Motivation
A directed polymer in a random environment is a random up-right lattice path whose law is reweighted by random site weights. Its free energy, the logarithm of the partition function, is believed to belong to the Kardar–Parisi–Zhang (KPZ) universality class: for a path of length of order N, the free energy fluctuates on the scale N1/3 and the path wanders on the scale N2/3. For zero-temperature analogues (last-passage percolation with exponential or geometric weights) these exponents were established through exact formulas from random matrix theory (Johansson 2000) and later through a probabilistic coupling argument based on the Burke property of queues (Balázs–Cator–Seppäläinen 2006).
For directed polymers at positive temperature no model with the KPZ exponents was known until Seppäläinen (arXiv:0911.2446, Ann. Probab. 2012) introduced the log-gamma polymer, whose weights are reciprocals of gamma variables, and proved that its free energy has variance of order N2/3 in the characteristic direction. The model has since become a basic exactly solvable polymer:
- 2009: Seppäläinen, the log-gamma polymer with boundary conditions; variance bounds of order N2/3 and path fluctuation exponent 2/3, by a Burke property and a variance identity.
- 2013: Borodin, Corwin and Remenik, Fredholm determinant formula and Tracy–Widom GUE limit of the free energy, for a range of parameters.
- 2014: Corwin, O'Connell, Seppäläinen and Zygouras, Tropical combinatorics and Whittaker functions, an exact formula for the law of the partition function via the geometric RSK correspondence.
The present mission formalizes the 2009 variance theorem, which needs neither of the later exact formulas.
Setting
Sites are Z+2={0,1,2,…}2 and N={1,2,…}. A weight configuration assigns a positive number Yi,j to each site. On the axes, Ui,0=Yi,0 and V0,j=Y0,j for i,j∈N are the boundary weights, and Yi,j, i,j∈N, are the bulk weights.
An up-right path from (0,0) to (m,n) is a sequence x0=(0,0),x1,…,xm+n=(m,n) whose steps are (1,0) or (0,1). The partition function is
Zm,n=x∑k=1∏m+nYxk,
the weight of the origin excluded, Z0,0=1. The quenched polymer measure gives the path x probability Qm,nω(x)=Zm,n−1∏k=1m+nYxk, and the annealed measure is its average Pm,n=EQm,nω over the environment. The exit points ξx and ξy are the numbers of initial steps the path takes along the x-axis and along the y-axis.
Assumption (2.4). Fix 0<θ<μ. The weights {Ui,0,V0,j,Yi,j:i,j∈N} are independent with
Ui,0−1∼Gamma(θ,1),V0,j−1∼Gamma(μ−θ,1),Yi,j−1∼Gamma(μ,1).
Let Ψ0=(logΓ)′ and Ψ1=Ψ0′ be the digamma and trigamma functions. The characteristic direction is (Ψ1(μ−θ),Ψ1(θ)). For a real scaling parameter N and a constant γ, the endpoint satisfies
∣m−NΨ1(μ−θ)∣≤γN2/3and∣n−NΨ1(θ)∣≤γN2/3(2.6).
Formalization targets
Goal: Theorem 2.1
There are constants 0<C1,C2<∞ and N0, depending on θ,μ,γ, such that under (2.4) and (2.6)
Var(logZm,n)≤C2N2/3(N≥1),C1N2/3≤Var(logZm,n)(N≥N0).
Milestones
The upper bound runs through the Burke property and the variance identity:
- Lemma 3.1 (monotonicity of the recursion (3.2)), Lemma 3.2 (gamma reversibility), Theorem 3.3 (Burke property), the mean (2.5), ElogZm,n=−mΨ0(θ)−nΨ0(μ−θ).
- Theorem 3.7, the variance identity
Var[logZm,n]=nΨ1(μ−θ)−mΨ1(θ)+2Em,n[i=1∑ξxL(θ,Yi,0−1)].
- Lemma 4.1 (variance comparison in θ), Lemma 4.2, the exit-point bound (4.32) E(ξx)≤CN2/3, Lemma 4.3 (quenched exit-point tails).
The lower bound runs through partition-function comparisons:
- Lemma 5.1, Lemma 5.4 (coupling), Lemma 5.5(i), Proposition 5.3 (limδ↘0limNP{1≤ξx≤δN2/3}=0), Corollary 5.6 (Var≥cN2/3, c>0).
Significance
The result. Theorem 2.1 was the first proof of the KPZ fluctuation exponent 1/3 for a directed polymer at positive temperature. Its upper bound also yields a strong law of large numbers for N−1logZm,n (2.7) and, with Theorem 3.3, a central limit theorem off the characteristic direction (Corollary 2.2). The exit-point estimates of Sections 4 and 5 give the path fluctuation exponent 2/3 (Theorem 2.3) and are reused for the polymer without boundaries and the point-to-line polymer (Theorems 2.4–2.6).
Formalizing it. The theorem has been proved since 2009; no formal proof of it in a proof assistant is known. A formalization checks a proof with many interacting estimates and two corrected slips (below). The definitions made here (the lattice-path partition function, the inverse-gamma environment, the recursion (3.2), exit points, quenched and annealed measures) are the base for later missions on Theorems 2.3–2.7 of the same paper. Lemma 3.2 contains a gamma-distribution characterization (Lukacs' theorem) of independent interest.
Difficulty
The obvious route to a variance bound, a martingale decomposition of logZm,n over the mn independent weights, gives only Var=O(m+n), i.e. order N; it cannot see the cancellation that produces N2/3. The order N2/3 is specific to the characteristic direction: off it, logZm,n satisfies a central limit theorem with variance of larger order (Corollary 2.2), so any argument must use the exact relation between the boundary parameters θ,μ−θ and the endpoint (m,n). The upper bound requires controlling the annealed exit point E(ξx) at the scale N2/3, with tail estimates whose constants are uniform in the parameters. The lower bound is a separate statement: the path must not exit an axis at distance o(N2/3) from the origin with non-vanishing probability, which no upper-bound estimate implies.
Formalization scope
Source: arXiv:0911.2446v4 (26 Aug 2015, revised version); its printed page numbers equal the PDF's. All declarations are in the namespace LogGammaPolymer.Variance.
- Sites are
ℕ × ℕ; a path is a step sequence with a fixed number of east steps; Z is a finite sum over these paths with the starting weight excluded. The environment Env θ μ P bundles one weight family Y : ℕ × ℕ → Ω → ℝ, measurability, mutual independence of every weight off the origin, and the three laws as images under y↦y−1 equal to Mathlib's gammaMeasure (shape, rate 1). Positivity of the weights is not assumed pointwise in the probabilistic statements; it holds almost surely. The deterministic lemmas (3.1, 5.1, 5.4) are stated for every weight function positive off the origin.
- N is real and N2/3 is a real power. Variances use Mathlib's
variance, and every upper bound or identity also asserts logZm,n∈L2 (or integrability of the averaged quantity), so that the junk value 0 of variance and of the Bochner integral cannot satisfy it.
- Constants come after the parameters (θ,μ,γ) and before the probability space (universe
Type), the environment, N and (m,n). Upper limits in N are stated as "for every η>0 there is N0 with the bound +η for N≥N0". The compact-set uniformity of Lemmas 4.1, 4.3 and (4.32) is formalized. The remark after Theorem 2.1 on uniform constants is not.
- Corrected slips. (i) Theorem 2.1 prints the lower bound for all N≥1. It fails at N=1, θ=1, μ=2, γ=2 with (m,n)=(0,0), where the variance is 0. The lower bound is stated for N≥N0, which is what Corollary 5.6 proves. (ii) The "only if" of Lemma 3.2 fails for the constants U=V=1, Y=1/2. The hypothesis "U is not a.s. constant" is added. (iii) Corollary 5.6 states c>0 explicitly.
- Theorem 3.3 is stated for down-right paths that coincide with the axes outside a finite portion. The paper reduces the general case to these.
- Not included: Lemma 3.5 (reversal), Proposition 3.4, Lemma 5.5(ii).
A formalization in which Z includes the origin's weight, the laws are not exactly the inverse gammas with shapes θ,μ−θ,μ and rate 1, independence is dropped, C1=0 is allowed, or the constants depend on the environment or on N does not state Theorem 2.1.
Needed infrastructure: gamma–beta algebra and a Lukacs-type characterization, independence of finite families built by the recursion (3.2), differentiation of expectations in the shape parameter, and moment bounds for sums of i.i.d. variables. All of these are reusable beyond this mission. Proofs of any milestone, and of supporting lemmas such as (3.3)–(3.4), are welcome.
Selected references
- T. Seppäläinen, Scaling for a one-dimensional directed polymer with boundary conditions, Ann. Probab. 40 (2012) 19–73; revised version arXiv:0911.2446v4. https://arxiv.org/abs/0911.2446
- K. Johansson, Shape fluctuations and random matrices, Comm. Math. Phys. 209 (2000) 437–476. https://arxiv.org/abs/math/9903134
- M. Balázs, E. Cator, T. Seppäläinen, Cube root fluctuations for the corner growth model associated to the exclusion process, Electron. J. Probab. 11 (2006) 1094–1132. https://arxiv.org/abs/math/0603306
- I. Corwin, N. O'Connell, T. Seppäläinen, N. Zygouras, Tropical combinatorics and Whittaker functions, Duke Math. J. 163 (2014) 513–563. https://arxiv.org/abs/1110.3489
- A. Borodin, I. Corwin, D. Remenik, Log-gamma polymer free energy fluctuations via a Fredholm determinant identity, Comm. Math. Phys. 324 (2013) 215–232. https://arxiv.org/abs/1206.4573
- E. Lukacs, A characterization of the gamma distribution, Ann. Math. Statist. 26 (1955) 319–324. https://doi.org/10.1214/aoms/1177728549