520 research outputs found
Asymmetric spatial structure of zero modes for birefringent Dirac fermions
We study the zero energy modes that arise in an unusual vortex configuration
involving both the kinetic energy and an appropriate mass term in a model which
exhibits birefringent Dirac fermions as its low energy excitations. We find the
surprising feature that the ratio of the length scales associated with states
centered on vortex and anti-vortex topological defects can be arbitrarily
varied but that fractionalization of quantum numbers such as charge is
unaffected. We discuss this situation from a symmetry point of view and present
numerical results for a specific lattice model realization of this scenario.Comment: 7 pages, 6 figure
Transport in a periodically--driven tilted lattice via the extended reservoir approach: Stability criterion for recovering the continuum limit
Extended reservoirs provide a framework for capturing macroscopic, continuum
environments, such as metallic electrodes driving a current through a nanoscale
contact, impurity, or material. We examine the application of this approach to
periodically--driven systems, specifically in the context of quantum transport.
As with non--equilibrium steady states in time--independent scenarios, the
current displays a Kramers' turnover including the formation of a plateau
region that captures the physical, continuum limit response. We demonstrate
that a simple stability criteria identifies an appropriate relaxation rate to
target this physical plateau. Using this approach, we study quantum transport
through a periodically--driven tilted lattice coupled to two metallic
reservoirs held at a finite bias and temperature. We use this model to
benchmark the extended reservoir approach and assess the stability criteria.
When the system and reservoir are weakly coupled, the approach recovers
well--understood physical behavior in this limit. Extended reservoirs enable
addressing strong coupling and non--linear response as well, where we analyze
how transport responds to the dynamics inside the driven lattice. These results
set the foundations for the use of extended reservoir approach for
periodically-driven, quantum systems, such as many--body Floquet states
The confluence of fractured resonances at points of dynamical, many--body flare
Resonant transport occurs when there is a matching of frequencies across some
spatial medium, increasing the efficiency of shuttling particles from one
reservoir to another. We demonstrate that in a periodically driven, many--body
titled lattice there are sets of spatially fractured resonances. These
``emanate'' from two essential resonances due to scattering off internal
surfaces created when the driving frequency and many--body interaction strength
vary, a scattering reminiscent of lens flare. The confluence of these fractured
resonances dramatically enhances transport. At one confluence, the interaction
strength is finite and the essential resonance arises due to the interplay of
interaction with the counter--rotating terms of the periodic drive. The other
forms where several paths split by the many--body interaction merge in the
non--interacting limit. We discuss the origin and structure of the fractured
resonances, as well as the scaling of the conductance on system parameters.
These results furnish a new example of the richness of open, driven, many--body
systems.Comment: comments welcome
On the flat cohomology of binary norm forms
Let be an order of index in the maximal order of a
quadratic number field . Let
be the orthogonal -group of the
associated norm form . We describe the structure of the pointed set
, which classifies
quadratic forms isomorphic (properly or improperly) to in the flat
topology. Gauss classified quadratic forms of fundamental discriminant and
showed that the composition of any binary -form of discriminant
with itself belongs to the principal genus. Using cohomological
language, we extend these results to forms of certain non-fundamental
discriminants.Comment: 24 pages, submitted. Comments are welcom
Discrete molecular dynamics simulations of peptide aggregation
We study the aggregation of peptides using the discrete molecular dynamics
simulations. At temperatures above the alpha-helix melting temperature of a
single peptide, the model peptides aggregate into a multi-layer parallel
beta-sheet structure. This structure has an inter-strand distance of 0.48 nm
and an inter-sheet distance of 1.0 nm, which agree with experimental
observations. In this model, the hydrogen bond interactions give rise to the
inter-strand spacing in beta-sheets, while the Go interactions among side
chains make beta-strands parallel to each other and allow beta-sheets to pack
into layers. The aggregates also contain free edges which may allow for further
aggregation of model peptides to form elongated fibrils.Comment: 15 pages, 8 figure
Investigative approaches: Lessons learned from the RaDonda Vaught case
Accidental patient harms occur frequently in healthcare, but their exact prevalence and interventions that will best prevent them are still poorly understood. In rare cases, healthcare providers who have contributed to accidental patient harm may be criminally prosecuted to obtain justice for the patient and family or to set an example, which theoretically prevents other providers from making similar mistakes due to fear of punishment. A recent case where this strategy was chosen is the RaDonda L. Vaught vs. Tennessee (2022) criminal case. The present article discusses this case and its ramifications, as well as provides concrete recommendations for actions that healthcare organizations should take to foster a safer and more resilient healthcare system. Recommendations include placing an emphasis on just culture; ensuring timely, systems-level investigations of all incidents; creating and facilitating participation in a national reporting system; incorporating Human Factors professionals at multiple levels of organizations; and establishing a national safety board for medicine
Theory of interacting electrons on the honeycomb lattice
The low-energy theory of electrons interacting via repulsive short-range
interactions on graphene's honeycomb lattice at half filling is presented. The
exact symmetry of the Lagrangian with local quartic terms for the Dirac field
dictated by the lattice is D_2 x U_c(1) x (time reversal), where D_2 is the
dihedral group, and U_c(1) is a subgroup of the SU_c(2) "chiral" group of the
non-interacting Lagrangian, that represents translations in Dirac language. The
Lagrangian describing spinless particles respecting this symmetry is
parameterized by six independent coupling constants. We show how first imposing
the rotational, then Lorentz, and finally chiral symmetry to the quartic terms,
in conjunction with the Fierz transformations, eventually reduces the set of
couplings to just two, in the "maximally symmetric" local interacting theory.
We identify the two critical points in such a Lorentz and chirally symmetric
theory as describing metal-insulator transitions into the states with either
time-reversal or chiral symmetry being broken. In the site-localized limit of
the interacting Hamiltonian the low-energy theory describes the continuous
transitions into the insulator with either a finite Haldane's (circulating
currents) or Semenoff's (staggered density) masses, both in the universality
class of the Gross-Neveu model. The picture of the metal-insulator transition
on a honeycomb lattice emerges at which the residue of the quasiparticle pole
at the metallic and the mass-gap in the insulating phase both vanish
continuously as the critical point is approached. We argue that the Fermi
velocity is non-critical as a consequence of the dynamical exponent being fixed
to unity by the emergent Lorentz invariance. Effects of long-range interaction
and the critical behavior of specific heat and conductivity are discussed.Comment: 16 revtex pages, 4 figures; typos corrected, new and updated
references; published versio
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