Journal
PHYSICAL REVIEW D
Volume 91, Issue 5, Pages -Publisher
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.91.054008
Keywords
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Funding
- U.S. Department of Energy INCITE program at Oak Ridge National Lab
- NSF Teragrid at the Texas Advanced Computer Center
- Pittsburgh Supercomputer Center
- Jefferson Lab
- U.S. Department of Energy [DE-AC05-06OR23177]
- U.S. Department of Energy Early Career award [DE-SC0006765]
- Science and Technology Facilities Council (UK) [ST/L000385/1]
- Direct For Computer & Info Scie & Enginr [0832315] Funding Source: National Science Foundation
- Office of Advanced Cyberinfrastructure (OAC) [0832315] Funding Source: National Science Foundation
- Science and Technology Facilities Council [ST/J000434/1, ST/L000385/1] Funding Source: researchfish
- STFC [ST/J000434/1, ST/L000385/1] Funding Source: UKRI
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Coupled-channel pi K and eta K scattering amplitudes are determined by studying the finite-volume energy spectra obtained from dynamical lattice QCD calculations. Using a large basis of interpolating operators, including both those resembling a q (q) over barq construction and those resembling a pair of mesons with relative momentum, a reliable excited-state spectrum can be obtained. Working at m(pi) = 391 MeV, we find a gradual increase in the J(P) =0(+) pi K phase shift which may be identified with a broad scalar resonance that couples strongly to pi K and weakly to eta K. The low-energy behavior of this amplitude suggests a virtual bound state that may be related to the. resonance. A bound state with J(P) = 1(-) is found very close to the pi K threshold energy, whose coupling to the pi K channel is compatible with that of the experimental K star(892). Evidence is found for a narrow resonance in J(P) = 2(+). Isospin-3/2 pi K scattering is also studied, and nonresonant phase shifts spanning the whole elastic scattering region are obtained.
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