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arXiv:cond-mat/9502088 · Zeitschrift für Physik B Condensed Matter

Functional bosonization of interacting fermions in arbitrary dimensions

Peter Kopietz, Kurt Schönhammer

Published Mar 1, 1996• 50 citations
arXivHTMLPDF
DOI
10.1007/s002570050119

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We find analytic models that can perfectly transfer, without state initialization or remote collaboration, arbitrary functions in two- and three-dimensional interacting bosonic and fermionic networks. This provides for the possible experimental implementation of state transfer through bosonic or fermionic atoms trapped in optical lattices. A significant finding is that the state of a spin qubit can be perfectly transferred through a fermionic system. Families of Hamiltonians are described that are related to the linear models and that enable the perfect transfer of arbitrary functions. Furthermore, we propose methods for eliminating certain types of errors.
We develop a method that allows us to map models of interacting fermions onto bosonic models describing collective excitations in an arbitrary dimension. We present arguments that this mapping may become exact in the thermodynamic limit in the presence of a bath. The boson models can be written either in the form of a model of noninteracting bosons in a fluctuating auxiliary Hubbard-Stratonovich field or in the form of a superfield theory of interacting bosons. We show how one can study the latter version within the perturbation theory. Using a diagrammatic technique developed for the boson model we compare the first two orders of the perturbation theory with the corresponding results for the original fermion model and find a perfect agreement. As concerns the former representation, we suggest a scheme that may be suitable for Monte Carlo simulations. We demonstrate both analytically and numerically that the partition function of the boson model in the auxiliary Hubbard-Stratonovich field is, in contrast to the fermion model, always positive and thus the boson model can be suitable for the Monte Carlo routine. At the same time, our arguments showing the equivalence of the boson and fermion models in the thermodynamic limit are not completely rigorous and it is still to be investigated numerically how accurate the boson model can approximate the original fermion one.
In the bosonization theory, we propose in this paper a definition of ``quasiparticles'' for interacting fermions at arbitrary space dimenions. In dimensions higher than one, we show that the constructed quasiparticles are consistent with quasiparticle descriptions in the Landau--Fermi-liquid theory, whereas in one dimension the quasiparticles are nonperturbative objects (spinons and holons) obeying fractional statistics. Application of our theory to Fermion liquids with singular Landau interaction is discussed.