2020
Balm, Floris; Krikun, Alexander; Romero-Bermudez, Aurelio; Schalm, Koenraad; Zaanen, Jan
Isolated zeros destroy Fermi surface in holographic models with a lattice Tijdschriftartikel
In: JOURNAL OF HIGH ENERGY PHYSICS, nr. 1, 2020, ISSN: 1029-8479.
Abstract | Links | BibTeX | Tags: Holography and condensed matter physics (AdS/CMT); Space-Time Symmetries
@article{WOS:000514392000002,
title = {Isolated zeros destroy Fermi surface in holographic models with a
lattice},
author = {Floris Balm and Alexander Krikun and Aurelio Romero-Bermudez and Koenraad Schalm and Jan Zaanen},
doi = {10.1007/JHEP01(2020)151},
issn = {1029-8479},
year = {2020},
date = {2020-01-01},
journal = {JOURNAL OF HIGH ENERGY PHYSICS},
number = {1},
publisher = {SPRINGER},
address = {ONE NEW YORK PLAZA, SUITE 4600, NEW YORK, NY, UNITED STATES},
abstract = {We study the fermionic spectral density in a strongly correlated quantum
system described by a gravity dual. In the presence of periodically
modulated chemical potential, which models the effect of the ionic
lattice, we explore the shapes of the corresponding Fermi surfaces,
defined by the location of peaks in the spectral density at the Fermi
level. We find that at strong lattice potentials sectors of the Fermi
surface are unexpectedly destroyed and the Fermi surface becomes an
arc-like disconnected manifold. We explain this phenomenon in terms of a
collision of the Fermi surface pole with zeros of the fermionic Green's
function, which are explicitly computable in the holographic dual.},
keywords = {Holography and condensed matter physics (AdS/CMT); Space-Time Symmetries},
pubstate = {published},
tppubtype = {article}
}
We study the fermionic spectral density in a strongly correlated quantum
system described by a gravity dual. In the presence of periodically
modulated chemical potential, which models the effect of the ionic
lattice, we explore the shapes of the corresponding Fermi surfaces,
defined by the location of peaks in the spectral density at the Fermi
level. We find that at strong lattice potentials sectors of the Fermi
surface are unexpectedly destroyed and the Fermi surface becomes an
arc-like disconnected manifold. We explain this phenomenon in terms of a
collision of the Fermi surface pole with zeros of the fermionic Green's
function, which are explicitly computable in the holographic dual.
system described by a gravity dual. In the presence of periodically
modulated chemical potential, which models the effect of the ionic
lattice, we explore the shapes of the corresponding Fermi surfaces,
defined by the location of peaks in the spectral density at the Fermi
level. We find that at strong lattice potentials sectors of the Fermi
surface are unexpectedly destroyed and the Fermi surface becomes an
arc-like disconnected manifold. We explain this phenomenon in terms of a
collision of the Fermi surface pole with zeros of the fermionic Green's
function, which are explicitly computable in the holographic dual.
2016
Bagrov, A.; Kaplis, N.; Krikun, A.; Schalm, K.; Zaanen, J.
Holographic fermions at strong translational symmetry breaking: a Bianchi-VII case study Tijdschriftartikel
In: JOURNAL OF HIGH ENERGY PHYSICS, nr. 11, 2016, ISSN: 1029-8479.
Abstract | Links | BibTeX | Tags: Holography and condensed matter physics (AdS/CMT); Space-Time Symmetries
@article{WOS:000387686000001,
title = {Holographic fermions at strong translational symmetry breaking: a
Bianchi-VII case study},
author = {A. Bagrov and N. Kaplis and A. Krikun and K. Schalm and J. Zaanen},
doi = {10.1007/JHEP11(2016)057},
issn = {1029-8479},
year = {2016},
date = {2016-11-01},
journal = {JOURNAL OF HIGH ENERGY PHYSICS},
number = {11},
publisher = {SPRINGER},
address = {233 SPRING ST, NEW YORK, NY 10013 USA},
abstract = {It is presently unknown how strong lattice potentials influence the
fermion spectral function of the holographic strange metals predicted by
the AdS/CFT correspondence. This embodies a crucial test for the
application of holography to condensed matter experiments. We show that
for one particular momentum direction this spectrum can be computed for
arbitrary strength of the effective translational symmetry breaking
potential of the so-called Bianchi-VII geometry employing ordinary
differential equations. Deep in the strange metal regime we find rather
small changes to the single-fermion response computed by the emergent
quantum critical IR, even when the potential becomes relevant in the
infra-red. However, in the regime where holographic quasi-particles
occur, defining a Fermi surface in the continuum, they acquire a finite
lifetime at any finite potential strength. At the transition from
irrelevancy to relevancy of the Bianchi potential in the deep infra-red
the quasi-particle remnants disappear completely and the fermion
spectrum exhibits a purely relaxational behaviour.},
keywords = {Holography and condensed matter physics (AdS/CMT); Space-Time Symmetries},
pubstate = {published},
tppubtype = {article}
}
It is presently unknown how strong lattice potentials influence the
fermion spectral function of the holographic strange metals predicted by
the AdS/CFT correspondence. This embodies a crucial test for the
application of holography to condensed matter experiments. We show that
for one particular momentum direction this spectrum can be computed for
arbitrary strength of the effective translational symmetry breaking
potential of the so-called Bianchi-VII geometry employing ordinary
differential equations. Deep in the strange metal regime we find rather
small changes to the single-fermion response computed by the emergent
quantum critical IR, even when the potential becomes relevant in the
infra-red. However, in the regime where holographic quasi-particles
occur, defining a Fermi surface in the continuum, they acquire a finite
lifetime at any finite potential strength. At the transition from
irrelevancy to relevancy of the Bianchi potential in the deep infra-red
the quasi-particle remnants disappear completely and the fermion
spectrum exhibits a purely relaxational behaviour.
fermion spectral function of the holographic strange metals predicted by
the AdS/CFT correspondence. This embodies a crucial test for the
application of holography to condensed matter experiments. We show that
for one particular momentum direction this spectrum can be computed for
arbitrary strength of the effective translational symmetry breaking
potential of the so-called Bianchi-VII geometry employing ordinary
differential equations. Deep in the strange metal regime we find rather
small changes to the single-fermion response computed by the emergent
quantum critical IR, even when the potential becomes relevant in the
infra-red. However, in the regime where holographic quasi-particles
occur, defining a Fermi surface in the continuum, they acquire a finite
lifetime at any finite potential strength. At the transition from
irrelevancy to relevancy of the Bianchi potential in the deep infra-red
the quasi-particle remnants disappear completely and the fermion
spectrum exhibits a purely relaxational behaviour.