2 research outputs found
Isospin-1/2 scattering and the lightest resonance from lattice QCD
Isospin-1/2 scattering amplitudes are computed using lattice QCD,
working in a single volume of approximately and with a
light quark mass corresponding to MeV. The spectrum of the
elastic energy region is computed yielding 20 energy levels. Using the
L\"uscher finite-volume quantisation condition these energies are translated
into constraints on the infinite volume scattering amplitudes. For the first
time, we find a complex resonance pole from lattice QCD, strongly
coupled to the -wave channel, with a mass MeV and a
width MeV. Combined with earlier work investigating the
, and with heavier light quarks, similar couplings
between each of these scalar states and their relevant meson-meson scattering
channels are determined. The mass of the is consistently found well
below that of the , in contrast to the currently reported
experimental result.Comment: 39 pages, 13 figure
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Coupled-channel Dπ, Dη and D<inf>s</inf>K¯ scattering from lattice QCD
We present the first lattice QCD study of coupled-channel , and
scattering in isospin-1/2 in three partial waves. Using
distillation, we compute matrices of correlation functions with bases of
operators capable of resolving both meson and meson-meson contributions to the
spectrum. These correlation matrices are analysed using a variational approach
to extract the finite-volume energy eigenstates. Utilising L\"uscher's method
and its extensions, we constrain scattering amplitudes in , and -wave
as a function of energy. By analytically continuing the scattering amplitudes
to complex energies, we investigate the -matrix singularities. Working at
MeV, we find a pole corresponding to a
near-threshold bound state with a large coupling to . We also find a
deeply bound state, and evidence for a narrow
resonance coupled predominantly to . Elastic scattering in the
isospin- channel is studied and we find a weakly repulsive interaction in
-wave.GM acknowledges support from the Herchel Smith Fund at the University of Cambridge and the Deutsche Forschungsgemeinschaft (DFG) under contract KN 947/1-2. SMR acknowledges support from Science Foundation Ireland [RFP-PHY-3201]. CET acknowledges support from the U.K. Science and Technology Facilities Council (STFC) [grant ST/L000385/1] and the Isaac Newton Trust/University of Cambridge Early Career Support Scheme [RG74916]. The software codes Chroma [58] and QUDA [59, 60] were used to perform this work at Jeerson Laboratory under the USQCD Initiative and the LQCD ARRA project, and on the Lonsdale cluster maintained by the Trinity Centre for High Performance Computing funded through grants from Science Foundation Ireland (SFI). This work also used the DiRAC Data Analytic system at the University of Cambridge, operated by the University of Cambridge High Performance Computing Service on behalf of the STFC DiRAC HPC Facility (www.dirac.ac.uk). This equipment was funded by BIS National E-infrastructure capital grant ST/K001590/1, STFC capital grants ST/H008861/1 and ST/H00887X/1, and STFC DiRAC Operations grant ST/K00333X/1. DiRAC is part of the National E-Infrastructure. This research also used the Wilkes GPU cluster at the University of Cambridge High Performance Computing Service (http://www.hpc.cam.ac.uk/), provided by Dell Inc., NVIDIA and Mellanox, and part funded by STFC with industrial sponsorship from Rolls Royce and Mitsubishi Heavy Industries. Gauge con gurations were generated using resources awarded from the U.S. Department of Energy INCITE program at Oak Ridge National Laboratory, the NSF Teragrid at the Texas Advanced Computer Center and the Pittsburgh Supercomputer Center, as well as at Jeerson Lab.This is the final version of the article. It first appeared from Springer via https://doi.org/10.1007/JHEP10(2016)01