Bose-Fermi dualities for arbitrary one-dimensional quantum systems in
the universal low energy regime
- URL: http://arxiv.org/abs/2009.00624v3
- Date: Sat, 17 Oct 2020 06:59:10 GMT
- Title: Bose-Fermi dualities for arbitrary one-dimensional quantum systems in
the universal low energy regime
- Authors: Manuel Valiente
- Abstract summary: I consider general interacting systems of quantum particles in one spatial dimension.
These consist of bosons or fermions, which can have any number of components, arbitrary spin or a combination thereof.
The single-particle dispersion can be Galilean (non-relativistic), relativistic, or have any other form that may be relevant for the continuum limit of lattice theories.
- Score: 0.2741266294612775
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: I consider general interacting systems of quantum particles in one spatial
dimension. These consist of bosons or fermions, which can have any number of
components, arbitrary spin or a combination thereof, featuring low-energy two-
and multiparticle interactions. The single-particle dispersion can be Galilean
(non-relativistic), relativistic, or have any other form that may be relevant
for the continuum limit of lattice theories. Using an algebra of generalized
functions, statistical transmutation operators that are genuinely unitary are
obtained, putting bosons and fermions in a one-to-one correspondence without
the need for a short-distance hard core. In the non-relativistic case,
low-energy interactions for bosons yield, order by order, fermionic dual
interactions that correspond to the standard low-energy expansion for fermions.
In this way, interacting fermions and bosons are fully equivalent to each other
at low energies. While the Bose-Fermi mappings do not depend on microscopic
details, the resulting statistical interactions heavily depend on the kinetic
energy structure of the respective Hamiltonians. These statistical interactions
are obtained explicitly for a variety of models, and regularized and
renormalized in the momentum representation, which allows for theoretically and
computationally feasible implementations of the dual theories. The mapping is
rewritten as a gauge interaction, and one-dimensional anyons are also
considered.
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