Antonio González-Arroyo
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Antonio González-Arroyo has a total of 205 co-authors. Here are the top co-authors by number of shared publications:
- Margarita García Pérez
Universidad Autónoma de Madrid
75 shared publications - Masanori Okawa
Hiroshima University
45 shared publications - Masanori Okawa
Hiroshima University
18 shared publications - Ken-Ichi Ishikawa
Hiroshima University
14 shared publications - Liam Keegan
Theoretical Physics Department CERN 1211 Geneva 23 Switzerland
12 shared publications - Claudio Bonanno
University of Pisa
10 shared publications
Latest Publications
- Open Access
- 1 April 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (4) , 15
Universal features of chiral symmetry breaking in large-N QCD
A bstract: We investigate the universal features of chiral symmetry breaking in large- N QCD by comparing non-perturbative determinations of the low-lying Dirac spectrum with chiral Random Matrix Theory (RMT) predictions. Our numerical Monte Carlo calculations are based on a chiral lattice discretization of the Dirac operator, and exploit twisted volume reduction to reach N as large as 841. Matching lattice data with RMT analytic results, we are able to extract the large- N chiral condensate, which is compared with a recent determination obtained with non-chiral Wilson quarks from twisted volume-reduced models.
- 1 April 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (4) , 15
Open AccessUniversal features of chiral symmetry breaking in large-N QCD
A bstract: We investigate the universal features of chiral symmetry breaking in large- N QCD by comparing non-perturbative determinations of the low-lying Dirac spectrum with chiral Random Matrix Theory (RMT) predictions. Our numerical Monte Carlo calculations are based on a chiral lattice discretization of the Dirac operator, and exploit twisted volume reduction to reach N as large as 841. Matching lattice data with RMT analytic results, we are able to extract the large- N chiral condensate, which is compared with a recent determination obtained with non-chiral Wilson quarks from twisted volume-reduced models.
- Open Access
- 12 December 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (12) , 96
Non-perturbative determination of meson masses and low-energy constants in large-N QCD
A bstract: We provide first-principles non-perturbative determinations of the low-lying meson mass spectrum of large- N QCD in the ’t Hooft limit N f / N → 0, as well as of three low-energy constants appearing in the QCD chiral expansion: the quark condensate Σ, the pion decay constant F π , and the next-to-leading-order coupling $${\overline{{\ell}} }_{4}$$ . Using the excited state masses in the π and ρ channels, we are able to investigate the behavior of their radial Regge trajectories. Concerning QCD low-energy constants, we are able to assess the magnitude of sub-leading corrections in 1/ N by combining our N = ∞ results with previous finite- N determinations. Our calculation exploits large- N twisted volume reduction to efficiently perform numerical Monte Carlo simulations of the large- N lattice discretized theory. We employ several values of N up to N = 841, 5 values of the lattice spacing, and several values of the quark mass, to achieve controlled continuum and chiral extrapolations.- 12 December 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (12) , 96
Open AccessNon-perturbative determination of meson masses and low-energy constants in large-N QCD
A bstract: We provide first-principles non-perturbative determinations of the low-lying meson mass spectrum of large- N QCD in the ’t Hooft limit N f / N → 0, as well as of three low-energy constants appearing in the QCD chiral expansion: the quark condensate Σ, the pion decay constant F π , and the next-to-leading-order coupling $${\overline{{\ell}} }_{4}$$ . Using the excited state masses in the π and ρ channels, we are able to investigate the behavior of their radial Regge trajectories. Concerning QCD low-energy constants, we are able to assess the magnitude of sub-leading corrections in 1/ N by combining our N = ∞ results with previous finite- N determinations. Our calculation exploits large- N twisted volume reduction to efficiently perform numerical Monte Carlo simulations of the large- N lattice discretized theory. We employ several values of N up to N = 841, 5 values of the lattice spacing, and several values of the quark mass, to achieve controlled continuum and chiral extrapolations. - Open Access
- 10 October 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (10)
A T2 × R2 roadmap to confinement in SU(2) Yang-Mills theory
A bstract: We study the behaviour of SU(2) Yang-Mills fields on a T 2 × R 2 geometry where the two-torus is equipped with twisted boundary conditions. We monitor the evolution of the dynamics of the system as a function of the torus size l s . For small sizes the behaviour of the system is well understood in terms of semiclassical predictions. In our case, the long distance structure is that of a two-dimensional gas of vortex-like fractional instantons with size and density growing with l s . Our lattice Monte Carlo simulations confirm the semiclassical predictions and allow the determination of the relevant scale signalling the transition to the non-dilute situation. At low densities the string tension takes the standard value of a 2D center-vortex gas, growing with the density and approaching the value measured at infinite volume. Our work includes preliminary studies of the extension to SU(N) and to the region of large sizes in which boundary conditions are irrelevant, and all physical scales are determined by the Λ parameter.
- 10 October 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (10)
Open AccessA T2 × R2 roadmap to confinement in SU(2) Yang-Mills theory
A bstract: We study the behaviour of SU(2) Yang-Mills fields on a T 2 × R 2 geometry where the two-torus is equipped with twisted boundary conditions. We monitor the evolution of the dynamics of the system as a function of the torus size l s . For small sizes the behaviour of the system is well understood in terms of semiclassical predictions. In our case, the long distance structure is that of a two-dimensional gas of vortex-like fractional instantons with size and density growing with l s . Our lattice Monte Carlo simulations confirm the semiclassical predictions and allow the determination of the relevant scale signalling the transition to the non-dilute situation. At low densities the string tension takes the standard value of a 2D center-vortex gas, growing with the density and approaching the value measured at infinite volume. Our work includes preliminary studies of the extension to SU(N) and to the region of large sizes in which boundary conditions are irrelevant, and all physical scales are determined by the Λ parameter.
- Open AccessA $T_2 \times R^2$ roadmap to Confinement in SU(2) Yang-Mills theoryWe study the behaviour of \SU{2} Yang-Mills fields on a $T_2\times R^2$ geometry where the two-torus is equipped with twisted boundary conditions. We monitor the evolution of the dynamics of the system as a function of the torus size $l_s$. For small sizes the behaviour of the system is well understood in terms of semiclassical predictions. In our case, the long distance structure is that of a two-dimensional gas of vortex-like fractional instantons with size and density growing with $l_s$. Our lattice Monte Carlo simulations confirm the semiclassical predictions and allow the determination of the relevant scale signalling the transition to the non-dilute situation. At low densities the string tension takes the standard value of a 2D center-vortex gas, growing with the density and approaching the value measured at infinite volume. Our work includes preliminary studies of the extension to \SU{N} and to the region of large sizes in which boundary conditions are irrelevant, and all physical scales are determined by the $Λ$ parameter.Open AccessA $T_2 \times R^2$ roadmap to Confinement in SU(2) Yang-Mills theoryWe study the behaviour of \SU{2} Yang-Mills fields on a $T_2\times R^2$ geometry where the two-torus is equipped with twisted boundary conditions. We monitor the evolution of the dynamics of the system as a function of the torus size $l_s$. For small sizes the behaviour of the system is well understood in terms of semiclassical predictions. In our case, the long distance structure is that of a two-dimensional gas of vortex-like fractional instantons with size and density growing with $l_s$. Our lattice Monte Carlo simulations confirm the semiclassical predictions and allow the determination of the relevant scale signalling the transition to the non-dilute situation. At low densities the string tension takes the standard value of a 2D center-vortex gas, growing with the density and approaching the value measured at infinite volume. Our work includes preliminary studies of the extension to \SU{N} and to the region of large sizes in which boundary conditions are irrelevant, and all physical scales are determined by the $Λ$ parameter.
- Open Access
- 21 March 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (3) , 1-20
The mass of the gluino-glue bound state in large-N $ \mathcal{N} $ = 1 Supersymmetric Yang-Mills theoryWe provide a first-principles non-perturbative determination of the mass of the lightest gluino-gluon bound state (gluino-glue) in large-N $$ \mathcal{N} $$ = 1 Supersymmetric Yang-Mills theory by means of numerical Monte Carlo simulations of the lattice-discretized theory, and exploiting large-N twisted volume reduction. Our large-N determination is consistent with naive extrapolation of previously-known SU(2) and SU(3) results.- 21 March 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (3) , 1-20
Open AccessThe mass of the gluino-glue bound state in large-N $ \mathcal{N} $ = 1 Supersymmetric Yang-Mills theoryWe provide a first-principles non-perturbative determination of the mass of the lightest gluino-gluon bound state (gluino-glue) in large-N $$ \mathcal{N} $$ = 1 Supersymmetric Yang-Mills theory by means of numerical Monte Carlo simulations of the lattice-discretized theory, and exploiting large-N twisted volume reduction. Our large-N determination is consistent with naive extrapolation of previously-known SU(2) and SU(3) results. - Open AccessFractional instantons and Confinement: first results on a $T_2\times R^2$ roadmap
We report results obtained for SU(2) Yang-Mills theory on a four dimensional torus with two directions much smaller than the other two. The small 2-torus is equipped with twisted boundary conditions. This construction provides a way to interpolate from a region in which semiclassical methods can be applied (for small 2-torus size) to the standard infinite volume case. Our simulations at small torus sizes show how the topological charge and the string tension result from a gas of vortex-like fractional instantons. As the size becomes larger the density increases and the separation of structures tends to a constant in agreement with the fractional instanton liquid model picture of the Yang-Mills vacuum.
Open AccessFractional instantons and Confinement: first results on a $T_2\times R^2$ roadmapWe report results obtained for SU(2) Yang-Mills theory on a four dimensional torus with two directions much smaller than the other two. The small 2-torus is equipped with twisted boundary conditions. This construction provides a way to interpolate from a region in which semiclassical methods can be applied (for small 2-torus size) to the standard infinite volume case. Our simulations at small torus sizes show how the topological charge and the string tension result from a gas of vortex-like fractional instantons. As the size becomes larger the density increases and the separation of structures tends to a constant in agreement with the fractional instanton liquid model picture of the Yang-Mills vacuum.
- Open Access
- 10 February 2025
- Published by Sissa Medialab Srl
- Vol. 466, 408
Fractional instantons and Confinement: first results on a $T_2 \times R^2$ roadmapWe report results obtained for SU(2) Yang-Mills theory on a 4d torus with two directions much smaller than the other two. The small 2-torus is equipped with twisted boundary conditions. This construction provides a way to interpolate from a region in which semiclassical methods can be applied (for small 2-torus size) to the standard infinite volume case. Our simulations at small torus sizes show how the topological charge and the string tension result from a gas of vortex-like fractional instantons. As the size becomes larger the density increases and the separation of structures tends to a constant in agreement with the fractional instanton liquid model picture of the Yang-Mills vacuum.
- 10 February 2025
- Published by Sissa Medialab Srl
- Vol. 466, 408
Open AccessFractional instantons and Confinement: first results on a $T_2 \times R^2$ roadmapWe report results obtained for SU(2) Yang-Mills theory on a 4d torus with two directions much smaller than the other two. The small 2-torus is equipped with twisted boundary conditions. This construction provides a way to interpolate from a region in which semiclassical methods can be applied (for small 2-torus size) to the standard infinite volume case. Our simulations at small torus sizes show how the topological charge and the string tension result from a gas of vortex-like fractional instantons. As the size becomes larger the density increases and the separation of structures tends to a constant in agreement with the fractional instanton liquid model picture of the Yang-Mills vacuum.
- Open Access
- 10 January 2025
- Published by Sissa Medialab Srl
- Vol. 466, 392
The gluino condensate of large-$N$ SUSY Yang–Mills
We present the first lattice determination of the SUSY $\mathrm{SU}(N)$ Yang–Mills gluino condensate at large $N$. We exploit large-$N$ twisted volume reduction, and present two determinations based on the Banks–Casher relation and on a Gell-Mann–Oakes–Renner-like formula, both giving perfectly compatible results. By expressing the lattice results in the Novikov–Shifman–Vainshtein–Zakharov scheme, we are able for the first time to compare lattice and analytical computations, resolving a 40-year-long debate about the actual value and $N$-dependence of the gluino condensate.- 10 January 2025
- Published by Sissa Medialab Srl
- Vol. 466, 392
Open AccessThe gluino condensate of large-$N$ SUSY Yang–Mills
We present the first lattice determination of the SUSY $\mathrm{SU}(N)$ Yang–Mills gluino condensate at large $N$. We exploit large-$N$ twisted volume reduction, and present two determinations based on the Banks–Casher relation and on a Gell-Mann–Oakes–Renner-like formula, both giving perfectly compatible results. By expressing the lattice results in the Novikov–Shifman–Vainshtein–Zakharov scheme, we are able for the first time to compare lattice and analytical computations, resolving a 40-year-long debate about the actual value and $N$-dependence of the gluino condensate. - Open Access
The gluino condensate of large-$N$ SUSY Yang-Mills
We present the first lattice determination of the SUSY $\mathrm{SU}(N)$ Yang-Mills gluino condensate at large $N$. We exploit large-$N$ twisted volume reduction, and present two determinations based on the Banks-Casher relation and on a Gell-Mann-Oakes-Renner-like formula, both giving perfectly compatible results. By expressing the lattice results in the Novikov-Shifman-Vainshtein-Zakharov scheme, we are able for the first time to compare lattice and analytical computations, resolving a 40-year-long debate about the actual value and $N$-dependence of the gluino condensate.Open AccessThe gluino condensate of large-$N$ SUSY Yang-Mills
We present the first lattice determination of the SUSY $\mathrm{SU}(N)$ Yang-Mills gluino condensate at large $N$. We exploit large-$N$ twisted volume reduction, and present two determinations based on the Banks-Casher relation and on a Gell-Mann-Oakes-Renner-like formula, both giving perfectly compatible results. By expressing the lattice results in the Novikov-Shifman-Vainshtein-Zakharov scheme, we are able for the first time to compare lattice and analytical computations, resolving a 40-year-long debate about the actual value and $N$-dependence of the gluino condensate. - Open Access
- 5 November 2024
- Published by Sissa Medialab Srl
- Vol. 453, 374
The chiral condensate at large $N$We present results for the large-$N$ limit of the chiral condensate computed from twisted reduced models. We followed a two-fold strategy, one constiting in extracting the condensate from the quark-mass dependence of the pion mass, the other consisting in extracting the condensate from the mode number of the Dirac operator.
- 5 November 2024
- Published by Sissa Medialab Srl
- Vol. 453, 374
Open AccessThe chiral condensate at large $N$We present results for the large-$N$ limit of the chiral condensate computed from twisted reduced models. We followed a two-fold strategy, one constiting in extracting the condensate from the quark-mass dependence of the pion mass, the other consisting in extracting the condensate from the mode number of the Dirac operator.