Relativistic path integral and relativistic Hamiltonians in QCD and QED
Yu. A. Simonov (Institute of Theoretical, Experimental Physics,, Moscow, Russia)

TL;DR
This paper derives a new explicit form of the quark-antiquark Green's function using the proper-time path integral, leading to an instantaneous Hamiltonian applicable to mesons in magnetic fields, advancing theoretical understanding in QCD and QED.
Contribution
It introduces a novel parametric form of the Green's function and Hamiltonian for quark-antiquark systems in gluonic and electromagnetic fields.
Findings
Explicit form of the Green's function derived
Hamiltonian solutions provided for mesons in magnetic fields
Enhanced theoretical framework for QCD and QED interactions
Abstract
The proper-time 4d path integral is used as a starting point to derive the new explicit parametric form of the quark-antiquark Green's function in gluonic and QED fields, entering as a common Wilson loop. The subsequent vacuum averaging of the latter allows to derive the instantaneous Hamiltonian. The explicit form and solutions are given in the case of the mesons in magnetic field.
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