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@ARTICLE{Hohenadler:885474,
author = {Hohenadler, Martin and Assaad, Fakher F.},
title = {{O}rthogonal metal in the {H}ubbard model with liberated
slave spins},
journal = {Physical review / B},
volume = {100},
number = {12},
issn = {2469-9950},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2020-03857},
pages = {125133},
year = {2019},
abstract = {A two-dimensional Falicov-Kimball model, equivalent to the
Hubbard model in an unconstrained slave-spin representation,
is studied by quantum Monte Carlo simulations. The focus is
on a fractionalized metallic phase that is characterized in
terms of spectral, thermodynamic, and transport properties,
including a comparison to the half-filled Hubbard model. The
properties of this phase, most notably a single-particle gap
but gapless spin and charge excitations, can in principle be
understood in the framework of orthogonal metals. However,
important and interesting differences arise in the present
setting compared to single-particle mean-field theories and
other models. We also discuss the role of the local
constraints from the slave-spin representation within an
extended phase diagram that includes the spatial dimension
as a parameter, thereby making contact with previous work in
infinite dimensions. Finally, we highlight the absence of
$π$-flux configurations in the slave-spin formulation, in
particular in the context of topologically ordered
fractional phases predicted at the mean-field level.},
ddc = {530},
pnm = {899 - ohne Topic (POF4-899) / Numerical simulations of
strongly correlated electron systems. $(hwb03_20190501)$},
pid = {G:(DE-HGF)POF4-899 / $G:(DE-Juel1)hwb03_20190501$},
typ = {PUB:(DE-HGF)16},
doi = {10.1103/PhysRevB.100.125133},
url = {https://juser.fz-juelich.de/record/885474},
}