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Hauptverfasser: Pavan, Kaczmarek, Olaf, Moore, Guy D., Schmidt, Christian
Format: Preprint
Veröffentlicht: 2026
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Online-Zugang:https://arxiv.org/abs/2604.02122
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author Pavan
Kaczmarek, Olaf
Moore, Guy D.
Schmidt, Christian
author_facet Pavan
Kaczmarek, Olaf
Moore, Guy D.
Schmidt, Christian
contents The energy-momentum tensor (EMT) is the conserved current corresponding to space-time translation symmetry. Its applications are remarkably diverse, ranging from the thermodynamics to the calculation of transport coefficients. While the EMT is well-defined in the continuum up to a total derivative, with its coefficients fixed by Ward identities, its extension to lattice QCD is not straightforward. The primary challenge arises from the breaking of continuous space-time symmetries by the discrete lattice regulator. Although the EMT can be constructed on the lattice in a way that yields the correct continuum limit, the operators are not uniquely defined. In this proceeding, we construct the EMT for both pure-gauge theory and full QCD, discussing its renormalization in the specific context of determining the coefficients required for shear viscosity. In this context, we present a comparative analysis of the trace anomaly, number density, pressure, energy density and enthalpy density with imaginary chemical potential for multiple $β$ values at approximately the same temperature, aimed for the continuum limit.
format Preprint
id arxiv_https___arxiv_org_abs_2604_02122
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Non-perturbative Renormalization of the EMT in Full QCD
Pavan
Kaczmarek, Olaf
Moore, Guy D.
Schmidt, Christian
High Energy Physics - Lattice
The energy-momentum tensor (EMT) is the conserved current corresponding to space-time translation symmetry. Its applications are remarkably diverse, ranging from the thermodynamics to the calculation of transport coefficients. While the EMT is well-defined in the continuum up to a total derivative, with its coefficients fixed by Ward identities, its extension to lattice QCD is not straightforward. The primary challenge arises from the breaking of continuous space-time symmetries by the discrete lattice regulator. Although the EMT can be constructed on the lattice in a way that yields the correct continuum limit, the operators are not uniquely defined. In this proceeding, we construct the EMT for both pure-gauge theory and full QCD, discussing its renormalization in the specific context of determining the coefficients required for shear viscosity. In this context, we present a comparative analysis of the trace anomaly, number density, pressure, energy density and enthalpy density with imaginary chemical potential for multiple $β$ values at approximately the same temperature, aimed for the continuum limit.
title Non-perturbative Renormalization of the EMT in Full QCD
topic High Energy Physics - Lattice
url https://arxiv.org/abs/2604.02122