TY - JOUR
T1 - P -wave ππ scattering and the ρ resonance from lattice QCD
AU - Alexandrou, Constantia
AU - Leskovec, Luka
AU - Meinel, Stefan
AU - Negele, John
AU - Paul, Srijit
AU - Petschlies, Marcus
AU - Pochinsky, Andrew
AU - Rendon, Gumaro
AU - Syritsyn, Sergey
N1 - Funding Information:
We are grateful to Kostas Orginos for providing the gauge field ensemble, which was generated using resources provided by XSEDE (supported by National Science Foundation Grant No. ACI-1053575). We thank Raul Briceño, Sean Fleming, Doug Toussaint, and Bira Van Kolck for valueable discussions. S. M. and G. R. are supported by National Science Foundation Grant No. PHY-1520996; S. M. and S. S. also acknowledge support by the RHIC Physics Fellow Program of the RIKEN BNL Research Center. J. N. and A. P. were supported in part by the U.S. Department of Energy Office of Nuclear Physics under Grants No. DE-SC-0011090 and No. DE-FC02-06ER41444. We acknowledge funding from the European Union’s Horizon 2020 research and innovation programme under the Marie Sklodowska-Curie grant agreement No. 642069. S. P. is a Marie Sklodowska-Curie fellow supported by the HPC-LEAP joint doctorate program. This research used resources of the National Energy Research Scientific Computing Center, a DOE Office of Science User Facility supported by the Office of Science of the U.S. Department of Energy under Contract No. DE-AC02-05CH11231. The computations were performed using the Qlua software suite [77] .
Publisher Copyright:
© 2017 American Physical Society.
PY - 2017/8/1
Y1 - 2017/8/1
N2 - We calculate the parameters describing elastic I=1, P-wave ππ scattering using lattice QCD with 2+1 flavors of clover fermions. Our calculation is performed with a pion mass of mπ≈320 MeV and a lattice size of L≈3.6 fm. We construct the two-point correlation matrices with both quark-antiquark and two-hadron interpolating fields using a combination of smeared forward, sequential and stochastic propagators. The spectra in all relevant irreducible representations for total momenta |P→|≤32πL are extracted with two alternative methods: a variational analysis as well as multiexponential matrix fits. We perform an analysis using Lüscher's formalism for the energies below the inelastic thresholds, and investigate several phase shift models, including possible nonresonant contributions. We find that our data are well described by the minimal Breit-Wigner form, with no statistically significant nonresonant component. In determining the ρ resonance mass and coupling we compare two different approaches: fitting the individually extracted phase shifts versus fitting the t-matrix model directly to the energy spectrum. We find that both methods give consistent results, and at a pion mass of amπ=0.18295(36)stat obtain gρππ=5.69(13)stat(16)sys, amρ=0.4609(16)stat(14)sys, and amρ/amN=0.7476(38)stat(23)sys, where the first uncertainty is statistical and the second is the systematic uncertainty due to the choice of fit ranges.
AB - We calculate the parameters describing elastic I=1, P-wave ππ scattering using lattice QCD with 2+1 flavors of clover fermions. Our calculation is performed with a pion mass of mπ≈320 MeV and a lattice size of L≈3.6 fm. We construct the two-point correlation matrices with both quark-antiquark and two-hadron interpolating fields using a combination of smeared forward, sequential and stochastic propagators. The spectra in all relevant irreducible representations for total momenta |P→|≤32πL are extracted with two alternative methods: a variational analysis as well as multiexponential matrix fits. We perform an analysis using Lüscher's formalism for the energies below the inelastic thresholds, and investigate several phase shift models, including possible nonresonant contributions. We find that our data are well described by the minimal Breit-Wigner form, with no statistically significant nonresonant component. In determining the ρ resonance mass and coupling we compare two different approaches: fitting the individually extracted phase shifts versus fitting the t-matrix model directly to the energy spectrum. We find that both methods give consistent results, and at a pion mass of amπ=0.18295(36)stat obtain gρππ=5.69(13)stat(16)sys, amρ=0.4609(16)stat(14)sys, and amρ/amN=0.7476(38)stat(23)sys, where the first uncertainty is statistical and the second is the systematic uncertainty due to the choice of fit ranges.
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U2 - 10.1103/PhysRevD.96.034525
DO - 10.1103/PhysRevD.96.034525
M3 - Article
AN - SCOPUS:85029169638
SN - 2470-0010
VL - 96
JO - Physical Review D
JF - Physical Review D
IS - 3
M1 - 034524
ER -