Statistical mechanics via asymptotics of symmetric functions

Similar documents
Uniformly Random Lozenge Tilings of Polygons on the Triangular Lattice

Fluctuations of random tilings and discrete Beta-ensembles

Fluctuations of random tilings and discrete Beta-ensembles

Around tilings of a hexagon

Central Limit Theorem for discrete log gases

Gaussian Free Field in beta ensembles and random surfaces. Alexei Borodin

Rectangular Young tableaux and the Jacobi ensemble

Gaussian Free Field in (self-adjoint) random matrices and random surfaces. Alexei Borodin

The Arctic Circle re-revisited

Refined Cauchy/Littlewood identities and partition functions of the six-vertex model

A third-order phase transition in random domino tilings

Random Tilings Workshop Schedule

Six-vertex model partition functions and symmetric polynomials of type BC

Geometric RSK, Whittaker functions and random polymers

Two-periodic Aztec diamond

Fully Packed Loops Model: Integrability and Combinatorics. Plan

Integrable Probability. Alexei Borodin

Combinatorial bases for representations. of the Lie superalgebra gl m n

Universality of distribution functions in random matrix theory Arno Kuijlaars Katholieke Universiteit Leuven, Belgium

Triangular matrices and biorthogonal ensembles

Convolutions and fluctuations: free, finite, quantized.

From longest increasing subsequences to Whittaker functions and random polymers

Enumeration of domino tilings of a double Aztec rectangle

arxiv: v2 [math.pr] 28 May 2013

From alternating sign matrices to Painlevé VI

Lozenge Tilings and Hurwitz Numbers

Dimer Problems. Richard Kenyon. August 29, 2005

Airy and Pearcey Processes

Central Limit Theorems for linear statistics for Biorthogonal Ensembles

Tiling expression of minors

Domino shuffling on Novak half-hexagons and Aztec half-diamonds

Fluctuations of interacting particle systems

The dimer model: universality and conformal invariance. Nathanaël Berestycki University of Cambridge. Colloque des sciences mathématiques du Québec

On the Error Bound in the Normal Approximation for Jack Measures (Joint work with Le Van Thanh)

Primes, partitions and permutations. Paul-Olivier Dehaye ETH Zürich, October 31 st

Domino shuffling and TASEP. Xufan Zhang. Brown Discrete Math Seminar, March 2018

arxiv: v3 [math-ph] 4 Jun 2017

On some combinatorial aspects of Representation Theory

5-VERTEX MODELS, GELFAND-TSETLIN PATTERNS AND SEMISTANDARD YOUNG TABLEAUX

Integrable structure of various melting crystal models

Littlewood Richardson polynomials

REPRESENTATION THEORY WEEK 7

DOMINO TILINGS INVARIANT GIBBS MEASURES

Topological Matter, Strings, K-theory and related areas September 2016

Statistical Mechanics and Combinatorics : Lecture IV

Integrable probability: Beyond the Gaussian universality class

Shifted symmetric functions I: the vanishing property, skew Young diagrams and symmetric group characters

ALGEBRAIC COMBINATORICS

Classical Lie algebras and Yangians

limit shapes beyond dimers

Fourier-like bases and Integrable Probability. Alexei Borodin

Schur polynomials, banded Toeplitz matrices and Widom s formula

Smith Normal Form and Combinatorics

Powers of the Vandermonde determinant, Schur functions, and the dimension game

The dilute Temperley-Lieb O(n = 1) loop model on a semi infinite strip: the sum rule

arxiv: v1 [math.co] 18 Oct 2018

arxiv: v1 [math.co] 25 May 2011

Determinantal measures related to big q-jacobi polynomials

Correlation function of Schur process with application to local geometry of a random 3-dimensional Young diagram

h r t r 1 (1 x i=1 (1 + x i t). e r t r = i=1 ( 1) i e i h r i = 0 r 1.

Domino tilings, non-intersecting Random Motions and Critical Processes

MARKOV PROCESSES ON THE DUALS TO INFINITE-DIMENSIONAL CLASSICAL LIE GROUPS

MIMO Capacities : Eigenvalue Computation through Representation Theory

Algebra C Numerical Linear Algebra Sample Exam Problems

MATH 722, COMPLEX ANALYSIS, SPRING 2009 PART 5

Angular matrix integrals

A Formula for the Specialization of Skew Schur Functions

Standard Young Tableaux Old and New

Markov operators, classical orthogonal polynomial ensembles, and random matrices

The toggle group, homomesy, and the Razumov-Stroganov correspondence

THREE LECTURES ON QUASIDETERMINANTS

RANDOM MATRIX THEORY AND TOEPLITZ DETERMINANTS

Combinatorial Interpretation of the Scalar Products of State Vectors of Integrable Models

Random matrix pencils and level crossings

Beyond the Gaussian universality class

Exponential tail inequalities for eigenvalues of random matrices

What is the Relation between Eigenvalues & Singular Values? Mario Kieburg

Concentration Inequalities for Random Matrices

arxiv:math/ v1 [math.co] 13 Jul 2005

Double contour integral formulas for the sum of GUE and one matrix model

MONOMER CORRELATIONS ON THE SQUARE LATTICE. Mihai Ciucu Indiana University Department of Mathematics, Bloomington, IN 47405, USA

Random tilings and Markov chains for interlacing particles

Square-Triangle-Rhombus Random Tiling

Appearance of determinants for stochastic growth models

MOMENTS OF INERTIA ASSOCIATED WITH THE LOZENGE TILINGS OF A HEXAGON

Numerical Analysis Comprehensive Exam Questions

A MARKOV CHAIN ON THE SYMMETRIC GROUP WHICH IS SCHUBERT POSITIVE?

Topological vertex and quantum mirror curves

To appear in Monatsh. Math. WHEN IS THE UNION OF TWO UNIT INTERVALS A SELF-SIMILAR SET SATISFYING THE OPEN SET CONDITION? 1.

Maximal height of non-intersecting Brownian motions

Lecture I: Asymptotics for large GUE random matrices

Schur processes and dimer models

Statistical Mechanics & Enumerative Geometry:

On Tensor Products of Polynomial Representations

STABLE CLUSTER VARIABLES

Stochastic Differential Equations Related to Soft-Edge Scaling Limit

AN ASYMPTOTIC BEHAVIOR OF QR DECOMPOSITION

THE SMITH NORMAL FORM OF A SPECIALIZED JACOBI-TRUDI MATRIX

Log-Convexity Properties of Schur Functions and Generalized Hypergeometric Functions of Matrix Argument. Donald St. P. Richards.

Arctic circles, domino tilings and square Young tableaux

Transcription:

symmetric Statistical mechanics via of symmetric (University of Pennsylvania) based on: V.Gorin, G.Panova, Asymptotics of symmetric polynomials with applications to statistical mechanics and representation theory, Annals of Probability arxiv:0.064 G. Panova, with free, arxiv:408.047. April 05

symmetric Overview Characters of U( ), boundary of the Gelfand-Tsetlin graph......... Normalized : S λ (x,..., x k ; N) = s λ(x,..., x k, N k ) s λ ( N ) Alternating Sign Matrices (ASM)/ 6-Vertex model: 0 0 0 0 0 0 0 0 : : ζ y ζ x L

symmetric Tilings of a domain Ω (on a triangular lattice) with elementary rhombi of types ( lozenges ).

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5 4 4 5 4 4 4

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 4 5 5 4 4 4 4

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric The many faces of lozenge tilings 5 4 4 4 5 4 5

symmetric Limit behavior Question: Fix Ω in the plane and let grid size 0, what are the properties of uniformly random tilings of Ω? [Cohn Larsen Propp, 998] Hexagonal domain: Tiling is asymptotically frozen outside inscribed ellipse. [Kenyon Okounkov, 005] Polygonal domain: Tiling is asymptotically frozen outside inscribed algebraic curve..jpg [Cohn Kenyon Propp, 00; Kenyon-Okounkov-Sheffield, 006] There exists a limit shape for the surface of the height function (plane partition). 6

symmetric Behavior near the boundary, interlacing particles x x x x x x x N Horizontal lozenges near a flat boundary: interlacing particle configuration Gelfand-Tsetlin patterns. Question: What is the joint distribution of {x i j }k i= as N (scale = N )? x x x x x x with an explanation what the answer should be. Subsequent results: [Gorin-P,0], [Novak, 04],[Mkrtchyan, 0, periodic weights, unbounded 7

symmetric Behavior near the boundary, interlacing particles x x x x x x x N Horizontal lozenges near a flat boundary: interlacing particle configuration Gelfand-Tsetlin patterns. x x x x x x Question: What is the joint distribution of {x i j }k i= as N (scale = N )? Conjecture [Okounkov Reshetikhin, 006 ]: The joint distribution converges to a GUE-corners (aka GUE-minors) process: eigenvalues of GUE matrices. Proven for the hexagon by Johansson- Nordenstam (006). with an explanation what the answer should be. Subsequent results: [Gorin-P,0], [Novak, 04],[Mkrtchyan, 0, periodic weights, unbounded 7

symmetric GUE in tilings: our setup Domain Ω λ(n) : width N and the positions λ(n) + N > λ(n) + N > > λ(n) N of its N horizontal lozenges at the right boundary. +4 + + 8 + 0 8 + 9 8 + 8 8 + 7 8 + 6 4 5 + λ(5) = (4,,, 0, 0) Note: N Ω λ(n) is not necessarily a finite polygon as N, e.g. λ(n) = (N, N,...,, ) 0 + 5 0 + 4 0 + 0 + 0 + 0 + 0 E.g. λ = (a,..., a, 0,..., 0) }{{}}{{} c b the hexagon with side lengths (a, b, c, a, b, c). 8

symmetric Plane partitions/gelfand-tsetlin patterns λ + N x x x Line j = λ + N λn N 5 4 4 4 0 0 0 λ = (5, 4,,, 0) x = (4,, 0) 4 0 0 0 0 0 0 λ = (4,,, 0, 0) Question: What is the joint distribution of the positions rescaling) near the boundary as N (i.e. lattice scale = N )? { } xj i (under correct 9

symmetric Answers: the Gaussian Unitary Ensemble (GUE) Gaussian Unitary Ensemble: matrices [X ij ] i,j : X = X T ReX ij, ImX ij i.i.d. N (0, /) for i j and X ii i.i.d. N (0, ) a a a a 4 a a a a 4 a a a a 4 a 4 a 4 a 4 a 44 (x k xk xk k ) eigenvalues of [X i,j ] k i,j= (top k k). Interlacing condition: x j i xj i xj i x 4 x 4 x 4 x4 4 x x x x x The joint distribution of {x j i } i j k is known as GUE corners (also, GUE-minors) process, =: GUE k. x 0

symmetric GUE in tilings: our results Limit profile f (t) of λ(n) as N ( : ) λ(n) i i N f N N λ(n) f (t) Ω λ(n) domain: Theorem (Gorin-P (0), Novak (04)) Let λ(n) = (λ (N)... λ N (N)), N =,,... be a partition. If a piecewise-differentiable weakly decreasing function f (t) (limit profile of λ(n)) s.t. N ( ) λ i (N) i N f = o( N) as N N i= and also sup i,n λ i (N)/N <. Let Υ k λ(n) = {xj i } be the collection of the positions of the horizontal lozenges on lines j =,..., k. Then for every k as N x λ + N λ + N Υ k λ(n) NE(f ) NS(f ) GUE k (GUE-corners proc. rank k) x in the sense of weak convergence, where x E(f ) = f (t)dt, 0 Line j = λn S(f ) = f (t) dt E(f ) + f (t)( t)dt. 0 0

symmetric Towards the proof:...or more generally symmetric, Lie group characters. Irreducible (rational) representations V λ of GL(N) (or U(N)) are indexed by dominant weights (signatures/young diagrams/integer partitions) λ: where λ i Z, e.g. λ = (4,, ), λ λ λ N, : s λ (x,..., x N ) characters of V λ. Weyl s determinantal formula: s λ (x,..., x N ) = [ det x λ j +N j i ] N ij= i<j (x i x j ) Semi-Standard Young tableaux( Gelfand-Tsetlin patterns) of shape λ : s (,) (x, x, x ) = s (x, x, x ) = x x +x x +x x +x x x +x x x +x x x.

symmetric Main object: Normalized N k {}}{ S λ(n) (x,..., x k ) := s λ(n)(x,..., x k,,..., ) s λ(n) (,..., ) }{{} N or more generally normalized Lie group characters: X γ(n) (x,..., x k ) := χ γ(n)(x,..., x k, N k ) χ γ(n) ( N ) Meaning also via the Harish-Chandra/Itzykson Zuber integral: s λ (e a,..., e an ) s λ (,..., ) = a i a j bj =λ j +N j e a i e a j i<j exp(trace(aubu ))du U(N)

symmetric Integral formula, k = Theorem (Gorin-P) For any partition λ and any x C \ {0, } we have (N )! x z S λ (x; N, ) = (x ) N πi N C i= (z (λ i + N i)) dz, where the contour C includes all the poles of the integrand. Similar formulas hold for the other normalized Lie group characters. Theorem (Gorin-P) ( ) If λ(n) N f i [under certain convergence conditions], for all fixed y 0: N lim N N ln S λ(n)(e y ; N, ) = yw 0 F(w 0) ln(e y ), where F(w; f = 0 ln(w f (t) + t)dt, w0 root of F(w; f ) = y. If ( ) w λ(n) N f i [ other conv. cond.], for any fixed h R: N ( ) NE(f S λ(n) (e h/ N ; N, ) = exp )h + S(f )h + o(), where E(f ) = f (t)dt, S(f ) = f (t) dt E(f ) + f (t)( t)dt. 0 0 0 Remark. Similar statements hold for a larger class of, e.g symplectic characters, Jacobi...+ q analogues. Remark. Integral formula appears also in [Colomo,Pronko,Zinn-Justin], random matrix interpretation in [Guionnet Maida], new analysis in [Novak]... 4

symmetric From k = to general k, multiplicativity Theorem (Gorin-P ) Let D i, = x i, Vandermonde det. Then λ, k N, we have x i N k {}}{ S λ (x,..., x k ; N) = s λ(x,..., x k,,..., ) s λ (,..., ) }{{} N [ ] k det D j k (N i)! = (N )!(x i= i ) N k i, k i,j= S λ (x j ; N, )(x j ) N. (x,..., x k ) j= Corollary (Gorin-P) Suppose that the sequence λ(n) is such that, as N, ln ( S λ(n) (x; N, ) ) Ψ(x) uniformly on a compact M C. Then for any k N ln ( S λ(n) (x,..., x k ; N, ) ) lim = Ψ(x ) + + Ψ(x k ) N N uniformly on M k. More informally, under various regimes of convergence for λ(n) we have S λ(n) (x,..., x k ) S λ(n) (x ) S λ(n) (x k ). Similar for symplectic characters, Jacobi; and q-analogues. Note: appears in [de Gier, Nienhuis, 5

symmetric GUE in tilings I: combinatorics x 0 x x x 0 0 4 0 0 + + 4 5 +4 + Tilings of domain Ω λ(n) Gelfand-Tsetlin schemes with bottom row λ(n) 0 0 0 0 0 0 4 Semi-Standard Young Tableaux of shape λ(n) T = 5 4 4 5 5 5 Positions of the horizontal lozenges on line j: x j shape of the subtableaux of T of the entries,..., j. Note: actual positions on the d projection are at (x k + (k/, k/,..., k/, k/)) 6

symmetric GUE in tilings I: combinatorics x 0 x x x 0 0 4 0 0 + + 4 5 +4 + Tilings of domain Ω λ(n) Gelfand-Tsetlin schemes with bottom row λ(n) 0 0 0 0 0 0 4 Semi-Standard Young Tableaux of shape λ(n) T = 5 4 4 5 5 5 x = (,, 0). Positions of the horizontal lozenges on line j: x j shape of the subtableaux of T of the entries,..., j. Note: actual positions on the d projection are at (x k + (k/, k/,..., k/, k/)) 6

symmetric GUE in tilings II: moment generating Proposition In a uniformly random tiling of Ω λ the distribution of the positions of the horizontal lozenges on the kth line x k (λ) is given by: Prob{x k (λ) = η} = sη(k )s λ/η ( N k ) s λ ( N, ) where s λ/η is the skew Schur polynomial. Proof: combinatorial definition of as sums over SSYTs. Proposition For any variables y,..., y k, the following moment generating function of x k (as above) is given by N k {}}{ s E x k (y,..., y k ) s x k (,..., ) = s λ(y,..., y k,,..., ) = S λ (y,..., y k ). s λ (,..., ) }{{}}{{} k N 7

symmetric GUE in tilings III: MGF Proposition ( ) EB k (y; GUE k ) = exp (y + + y k ), where B k (y; ν) = s ν δ k (y,..., y k ) when ν strict partition. s ν δk (,..., ) }{{} k 8

symmetric GUE in tilings III: MGF Proposition ( ) EB k (y; GUE k ) = exp (y + + y k ), where B k (y; ν) = s ν δ k (y,..., y k ) when ν strict partition. s ν δk (,..., ) }{{} k Compare: s S λ (y,..., y k ) = E tiling x k (y,..., y k ) s x k (,..., ) = E tiling B k (y; x k + δ k ) }{{} k Proposition (Gorin-P) For any k real numbers h,..., h k and λ(n)/n f (as earlier) we have: ( h lim S NS(f λ(n) e ),..., e N ) h NS(f k ) e ( ) E(f ) ( ki= h NS(f ) i = exp ) k hi. i= 8

symmetric GUE in tilings III: MGF Proposition ( ) EB k (y; GUE k ) = exp (y + + y k ), where B k (y; ν) = s ν δ k (y,..., y k ) when ν strict partition. s ν δk (,..., ) }{{} k Compare: s S λ (y,..., y k ) = E tiling x k (y,..., y k ) s x k (,..., ) = E tiling B k (y; x k + δ k ) }{{} k Proposition (Gorin-P) For any k real numbers h,..., h k and λ(n)/n f (as earlier) we have: ( h lim S NS(f λ(n) e ),..., e N ) h NS(f k ) e ( ) E(f ) ( ki= h NS(f ) i = exp Theorem. Let Υ k λ(n) = {xk, x k,...} collection of positions of the horizontal lozenges on lines k, k,..., of tiling from Ω λ(n), then Υ k λ(n) NE(f ) GUE k (GUE-corners process of rank k). NS(f ) ) k hi. i= 8

symmetric Free boundary domains N M N T f (N, M) := λ : l(λ)=n,λ M tilings of Ω λ, set of all tilings in an N M N trapezoid with N free (unrestricted) horizontal rhombi on the right border. Symmetric tilings of the N M N N M N hexagon/ symmetric boxed Plane Partitions. M N Questions:. Existence of a limit shape (surface)? Equation derived in [Di Francesco Reshetikhin, 009].. Behavior near boundary (GUE?). 9

symmetric with free : GUE m n y y y Line k = λ + N λ + N λ N Theorem (P) Let Yn,m k = (y k,..., y k k ) denote the positions of the horizontal lozenges on the kth vertical line. As n, m with m/n a for 0 < a <, we have Y k n,m m/ n(a + a)/8 GUE k weakly as RVs. Moreover, the collection { } Y j k n,m m/ weakly converge as n(a +a)/8 j= RVs to the GUE corners process Proof method: Generating function for free boundary tilings is an SO n+ character: λ (m n ) s λ (x,..., x n) = det[xm+n i j det[x n i j x i j ] i,j n x i j ] i,j n = γ (m n )(x), Apply the same asymptotic techniques to this MGF as for GUE eigenvalues MGF as N. 0

symmetric with free : limit shape (limit surface) Theorem (P) Let n, m Z, such that m/n a as n, where a (0, + ). Let H(u, v) be the height function (plane partition) of the uniformly random lozenge tiling in T f (n, m),i.e. H(u, v) = n y nu nv v. For all u (0, ), u v 0, as n we have that H(u, v) converges uniformly in probability to a deterministic function L(u, v), referred to as the limit shape. Moreover, for any fixed u (0, ), the function L(u, v) is the distribution function of the limit measure m whose moments are given by r ( r x r m(dx) = R l) l (l + )! t l Φa(t), l=0 t= where Φ a(e y ) = y a + φ(y; a) and... h(y) = 4 ( (e y ) + ) + (e y + ) + 4(a + a) (e y ) φ(y; a) = ( a ( + ) ln h(y) ( a + )(e y ) ) ( a + ( ) ln h(y) ( a + )(e y ) ) + a ( ln h(y) + a (e y ) ) ( a ( ) ln h(y) + ( a )(e y ) )

symmetric with free : limit shape (limit surface) Theorem (P) Let n, m Z, such that m/n a as n, where a (0, + ). Let H(u, v) be the height function (plane partition) of the uniformly random lozenge tiling in T f (n, m),i.e. H(u, v) = n y nu nv v. For all u (0, ), u v 0, as n we have that H(u, v) converges uniformly in probability to a deterministic function L(u, v), referred to as the limit shape. Proof, idea: 4 Horizontal lozenges at line x = un at positions µ = y un distributed ρ (unif. on all tilings), giving a sequence of random measures m[µ] = ( µi ) δ. n n i S ρ(u,..., u N ) := µ:l(µ)=n ρ(µ) sµ(u,..., u N ) s µ( N. ) (and observe S ρ = γ m n (x,...,x N ) our MGF) γ (m n ) ( N ) Using this MGF, its and operators, obtain a concentration phenomenon: m[µ] m a deterministic measure, which is the limit shape L. 4 after [Borodin-Bufetov-Olshanski, Bufetov-Gorin]

symmetric with free : limit shape (limit surface) Theorem (P) Let n, m Z, such that m/n a as n, where a (0, + ). Let H(u, v) be the height function (plane partition) of the uniformly random lozenge tiling in T f (n, m),i.e. H(u, v) = n y nu nv v. For all u (0, ), u v 0, as n we have that H(u, v) converges uniformly in probability to a deterministic function L(u, v), referred to as the limit shape. Corollary (P) The height function of the uniformly random lozenge tilings of a half-hexagon with free right boundary converges (in probability) to a unique limit shape (surface) H(x, y), which coincides over the half-hexagon with the limit shape for the tilings of the full hexagon (fixed boundary). The shifted by m/ and rescaled by n(a + a)/8 positions of the horizontal lozenges on the k-th vertical line have the same joint distributions as n, m, which is GUE k.

symmetric 6 Vertex model / ASM Six vertex types: H H O O H O H H O H O H O H H a a b b c c 0 0 0 0 Alternating Sign Matrix: H H H A 6 vertex model configuration: 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 H H H O H O H O H O H O H H H H H O H O H O H O H O H H H H H O H O H O H O H O H H H H H H H H H O H O H O H O H O H H H H H H H O H O H O H O H O H

symmetric Definitions and background on ASMs Definition: A is an Alternating Sign Matrix ASM of size n if: n n A {0, +, } n n, A i,j =, A i,j = i= j= and (A i,k, i =... n s.t. A i,k 0) = (,,,,...,, ) A monotone triangle is a Gelfand-Tsetlin pattern with strictly increasing rows. 6 Vertex model ASM monotone triangles. Uniform measure on ASMs vertices in 6V model have same weights ( ice ). 0 0 0 0 0 0 ASM: 0 0 0 0 0 0 0 0 0 0 0 0 positions of s Monotone triangle: 4 5 in sum of first k rows 5 5 4 5 < Question: As n : Uniformly random ASM. What is the distribution of the positions of the s and s near the boundary Distribution of the top k rows of the monotone triangle? Known results: Limit behavior(conj): Behrend, Colomo, Pronko, Zinn-Justin, Di Francesco. Free fermions point (weight(,-)=) domino tilings, Aztec diamond. Exact gen. fs. for certain statistics (e.g. positions of s on boundary).

symmetric ASMs/6Vertex: new results k : ASM A: Ψ k (A) := j=:n, A kj = j Monotone triangle M = [m i j ] j i : Ψ k (M) = 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 j=:n, A kj = k j= j k mj k m k j j= 4 5 5 5 4 5 Ψ = + 5 4 = Ψ = ( + 5) (4) = Ψ = Ψ = ( + + 5) ( + 5) 4

symmetric ASMs/6Vertex: new results k : ASM A: Ψ k (A) := j=:n, A kj = j Monotone triangle M = [m i j ] j i : Ψ k (M) = 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 j=:n, A kj = k j= j k mj k m k j j= 4 5 5 5 4 5 Ψ = + 5 4 = Ψ = ( + 5) (4) = Ψ = Ψ = ( + + 5) ( + 5) Theorem (Gorin-P) If A unif. rand. n n ASM, then Ψ k (A) n/ n, k =,,... converge as n to the collection of i.i.d. Gaussian random variables, N(0, /8). 4

symmetric ASMs/6Vertex: new results k : ASM A: Ψ k (A) := j=:n, A kj = j Monotone triangle M = [m i j ] j i : Ψ k (M) = 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 j=:n, A kj = k j= j k mj k m k j j= 4 5 5 5 4 5 Ψ = + 5 4 = Ψ = ( + 5) (4) = Ψ = Ψ = ( + + 5) ( + 5) Theorem (Gorin-P) If A unif. rand. n n ASM, then Ψ k (A) n/ n, k =,,... converge as n to the collection of i.i.d. Gaussian random variables, N(0, /8). Using this Theorem on Ψ k (n) and the Gibbs property: Theorem (G, 0; Conjecture in [Gorin-P] ) Fix any k. The [centered,rescaled] positions of s on the first k rows (top k rows of the monotone triangle M) tend to the GUE-corners process: 8 ( [M] i=:k n ) GUE k. n 4

symmetric 6Vertex/ASMs: proofs Vertex weights at (i, j): type a : q ui qvj, type b : q vj qui, type c : (q q)u i v j (v,..., v N, u,..., u N parameters, q = exp(πi/) ) Weight W (ϑ) of a configuration ϑ is = weight(vtx). vtx ϑ Set λ(n) := (N, N, N, N,...,,, 0, 0) GT N. Proposition (Okada;Stroganov) Let ג N be the set of all 6-Vertex configurations on an N N grid. N W (ϑ) = ( ) N(N )/ (q q) N (v i u i ) s λ(n) (u,..., u N, v,..., v N ). ג ϑ N i= 5

symmetric 6Vertex/ASMs: proofs Vertex weights at (i, j): type a : q ui qvj, type b : q vj qui, type c : (q q)u i v j (v,..., v N, u,..., u N parameters, q = exp(πi/) ) Weight W (ϑ) of a configuration ϑ is = weight(vtx). vtx ϑ Set λ(n) := (N, N, N, N,...,,, 0, 0) GT N. Proposition Let x i =number of vertices of type x on row i, then collection of rows i,..., i m m q E N ( qv )âil ( l q vl q ) bil q q q (v l q )ĉjl l= ( n ) ( = v sλ(n) (v,..., v m, N m ) n ) l s λ(n) ( N = v l S λ(n) (v,..., v m) ) l= l= 5

symmetric 6Vertex/ASMs: proofs Vertex weights at (i, j): type a : q ui qvj, type b : q vj qui, type c : (q q)u i v j (v,..., v N, u,..., u N parameters, q = exp(πi/) ) Weight W (ϑ) of a configuration ϑ is = weight(vtx). vtx ϑ Set λ(n) := (N, N, N, N,...,,, 0, 0) GT N. Proposition Let x i =number of vertices of type x on row i, then collection of rows i,..., i m m q E N ( qv )âil ( l q vl q ) bil q q q (v l q )ĉjl l= ( n ) ( = v sλ(n) (v,..., v m, N m ) n ) l s λ(n) ( N = v l S λ(n) (v,..., v m) ) l= l= Proof of Theorem: Proposition moment generating function for Ψ k = â k as a normalized Schur function. Using c k k (bounded), approximate the weights to get the MGF for â k. Asymptotics: S λ(n) (e y / n,..., e y k / n ) = k i= [ nyi exp + 5 ] y i + o() 5

symmetric The dense loop model Finite grid (here: vertical strip of width L and height ) tiled with squares, boundary triangales: y ζ ζ x The mean total current between points x and y: F x,y the average number of paths connecting the and passing between x and y. Similar observables in the critical percolation model [Smirnov, 009]. L 6

symmetric : the mean current Let λ L = ( L L,,...,, 0, 0) Define: [ u L (ζ, ζ ; z,..., z L ) = ( ) L χλ ı ln L+ (ζ, z,..., z L )χ λ L+ (ζ, z,..., z L ) ] χ λ L (z,..., z L )χ λ L+ (ζ, ζ, z,..., z L ) where χ ν is the character for the irreducible representation of highest weight ν of the symplectic group Sp(C). X (j) L = z j z j u L (ζ, ζ ; z,..., z L ) Y L = w w u L+(ζ, ζ ; z,..., z L, vq, w) v=w, Proposition (De Gier, Nienhuis, Ponsaing) Under certain assumptions the mean total current between two horizontally adjacent points is X (j) L = F (j,i),(j+,i), and Y is the mean total current between two vertically adjacent points in the strip of width L: Y (j) L = F (j,i),(j,i+). 7

symmetric : of the mean current Theorem As L we have and X (j) L zj =z; z i =, i j = i 4L (z z ) + o ( ) L Y L = i ( ) zi =, i=,...,l 4L (w w ) + o L Remark. When z =, F (j,i),(j+,i) is (trivially) identically zero. Remark. The fully homogeneous case when w = exp iπ/6, q = e πi/, then ( ) Y L = L + o. L Proof: same type of asymptotic methods and results hold for symplectic characters + some tricks with the multivariate formula. 8

symmetric Thank you 9