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Multi-grid HMC for Ginsparg-Wilson fermions
High Energy Physics - Lattice · Submitted 20 Oct 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Because the bulk of the work takes place on the coarse lattice, including the calculation of most observables, this method saves over an order of magnitude in computer time over previous methods.
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The abstract, sentence by sentence
I describe a method that places the fermion fields and the gauge fields on different lattice spacings during the Hybrid Monte Carlo generation of Ginsparg-Wilson dynamical ensembles. The idea is motivated by Wilson's formulation of the renormalisation group. After outlining the underlying theory, I describe a method to perform most of the work of the HMC on a coarse lattice, only requiring to convert to and from the fine lattice once for each independent configuration. Because the bulk of the work takes place on the coarse lattice, including the calculation of most observables, this method saves over an order of magnitude in computer time over previous methods.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | I describe a method that places the fermion fields and the gauge fields on different lattice spacings during the Hybrid Monte Carlo generation of Ginsparg-Wilson dynamical ensembles. | contribution 0.62 | 0.85 | 0.12 | asserted 0.99 |
| s1 | The idea is motivated by Wilson's formulation of the renormalisation group. | background 1.00 | 0.08 | 0.02 | asserted 0.98 |
| s2 | After outlining the underlying theory, I describe a method to perform most of the work of the HMC on a coarse lattice, only requiring to convert to and from the fine lattice once for each independent configuration. | method 0.98 | 0.81 | 0.14 | asserted 0.99 |
| s3 | Because the bulk of the work takes place on the coarse lattice, including the calculation of most observables, this method saves over an order of magnitude in computer time over previous methods. | result 0.98 | 0.85 | 0.78 | asserted 1.00 |
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The paper
Original abstract
I describe a method that places the fermion fields and the gauge fields on different lattice spacings during the Hybrid Monte Carlo generation of Ginsparg-Wilson dynamical ensembles. The idea is motivated by Wilson's formulation of the renormalisation group. After outlining the underlying theory, I describe a method to perform most of the work of the HMC on a coarse lattice, only requiring to convert to and from the fine lattice once for each independent configuration. Because the bulk of the work takes place on the coarse lattice, including the calculation of most observables, this method saves over an order of magnitude in computer time over previous methods.
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How the literature uses it
1 arXiv paper cite this in 1 sentence
What it cites · 4 sentences without a confident label
Uses the method or tool of 1 paper
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Therefore, the Yang-Mills action can be written as [equation] This can obviously and easily be extended to any lattice formulation of the Dirac operator, although for any Dirac operator which is not ultra local, including the overlap, the numerical implementation requires a stochastic estimate, either following the method proposed in [ref] , or by using a Gaussian heat-bath and a rational approximation of the exponential.
The Kentucky Noisy Monte Carlo Algorithm for Wilson Dynamical Fermions · Gauge Action · 0.88
Cites as background 3 papers
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Overlap fermions [ref] are unquestionably the theoretically cleanest formulation of lattice QCD, because they alone exactly fulfil the Ginsparg-Wilson relation [ref] and satisfy an exact chiral symmetry on the lattice [ref] .
Chiral Fermions on the Lattice · Introduction · 0.90
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Overlap fermions [ref] are unquestionably the theoretically cleanest formulation of lattice QCD, because they alone exactly fulfil the Ginsparg-Wilson relation [ref] and satisfy an exact chiral symmetry on the lattice [ref] .
Exact chiral symmetry on the lattice and the Ginsparg-Wilson relation · Introduction · 0.90
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The idea of using the trace of a function of the Dirac operator to simulate the gauge action was first proposed in [ref] .
A Framework for Systematic Study of QCD Vacuum Structure II: Coherent Lattice QCD · Gauge Action · 0.92
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