Jorge A. Revelli
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Jorge A. Revelli has a total of 16 co-authors. Here are the top co-authors by number of shared publications:
- Horacio S. Wio
Institute for Cross-Disciplinary Physics and Complex Systems (IFISC), UIB-CSIC, Universitat de les Illes Balears, E-07122 Palma de Mallorca, Spain
4 shared publications - Roberto Raúl Deza
Departamento de Física, Facultad de Ciencias Exactas y Naturales, Universidad Nacional de Mar del Plata, Deán Funes 3350, 7600 Mar del Plata, Argentina
4 shared publications - Marcos E. Gaudiano
Facultad de Matemática, Astronomía, Física y Computación., Universidad Nacional de Córdoba, Córdoba, Argentina
2 shared publications - Miguel Angel Rodríguez
Instituto de Física de Cantabria (IFCA), CSIC-UNICAN, E-39005 Santander, Spain
2 shared publications A.D. Sánchez
1 shared publication- Carlos Escudero
Departamento de Matemáticas Fundamentales, Universidad Nacional de Educación a Distancia, Madrid, Spain
1 shared publication
Latest Publications
- Open Access
The KPZ Equation of Kinetic Interface Roughening: A Variational Perspective
Interfaces of rather different natures—as, e.g., bacterial colony or forest fire boundaries, or semiconductor layers grown by different methods (MBE, sputtering, etc.)—are self-affine fractals, and feature scaling with universal exponents (depending on the substrate’s dimensionality d and global topology, as well as on the driving randomness’ spatial and temporal correlations but not on the underlying mechanisms). Adding lateral growth as an essential (non-equilibrium) ingredient to the known equilibrium ones (randomness and interface relaxation), the Kardar–Parisi–Zhang (KPZ) equation succeeded in finding (via the dynamic renormalization group) the correct exponents for flat substrates and (spatially and temporally) uncorrelated randomness. It is this interplay which gives rise to the unique, non-Gaussian scaling properties characteristic of the specific, universal type of non-equilibrium roughening. Later on, the asymptotic statistics of process fluctuations in the scaling regime was also analytically found for substrates. For substrates, however, one has to rely on numerical simulations. Here we review a variational approach that allows for analytical progress regardless of substrate dimensionality. After reviewing our previous numerical results in , 2, and 3 on the time evolution of one of the functionals—which we call the non-equilibrium potential (NEP)—as well as its scaling behavior with the nonlinearity parameter , we discuss the stochastic thermodynamics of the roughening process and the memory of process in KPZ and in the related Golubović–Bruinsma (GB) model, providing numerical evidence for the significant dependence on initial conditions of the NEP’s asymptotic behavior in both models. Finally, we highlight some open questions.Open AccessThe KPZ Equation of Kinetic Interface Roughening: A Variational Perspective
Interfaces of rather different natures—as, e.g., bacterial colony or forest fire boundaries, or semiconductor layers grown by different methods (MBE, sputtering, etc.)—are self-affine fractals, and feature scaling with universal exponents (depending on the substrate’s dimensionality d and global topology, as well as on the driving randomness’ spatial and temporal correlations but not on the underlying mechanisms). Adding lateral growth as an essential (non-equilibrium) ingredient to the known equilibrium ones (randomness and interface relaxation), the Kardar–Parisi–Zhang (KPZ) equation succeeded in finding (via the dynamic renormalization group) the correct exponents for flat substrates and (spatially and temporally) uncorrelated randomness. It is this interplay which gives rise to the unique, non-Gaussian scaling properties characteristic of the specific, universal type of non-equilibrium roughening. Later on, the asymptotic statistics of process fluctuations in the scaling regime was also analytically found for substrates. For substrates, however, one has to rely on numerical simulations. Here we review a variational approach that allows for analytical progress regardless of substrate dimensionality. After reviewing our previous numerical results in , 2, and 3 on the time evolution of one of the functionals—which we call the non-equilibrium potential (NEP)—as well as its scaling behavior with the nonlinearity parameter , we discuss the stochastic thermodynamics of the roughening process and the memory of process in KPZ and in the related Golubović–Bruinsma (GB) model, providing numerical evidence for the significant dependence on initial conditions of the NEP’s asymptotic behavior in both models. Finally, we highlight some open questions. - 1 December 2025
- Published by American Physical Society (APS) in Physical Review E
- Vol. 112 (6) , 064302
Statistical complexity as a diagnostic of critical behavior in a 2D Sznajd model
We investigate the dynamics of a two-dimensional Sznajd model in which a third ideological position emerges spontaneously from local interactions between agents. Starting from random initial conditions, we observe that this emergent position arises solely as a result of the interaction dynamics, and not from predefined agent states. We analyze the system's behavior as a function of social apathy, modeled as the fraction of nonparticipating agents, and identify a critical apathy threshold that separates distinct regimes of opinion dominance. To quantify the interplay between disorder and structure in the system, we employ the complexity-entropy plane. This analysis reveals that the system is robust to asymmetries in initial conditions; its macroscopic behavior remains qualitatively unchanged. Furthermore, we find that statistical complexity reaches a maximum near the transition region, highlighting the emergence of rich collective dynamics characterized by abrupt topological changes parametrized by apathy.
- 1 December 2025
- Published by American Physical Society (APS) in Physical Review E
- Vol. 112 (6) , 064302
Statistical complexity as a diagnostic of critical behavior in a 2D Sznajd model
We investigate the dynamics of a two-dimensional Sznajd model in which a third ideological position emerges spontaneously from local interactions between agents. Starting from random initial conditions, we observe that this emergent position arises solely as a result of the interaction dynamics, and not from predefined agent states. We analyze the system's behavior as a function of social apathy, modeled as the fraction of nonparticipating agents, and identify a critical apathy threshold that separates distinct regimes of opinion dominance. To quantify the interplay between disorder and structure in the system, we employ the complexity-entropy plane. This analysis reveals that the system is robust to asymmetries in initial conditions; its macroscopic behavior remains qualitatively unchanged. Furthermore, we find that statistical complexity reaches a maximum near the transition region, highlighting the emergence of rich collective dynamics characterized by abrupt topological changes parametrized by apathy.
- 4 October 2025
- Published by Elsevier in Chaos, Solitons & Fractals
- Vol. 201
Entropic analysis of a hierarchically organized Axelrod model
- 4 October 2025
- Published by Elsevier in Chaos, Solitons & Fractals
- Vol. 201
Entropic analysis of a hierarchically organized Axelrod model
- 18 August 2025
- Published by World Scientific Pub Co Pte Ltd in Advances in Complex Systems
- Vol. 28 (07)
HIERARCHICAL CORRELATION OF JOINT PATTERNS OF URBAN PROTESTS
In this paper, we use an entropic formalism to compare the temporal strike patterns of two important unions in Córdoba city, Argentina. Despite being uncorrelated, the combined impact of the protests is not simply additive. This is reflected in the form of emerging nonlinear effects. The formalism allows for a study of system’s controllability aspects described in terms of entropic regimes. The analysis enables the characterization of correlations between overlapping periods of protest activity. It makes possible to quantitatively point out how in principle low-intensity seasons of independent strikes can often form a joint pattern of protests with higher social conflict.
- 18 August 2025
- Published by World Scientific Pub Co Pte Ltd in Advances in Complex Systems
- Vol. 28 (07)
HIERARCHICAL CORRELATION OF JOINT PATTERNS OF URBAN PROTESTS
In this paper, we use an entropic formalism to compare the temporal strike patterns of two important unions in Córdoba city, Argentina. Despite being uncorrelated, the combined impact of the protests is not simply additive. This is reflected in the form of emerging nonlinear effects. The formalism allows for a study of system’s controllability aspects described in terms of entropic regimes. The analysis enables the characterization of correlations between overlapping periods of protest activity. It makes possible to quantitatively point out how in principle low-intensity seasons of independent strikes can often form a joint pattern of protests with higher social conflict.
- Open Access
- 30 January 2025
- Published by Qeios Ltd
Review of: "The Information Theory of Self-Organization Phenomena in Thermal Systems"
In this work, authors study the single Brownian motion and the multiple-particle system motion as well, by using Information Theory, the article tries to show an ambitious theoretical framework unifying Information Theory, Thermodynamics, and Compl...
- 30 January 2025
- Published by Qeios Ltd
Open AccessReview of: "The Information Theory of Self-Organization Phenomena in Thermal Systems"
In this work, authors study the single Brownian motion and the multiple-particle system motion as well, by using Information Theory, the article tries to show an ambitious theoretical framework unifying Information Theory, Thermodynamics, and Compl...
- Open Access
- 19 October 2022
- Published by Elsevier in Chaos, Solitons & Fractals
- Vol. 165
The nonequilibrium potential today: A short review
- 19 October 2022
- Published by Elsevier in Chaos, Solitons & Fractals
- Vol. 165
Open AccessThe nonequilibrium potential today: A short review
- 1 February 2022
- Published by Elsevier in Physica A: Statistical Mechanics and its Applications
- Vol. 587
On the role of structured initial conditions in the Schelling model
- 1 February 2022
- Published by Elsevier in Physica A: Statistical Mechanics and its Applications
- Vol. 587
On the role of structured initial conditions in the Schelling model
- Open Access
- 29 June 2010
- Published by American Physical Society (APS) in Physical Review E
- Vol. 81 (6) , 066706
Discretization-related issues in the Kardar-Parisi-Zhang equation: Consistency, Galilean-invariance violation, and fluctuation-dissipation relation
In order to perform numerical simulations of the Kardar-Parisi-Zhang (KPZ) equation, in any dimensionality, a spatial discretization scheme must be prescribed. The known fact that the KPZ equation can be obtained as a result of a Hopf-Cole transformation applied to a diffusion equation (with multiplicative noise) is shown here to strongly restrict the arbitrariness in the choice of spatial discretization schemes. On one hand, the discretization prescriptions for the Laplacian and the nonlinear (KPZ) term cannot be independently chosen. On the other hand, since the discretization is an operation performed on space and the Hopf-Cole transformation is local both in space and time, the former should be the same regardless of the field to which it is applied. It is shown that whereas some discretization schemes pass both consistency tests, known examples in the literature do not. The requirement of consistency for the discretization of Lyapunov functionals is argued to be a natural and safe starting point in choosing spatial discretization schemes. We also analyze the relation between real-space and pseudospectral discrete representations. In addition we discuss the relevance of the Galilean-invariance violation in these consistent discretization schemes and the alleged conflict of standard discretization with the fluctuation-dissipation theorem, peculiar of one dimension.
- 29 June 2010
- Published by American Physical Society (APS) in Physical Review E
- Vol. 81 (6) , 066706
Open AccessDiscretization-related issues in the Kardar-Parisi-Zhang equation: Consistency, Galilean-invariance violation, and fluctuation-dissipation relation
In order to perform numerical simulations of the Kardar-Parisi-Zhang (KPZ) equation, in any dimensionality, a spatial discretization scheme must be prescribed. The known fact that the KPZ equation can be obtained as a result of a Hopf-Cole transformation applied to a diffusion equation (with multiplicative noise) is shown here to strongly restrict the arbitrariness in the choice of spatial discretization schemes. On one hand, the discretization prescriptions for the Laplacian and the nonlinear (KPZ) term cannot be independently chosen. On the other hand, since the discretization is an operation performed on space and the Hopf-Cole transformation is local both in space and time, the former should be the same regardless of the field to which it is applied. It is shown that whereas some discretization schemes pass both consistency tests, known examples in the literature do not. The requirement of consistency for the discretization of Lyapunov functionals is argued to be a natural and safe starting point in choosing spatial discretization schemes. We also analyze the relation between real-space and pseudospectral discrete representations. In addition we discuss the relevance of the Galilean-invariance violation in these consistent discretization schemes and the alleged conflict of standard discretization with the fluctuation-dissipation theorem, peculiar of one dimension.
- 3 March 2009
- Published by Springer Nature in The European Physical Journal B
- Vol. 69 (1) , 71-80
Stochastic resonance in extended systems
- 3 March 2009
- Published by Springer Nature in The European Physical Journal B
- Vol. 69 (1) , 71-80
Stochastic resonance in extended systems