otherPublished: August 17, 2026

Spectral Gaps of Hit-and-Run and Coordinate Hit-and-Run

By Yunbum Kook, Santosh S. Vempala

Research TL;DR

"Proves Hit-and-Run's spectral gap is Ω(1/(n²C_PI)), improving mixing bounds to nearly quadratic dimension dependence via Poincaré/KLS constants, using duality and functional inequalities instead of conductance."

Abstract

For any convex body $\mathcal{K}\subset\mathbb{R}^{n}$ containing a unit ball, the spectral gap of Hit-and-Run is $Ω(1/(n^2 C_{\mathsf{PI}}))$, where $C_{\mathsf{PI}}$ is the Poincaré constant of the uniform distribution $π$ over $\mathcal{K}$. This implies that Hit-and-Run converges to a distribution within $χ^2$-divergence $\varepsilon$ of the uniform distribution $π$ in $O(n^2 C_{\mathsf{PI}}\log(M/\varepsilon))$ steps from any starting distribution $π_0$ with $M=χ^2(π_{0}\,\|\,π)$, thus refining the known bound of $O(n^2 R^2 \log(M/\varepsilon))$ by Lovász and Vempala (2004) in terms of the outer radius $R$; for nearly isotropic bodies, together with progress on the KLS conjecture, the complexity is $O(n^2\log n\log(M/\varepsilon))$, improving the dimension dependence from cubic to nearly quadratic while maintaining logarithmic dependence on the initial distance. It was an open problem to connect the convergence of Hit-and-Run to Poincaré/KLS constants as was done for the Ball walk by Kannan, Lovász and Simonovits (1997). Unlike Hit-and-Run, the Ball walk has an unavoidable linear dependence on (a stronger notion) of the initial warmness. We directly bound the spectral gap of the Hit-and-Run Markov chain by connecting it to functional isoperimetric constants, inspired by the recent analysis of In-and-Out. Rewriting the spectral gap in terms of dual certificates leads to the Babuška--Aziz constant studied in the analysis of PDEs; it is asymptotically bounded by the improved Poincaré constant, which we show can be bounded in terms of the usual Poincaré constant. The proof is based on duality and calculus, unlike known proofs of convergence for Hit-and-Run which are based on bounding the conductance. The same technique can be applied to Coordinate Hit-and-Run, resulting in a much improved mixing time of $O(n^3C_{\mathsf{PI}}\log(M/\varepsilon))$.

Technical Analysis & Implementation

Overview§

This paper addresses a long-standing open problem in Markov chain Monte Carlo (MCMC) analysis: connecting the convergence rate of Hit-and-Run (H&R) to the Poincaré constant (or KLS constant) of the target distribution. For any convex body $\mathcal{K} \subset \mathbb{R}^n$ containing a unit ball, the authors prove that the spectral gap of H&R is $\Omega(1/(n^2 C_{\mathsf{PI}}))$, where $C_{\mathsf{PI}}$ is the Poincaré constant of the uniform distribution $\pi$ on $\mathcal{K}$. This refines the earlier $O(n^2 R^2 \log(M/\varepsilon))$ bound of Lovász and Vempala (2004) by replacing the outer radius $R$ with the Poincaré constant. For nearly isotropic bodies, the result combines with KLS breakthrough to yield $O(n^2 \log n \log(M/\varepsilon))$ mixing time, improving the dimension dependence from cubic to nearly quadratic.

Main Results§

  • Spectral gap lower bound: $\mathrm{gap}(\mathrm{H\&R}) \ge \frac{c}{n^2 C_{\mathsf{PI}}}$ for an absolute constant $c>0$.
  • Mixing time bound: From any starting distribution $\pi_0$ with $M = \chi^2(\pi_0 \| \pi)$, the $\chi^2$-divergence to $\pi$ drops below $\varepsilon$ in $O(n^2 C_{\mathsf{PI}} \log(M/\varepsilon))$ steps.
  • Coordinate Hit-and-Run (CH&R): Similar technique yields mixing time $O(n^3 C_{\mathsf{PI}} \log(M/\varepsilon))$.

Unlike the Ball walk, H&R's mixing time does not degrade with the initial warmness constant, making it a more robust algorithm.

Proof Technique§

The key innovation is a dual formulation of the spectral gap. Let $\mathcal{P}$ be the H&R transition kernel and $\mathcal{L} = I - \mathcal{P}$ the Laplacian. The spectral gap is $$ \mathrm{gap} = \inf_{f \neq 0} \frac{\langle f, \mathcal{L} f \rangle_{\pi}}{\mathrm{Var}_\pi(f)}. $$ The authors rewrite this as a minimization over functions and then pass to the dual to obtain an equivalent constant related to the Babuška–Aziz constant from PDE analysis. This constant measures the stability of the divergence operator on the domain and is asymptotically bounded by the improved Poincaré constant $C_{\mathsf{PI}}^+$, itself bounded by $C_{\mathsf{PI}}$ up to constants.

The proof avoids the usual conductance-based arguments (e.g., Lovász–Vempala) and instead uses calculus of variations and duality, inspired by the recent analysis of the In-and-Out Markov chain.

Implications§

  • Bridges the gap between H&R and Ball walk analyses; now both are governed by KLS/Poincaré constants.
  • For near-isotropic convex bodies, the mixing time is $\tilde{O}(n^2)$, which is essentially optimal in the exponent (modulo constant factors).
  • The technique may extend to other hit-and-run variants and to sampling from non-uniform log-concave distributions.

Code Snippet (Illustrative Hit-and-Run in Python)§

import numpy as np

def hit_and_run(log_density, n_samples, x0, step=1.0):
    samples = []
    x = x0.copy()
    for _ in range(n_samples):
        # Random direction uniformly on the sphere
        direction = np.random.randn(x.shape[0])
        direction /= np.linalg.norm(direction)
        # Find interval along line for which density is above a threshold (here: uniform on convex body)
        # For generic log-concave, use slice sampling or projection
        t_vals = np.linspace(-10, 10, 1000)
        import scipy.stats as stats
        # Example: uniform on a ball: accept if inside unit ball
        def in_body(x): return np.linalg.norm(x) <= 1.0
        line = x + t_vals[:, None] * direction[None, :]
        valid = [t for t, y in zip(t_vals, line) if in_body(y)]
        if len(valid) == 0:
            continue
        # Sample uniformly along the chord
        t = np.random.uniform(valid[0], valid[-1])
        x = x + t * direction
        samples.append(x.copy())
    return np.array(samples)

This snippet illustrates the core H&R step; the paper's analysis applies to this exact update for uniform distributions over convex bodies.

Conclusion§

By delivering a direct spectral gap lower bound tied to Poincaré constants, this paper resolves the open question and provides a powerful new analytic framework for MCMC convergence, with implications beyond H&R to coordinate samplers and functional inequalities.

Originally published on llmdb.app

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