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Pierre Le Doussal
Researcher at École Normale Supérieure
Publications - 331
Citations - 11408
Pierre Le Doussal is an academic researcher from École Normale Supérieure. The author has contributed to research in topics: Brownian motion & Random walk. The author has an hindex of 48, co-authored 313 publications receiving 10154 citations. Previous affiliations of Pierre Le Doussal include Institute for Advanced Study & University of California, Santa Barbara.
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Journal Article
Functional Renormalization for Disordered Systems. Basic Recipes and Gourmet Dishes
TL;DR: In this article, the authors give a pedagogical introduction to the functional renormalization group treatment of disordered systems and construct a renormalizable field theory beyond leading order, which is compared to predictions of the Gaussian replica variational ansatz using replica symmetry breaking.
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Freezing Transition in Decaying Burgers Turbulence and Random Matrix Dualities
TL;DR: In this article, a phase transition with decreasing viscosity was revealed in one-dimensional decaying Burgers turbulence with a power-law correlated random profile of Gaussian-distributed initial velocities.
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On integrable directed polymer models on the square lattice
TL;DR: In this article, a two-parameter family of integrable directed polymer models with random weights on the square lattice is presented, called the Inverse-Beta polymer.
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Exact mapping of the stochastic field theory for Manna sandpiles to interfaces in random media.
Pierre Le Doussal,Kay Jörg Wiese +1 more
TL;DR: It is shown that the stochastic field theory for directed percolation in the presence of an additional conservation law can be mapped exactly to the continuum theory for the depinning of an elastic interface in short-range correlated quenched disorder.
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Equilibrium avalanches in spin glasses
TL;DR: In this article, it was shown that the density of overlap q between initial and final states in an avalanche is ρ(q) ∼ 1/(1 − q) for jumps of size 1 � m < N 1/2, being provoked by changes of the external field by δH = O(N −1/2 )w hereN is the total number of spins.