Marco Baity-Jesi
Complutense University of Madrid
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Publication
Featured researches published by Marco Baity-Jesi.
Physical Review B | 2013
Marco Baity-Jesi; Raquel A. Baños; A. Cruz; L. A. Fernandez; J. M. Gil-Narvion; A. Gordillo-Guerrero; D. Iñiguez; A. Maiorano; F. Mantovani; Enzo Marinari; V. Martin-Mayor; J. Monforte-Garcia; A. Muñoz Sudupe; D. Navarro; Giorgio Parisi; S. Perez-Gaviro; Marcello Pivanti; Federico Ricci-Tersenghi; J. J. Ruiz-Lorenzo; Sebastiano Fabio Schifano; B. Seoane; A. Tarancón; R. Tripiccione; D. Yllanes
We report a high-precision finite-size scaling study of the critical behavior of the three-dimensional Ising Edwards-Anderson model (the Ising spin glass). We have thermalized lattices up to L = 40 using the Janus dedicated computer. Our analysis takes into account leading-order corrections to scaling. We obtain Tc = 1.1019(29) for the critical temperature, ν = 2.562(42) for the thermal exponent, η = −0.3900(36) for the anomalous dimension, and ω = 1.12(10) for the exponent of the leading corrections to scaling. Standard (hyper)scaling relations yield α = −5.69(13), β = 0.782(10), and γ = 6.13(11). We also compute several universal quantities at Tc.
Physical Review B | 2014
Marco Baity-Jesi; L. A. Fernandez; V. Martin-Mayor; J. M. Sanz
We characterize the phase diagram of anisotropic Heisenberg spin glasses, finding both the spin and the chiral glass transition. We remark on the presence of strong finite-size effects in the chiral sector. On the spin glass sector, we find that the universality class is that of Ising spin glasses. Our data are compatible with a unique phase transition for the chiral and spin glass sector. We focus on keeping finite-size effects under control, and we stress that they are important to understand experiments. Thanks to large GPU clusters we have been able to thermalize cubic lattices with up to 643 spins, over a vast range of temperatures (hence, of relaxation times).
European Physical Journal-special Topics | 2012
Marco Baity-Jesi; Raquel A. Baños; A. Cruz; L. A. Fernandez; J. M. Gil-Narvion; A. Gordillo-Guerrero; M. Guidetti; D. Iñiguez; A. Maiorano; F. Mantovani; Enzo Marinari; V. Martin-Mayor; J. Monforte-Garcia; A. Muñoz Sudupe; D. Navarro; Giorgio Parisi; Marcello Pivanti; S. Perez-Gaviro; Federico Ricci-Tersenghi; J. J. Ruiz-Lorenzo; Sebastiano Fabio Schifano; B. Seoane; A. Tarancón; P. Tellez; R. Tripiccione; D. Yllanes
We describe Janus, a massively parallel FPGA-based computer optimized for the simulation of spin glasses, theoretical models for the behavior of glassy materials. FPGAs (as compared to GPUs or many-core processors) provide a complementary approach to massively parallel computing. In particular, our model problem is formulated in terms of binary variables, and floating-point operations can be (almost) completely avoided. The FPGA architecture allows us to run many independent threads with almost no latencies in memory access, thus updating up to 1024 spins per cycle. We describe Janus in detail and we summarize the physics results obtained in four years of operation of this machine; we discuss two types of physics applications: long simulations on very large systems (which try to mimic and provide understanding about the experimental non-equilibrium dynamics), and low-temperature equilibrium simulations using an artificial parallel tempering dynamics. The time scale of our non-equilibrium simulations spans eleven orders of magnitude (from picoseconds to a tenth of a second). On the other hand, our equilibrium simulations are unprecedented both because of the low temperatures reached and for the large systems that we have brought to equilibrium. A finite-time scaling ansatz emerges from the detailed comparison of the two sets of simulations. Janus has made it possible to perform spin-glass simulations that would take several decades on more conventional architectures. The paper ends with an assessment of the potential of possible future versions of the Janus architecture, based on state-of-the-art technology.
Computer Physics Communications | 2014
Marco Baity-Jesi; Raquel A. Baños; A. Cruz; L. A. Fernandez; J. M. Gil-Narvion; A. Gordillo-Guerrero; D. Iñiguez; A. Maiorano; F. Mantovani; Enzo Marinari; V. Martin-Mayor; J. Monforte-Garcia; A. Muñoz Sudupe; D. Navarro; Giorgio Parisi; S. Perez-Gaviro; Marcello Pivanti; Federico Ricci-Tersenghi; J. J. Ruiz-Lorenzo; Sebastiano Fabio Schifano; B. Seoane; A. Tarancón; R. Tripiccione; D. Yllanes
This paper describes the architecture, the development and the implementation of Janus II, a new generation application-driven number cruncher optimized for Monte Carlo simulations of spin systems (mainly spin glasses). This domain of computational physics is a recognized grand challenge of high-performance computing: the resources necessary to study in detail theoretical models that can make contact with experimental data are by far beyond those available using commodity computer systems. On the other hand, several specific features of the associated algorithms suggest that unconventional computer architectures – that can be implemented with available electronics technologies – may lead to order of magnitude increases in performance, reducing to acceptable values on human scales the time needed to carry out simulation campaigns that would take centuries on commercially available machines. Janus II is one such machine, recently developed and commissioned, that builds upon and improves on the successful JANUS machine, which has been used for physics since 2008 and is still in operation today. This paper describes in detail the motivations behind the project, the computational requirements, the architecture and the implementation of this new machine and compares its expected performances with those of currently available commercial systems.
Physical Review E | 2014
Marco Baity-Jesi; Raquel A. Baños; A. Cruz; L. A. Fernandez; J. M. Gil-Narvion; A. Gordillo-Guerrero; D. Iñiguez; A. Maiorano; F. Mantovani; Enzo Marinari; V. Martin-Mayor; J. Monforte-Garcia; A. Muñoz Sudupe; D. Navarro; Giorgio Parisi; S. Perez-Gaviro; Marcello Pivanti; Federico Ricci-Tersenghi; J. J. Ruiz-Lorenzo; Sebastiano Fabio Schifano; B. Seoane; A. Tarancón; R. Tripiccione; D. Yllanes
We study the off-equilibrium dynamics of the three-dimensional Ising spin glass in the presence of an external magnetic field. We have performed simulations both at fixed temperature and with an annealing protocol. Thanks to the Janus special-purpose computer, based on field-programmable gate array (FPGAs), we have been able to reach times equivalent to 0.01 s in experiments. We have studied the system relaxation both for high and for low temperatures, clearly identifying a dynamical transition point. This dynamical temperature is strictly positive and depends on the external applied magnetic field. We discuss different possibilities for the underlying physics, which include a thermodynamical spin-glass transition, a mode-coupling crossover, or an interpretation reminiscent of the random first-order picture of structural glasses.
Physical Review Letters | 2015
Marco Baity-Jesi; V. Martin-Mayor; Giorgio Parisi; S. Perez-Gaviro
In the three-dimensional Heisenberg spin glass in a random field, we study the properties of the inherent structures that are obtained by an instantaneous cooling from infinite temperature. For a not too large field the density of states g(ω) develops localized soft plastic modes and reaches zero as ω(4) (for large fields a gap appears). When we perturb the system adding a force along the softest mode, one reaches very similar minima of the energy, separated by small barriers, that appear to be good candidates for classical two-level systems.
Journal of Statistical Mechanics: Theory and Experiment | 2014
Marco Baity-Jesi; Raquel A. Baños; A. Cruz; L. A. Fernandez; J. M. Gil-Narvion; A. Gordillo-Guerrero; D. Iñiguez; A. Maiorano; F. Mantovani; Enzo Marinari; V. Martin-Mayor; J. Monforte-Garcia; A. Muñoz Sudupe; D. Navarro; Giorgio Parisi; S. Perez-Gaviro; M Pivanti; Federico Ricci-Tersenghi; J. J. Ruiz-Lorenzo; Sebastiano Fabio Schifano; B. Seoane; A. Tarancón; R. Tripiccione; D. Yllanes
We perform equilibrium parallel-tempering simulations of the 3D Ising Edwards-Anderson spin glass in a field, using the Janus computer. A traditional analysis shows no signs of a phase transition. Yet, we encounter dramatic fluctuations in the behaviour of the model: Averages over all the data only describe the behaviour of a small fraction of it. Therefore we develop a new approach to study the equilibrium behaviour of the system, by classifying the measurements as a function of a conditioning variate. We propose a finite-size scaling analysis based on the probability distribution function of the conditioning variate, which may accelerate the convergence to the thermodynamic limit. In this way, we find a non-trivial spectrum of behaviours, where a part of the measurements behaves as the average, while the majority of them shows signs of scale invariance. As a result, we can estimate the temperature interval where the phase transition in a field ought to lie, if it exists. Although this would be critical regime is unreachable with present resources, the numerical challenge is finally well posed.
programmable devices and embedded systems | 2013
Marco Baity-Jesi; Raquel A. Baños; A. Cruz; L. A. Fernandez; J. M. Gil-Narvion; A. Gordillo-Guerrero; D. Iñiguez; A. Maiorano; F. Mantovani; E. Marinari; V. Martin-Mayor; J. Monforte-Garcia; A. Muñoz Sudupe; D. Navarro; Giorgio Parisi; S. Perez-Gaviro; Marcello Pivanti; Federico Ricci-Tersenghi; J. J. Ruiz-Lorenzo; Sebastiano Fabio Schifano; B. Seoane; A. Tarancón; R. Tripiccione; D. Yllanes
Abstract Spin-glasses have become one of the most computing-demanding problems of the last 50 years in Statistical Physics. These extremely slow systems represent a clear example of an easy-to-describe but hard-to-simulate numerical problem. We have developed an FPGAs architecture, called Janus, able to exploit the simplicity of the problem by an extensive parallelization of the computing units. In this work we describe the architecture after motivating the problem. We give the performance figures compared with other more usual architectures. We have obtained a clear advantage in terms of computing power which produced several top results in the field. In addition, we describe the current development of the next generation of the infrastructure: Janus II.
Physical Review Letters | 2017
Marco Baity-Jesi; D. Yllanes; A. Muñoz-Sudupe; J. Monforte-Garcia; J. M. Gil-Narvion; D. Iñiguez; A. Gordillo-Guerrero; Enrico Calore; Federico Ricci-Tersenghi; A. Tarancón; R. Tripiccione; A. Maiorano; Enzo Marinari; B. Seoane; Giorgio Parisi; Sebastiano Fabio Schifano; S. Perez-Gaviro; V. Martin-Mayor; A. Cruz; J. J. Ruiz-Lorenzo; D. Navarro; L. A. Fernandez
We first reproduce on the Janus and Janus II computers a milestone experiment that measures the spin-glass coherence length through the lowering of free-energy barriers induced by the Zeeman effect. Secondly, we determine the scaling behavior that allows a quantitative analysis of a new experiment reported in the companion Letter [S. Guchhait and R. Orbach, Phys. Rev. Lett. 118, 157203 (2017)].PRLTAO0031-900710.1103/PhysRevLett.118.157203 The value of the coherence length estimated through the analysis of microscopic correlation functions turns out to be quantitatively consistent with its measurement through macroscopic response functions. Further, nonlinear susceptibilities, recently measured in glass-forming liquids, scale as powers of the same microscopic length.
Journal of Statistical Physics | 2017
Marco Baity-Jesi; Carl P. Goodrich; Andrea J. Liu; Sidney R. Nagel; James P. Sethna
We study the shear jamming of athermal frictionless soft spheres, and find that in the thermodynamic limit, a shear-jammed state exists with different elastic properties from the isotropically-jammed state. For example, shear-jammed states can have a non-zero residual shear stress in the thermodynamic limit that arises from long-range stress-stress correlations. As a result, the ratio of the shear and bulk moduli, which in isotropically-jammed systems vanishes as the jamming transition is approached from above, instead approaches a constant. Despite these striking differences, we argue that in a deeper sense, the shear jamming and isotropic jamming transitions actually have the same symmetry, and that the differences can be fully understood by rotating the six-dimensional basis of the elastic modulus tensor.