characteristics of disordered systems in the strong localization regime, i.e., when either the random potential is big or the energy is close to a spectral edge. The method is based on the hypothesis that the relevant realizations of the random potential in the strong localization regime have the form of a collection of deep random wells that are uniformly and chaotically distributed in space with a sufficiently small density. Assuming this and using the density expansion, we show first that the density of wells coincides in leading order with the density of states. Thus the density of states is in fact the small parameter of the theory in the strong localization regime. Then we derive the Mott formula for the low frequency conductivity and the asymptotic formulae for certain two-point correlators when the difference of the respective energies is small. }
}


@ARTICLE{1999EL.....47..175T,
  AUTHOR = {{Tourin}, A. and {Derode}, A. and {Fink}, M.},
  TITLE = {{Dynamic time reversal of randomly backscattered acoustic waves}},
  JOURNAL = {Europhysics Letters},
  YEAR = 1999,
  MONTH = JUL,
  VOLUME = 47,
  PAGES = {175-181},
  ADSURL = {http://adsabs.harvard.edu/cgi-bin/nph-bib_query?bibcode=1999EL.....47..175T&db_key=PHY},
  ADSNOTE = {Provided by the Smithsonian/NASA Astrophysics Data System},
  ROPSECTIONS = {MULTISCATT DISORDER}
}

@COMMENT{{ThisfilehasbeengeneratedbyPybliographer}}


@PHDTHESIS{schreiber1997systemes,
  AUTHOR = {Georg R. Schreiber},
  TITLE = {Syst{\`e}mes d{\'e}sordonn{\'e}s et frustr{\'e}s:
                  mod{\`e}les champ moyen et probl{\`e}mes
                  d'optimisation combinatoire},
  SCHOOL = {CEA/Saclay, SPhT},
  YEAR = {1997},
  ADDRESS = {UNIVERSITE PARIS SUD - PARIS XI},
  MONTH = {novembre},
  ROPSECTIONS = {THESIS PHYSX DISORDER REPLICA PHASE_T},
  URL = {http://theses-en-ligne.ccsd.cnrs.fr/documents/archives0/00/00/08/25/index_fr.html},
  PS = {/sci_docs/physics/papers/thesis/schreiber1997systemes.ps.gz},
  ABSTRACT = {In the present Ph.D. dissertation I present results
                  concerning disordered and frustrated models of
                  relevance in statistical mechanics and in
                  combinatorial optimization. As an application of
                  spin glass theory I study the disordered and
                  frustrated Blume-Emery-Griffiths model. The model is
                  treated in its mean-field approximation using
                  replicas. Within the Ansatz of replica-symmetry, I
                  present a complete numerical solution; I also
                  discuss effects of replica symmetry breaking. The
                  stability of the RS solution is studied and the
                  regions of instability inferred. The phase diagram
                  exhibits first and second order transitions. The
                  tricritical point is still present in the frustrated
                  model, in agreement with former work. A version of
                  the BEG model with disordered chemical potential is
                  also studied. The calculations confirm that the
                  disorder decreases the tricritical
                  temperature. Next, I consider the graph partitioning
                  problem, a combinatorial optimization problem,
                  which, from the point of view of statistical
                  mechanics is a spin glass model with the constraint
                  of zero magnetisation. I focus on the statistical
                  properties of low energy solutions generated by
                  "heuristic" algorithms designed to solve such hard
                  combinatorial optimization problems. Several
                  heuristics proposed to solve this problem were
                  implemented. Scaling laws are obtained; in
                  particular, the average cost and its variance grow
                  linearly with the number of vertices of the
                  graphs. As a consequence the cost found by the
                  heuristics is self-averaging. I suggest that this
                  property is quite general, valid for random
                  solutions, quasi-optimal solutions, and probably for
                  the optimum solutions, too. Furthermore a ranking
                  method is proposed and illustrated on an ensemble of
                  graph partitioning problems. This ranking procedure
                  takes into account the quality of the solution as
                  well as the time necessary to find that solution. In
                  the third part of this dissertation I study in
                  detail the zero-temperatures properties of spin
                  glasses on sparse random graphs with fixed
                  connectivity. Spin glasses on these graphs may be
                  considered as a more realistic approximation to real
                  spin glasses as represented by the model of
                  Sherrington and Kirkpatrick. I have designed a new
                  algorithm for finding low energy states. Second, I
                  present a method for deriving the ground state
                  energy from heuristic algorithms, even though they
                  are not guaranteed to find the optimum. Third, I
                  present a numerical test of a conjecture due to
                  Banavar, Sherrington and Sourlas, giving the large
                  volume energy density of the ground states as
                  function of the connectivity. The distribution of
                  the order parameter is found to be non-trivial, and
                  I give evidence for the presence of ultrametricity
                  for all values of the connectivity. These results
                  confirm the expectation that the remarquable
                  properties of the infinite range
                  Sherrington-Kirkpatrick model carry over to more
                  realistic models, as for example the spin glass
                  model on random graphs with finite connectivity
                  studied in the present work. }
}


@ARTICLE{bk94,
  AUTHOR = {D. Belitz and T. R. Kirkpatrick},
  TITLE = {The Anderson-Mott transition},
  JOURNAL = {Rev. Mod. Phys.},
  YEAR = {1994},
  OPTKEY = {},
  VOLUME = {\textbf{66}},
  OPTNUMBER = {2},
  PAGES = {261-380},
  OPTMONTH = {April},
  OPTNOTE = {},
  OPTANNOTE = {},
  ROPSECTIONS = {QFT DISORDER CORREL}
}


@ARTICLE{bk97,
  AUTHOR = {D. Belitz and T. R. Kirkpatrick},
  TITLE = {Theory of many-fermion systems},
  JOURNAL = {\PRB},
  YEAR = {1997},
  OPTKEY = {},
  VOLUME = {\textbf{56}},
  OPTNUMBER = {},
  PAGES = {6513-6541},
  OPTMONTH = {},
  NOTE = {\textnormal{\texttt{cond-mat/9703164}}},
  OPTANNOTE = {},
  PDF = {/sci_docs/physics/papers/PRB/theory.pdf.gz},
  ROPSECTIONS = {QFT DISORDER CORREL}
}


@ARTICLE{bk98,
  AUTHOR = {D. Belitz and T. R. Kirkpatrick},
  TITLE = {Theory of many-fermion systems. II. The case of Coulomb interactions},
  JOURNAL = {\PRB},
  YEAR = {1998},
  OPTKEY = {},
  VOLUME = {\textbf{58}},
  OPTNUMBER = {15},
  PAGES = {9710-9720},
  OPTMONTH = {},
  OPTANNOTE = {},
  PDF = {/sci_docs/physics/papers/PRB/theoryII.pdf.gz},
  ROPSECTIONS = {QFT DISORDER CORREL}
}


@INCOLLECTION{bkqpt,
  AUTHOR = {T. R. Kirkpatrick and D. Belitz},
  TITLE = {Quantum phase transitions in electronic systems},
  BOOKTITLE = {Electron correlation in the solid state},
  OPTCROSSREF = {},
  OPTKEY = {},
  PAGES = {297-370},
  PUBLISHER = {Imperial College Press},
  YEAR = {1999},
  EDITOR = {N. H. March},
  OPTVOLUME = {},
  OPTNUMBER = {},
  OPTSERIES = {},
  OPTTYPE = {},
  OPTCHAPTER = {},
  ADDRESS = {London},
  OPTEDITION = {},
  OPTMONTH = {},
  NOTE = {\textnormal{\texttt{cond-mat/9707001}}},
  OPTANNOTE = {},
  ROPSECTIONS = {QFT DISORDER CORREL PHASE_T}
}


This file has been generated by bibtex2html 1.46 . Bibliography collected by S. Correia.