Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Fisher Curvature Scaling at Critical Points: An Exact Information-Geometric Exponent from Periodic Boundary Conditions

Maxim Zhuravlev

Published Mar 10, 2026• 0 citations
Publisher

Abstract

Proposes a new critical exponent d_R for Fisher curvature scaling and proves d_R = (dnu + 2eta)/(d*nu + eta). Validated on 2D Ising (exact TM L=3-9, MCMC L=10-24), 3D Ising, 2D Potts q=3,4. Published on arXiv as 2603.07651.
DOI
10.5281/zenodo.18942480

Related papers

Fisher Curvature Scaling at Critical Points: An Exact Information-Geometric Exponent

Maxim Zhuravlev

Introduces a novel scaling exponent d_R = (d*nu + 2*eta)/(d*nu + eta) for scalar curvature on per-bond Fisher manifolds at criticality. Confirmed to 4 significant figures for 2D Ising (d_R = 10/9). Extended predictions for 3D Ising, Potts q=3, and Potts q=4 validated numerically.

•Feb 27, 2026•0 citations

The Scaling Closure Theorem: Fisher Curvature Exponents from CFT Structure at Statistical Critical Points

Maxim Zhuravlev

Proves the Scaling Closure Theorem: d_R = (d*nu + 2*eta)/(d*nu + eta) from five structural assumptions (A1-A5) about the microscopic Fisher manifold at criticality. A1 (Ricci decomposition) and A2 (Z_2 fusion) and A4 (eigenvalue anisotropy) are proved as theorems. A3 (diagonal block cancellation) at 99.95%+ and A5 (triangle non-cancellation) at 99.9%+. Universality verified across 8 CFT classes including 2D Ising, Potts q=3,4, 3D Ising/XY/Heisenberg, BKT, and Gaussian. Companion proof paper for the Prediction Letter (arXiv:2603.07651).

•Mar 10, 2026•0 citations

Fisher Curvature Scaling at Critical Points: An Exact Information-Geometric Exponent from Periodic Boundary Conditions

Maxim Zhuravlev

We study the scalar curvature of the Fisher information metric on the microscopic coupling-parameter manifold of lattice spin models at criticality. For a $d$-dimensional lattice with periodic boundary conditions and $n = L^d$ sites, the Fisher manifold has $m = d \cdot n$ dimensions (one per bond), and we find $|\mathcal{R}(J_c)| \sim n^{d_R}$ with $d_R = (dν+ 2η)/(dν+ η)$, where $ν$ and $η$ are the correlation-length and anomalous-dimension critical exponents. For 2D Ising ($ν= 1$, $η= 1/4$), this predicts $d_R = 10/9$, confirmed by exact transfer-matrix computations ($L = 6$--$9$: $d_R = 1.1115 \pm 0.0002$) and multi-seed MCMC through $L = 24$. For 3D Ising ($ν= 0.630$, $η= 0.0363$), the prediction $d_R = 1.019$ is consistent with MCMC on $L^3$ tori up to $L = 10$ (power-law fit: $d_R = 1.040$). For 2D Potts $q = 3$ (predicted $33/29 \approx 1.138$), FFT-MCMC through $L = 40$ shows $d_\mathrm{eff}$ oscillating non-monotonically around $\sim 1.20$, consistent with $O(1/(\ln L)^2)$ logarithmic corrections. For $q = 4$ (predicted $22/19$), effective exponents oscillate with strong logarithmic corrections. The Ricci decomposition identity $R_3 = -R_1/2$, $R_4 = -R_2/2$ holds to 5--6 digits for all models. This exponent is distinct from Ruppeiner thermodynamic curvature and reflects the collective geometry of the growing Fisher manifold. We provide falsification criteria and predictions for additional universality classes.

arXiv:2603.07651•Mar 8, 2026•0 citations

Exact Asymptotics of the Fisher Information Metric at Statistical Critical Points

Maxim Zhuravlev

Rigorous asymptotic analysis of the Fisher information metric near criticality. Derives the d_R scaling exponent analytically via Brillouin zone mode decomposition and proves convergence properties.

•Feb 27, 2026•0 citations

Rigorous Asymptotics of Fisher Curvature Scaling on Cylindrical Ising Lattices

Maxim Zhuravlev

SUPERSEDED: Central theorem (c_2 ~ L^{2/9}) FALSIFIED by ultra-fine transfer-matrix data (Session 51). Actual behavior: c_2 grows sub-logarithmically (~ln(L)), not as a power law. The d_R exponent itself remains valid (see Prediction Letter arXiv:2603.07651). Record retained for transparency. Negative-result rewrite available separately.

•Mar 10, 2026•0 citations

Finite-size scaling and corrections in the Ising model with Brascamp-Kunz boundary conditions

Wolfhard Janke E, Ralph Kenna B

The Ising model in two dimensions with the special boundary conditions of Brascamp and Kunz is analyzed. Leading and subdominant scaling behavior of the Fisher zeros are determined exactly. The exact finite-size scaling, with corrections, of the specific heat is determined both at critical and effective critical (pseudocritical) points. The shift exponents associated with the scaling of these effective critical points are not the same as the inverse correlation length critical exponent. All corrections to scaling are analytic.

arXiv:cond-mat/0103332•Physical review. B, Condensed matter•Jan 24, 2002•66 citations
Proves the Scaling Closure Theorem: d_R = (d*nu + 2*eta)/(d*nu + eta) from five structural assumptions (A1-A5) about the microscopic Fisher manifold at criticality. A1 (Ricci decomposition) and A2 (Z_2 fusion) and A4 (eigenvalue anisotropy) are proved as theorems. A3 (diagonal block cancellation) at 99.95%+ and A5 (triangle non-cancellation) at 99.9%+. Universality verified across 8 CFT classes including 2D Ising, Potts q=3,4, 3D Ising/XY/Heisenberg, BKT, and Gaussian. Companion proof paper for the Prediction Letter (arXiv:2603.07651).
We study the scalar curvature of the Fisher information metric on the microscopic coupling-parameter manifold of lattice spin models at criticality. For a ddd-dimensional lattice with periodic boundary conditions and n=Ldn = L^dn=Ld sites, the Fisher manifold has m=d⋅nm = d \cdot nm=d⋅n dimensions (one per bond), and we find ∣R(Jc)∣∼ndR|\mathcal{R}(J_c)| \sim n^{d_R}∣R(Jc​)∣∼ndR​ with dR=(dν+2η)/(dν+η)d_R = (dν+ 2η)/(dν+ η)dR​=(dν+2η)/(dν+η), where ννν and ηηη are the correlation-length and anomalous-dimension critical exponents. For 2D Ising (ν=1ν= 1ν=1, η=1/4η= 1/4η=1/4), this predicts dR=10/9d_R = 10/9dR​=10/9, confirmed by exact transfer-matrix computations (L=6L = 6L=6--999: dR=1.1115±0.0002d_R = 1.1115 \pm 0.0002dR​=1.1115±0.0002) and multi-seed MCMC through L=24L = 24L=24. For 3D Ising (ν=0.630ν= 0.630ν=0.630, η=0.0363η= 0.0363η=0.0363), the prediction dR=1.019d_R = 1.019dR​=1.019 is consistent with MCMC on L3L^3L3 tori up to L=10L = 10L=10 (power-law fit: dR=1.040d_R = 1.040dR​=1.040). For 2D Potts q=3q = 3q=3 (predicted 33/29≈1.13833/29 \approx 1.13833/29≈1.138), FFT-MCMC through L=40L = 40L=40 shows deffd_\mathrm{eff}deff​ oscillating non-monotonically around ∼1.20\sim 1.20∼1.20, consistent with O(1/(ln⁡L)2)O(1/(\ln L)^2)O(1/(lnL)2) logarithmic corrections. For q=4q = 4q=4 (predicted 22/1922/1922/19), effective exponents oscillate with strong logarithmic corrections. The Ricci decomposition identity R3=−R1/2R_3 = -R_1/2R3​=−R1​/2, R4=−R2/2R_4 = -R_2/2R4​=−R2​/2 holds to 5--6 digits for all models. This exponent is distinct from Ruppeiner thermodynamic curvature and reflects the collective geometry of the growing Fisher manifold. We provide falsification criteria and predictions for additional universality classes.
The Ising model in two dimensions with the special boundary conditions of Brascamp and Kunz is analyzed. Leading and subdominant scaling behavior of the Fisher zeros are determined exactly. The exact finite-size scaling, with corrections, of the specific heat is determined both at critical and effective critical (pseudocritical) points. The shift exponents associated with the scaling of these effective critical points are not the same as the inverse correlation length critical exponent. All corrections to scaling are analytic.