6533b851fe1ef96bd12a8e02
RESEARCH PRODUCT
The role of the Euclidean signature in lattice calculations of quasi-distributions and other non-local matrix elements
Raúl A. BriceñoMaxwell T. HansenChristopher Monahansubject
Quantum chromodynamicsPhysicsNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Lattice field theoryFOS: Physical sciencesObservableLattice QCD01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - LatticeQuantum mechanics0103 physical sciencesMinkowski spaceEuclidean geometryPerturbation theory (quantum mechanics)Integration by reduction formulae010306 general physicsMathematical physicsdescription
Lattice quantum chromodynamics (QCD) provides the only known systematic, nonperturbative method for first-principles calculations of nucleon structure. However, for quantities such as lightfront parton distribution functions (PDFs) and generalized parton distributions (GPDs), the restriction to Euclidean time prevents direct calculation of the desired observable. Recently, progress has been made in relating these quantities to matrix elements of spatially nonlocal, zero-time operators, referred to as quasidistributions. Even for these time-independent matrix elements, potential subtleties have been identified in the role of the Euclidean signature. In this work, we investigate the analytic behavior of spatially non-local correlation functions and demonstrate that the matrix elements obtained from Euclidean lattice QCD are identical to those obtained using the LSZ reduction formula in Minkowski space. After arguing the equivalence on general grounds, we also show that it holds in a perturbative calculation, where special care is needed to identify the lattice prediction. Finally we present a proof of the uniqueness of the matrix elements obtained from Minkowski and Euclidean correlation functions to all order in perturbation theory.
year | journal | country | edition | language |
---|---|---|---|---|
2017-03-17 |