We study the Dirac decomposition of the gauge-invariant quark propagator, whose imaginary part describes the hadronization of a quark as this interacts with the vacuum, and relate each of its coefficients to a specific sum rule for the chiral-odd and chiral-even quark spectral functions. Working at first in lightlike axial gauge, we obtain a new sum rule for the spectral function associated with the gauge-fixing vector and show that its second moment is, in fact, equal to zero. Then, we demonstrate that the first moment of the chiral-odd quark spectral function is equal in any gauge to the so-called inclusive jet mass, which is related to the mass of the particles produced in the hadronization of a quark. Finally, we present a gauge-dependent formula that connects the second moment of the chiral-even quark spectral function to invariant mass generation and final state rescattering in the hadronization of a quark.
Gauge invariant spectral analysis of quark hadronization dynamics
Andrea Signori
2023-01-01
Abstract
We study the Dirac decomposition of the gauge-invariant quark propagator, whose imaginary part describes the hadronization of a quark as this interacts with the vacuum, and relate each of its coefficients to a specific sum rule for the chiral-odd and chiral-even quark spectral functions. Working at first in lightlike axial gauge, we obtain a new sum rule for the spectral function associated with the gauge-fixing vector and show that its second moment is, in fact, equal to zero. Then, we demonstrate that the first moment of the chiral-odd quark spectral function is equal in any gauge to the so-called inclusive jet mass, which is related to the mass of the particles produced in the hadronization of a quark. Finally, we present a gauge-dependent formula that connects the second moment of the chiral-even quark spectral function to invariant mass generation and final state rescattering in the hadronization of a quark.File | Dimensione | Formato | |
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PhysRevD.108.114011.pdf
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