Laboratoire de Physique Théorique de la Matière Condensée

Your browser's timezone is %s, which is different to your settings. Do you want to change to your browser timezone? Yes Close

LPTMC Seminars

The seminars take place in room 523, corridor 12-13, 5th floor.

15.11.2025 - 13.12.2025
  • Antonio Picano (Collège de France)

    Date 12.12.2025 14:00 - 15:00
    Séminaires
  • Julien Randon-Furling (Centre Borelli, ENS Paris Saclay)

    09.12.2025 10:45 - 11:45
    Séminaires

    Salle 523, couloir 12-13, 5è étage

    First passages, survival probabilities & higher-dimensional convex hulls

    First I will present joint work with B. de Bruyne and S. Redner, on first-passage resetting, where the resetting of a random walk to a fixed position is triggered by a first-passage event of the walk itself. We define an optimization problem that is controlled by first-passage resetting: a cost is incurred whenever the particle is reset and a reward is obtained while the particle stays near the reset-trigger point. We derive the condition to optimize the net gain in this system, namely, the reward minus the cost. I will also talk about an extension of first-passage resetting into a minimalist dynamical model of wealth evolution and wealth sharing among N agents.

    Second, I will present joint work with G. Uribe Bravo and D. Zaporozhets. We focus on the convex hull of a single multidimensional random walk, with i.i.d. steps taken from any symmetric, continuous distribution. We investigate the persistence of vertices and faces on the hull. In particular we show that the corresponding distributions are universal, and follow three regimes closely linked to the Sparre Andersen theorem for one dimensional random walks.

    Third, time-permitting (hence, probably not...), I will turn to the convex hull of several multidimensional Gaussian random walks. Explicit formulas for the expected volume and expected number of faces are derived in terms of the Gaussian persistence probabilities. Special cases include the already known results about the convex hull of a single Gaussian random walk and the d-dimensional Gaussian polytope.

    References:

    de Bruyne, B., R.-F., J., Redner, S. (2020). Phys. Rev. Letters, 125(5), 050602

    de Bruyne, B., R.-F., J., Redner, S. (2021). J. Stat. Mech., 2021(10), 103405

    R.-F., J., Zaporozhets, D. (2024). J. Math. Sc., 281(1)

    R.-F., J., Uribe Bravo, G., Zaporozhets, D. to appear (2026)

  • Guido Giachetti (ENS)

    02.12.2025 10:45 - 11:45
    Séminaires

    Salle 523, couloir 12-13, 5è étage

    Integrable Dynamics and Thermalization in the Quantum O(n) Model at Large n

    The quantum O(n) model has long served as a valuable framework for studying both equilibrium and dynamical properties of quantum many-body systems. In this talk, we investigate its non-equilibrium dynamics following a quantum quench in the large-n limit. While the model is known to be tractable in this regime, we show that it is in fact integrable - with integrals of motions stemming from that of the classical Neumann model - thus enabling a complete analytical solution of its dynamics. This integrability reveals a synchronization mechanism that gives rise to persistent oscillations, interpretable as Higgs modes localized at the edge of the spectral band. We further demonstrate that the long-time behavior is governed by a Generalized Gibbs Ensemble (GGE), in contrast to previous expectations, and we obtain exact critical exponents differing from those commonly reported. Remarkably, integrability persists even in the presence of long-range couplings, allowing us to explore the crossover between mean-field and genuinely many-body regimes in terms of parametric Floquet resonances of the microscopic degrees of freedom.

  • Vincent Ouazan-Reboul (LPTMS)

    25.11.2025 10:45 - 11:45
    Séminaires

    Salle 523, couloir 12-13, 5è étage

    Complex interactions in and out of equilibrium

    One of the main challenges in the modeling of biological systems is that their physical behavior at all scales is
    dictated by intricate interactions between many different complex objects. In this talk, I will present theoretical
    results on two different systems where complex interactions play a key role, one equilibrium and the other active.

    I will first discuss the equilibrium self-assembly of proteins, which can be seen as particles with short-range
    anisotropic interactions. Strikingly, proteins with vastly different physico-chemical properties tend to form into
    similar fibrous pathological aggregates. By performing lattice Monte-Carlo simulations of three-dimensional particles, I
    will show that complex anisotropic iteractions lead to a great morphological diversity in the resulting assemblies. In
    particular, many choices of interactions lead to the formation of fibers, which are found to result from geometrical
    frustration. On the other hand, I will also demonstrate that anisotropy is a useful design tool for controlling the size
    and shape of equilibrium aggregates.

    In a second part, I will discuss the self-organization of mixtures of enzyme-like active particles. As opposed to the
    previous system, these objects are intrinsically out of equilibrium, and develop isotropic, long-ranged, non-reciprocal
    interactions. By using a combination of linear stability analysis and Brownian dynamics simulations, I will show that
    catalytically active particles can self-organize into droplet-like structures. My focus will be on the case where
    different species of enzymes participate in a biochemical reaction network. This different type of complexity, which
    stems from the existence of an intricate interaction network between different species instead of structural anisotropy,
    can be an intrinsic driver of self-organization and lead to novel collective dynamics.

  • Thibault Scoquart (LPT Toulouse/LPTMC)

    18.11.2025 10:45 - 11:45
    Séminaires

    Salle 523, couloir 12-13, 5è étage

    Scaling of many-body localization transitions: Correlations and dynamics in Fock space and real space

    Many-body localization (MBL) is a remarkable phenomenon where interacting quantum systems fail to thermalize due to disorder. Despite two decades of intense theoretical and numerical work, there is still no clear consensus on whether a true 1D MBL phase exists in the thermodynamic limit, or whether it eventually gives way to slow thermalization.

    After a broad introduction to the current open questions surrounding MBL, I will discuss recent results [1] on how MBL transitions scale with system size in several different disordered spin-½ models. By representing these models as effective tight-binding problems in Fock space—where “sites’’ correspond to many-body basis states and “hoppings’’ to interactions—we can explicitly identify the role of correlations between Fock-space energies and couplings in the onset of localization and the breakdown of ergodicity. Comparing models with and without such correlations (1D spin chains, quantum dot with all-to-all interactions, and the quantum random energy model) reveals strikingly different scaling behaviors for the critical disorder strength and transition width, which we predicted analytically and verified numerically. Finally, I will show how real-space dynamical probes that are accessible to modern simulators, such as the time evolution of the “generalized” imbalance, also capture the features of the transition from the Fock-space perspective, and allow us to construct consistent finite-size phase diagrams, in full agreement with spectral observables [2].

    [1] T. Scoquart, I. Gornyi and A. Mirlin, Role of Fock-space correlations in many-body localization, Phys. Rev. B 109, 214203, (2024)
    [2] T. Scoquart, I. Gornyi and A. Mirlin, Scaling of many-body localization transitions: Quantum dynamics in Fock space and real space, Phys. Rev. B 112, 064203 (2025)