I=1/2 S-wave and P-wave Kπ scattering and the κ and K* resonances from lattice QCD

被引:11
|
作者
Rendon, Gumaro [1 ]
Leskovec, Luka [2 ,3 ]
Meinel, Stefan [4 ]
Negele, John [5 ,6 ]
Paul, Srijit [7 ]
Petschlies, Marcus [8 ]
Pochinsky, Andrew [5 ,6 ]
Silvi, Giorgio [9 ]
Syritsyn, Sergey [10 ,11 ]
机构
[1] Brookhaven Natl Lab, Dept Phys, Upton, NY 11973 USA
[2] Thomas Jefferson Natl Accelerator Facil, Newport News, VA 23606 USA
[3] Old Dominion Univ, Dept Phys, Norfolk, VA 23529 USA
[4] Univ Arizona, Dept Phys, Tucson, AZ 85721 USA
[5] MIT, Lab Nucl Sci, Ctr Theoret Phys, 77 Massachusetts Ave, Cambridge, MA 02139 USA
[6] MIT, Dept Phys, Cambridge, MA 02139 USA
[7] Johannes Gutenberg Univ Mainz, Inst Kernphys, D-55099 Mainz, Germany
[8] Rheinische Friedrich Wilhelms Univ Bonn, Helmholtz Inst Strahlen & Kernphys, Nussallee 14-16, D-53115 Bonn, Germany
[9] Forschungszentrum Julich, Julich Supercomp Ctr, D-52425 Julich, Germany
[10] SUNY Stony Brook, Dept Phys & Astron, Stony Brook, NY 11794 USA
[11] Brookhaven Natl Lab, RIKEN BNL Res Ctr, Upton, NY 11973 USA
基金
美国国家科学基金会;
关键词
CHIRAL PERTURBATION-THEORY; CONTINUUM-LIMIT; CONSISTENCY CONDITIONS; ELASTIC-SCATTERING; STATES; SIGMA; MATRIX; LENGTH; ROY;
D O I
10.1103/PhysRevD.102.114520
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present a lattice-QCD determination of the elastic isospin-1/2 S-wave and P-wave K pi scattering amplitudes as a function of the center-of-mass energy using Luscher's method. We perform global fits of K-matrix parametrizations to the finite-volume energy spectra for all irreducible representations with total momenta up to root 32 pi/L; this includes irreducible representations (irreps) that mix the S- and P-waves. Several different parametrizations for the energy dependence of the K-matrix are considered. We also determine the positions of the nearest poles in the scattering amplitudes, which correspond to the broad K resonance in the S-wave and the narrow K*(892) resonance in the P-wave. Our calculations are performed with 2 + 1 dynamical clover fermions for two different pion masses of 317.2(2.2) and 175.9(1.8) MeV. Our preferred S-wave parametrization is based on a conformal map and includes an Adler zero; for the P-wave, we use a standard pole parametrization including Blatt-Weisskopf barrier factors. The S-wave K-resonance pole positions are found to be [0.86(12) - 0.309(50) i] GeV at the heavier pion mass and [0.499(55) - 0.379 (66)] GeV at thelighter pion mass. The P-wave K* -resonance pole positions are found to be [0.8951(64) - 0.00250(21)i] GeV at the heavier pion mass and [0.8718(82) - 0.0130(11)i] GeV at the lighter pion mass, which corresponds to couplings of g(K*K pi) = 5.02(26) and g(K*K pi) = 4.99(22), respectively.
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页数:22
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