Science1 distinct publisher3 min readUpdated
A classical belief-propagation scheme reached the regime Advantage2 operates in and was often more accurate, Physics World reports. Budget annealer time only after a classical baseline.
The Scientist · Science desk

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Joseph Tindall and colleagues at the Flatiron Institute in New York have simulated the time evolution of Ising spin glasses with a new tensor network scheme that, in many cases, is more accurate than the latest quantum annealers running the same problem [1][2]. That is consequential because a team of quantum computing researchers had recently run the same spin glass dynamics on D-Wave's Advantage2 annealer and claimed classical computers could not match their results [4].
The benchmark is a sensible one. An Ising spin glass is a lattice of spins pointing in random directions, a disordered state produced by different nearest-neighbour interactions for different pairs of spins [6]. Its difficulty grows with system size, which is exactly why it gets used to compare classical and quantum machines [7]. The Flatiron result is not a single lucky lattice: according to Physics World it scales in both two and three dimensions [3], and Tindall's group reports the classical scheme doing as well as, and sometimes better than, the annealer [5].
The mechanics matter for anyone judging how durable this is. Tensor networks encode a system as tensors whose legs, or bond indices, are joined by contraction; widening those legs raises the bond dimension and lets the network capture correlations more accurately [8]. The team wrote tensor network representations of both the spin glass Hamiltonian and the wave function [9]. The standing obstacle to time evolution is that entanglement accumulates as the state evolves, so bond indices must widen, driving up cost and sometimes making the calculation impossible [10].
Their workaround is belief propagation message passing for the contraction: instead of accounting exactly for every contribution, each tensor receives a compact summary of what the rest of the network looks like from its perspective [11]. Tindall describes this as a mean field approximation on each tensor's environment, because the messages arriving from each neighbour are assumed to be independent [12]. That approximation is the whole trade, and it bought enough headroom to evolve the system far longer than conventional tensor network schemes, far enough to reach the regime the annealer operates in [13].
Two cautions. First, this is one group's method against one machine, and Physics World has previously reported that some physicists were unconvinced by D-Wave's quantum advantage claim in the first place [14]. Second, the account gives no runtimes, node counts or hardware costs for the classical side [15], so "a classical computer can do this" is not yet the same statement as "a classical computer can do this cheaply."
What is settled is narrower and still useful: the premise that no classical method could reach this regime no longer holds for this problem [16]. The practical reading for anyone buying annealer hours is that the classical baseline is a moving target and has to be re-measured, not cited from a vendor deck.
Worth watching: whether an independent group reproduces the two- and three-dimensional results, whether the independence assumption behind belief propagation [12] degrades at larger sizes or longer times, and whether cost figures appear that let the comparison be made per dollar rather than per accuracy point.
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Ranked by verification strength, evidence, and original report placement.
Researchers at the Flatiron Institute in New York City used a new tensor network scheme to simulate how Ising spin glasses evolve in time.
In many cases the Flatiron classical method is more accurate than the latest quantum annealers running the same problem.
Joseph Tindall and colleagues at the Flatiron Institute have shown that a classical scheme can do as well as, and sometimes better than, the annealer.
Tindall and colleagues built a tensor network representation of both the Ising spin glass Hamiltonian and the wave function.
The team used a belief propagation message passing approach to perform the contraction, in which each tensor receives a compact summary of what the rest of the network looks like from its perspective, rather than accounting for every single contribution exactly.
Tindall says the approach can be understood as a mean field approximation on each tensor's environment, since the pieces of information reaching a given tensor from each of its neighbours are assumed to be independent.
Evidence-backed comparisons of source perspectives and observed adoption signals. Read the methodology
Which Builder, Operator, and Investor concerns the observed source mix emphasized—not a truth score.
Evidence, demonstrated adoption, hype gap, incentives, and confidence are assessed independently, each on its own current evidence. How these are measured.
Peer-reviewed result, single-outlet account, no cost data
The underlying work is described in Science and the account gives specific, checkable structure: method (tensor network plus belief-propagation contraction), three lattice geometries, and direction of the correlator-error comparison against Advantage2. Evidence is capped by a single covering publisher, no quantified bond dimension or runtime, no vendor or third-party rebuttal, and the cubic-lattice case being only same-order rather than better.
Research-stage with open-source tooling, no deployment data
Adoption evidence is limited to a published benchmark comparison and the group's statement that it maintains an open-source tensor network simulator library plus planned extensions to finite temperature and the Hubbard model. There are no users, deployments, downloads or third-party reproductions reported, so adoption reads as early research uptake only.
Slightly ahead of the reported numbers
The framing that the classical method is 'more accurate than the latest quantum annealers' runs a little ahead of the body detail, where the advantage holds on two geometries but is only same-order on the cubic lattice and depends on bond dimension being large enough, with no cost or runtime accounting on the classical side. The gap is small because the article hedges in its own headline and reports the mixed cubic-lattice case rather than omitting it.
Contested advantage narrative with stakes on both sides
The material itself frames an ongoing classical-versus-quantum competition: an annealer-side team claimed classical computers could not match Advantage2, and the article notes D-Wave's advantage claims already face physicist skepticism, while the academic group publishing the rebuttal gains standing from displacing that claim. Both positions carry reputational stakes; no funding, commercial or sponsorship relationships are disclosed in the cluster, so the score reflects visible narrative stakes rather than documented financial conflicts.
Moderate: solid method detail, thin corroboration
Confidence is held to the middle band because the finding rests on one publisher's account of one peer-reviewed paper, with no independent replication, no counterparty response, no quantitative cost data, and adoption evidence limited to the originating group's own tooling and benchmarks. The specificity of the method and geometry-level results keeps it from being lower.
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1 article · August 21, 2026