Solving the Bars-Green equation for moving mesons in two-dimensional QCD
arXiv:1708.09379 · doi:10.1007/JHEP11(2017)151
Abstract
The two-dimensional QCD in the large limit, generally referred to as the 't Hooft model, is numerically investigated in the axial gauge in a comprehensive manner. The corresponding Bethe-Salpeter equation for a bound pair, originally derived by Bars and Green in 1978, was first numerically tackled by Li and collaborators in late 1980s, yet only for the {\it stationary} mesons. In this paper, we make further progress by numerically solving the Bars-Green equation for {\it moving} mesons, ranging from the chiral pion to charmonium. By choosing several different quark masses, we computed the corresponding quark condensates, meson spectra and their decay constants for a variety of meson momenta, and found satisfactory agreement with their counterparts obtained using light-cone gauge, thus numerically verified the gauge and Poincaré invariance of the 't Hooft model. Moreover, we have explicitly confirmed that, as the meson gets more and more boosted, the large component of the Bars-Green wave function indeed approaches the corresponding 't Hooft light-cone wave function, while the small component of the wave function rapidly fades away.
v2, 25 pages, 12 figures, and 1 table; Some figures updated, references added, typo corrrected; to appear in JHEP
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- Matching the Quasi Meson Distribution Amplitude in RI/MOM scheme
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- One-Loop Hybrid Renormalization Matching Kernels for Quasi-Parton Distributions
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- Chiral Perturbation for Large Momentum Effective Field Theory
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- 1+1D Hadrons Minimize their Biparton Renyi Free Energy
- Mapping Parton Distributions of Hadrons with Lattice QCD
- Quark-hadron duality for heavy meson mixings in the 't Hooft model
- Light-front dynamic analysis of the longitudinal charge density using the solvable scalar field model in (1+1) dimensions
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