Prof. Patella erforscht die präzise Berechnung von Teilcheneigenschaften und Wechselwirkungen durch Gitterfeld-Simulationen, insbesondere unter Berücksichtigung elektromagnetischer und Isospin-Brechungs-Effekte in der Quantenchromodynamik. Sein aktueller Fokus liegt auf der Entwicklung und Anwendung von C-periodischen Randbedingungen für vollständig dynamische QCD+QED-Simulationen, um hochpräzise Vorhersagen für fundamentale Parameter wie die anomales magnetisches Moment des Myons zu ermöglichen. Die Methoden ermöglichen es, theoretische Vorhersagen des Standardmodells mit experimentellen Messungen zu vergleichen und damit Grenzen neuer Physik zu testen. Die Arbeiten sind relevant für die Grundlagenphysik und Präzisionsmessungen in der Teilchenphysik.
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Prof. Dr. Agostino Patella
HU-FIS-Profil ↗GRK 2575/2: Überdenken der Quantenfeldtheorie
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GRK 2575/2: Überdenken der Quantenfeldtheorie
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Förderer: DFG Eigene Stelle (Sachbeihilfe) Zeitraum: 08/2018 - 11/2020 Projektleitung: Dr. Debasish Banerjee, Prof. Dr. Agostino Patella
Förderer: DFG Graduiertenkolleg Zeitraum: 04/2020 - 09/2024 Projektleitung: Prof. Dr. Jan Plefka
Förderer: DFG Graduiertenkolleg Zeitraum: 10/2024 - 03/2029 Projektleitung: Prof. Dr. Jan Plefka
Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D, Particles, fields, gravitation, and cosmology · DOI
We discuss the lattice formulation of gauge theories with fermions in arbitrary representations of the color group and present in detail the implementation of the hybrid Monte Carlo (HMC)/rational HMC algorithm for simulating dynamical fermions. We discuss the validation of the implementation through an extensive set of tests and the stability of simulations by monitoring the distribution of the lowest eigenvalue of the Wilson-Dirac operator. Working with two flavors of Wilson fermions in the adjoint representation, benchmark results for realistic lattice simulations are presented. Runs are performed on different lattice sizes ranging from ${4}^{3}\ifmmode\times\else\texttimes\fi{}8$ to ${24}^{3}\ifmmode\times\else\texttimes\fi{}64$ sites. For the two smallest lattices we also report the measured values of benchmark mesonic observables. These results can be used as a baseline for rapid cross-checks of simulations in higher representations. The results presented here are the first steps toward more extensive investigations with controlled systematic errors, aiming at a detailed understanding of the phase structure of these theories, and of their viability as candidates for strong dynamics beyond the standard model.
Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D, Particles, fields, gravitation, and cosmology · DOI
The masses of the lowest-lying states in the meson and in the gluonic sector of an SU(2) gauge theory with two Dirac flavors in the adjoint representation are measured on the lattice at a fixed value of the lattice coupling $\ensuremath{\beta}=4/{g}_{0}^{2}=2.25$ for values of the bare fermion mass ${m}_{0}$ that span a range between the quenched regime and the massless limit, and for various lattice volumes. Even for light constituent fermions the lightest glueballs are found to be lighter than the lightest mesons. Moreover, the string tension between two static fundamental sources strongly depends on the mass of the dynamical fermions and becomes of the order of the inverse squared lattice linear size before the chiral limit is reached. The implications of these findings for the phase of the theory in the massless limit are discussed and a strategy for discriminating between the (near-)conformal and the confining scenario is outlined.
Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D, Particles, fields, gravitation, and cosmology · DOI
We study the gauge sector of minimal walking technicolor, which is an $SU(2)$ gauge theory with ${n}_{f}=2$ flavors of Wilson fermions in the adjoint representation. Numerical simulations are performed on lattices ${N}_{t}\ifmmode\times\else\texttimes\fi{}{N}_{s}^{3}$, with ${N}_{s}$ ranging from 8 to 16 and ${N}_{t}=2{N}_{s}$, at fixed $\ensuremath{\beta}=2.25$, and varying the fermion bare mass ${m}_{0}$, so that our numerical results cover the full range of fermion masses from the quenched region to the chiral limit. We present results for the string tension and the glueball spectrum. A comparison of mesonic and gluonic observables leads to the conclusion that the infrared dynamics is given by an $SU(2)$ pure Yang-Mills theory with a typical energy scale for the spectrum sliding to zero with the fermion mass. The typical mesonic mass scale is proportional to and much larger than this gluonic scale. Our findings are compatible with a scenario in which the massless theory is conformal in the infrared. An analysis of the scaling of the string tension with the fermion mass toward the massless limit allows us to extract the chiral condensate anomalous dimension ${\ensuremath{\gamma}}_{*}$, which is found to be ${\ensuremath{\gamma}}_{*}=0.22\ifmmode\pm\else\textpm\fi{}0.06$.