Shirshendu GangulyI am an Assistant Professor in the Department of Statistics at UC Berkeley. 
ResearchI am broadly interested in probability theory and its applications. Recently I have been working on problems in Disordered metric geometries with focus on geometry of geodesics in percolation models, Scaling limits and Phase transitions in statistical mechanics, Large deviations and counting problems in sparse nonlinear settings, Mixing time of Markov Chains, Random walk on graphs and Random Matrix theory.
A complete list of publications and preprints is given here. My CV. 
Education and past employment. 
Teaching. 
Some Recent Works 
Improving the HammersleyWelsh bound on the number of Self Avoiding Walks. Let c_n=c_n(d) denote the number of selfavoiding walks of length n starting at the origin in the Euclidean nearestneighbour lattice ℤ^d. Let μ denote the connective constant of ℤd. In 1962, Hammersley and Welsh [HW62] proved that, for each d≥2, there exists a constant C>0 such that c_n≤exp(Cn^1/2)μ^n for all n∈ℕ. While it is anticipated that c_nμ^(−n) has a powerlaw growth in n, the best known upper bound in dimension two has remained of the form n^(1/2) inside the exponential. We consider two planar lattices and prove that c_n≤exp(Cn^(1/2−ϵ))μ^n for an explicit constant ϵ>0 (where here μ denotes the connective constant for the lattice in question). The result is conditional on a lower bound on the number of selfavoiding polygons of length n, which is proved to hold on the hexagonal lattice ℍ for all n, and subsequentially in n for ℤ2. A powerlaw upper bound on cnμ−n for ℍ is also proved, contingent on a nonquantitative assertion concerning this lattice's connective constant. 
Aging properties of polymer weight profile. For directed last passage percolation on ℤ2 with exponential passage times on the vertices, let T_n denote the last passage time from (0,0) to (n,n). We consider asymptotic two point correlation functions of the sequence T_n. In particular we consider Corr(T_n,T_r) for r≤n where r,n→∞ with r≪n or n−r≪n. We show that in the former case Corr(T_n,T_r)=Θ((r/n)^1/3) whereas in the latter case 1−Corr(T_n,T_r)=Θ(((n−r)/n)^2/3). The argument revolves around finer understanding of polymer geometry and is expected to go through for a larger class of integrable models of last passage percolation. As byproducts of the proof, we also get a couple of other results of independent interest: Quantitative estimates for locally Brownian nature of prelimits of Airy2 process coming from exponential LPP, and precise variance estimates for lengths of polymers constrained to be inside thin rectangles at the transversal fluctuation scale. 
Delocalization of eigenvectors of high girth graphs We prove improved bounds on how localized an eigenvector of a high girth regular graph can be, and present examples showing that these bounds are close to sharp. This study was initiated by Brooks and Lindenstrauss (2009) who relied on the observation that certain suitably normalized averaging operators on high girth graphs are hypercontractive and can be used to approximate projectors onto the eigenspaces of such graphs. Our construction is probabilistic and involves gluing together a pair of trees while maintaining high girth as well as control on the eigenvectors and could be of independent interest. 
Fluctuation exponents, delocalization and large deviation of polymers Delocalization of polymers in lower tail large deviation. (with Riddhipratim Basu, Allan Sly) Arxiv Upper tail large deviations in First Passage Percolation. (with Riddhipratim Basu, Allan Sly) Arxiv The competition between local Brownian roughness and global parabolic curvature experienced in many random interface models reflects an important aspect of the KPZ universality class. It may be summarised by an exponent triple (1/2,1/3,2/3) representing local interface fluctuation, local roughness (or inward deviation) and convex hull facet length. In the first article, we offer a new perspective on this phenomenon. We consider directed last passage percolation model in the plane, and constrain the maximizing path under the additional requirement of enclosing an atypically large area. We prove that the exponent triple is now (2/3,1/2,3/4). This phenomenon appears to be shared among various isoperimetrically extremal circuits in local randomness. In the second article, we consider the large deviation regime, i.e., when the geodesic has much smaller (lower tail) or larger (upper tail) weight than typical. How the geometry of the geodesic changes under such a large deviation event was considered by Dueschel and Zeitouni (1998) where it was shown that the geodesic (from (0,0) to (n,n), say) remain concentrated around the straight line joining the end points in the upper tail large deviation regime, but left open the corresponding question in the lower tail. We answer their question by establishing a contrasting behaviour in the lower tail large deviation regime; we show that conditioned on the latter, in both the models, the geodesic is not concentrated around any deterministic curve. In the third article we establish a precise large deviation principle for the upper tail in First passage percolation which had remained open since Kesten's seminal work in 1986 which established the asymptotic decay rate of probabilities. 
Escape rates of Random walk on stationary graphs. We show that for any stationary random graph (G,p) of annealed polynomial growth there is an infinite sequence of times {t_n} at which the random walk {X_t} on (G,p) is at most diffusive. This result is new even in the case when G is a stationary random subgraph of Z^d. Combined with the work of Benjamini, DuminilCopin, Kozma, and Yadin (2015), it implies that G almost surely does not admit a nonconstant harmonic function of sublinear growth. To complement this, we argue that passing to a subsequence of times {t_n} is necessary, as there are stationary random graphs of (almost sure) polynomial growth where the random walk is almost surely superdiffusive at an infinite subset of times. 
Gibbs measure on Random Matrices and Lattice gauge theory. Lattice Gauge theories have been studied in the physics literature as discrete approximations to quantum YangMills theory for a long time. Primary statistics of interest in these models are expectations of the so called “Wilson loop variables”. In this article we continue the program initiated by Chatterjee (2015) to understand Wilson loop expectations in Lattice Gauge theories in a certain limit through gaugestring duality. The objective in this paper is to better understand the underlying combinatorics in the strong coupling regime, by giving a more geometric picture of string trajectories involving correspondence to objects such as decorated trees and noncrossing partitions. Using connections with Free Probability theory, we provide an elaborate description of loop expectations in the the planar setting, which provides certain insights about structures of higher dimensional trajectories as well. Exploiting this, we construct a counter example showing that in any dimension, the Wilson loop area law lower bound does not hold in full generality. 
Competitive Erosion Competitive erosion is conformally invariant (with Yuval Peres) To appear in Communications in Mathematical Physics (2018) Arxiv Formation of large scale random structure by competitive erosion. (with Lionel Levine and Sourav Sarkar) Arxiv We study a graphtheoretic model of interface dynamics called Competitive Erosion. Each vertex of the graph is occupied by a particle, which can be either red or blue. New red and blue particles are emitted alternately from their respective bases and perform random walk. On encountering a particle of the opposite color they remove it and occupy its position. Based on conformally invariant nature of reflected brownian motion Propp conjectured in 2003 that at stationarity, with high probability the blue and the red regions are separated by an orthogonal circular arc on the disc and by a suitable hyperbolic geodesic on a general simply connected domain. In the first article we study Competitive Erosion on the cylinder graph which has a relatively simple geometry. In the second article we confirm Propp's prediction on smooth enough planar simply connected domains. In the third article we study a variant on the line with the same source for both the particles which exhibit a random interface dynamics unlike the former cases. 
Large deviation and counting problems in sparse settings. Upper tails for arithmetic progressions in a random set (with with Bhaswar B. Bhattacharya, Xuancheng Shao, Yufei Zhao). To appear in International Mathematics Research Notices (2018). Arxiv The upper tail problem in the ErdosRenyi random graph G∼G(n,p) asks to estimate the probability that the number of copies of a graph H in G exceeds its expectation by a factor 1+δ. Chatterjee and Dembo (2014) showed that in the sparse regime of p→0 as n→∞ with p bigger than an inverse power of n, this problem reduces to a natural variational problem on weighted graphs, which was thereafter asymptotically solved by two of the authors in the case where H is a clique. Here we extend the latter work to any fixed graph H and determine a function cH(δ) such that, for p as above and any fixed δ >0, the logarithm of the upper tail probability properly normalized converges to cH(δ). As it turns out, the leading order constant in the large deviation rate function, cH(δ), is governed by the independence polynomial of H. The second article investigates similar questions in the setting of counting arithmetic progressions in random subsets of Z/nZ reducing large deviation questions to extremal problems in additive combinatorics. 
Self organized criticality Activated Random walk on a cycle. (with Riddhipratim Basu, Christopher Hoffman and Jacob Richey).To appear in AIHP (2018). Arxiv We consider Activated Random Walk (ARW), a model which generalizes the Stochastic Sandpile, one of the canonical examples of self organized criticality. Informally ARW is a particle system on Z, with initial mass density μ > 0 of active particles. Active particles do a symmetric random walk at rate one and fall asleep at rate λ > 0. Sleepy particles become active on coming in contact with other active particles. We investigate the question of fixation/nonfixation of the process and show for small enough λ the critical mass density for fixation is strictly less than one. Moreover, the critical density goes to zero as λ tends to zero. This positively answers two open questions from Dickman, Rolla, Sidoravicius (J. Stat. Phys., 2010) and Rolla, Sidoravicius (Invent. Math., 2012).
