QFT.bib

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

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


@ARTICLE{frolich2001asymptotic,
  AUTHOR = {J. Fröhlich1 and M. Griesemer and B. Schlein},
  TITLE = {Asymptotic Electromagnetic Fields in Models of
                  Quantum-Mechanical Matter Interacting with the
                  Quantized Radiation Field },
  JOURNAL = {Advances in Mathematics},
  YEAR = {2001},
  VOLUME = {164},
  NUMBER = {2},
  PAGES = {349-398},
  OPTMONTH = {December},
  PDF = {/sci_docs/math/advmath/frolich2001asymptotic.pdf},
  ROPSECTIONS = {QFT},
  ABSTRACT = {In models of (non-relativistic and
                  pseudo-relativistic)electrons interacting with
                  static nuclei and with the
                  (ultraviolet-cutoff)quantized radiation field,the
                  existence of asymptotic electromagnetic fields is
                  established.Our results yield some mathe- matically
                  rigorous understanding of Rayleigh scattering and of
                  the phenomenon of relaxation of isolated atoms to
                  their ground states.Our proofs are based on prop-
                  agation estimates for electrons inspired by similar
                  estimates known from N -body scattering theory.}
}


@ARTICLE{polonyi2001lectures,
  AUTHOR = {J. Polonyi},
  TITLE = {Lectures on the functional renormalization group
                  method},
  JOURNAL = {hep-th},
  YEAR = {2001},
  ROPSECTIONS = {RG QFT},
  URL = {http://fr.arxiv.org/abs/hep-th/0110026},
  PS = {/sci_docs/physics/papers/arxiv/polonyi2001lectures.ps.gz}
}


@ARTICLE{faussurier2001effective,
  AUTHOR = {G. Faussurier},
  TITLE = {Effective Classical Potential},
  JOURNAL = {Annals of Physics},
  YEAR = {2001},
  VOLUME = {294},
  NUMBER = {2},
  PAGES = {203-233},
  MONTH = {December},
  PDF = {/sci_docs/physics/papers/AnnPhys/faussurier2002effective.pdf},
  ROPSECTIONS = {QFT},
  ABSTRACT = { A new method for approximating a quantum-mechanical
                  partition function by an effective classical
                  partition function is proposed. The associated
                  effective classical potential is found by using a
                  variational procedure and a Gaussian Ansatz to
                  estimate the statistical weight of paths starting
                  and ending at the same point in the path-integral
                  representation of the partition function. This
                  method can be generalized to a
                  variational-convergent calculation of
                  path-integral. This systematic technique involves
                  neither perturbation nor stochastic
                  processes. Numerical results are presented and
                  discussed for quartic, sextic, mixed quartic-sextic,
                  and double-well anharmonic oscillators.}
}


@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{angelis1998berezin,
  AUTHOR = {G F De Angelis and G Jona-Lasinio and V
                  Sidoravicius},
  TITLE = {Berezin integrals and Poisson processes},
  JOURNAL = {J. Phys. A: Math. Gen.},
  YEAR = {1998},
  VOLUME = {31},
  PAGES = {289--308},
  PDF = {/sci_docs/physics/papers/JPhysA/angelis1998berezin.pdf},
  ROPSECTIONS = {ALGEBRA GRASSMANN QFT},
  ABSTRACT = {We show that the calculation of Berezin integrals
                  over anticommuting variables can be reduced to the
                  evaluation of expectations of functionals of Poisson
                  processes via an appropriate Feynman Kac formula. In
                  this way the tools of ordinary analysis can be
                  applied to Berezin integrals and, as an example, we
                  prove a simple upper bound. Possible applications of
                  our results are briefly mentioned.}
}


@ARTICLE{beccaria1999exact,
  AUTHOR = {M. Beccaria and C. Presilla and G. F. De Angelis and
                  G. Jona-Lasinio},
  TITLE = {An exact representation of the fermion dynamics in
                  terms of Poisson processes and its connection with
                  Monte Carlo algorithms},
  JOURNAL = {Europhys. Lett.},
  YEAR = {1999},
  VOLUME = {48},
  NUMBER = {3},
  PAGES = {243--249},
  MONTH = {November},
  ROPSECTIONS = {GRASSMANN QFT},
  PDF = {/sci_docs/physics/papers/EuroPhysLett/beccaria1999exact.pdf},
  ABSTRACT = {We present a simple derivation of a Feynman-Kac type
                  formula to study fermionic systems. In this approach
                  the real time or the imaginary time dynamics is
                  expressed in terms of the evolution of a collection
                  of Poisson processes. This formula leads to a family
                  of algorithms parametrized by the values of the jump
                  rates of the Poisson processes. From these an
                  optimal algorithm can be chosen which coincides with
                  the Green Function Monte Carlo method in the limit
                  when the latter becomes exact.}
}


@ARTICLE{zeh2003quantization,
  AUTHOR = {H. D. Zeh},
  TITLE = {There is no "first" quantization},
  JOURNAL = {Physics Letters A},
  YEAR = {2003},
  VOLUME = {309},
  NUMBER = {5--6},
  PAGES = {329--334},
  MONTH = {March},
  ROPSECTIONS = {QFT QUANTPHYS},
  PDF = {/sci_docs/physics/papers/PhysLettA/zeh2003quantization.pdf},
  ABSTRACT = {The introduction of spinor and other massive fields by
  "quantizing" particles (corpuscles) is conceptually misleading. Only
  spatial fields must be postulated to form the fundamental objects to
  be quantized (that is, to define a formal basis for all quantum
  states), while apparent "particles" are a mere consequence of
  decoherence. This conclusion is also supported by the nature of
  gauge fields.}
}


@ARTICLE{raifeartaigh2000gauge,
  AUTHOR = {Lochlainn O'Raifeartaigh and Norbert Straumann},
  TITLE = {Gauge theory: Historical origins and some modern developments},
  JOURNAL = {Reviews of Modern Physics},
  YEAR = {2000},
  VOLUME = {72},
  NUMBER = {1},
  PAGES = {1--23},
  MONTH = {January},
  ROPSECTIONS = {SURVEY QFT},
  PDF = {/sci_docs/physics/papers/RMP/raifeartaigh2000gauge.pdf},
  ABSTRACT = {One of the major developments of twentieth-century
  physics has been the gradual recognition that a common feature of
  the known fundamental interactions is their gauge structure. In this
  article the authors review the early history of gauge theory, from
  Einstein's theory of gravitation to the appearance of non-Abelian
  gauge theories in the fifties. The authors also review the early
  history of dimensional reduction, which played an important role in
  the development of gauge theory. A description is given of how, in
  recent times, the ideas of gauge theory and dimensional reduction
  have emerged naturally in the context of string theory and
  noncommutative geometry. }
}

@COMMENT{{ThisfilehasbeengeneratedbyPybliographer}}


@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}
}


@ARTICLE{frohlich2001asymptotic,
  AUTHOR = {J.Fröhlich and M.Griesemer and B.Schlein},
  TITLE = {Asymptotic Electromagnetic Fields in Models of Quantum-Mechanical Matter Interacting with the Quantized Radiation Field },
  JOURNAL = {Adv. Math.},
  YEAR = {2001},
  VOLUME = {164},
  PAGES = {349-398},
  ROPSECTIONS = {QFT},
  PDF = {/mathpapers/AdvMath/frolich2001asymptotic.pdf},
  ABSTRACT = {In models of
(non-relativistic and pseudo-relativistic)electrons interacting with
static nuclei and with the (ultraviolet-cutoff)quantized radiation
field,the existence of asymptotic electromagnetic fields is
established.Our results yield some mathe- matically rigorous
understanding of Rayleigh scattering and of the phenomenon of
relaxation of isolated atoms to their ground states.Our proofs are
based on prop- agation estimates for electrons inspired by similar
estimates known from N -body scattering theory.}
}


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