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arXiv:2609.38044

A Tale of Two Walks: From Kac to KMP and Back

Qian Chen, Jingcheng Liu, Minglong Qin, Leonard J. Schulman, Fang Song, Penghui Yao, Mingnan Zhao

quant-phcs.DSmath.PRSubmitted Sep 29, 2026• Announced Sep 30, 2026• 0 citations• Revised Nov 2, 2026 (v2)
v1 · Sep 29, 2026v2 · Nov 2, 2026
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Abstract

We reveal an unexpected connection between two interacting particle systems: Kac's walk and the Kipnis-Marchioro-Presutti (KMP) process. We first establish a mixing-time analogue of Aldous's conjecture for the KMP process on general graphs: the mixing time of the $t$-particle process on any connected $d$-vertex graph is at most $O(\log d)$ times the corresponding single-particle mixing time, uniformly in $t$. As an application, we improve the mixing-time bound for coordinate hit-and-run on the $n$-dimensional standard simplex from $\widetilde{O}(n^3)$ [KV26] to $O(n\log n)$, while removing the dependence on the initial distribution. We then show that the twirling channel induced by the parallel Kac's walk on the symmetric subspace can be exactly encoded by a Markov chain on partitions, which naturally lifts to a parallel KMP chain on the complete graph. We prove that $O(\log d+\log(1/\varepsilon))$ repetitions of the parallel Kac's walk suffice to approximate Haar twirling on the symmetric subspace of $(\mathbb{C}^d)^{\otimes t}$ to error $\varepsilon$, uniformly in all $t$. Our main technical contribution is a new structural property of KMP-type dynamics: conditional product structure, which holds for both the standard KMP processes on general graphs and the parallel KMP processes on complete graphs. Conditioned on suitable auxiliary randomness, the evolution of the labeled KMP process factorizes into independent single-particle updates. Combining this structure with an exact coupling inspired by the analysis of Kac's walk, we remove the dependence on the number of particles from the mixing bounds for both unlabeled KMP models. This bypasses the $\log(π_{\min}^{-1})$ dependency from spectral-gap arguments, which is often prohibitively large for many-particle systems. Using this framework, we prove mixing bounds that are sharp up to logarithmic factors for both unlabeled KMP models.

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We reveal an unexpected connection between two interacting particle systems: Kac's walk and the Kipnis-Marchioro-Presutti (KMP) process. We first establish a mixing-time analogue of Aldous's conjecture for the KMP process on general graphs: the mixing time of the ttt-particle process on any connected ddd-vertex graph is at most O(log⁡d)O(\log d)O(logd) times the corresponding single-particle mixing time, uniformly in ttt. As an application, we improve the mixing-time bound for coordinate hit-and-run on the nnn-dimensional standard simplex from O~(n3)\widetilde{O}(n^3)O(n3) [KV26] to O(nlog⁡n)O(n\log n)O(nlogn), while removing the dependence on the initial distribution. We then show that the twirling channel induced by the parallel Kac's walk on the symmetric subspace can be exactly encoded by a Markov chain on partitions, which naturally lifts to a parallel KMP chain on the complete graph. We prove that O(log⁡d+log⁡(1/ε))O(\log d+\log(1/\varepsilon))O(logd+log(1/ε)) repetitions of the parallel Kac's walk suffice to approximate Haar twirling on the symmetric subspace of (Cd)⊗t(\mathbb{C}^d)^{\otimes t}(Cd)⊗t to error ε\varepsilonε, uniformly in all ttt.
Our main technical contribution is a new structural property of KMP-type dynamics: conditional product structure, which holds for both the standard KMP processes on general graphs and the parallel KMP processes on complete graphs. Conditioned on suitable auxiliary randomness, the evolution of the labeled KMP process factorizes into independent single-particle updates. Combining this structure with an exact coupling inspired by the analysis of Kac's walk, we remove the dependence on the number of particles from the mixing bounds for both unlabeled KMP models. This bypasses the log⁡(πmin⁡−1)\log(π_{\min}^{-1})log(πmin−1​) dependency from spectral-gap arguments, which is often prohibitively large for many-particle systems. Using this framework, we prove mixing bounds that are sharp up to logarithmic factors for both unlabeled KMP models.
Kac's walk is a classical local random walk whose action on a single real unit vector in dimension ddd mixes in total variation in Θ(dlog⁡d)Θ(d\log d)Θ(dlogd) sequential steps~\cite{PS17}. Lu, Qin, Song, Yao, and Zhao introduced a parallel version of Kac's walk that mixes a single quantum state in O(log⁡d)O(\log d)O(logd) rounds~\cite{LQSY+26}. After discretizing the randomness and replacing it by suitable pseudorandom primitives, this parallel walk gives rise to pseudorandom state scramblers, and was subsequently shown to yield pseudorandom unitaries~\cite{LQSY+25}. We study what happens when the parallel Kac's walk acts simultaneously on kkk orthonormal quantum states. We prove that, for any 1≤k<d1\leq k < d1≤k<d, after O ⁣((k+log⁡d)log⁡(d/ε))O\!\left((k+\log d)\log(d/\varepsilon)\right)O((k+logd)log(d/ε)) steps, the joint distribution of the kkk output states is ε\varepsilonε-close, in both Wasserstein and total variation distance, to that obtained by applying a common Haar-random unitary to the same inputs. This generalizes the dispersing property of the parallel Kac's walk from a single quantum state to multiple orthonormal quantum states. Equivalently, viewing an ordered collection of kkk orthonormal states as a point on the complex Stiefel manifold Vd,k={X∈Cd×k:X†X=Ik}V_{d,k}=\{X\in\mathbb C^{d\times k}:X^\dagger X=I_k\}Vd,k​={X∈Cd×k:X†X=Ik​}, we show that the parallel Kac's walk mixes rapidly on Vd,kV_{d,k}Vd,k​, with both Wasserstein and total variation mixing times bounded by O ⁣((k+log⁡d)log⁡(d/ε))O\!\left((k+\log d)\log(d/\varepsilon)\right)O((k+logd)log(d/ε)). This extends the Wasserstein mixing result of Pillai, Smith, and Vaikuntanathan for the standard Kac's walk on real Stiefel manifolds~\cite{PSV26}.
Most approximation algorithms for #P\mathit{P}P-complete problems (e.g., evaluating the partition function of a monomer-dimer or ferromagnetic Ising system) work by reduction to the problem of approximate sampling from a distribution $\ensuremath{\pi}$ over a large set S\mathcal{S}S. This problem is solved using the Markov chain Monte Carlo method: a sparse, reversible Markov chain PPP on S\mathcal{S}S with stationary distribution $\ensuremath{\pi}$ is run to near equilibrium. The running time of this random walk algorithm, the so-called mixing time of PPP, is $O({\ensuremath{\delta}}^{\ensuremath{-}1}\text{ }\text{log}\text{ }1∕{\ensuremath{\pi}}_{\ensuremath{\ast}})$ as shown by Aldous, where $\ensuremath{\delta}$ is the spectral gap of PPP and ${\ensuremath{\pi}}_{\ensuremath{\ast}}$ is the minimum value of $\ensuremath{\pi}$. A natural question is whether a speedup of this classical method to $O(\sqrt{{\ensuremath{\delta}}^{\ensuremath{-}1}}\text{ }\text{log}\text{ }1∕{\ensuremath{\pi}}_{\ensuremath{\ast}})$ is possible using quantum walks. We provide evidence for this possibility using quantum walks that decohere under repeated randomized measurements. We show that (i) decoherent quantum walks always mix, just like their classical counterparts, (ii) the mixing time is a robust quantity, essentially invariant under any smooth form of decoherence, and (iii) the mixing time of the decoherent quantum walk on a periodic lattice Znd{\mathbb{Z}}_{n}^{d}Znd​ is O(nd log d)O(nd\text{ }\text{log}\text{ }d)O(nd log d), which is indeed $O(\sqrt{{\ensuremath{\delta}}^{\ensuremath{-}1}}\text{ }\text{log}\text{ }1∕{\ensuremath{\pi}}_{\ensuremath{\ast}})$ and is asymptotically no worse than the diameter of Znd{\mathbb{Z}}_{n}^{d}Znd​ (the obvious lower bound) up to at most a logarithmic factor.
Continuous-time quantum walks on graphs is a generalization of continuous-time Markov chains on discrete structures. Moore and Russell proved that the continuous-time quantum walk on the nnn-cube is instantaneous exactly uniform mixing but has no average mixing property. On complete (circulant) graphs KnK_{n}Kn​, the continuous-time quantum walk is neither instantaneous (except for n=2,3,4n=2,3,4n=2,3,4) nor average uniform mixing (except for n=2n=2n=2). We explore two natural {\em group-theoretic} generalizations of the nnn-cube as a GGG-circulant and as a bunkbed $G \rtimes \Int_{2}$, where GGG is a finite group. Analyses of these classes suggest that the nnn-cube might be special in having instantaneous uniform mixing and that non-uniform average mixing is pervasive, i.e., no memoryless property for the average limiting distribution; an implication of these graphs having zero spectral gap. But on the bunkbeds, we note a memoryless property with respect to the two partitions. We also analyze average mixing on complete paths, where the spectral gaps are nonzero.
Quantum mixing is a category of processes of reaching a stationary state when starting from a single initial vertex via quantum walks. In this thesis, we introduce the quantum mixing processes based on the framework of controlled quantum walks in [DH17a]. We first discuss why Szegedy's walks are not well-suited for the quantum mixing processes. We then show that the controlled quantum walk is a suitable framework for achieving a quadratic speed-up in the quantum mixing processes, because of its relationship with interpolated walks [KMOR16] and the phase estimation algorithm [CEMM98]. Accordingly, we give two definitions of quantum mixing times via controlled quantum walks: instant quantum mixing time and average quantum mixing time. We later prove the bounds of these two quantum mixing times on complete graphs. We also prove the upper bound of the average quantum mixing times on cycle graphs. To have clearer views on the bounds of instant and average quantum mixing times, we then discuss and present the simulations of quantum mixing processes, with four types of graphs (complete graphs, cycle graphs, 2-dimensional tori and dumbbell graphs) as examples. The simulations include the quantum mixing processes with the same ~θ (an important parameter in the controlled quantum walk operator) as in [DH17a], and the suitable range of ~θ that achieves the quadratic speed-up for different types of graphs. Inspired by the quantum search algorithm via controlled quantum walks in [DH17a], we adapt this algorithm to a new algorithm of quantum mixing, which generates samples from the stationary distribution of the Markov chain, with its runtime upper bounded by the quantum hitting time, which is quadratically faster than the classical hitting process.
Quantum walks have been linked to acceleration in various information processing tasks, and proposed as a possible model for quantum-enhanced behavior in biological systems.These links and acceleration claims have been made with various levels of detail.Here we consider discrete-time quantum walks, and focus on the task of mixing, i.e., distributing the state over a graph.Previous papers have observed that the so-called coined quantum walks can accelerate mixing on certain graphs with respect to the optimal classical Markov chain.We here show that the same speedup can be attained with a classical process, if a similar classical coin is added.We establish a precise correspondence between the mixing performance of quantum walks and such "lifted walks" for all (finite) graphs, and thereby improve known bounds on quantum walk mixing time.We conclude that the advantage of quantum walks with respect to classical processes is not in the mixing speed of the optimal design.However, a notable quantum advantage might reside in the fact that the mixing speed obtained with suboptimal designs, due to for instance limited graph knowledge, appears to be generically faster.
This paper gives new observations on the mixing dynamics of a continuous-time quantum walk on circulants and their bunkbeds. These bunkbeds are defined through two standard graph operators: the join G + H and the Cartesian product G \cprod H of graphs G and H. Our results include the following: (i) The quantum walk is average uniform mixing on circulants with bounded eigenvalue multiplicity; this extends a known fact about the cycles C_{n}. (ii) Explicit analysis of the probability distribution of the quantum walk on the join of circulants; this explains why complete multipartite graphs are not average uniform mixing, using the fact K_{n} = K_{1} + K_{n-1} and K_{n,\ldots,n} = \overline{K}_{n} + \ldots + \overline{K}_{n}. (iii) The quantum walk on the Cartesian product of a mmm-vertex path P_{m} and a circulant G, namely, P_{m} \cprod G, is average uniform mixing if G is; this highlights a difference between circulants and the hypercubes Q_{n} = P_{2} \cprod Q_{n-1}. Our proofs employ purely elementary arguments based on the spectra of the graphs.