Finite-volume Hamiltonian method for coupled channel interactions in lattice QCD
arXiv:1402.4868 · doi:10.1103/PhysRevC.90.055206
Abstract
Within a multi-channel formulation of scattering, we investigate the use of the finite-volume Hamiltonian approach to resolve scattering observables from lattice QCD spectra. The asymptotic matching of the well-known Lüscher formalism encodes a unique finite-volume spectrum. Nevertheless, in many practical situations, such as coupled-channel systems, it is advantageous to interpolate isolated lattice spectra in order to extract physical scattering parameters. Here we study the use of the Hamiltonian framework as a parameterisation that can be fit directly to lattice spectra. We find that with a modest amount of lattice data, the scattering parameters can be reproduced rather well, with only a minor degree of model dependence.
25 pages, 16 figures
References in corpus (6)
- Dynamical coupled-channel model of meson production reactions in the nucleon resonance region
- S and D-wave phase shifts in isospin-2 pi pi scattering from lattice QCD
- Isoscalar meson spectroscopy from lattice QCD
- Scalar mesons in a finite volume
- Scalar mesons moving in a finite volume and the role of partial wave mixing
- Two-Nucleon Systems in a Finite Volume: (II) 3S1-3D1 Coupled Channels and the Deuteron
Cited by in corpus (39)
- Hadronic molecules
- The states: experimental and theoretical status and perspectives
- Scattering processes and resonances from lattice QCD
- Chiral perturbation theory for heavy hadrons and chiral effective field theory for heavy hadronic molecules
- Lattice QCD Evidence that the Lambda(1405) Resonance is an Antikaon-Nucleon Molecule
- Three-body Unitarity in the Finite Volume
- Fate of the Tetraquark Candidate Zc(3900) from Lattice QCD
- Hamiltonian effective field theory study of the resonance in lattice QCD
- Towards grounding nuclear physics in QCD
- tetraquark resonances with lattice QCD potentials and the Born-Oppenheimer approximation
- Novel coupled channel framework connecting quark model and lattice QCD: an investigation on near-threshold states
- Two-nucleon S-wave interactions at the flavor-symmetric point with : a first lattice QCD calculation with the stochastic Laplacian Heaviside method
- Structure of the from Hamiltonian effective field theory
- Hamiltonian effective field theory study of the resonance in lattice QCD
- Structure of the Roper Resonance from Lattice QCD Constraints
- Two-flavor Simulations of the and the Role of the Channel
- The Tetraquark Candidate Zc(3900) from Dynamical Lattice QCD Simulations
- Partial Wave Mixing in Hamiltonian Effective Field Theory
- Nuclear Reactions from Lattice QCD
- Hamiltonian effective field theory in elongated or moving finite volume
- Two-particle scattering from finite-volume quantization conditions using the plane wave basis
- New insight into the exotic states strongly coupled with the from the
- Study of decuplet baryon resonances from lattice QCD
- Nucleon resonance structure in the finite volume of lattice QCD
- Regularisation in Nonperturbative Extensions of Effective Field Theory
- Toward establishing low-lying and hyperon resonances with the reaction
- Kaonic Hydrogen and Deuterium in Hamiltonian Effective Field Theory
- The investigations of the -wave states combining quark model and lattice QCD in the coupled channel framework
- Structure of the resonance
- Pion photoproduction of nucleon excited states with Hamiltonian effective field theory
- Inverse scattering problem with a bare state
- Investigation on the bottom analogs of the
- The odd-parity strange baryons below 1.8 GeV with Hamiltonian effective field theory
- Nucleon Excited States from Lattice QCD and Hamiltonian Effective Field Theory
- Light-quark baryon spectroscopy within ANL-Osaka dynamical coupled-channels approach
- From Extraction of Nucleon Resonances to LQCD
- Finite-volume Hamiltonian method for scattering in lattice QCD
- Rediscovery of Numerical Lüscher's Formula from the Neural Network
- Towards the continuum coupling in nuclear lattice effective field theory I: A three-particle model