64,252 research outputs found
Finite Density Matrix Renormalisation Group Algorithm for Anyonic Systems
The numerical study of anyonic systems is known to be highly challenging due
to their non-bosonic, non-fermionic particle exchange statistics, and with the
exception of certain models for which analytical solutions exist, very little
is known about their collective behaviour as a result. Meanwhile, the density
matrix renormalisation group (DMRG) algorithm is an exceptionally powerful
numerical technique for calculating the ground state of a low-dimensional
lattice Hamiltonian, and has been applied to the study of bosonic, fermionic,
and group-symmetric systems. The recent development of a tensor network
formulation for anyonic systems opened up the possibility of studying these
systems using algorithms such as DMRG, though this has proved challenging both
in terms of programming complexity and computational cost. This paper presents
the implementation of DMRG for finite anyonic systems, including a detailed
scheme for the implementation of anyonic tensors with optimal scaling of
computational cost. The anyonic DMRG algorithm is demonstrated by calculating
the ground state energy of the Golden Chain, which has become the benchmark
system for the numerical study of anyons, and is shown to produce results
comparable to those of the anyonic TEBD algorithm and superior to the
variationally optimised anyonic MERA, at far lesser computational cost.Comment: 24 pages, 37 figure files (25 floating figures). RevTeX 4.1. Minor
changes for clarity in Figs. 9 & 11, matching published versio
Tensor network states and algorithms in the presence of a global U(1) symmetry
Tensor network decompositions offer an efficient description of certain
many-body states of a lattice system and are the basis of a wealth of numerical
simulation algorithms. In a recent paper [arXiv:0907.2994v1] we discussed how
to incorporate a global internal symmetry, given by a compact, completely
reducible group G, into tensor network decompositions and algorithms. Here we
specialize to the case of Abelian groups and, for concreteness, to a U(1)
symmetry, often associated with particle number conservation. We consider
tensor networks made of tensors that are invariant (or covariant) under the
symmetry, and explain how to decompose and manipulate such tensors in order to
exploit their symmetry. In numerical calculations, the use of U(1) symmetric
tensors allows selection of a specific number of particles, ensures the exact
preservation of particle number, and significantly reduces computational costs.
We illustrate all these points in the context of the multi-scale entanglement
renormalization ansatz.Comment: 22 pages, 25 figures, RevTeX
Further Series Studies of the Spin-1/2 Heisenberg Antiferromagnet at T=0: Magnon Dispersion and Structure Factors
We have extended our previous series studies of quantum antiferromagnets at
zero temperature by computing the one-magnon dispersion curves and various
structure factors for the linear chain, square and simple cubic lattices. Many
of these results are new; others are a substantial extension of previous work.
These results are directly comparable with neutron scattering experiments and
we make such comparisons where possible.Comment: 15 pages, 12 figures, revised versio
Controlling Mixing Inside a Droplet by Time Dependent Rigid-body Rotation
The use of microscopic discrete fluid volumes (i.e., droplets) as
microreactors for digital microfluidic applications often requires mixing
enhancement and control within droplets. In this work, we consider a
translating spherical liquid droplet to which we impose a time periodic
rigid-body rotation which we model using the superposition of a Hill vortex and
an unsteady rigid body rotation. This perturbation in the form of a rotation
not only creates a three-dimensional chaotic mixing region, which operates
through the stretching and folding of material lines, but also offers the
possibility of controlling both the size and the location of the mixing. Such a
control is achieved by judiciously adjusting the three parameters that
characterize the rotation, i.e., the rotation amplitude, frequency and
orientation of the rotation. As the size of the mixing region is increased,
complete mixing within the drop is obtained.Comment: 6 pages, 6 figure
Matrix product states for anyonic systems and efficient simulation of dynamics
Matrix product states (MPS) have proven to be a very successful tool to study
lattice systems with local degrees of freedom such as spins or bosons.
Topologically ordered systems can support anyonic particles which are labeled
by conserved topological charges and collectively carry non-local degrees of
freedom. In this paper we extend the formalism of MPS to lattice systems of
anyons. The anyonic MPS is constructed from tensors that explicitly conserve
topological charge. We describe how to adapt the time-evolving block decimation
(TEBD) algorithm to the anyonic MPS in order to simulate dynamics under a local
and charge-conserving Hamiltonian. To demonstrate the effectiveness of anyonic
TEBD algorithm, we used it to simulate (i) the ground state (using imaginary
time evolution) of an infinite 1D critical system of (a) Ising anyons and (b)
Fibonacci anyons both of which are well studied, and (ii) the real time
dynamics of an anyonic Hubbard-like model of a single Ising anyon hopping on a
ladder geometry with an anyonic flux threading each island of the ladder. Our
results pertaining to (ii) give insight into the transport properties of
anyons. The anyonic MPS formalism can be readily adapted to study systems with
conserved symmetry charges, as this is equivalent to a specialization of the
more general anyonic case.Comment: 18 pages, 15 figue
Simulation of braiding anyons using Matrix Product States
Anyons exist as point like particles in two dimensions and carry braid
statistics which enable interactions that are independent of the distance
between the particles. Except for a relatively few number of models which are
analytically tractable, much of the physics of anyons remain still unexplored.
In this paper, we show how U(1)-symmetry can be combined with the previously
proposed anyonic Matrix Product States to simulate ground states and dynamics
of anyonic systems on a lattice at any rational particle number density. We
provide proof of principle by studying itinerant anyons on a one dimensional
chain where no natural notion of braiding arises and also on a two-leg ladder
where the anyons hop between sites and possibly braid. We compare the result of
the ground state energies of Fibonacci anyons against hardcore bosons and
spinless fermions. In addition, we report the entanglement entropies of the
ground states of interacting Fibonacci anyons on a fully filled two-leg ladder
at different interaction strength, identifying gapped or gapless points in the
parameter space. As an outlook, our approach can also prove useful in studying
the time dynamics of a finite number of nonabelian anyons on a finite
two-dimensional lattice.Comment: Revised version: 20 pages, 14 captioned figures, 2 new tables. We
have moved a significant amount of material concerning symmetric tensors for
anyons --- which can be found in prior works --- to Appendices in order to
streamline our exposition of the modified Anyonic-U(1) ansat
Quantum mechanics without spacetime II : noncommutative geometry and the free point particle
In a recent paper we have suggested that a formulation of quantum mechanics
should exist, which does not require the concept of time, and that the
appropriate mathematical language for such a formulation is noncommutative
differential geometry. In the present paper we discuss this formulation for the
free point particle, by introducing a commutation relation for a set of
noncommuting coordinates. The sought for background independent quantum
mechanics is derived from this commutation relation for the coordinates. We
propose that the basic equations are invariant under automorphisms which map
one set of coordinates to another- this is a natural generalization of
diffeomorphism invariance when one makes a transition to noncommutative
geometry. The background independent description becomes equivalent to standard
quantum mechanics if a spacetime manifold exists, because of the proposed
automorphism invariance. The suggested basic equations also give a quantum
gravitational description of the free particle.Comment: 8 page
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