Scaling Quantum Optimization to the Thousand-Qubit Scale with Distributed Quantum Sampling
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Introduction to the show: ident: Quantum Radio. Generated commentary on the latest quantum physics and condensed matter papers.
Kai: I'm Kai, and with me are Mira and Lev, guest researcher.
Mira: Today's paper: "Scaling Quantum Optimization to the Thousand-Qubit Scale with Distributed Quantum Sampling".
Kai: The gist: Scaling quantum optimization to thousand-qubit scale with distributed quantum sampling demonstrates an executable path for deploying gate-based quantum sampling on thousand-variable constrained optimization problems on current hardware.
Mira: First, who's behind it and why it matters.
Title and authors: Kai: So this paper, "Scaling Quantum Optimization to the Thousand-Qubit Scale with Distributed Quantum Sampling," it’s tackling the Minimum Birkhoff Decomposition problem, which is basically finding a sparse weighted sum of matchings for things like network scheduling and energy trading.
Mira: Yeah, and the authors are Amana Liaqat, Ahmed Darwish, Stephen DiAdamo, Dan Holme, Kieran McDowall, Emre Sahin, Naeimeh Mohseni, Giorgio Cortiana and Corey O’Meara. They're aiming to show how we can scale a quantum-assisted decomposition method.
Kai: What I find interesting is that they aren't just looking at small problems; they are specifically focusing on scaling this up to the thousand-qubit scale using distributed quantum sampling, which sounds like a big step for current hardware limitations.
Mira: Exactly, and it suggests a practical pathway for deploying gate-based quantum sampling directly onto those large-scale constrained optimization problems we have right now.
The paper's summary: Kai: So the core of what they’re doing here is combining several techniques to make this decomposition scalable, starting with single-layer QAOA to supply diverse matching candidates and optimizing their weights classically.
Mira: And then they use spectral partitioning to cut down on circuit width and routing overhead by clustering affinity matrix eigenvectors. It sounds like a lot of clever engineering just to manage the complexity.
Kai: They also combine local samples using batched Cartesian products or pruned beam search, which they then clean up with a greedy repair pass to make sure the resulting matchings are actually feasible.
Mira: That's where their main innovation is, though, in how they handle feasibility; they use an E-FCFW framework that augments the candidate pool with both the deterministic maximum-weight matching and these diverse samples.
Kai: So when you put it all together on a large system like the one thousand three hundred fifty-four-node PEGASE bus test case, they’re showing that this pipeline works to find lower residual decomposition error compared to simulated annealing and uniform random sampling baselines <ref:2610.10772#pg1,the 1,354-node PEGASE bus test case>.
The paper's improvements: Kai: What really stands out in terms of what they suggest is the practical improvement in execution speed; spectral circuit packing manages to reduce hardware execution time by approximately a factor of three.
Mira: That’s a significant throughput gain because it allows them to run independent subproblems concurrently on multiple quantum processors using disjoint regions of the one hundred fifty-six-qubit Heron lattice.
Kai: And they found that even when they use a fifty-qubit partition bound, the convergence stays close to what you'd see with the unpartitioned hardware run, which shows that this partitioning isn't just slowing things down too much in this instance <ref:2610.10772#pg2>.
Mira: But there’s a caveat here, though; they flag that aggressively truncating those quantum correlations degrades the quality of the candidate matchings, so you have to balance size against fidelity.
Conclusion: Kai: So to wrap up, the authors are showing an executable workflow for solving thousand-variable constrained optimization problems on current hardware by using this distributed sampling approach.
Mira: It establishes a distributed workflow that combines spectral partitioning and spatial circuit packing with classical feasibility repair, which is what makes it possible for large-scale deployment.
Lev: From an error correction standpoint, the key thing here is how they manage those candidate pools; they use a greedy pruning pass over the candidate edge set E˜ to resolve intra-partition and boundary collisions without introducing unselected edges.
Kai: So, while they show this pipeline works for the one thousand three hundred fifty-four-node PEGASE bus test case, the next step in their research is tackling partitions of at least one hundred qubits and systematically varying their density.
Mira: And that points toward a need to control partition density alongside the size, making sure they keep enough connectivity to preserve useful quantum correlations while keeping the routing depth manageable.
Lev: I think that’s where the real hardware challenge lies; getting those circuits mapped onto physical qubits without losing that useful sampling behavior is a major hurdle.
Kai: So yeah, "Scaling Quantum Optimization to the Thousand-Qubit Scale with Distributed Quantum Sampling" gives us a concrete path forward for deploying these algorithms in real-world scenarios.
Amana Liaqat, Ahmed Darwish, Stephen DiAdamo, *Dan Holme*, Kieran McDowall, Emre Sahin, Naeimeh Mohseni, Giorgio Cortiana, *Corey O’Meara*
Qoro Quantum Ltd. · Qoro Quantum GmbH · National Quantum Computing Centre · Quantum Software Lab, The University of Edinburgh · Hartree Centre, STFC · E.ON Digital Technology GmbH
quant-ph, cs.ET, math.OC
Submitted: 2026-10-07
Updated: 2026-10-07
Code: https://github.com/QoroQuantum/divi
License: http://creativecommons.org/licenses/by/4.0/
Importance score: 92/100
The gist: The gist: Scaling quantum optimization to thousand-qubit scale with distributed quantum sampling demonstrates an executable path for deploying gate-based quantum sampling on thousand-variable
Key concepts
- Minimum Birkhoff Decomposition (MBD)
- This is a challenging optimization problem used in network scheduling and energy trading. It seeks the sparsest weighted sum of matchings required to reconstruct a target demand matrix by minimizing the number of constituent matchings needed.
- QAOA with Single-Layer Sampling
- Quantum Approximate Optimization Algorithm (QAOA) is used here to generate diverse candidate matchings. A single-layer approach is employed, where the quantum circuit helps supply many potential solutions, which are then optimized classically for their weights.
- Spatial Circuit Packing
- This technique manages hardware resources by executing independent subproblems concurrently on multiple QPUs using disjoint sections of a large lattice. This reduces overall execution time and improves QPU utilization by packing circuits efficiently.
- Feasibility Repair
- When combining samples, candidate matchings often violate constraints (collisions). Feasibility repair resolves these issues by sorting the candidates and greedily accepting edges only if both endpoints are currently unoccupied, ensuring the final set of edges is always a valid matching.
Terminology
Summary
The gist: Scaling quantum optimization to thousand-qubit scale with distributed quantum sampling demonstrates an executable path for deploying gate-based quantum sampling on thousand-variable constrained optimization problems on current hardware.
Problem Formulation
The Minimum Birkhoff Decomposition (MBD) seeks a sparse weighted sum of matchings and is a challenging optimization problem with applications in network scheduling and energy trading<ref:2610.10772#pg2>. The MBD problem is formulated as an l0-norm minimization over symmetric doubly substochastic matrices to minimize the number of constituent matchings needed to reconstruct the demand matrix D∗<ref:2610.10772#pg4>. The objective function for the Extended Fully-Corrective Frank–Wolfe (E-FCFW) framework is the scaled squared Frobenius norm distance between the target demand D∗ and the approximation matrix D<ref:2610.10772#pg5>.
Methodology
The pipeline combines several techniques to scale quantum-assisted decomposition:
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Single-layer (p = 1) QAOA is used to supply di-∗ stephen@qoroquantum.de verse matching candidates and optimize their weights classically<ref:2610.10772#pg4>. The QUBO Hamiltonian C(x) is defined using the ordered-pair convention, where the penalty λ = 0.2 discourages collisions<ref:2610.10772#pg4>.
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Spectral partitioning is employed to reduce circuit width and routing overhead by clustering affinity-matrix eigenvectors<ref:2610.10772#pg5>.
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Local samples are combined by batched Cartesian products or pruned beam search, followed by a greedy repair pass to enforce matching feasibility<ref:2610.10772#pg6>.
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Spatial circuit packing executes independent subproblems concurrently on multiple QPUs using disjoint regions of the 156-qubit Heron lattice<ref:2610.10772#pg10>.
Experimental Results
The study evaluated the pipeline on the 1,354-node PEGASE bus test case, which requires 1,710 qubits in an unpartitioned encoding<ref:2610.10772#pg4>. The best reported hardware result uses a 50-qubit partition bound<ref:2610.10772#pg4>. Impressive results showed that repaired QAOA samples achieve lower residual decomposition error than both simulated annealing and uniform random sampling baselines<ref:2610.10772#pg7>.
The spatial circuit packing reduces hardware execution time by approximately a factor of three<ref:2610.10772#pg4>. Partitioning at ps = 50 retains convergence close to the unpartitioned hardware run, supporting its use to reduce circuit size without losing the useful sampling behavior in this instance<ref:2610.10772#pg7>.
Conclusion and Future Work
The results establish an executable distributed workflow for a problem class whose classical difficulty makes it relevant to the search for quantum advantage<ref:2610.10772#pg4>. The ps = 50 results provide evidence for this requirement, as aggressive truncation of quantum correlations degrades candidate quality<ref:2610.10772#pg6>. Future work will extend this evaluation across the full benchmark suite with comprehensive runtime accounting and comparisons against strong classical solvers<ref:2610.10772#pg4>. The next step is to target partitions of at least 100 qubits and vary their density systematically<ref:2610.10772#pg4>. The initial results show that the method consistently reaches the target tolerance within 15 outer iterations and achieves substantially sparser decompositions than classical greedy baselines<ref:2610.10772#pg9>.
How it works
The E-FCFW algorithm augments the candidate pool at each iteration by combining the deterministic maximum-weight matching MMW with a sampling subroutine that generates d diverse candidate matchings Msample<ref:2610.10772#pg4>. To restore feasibility without introducing unselected edges, greedy repair sorts the candidate edge set E˜ by descending residual weight and accepts an edge if and only if both endpoints are currently unoccupied<ref:2610.10772#pg6>. This procedure runs in O(E˜ log E˜) time and guarantees matching feasibility<ref:2610.10772#pg6>.
Partitioning and Packing Layouts
The PEGASE-1354 layout shows 41 subgraphs with an edge bound ps = 50, where colors distinguish neighboring partitions<ref:2610.10772#pg9>. Spatial circuit packing places four independent circuits on one Heron processor to be run simultaneously within the same QPU run for a higher ratio of QPU utilization<ref:2610.10772#pg10>. This reduces dispatch rounds by up to 4× in the reported configurations, and the observed PEGASE execution-time reduction is approximately 3×<ref:2610.10772#pg10>.
MPS Mirror Diagnostic
The MPS mirror diagnostic assesses truncation error using Maestro’s native mirror fidelity check, which implements a deterministic compute-uncompute diagnostic related to the mirror-circuit principle<ref:2610.10772#pg10>. Higher bond dimensions improve both mirror fidelity and final cost in Fig. 2(b)<ref:2610.10772#pg6>. Subgraphs that contain dense loop structures or clustered degree-3 junctions produce tightly coupled line graphs that require extensive SWAP routing when mapped back onto Heron’s physical qubits<ref:2610.10772#pg6>. The next scaling step should control partition density alongside size, retaining enough connectivity to preserve useful quantum correlations while keeping routed depth manageable<ref:2610.10772#pg4>.
Deployment on PEGASE-1354
The PEGASE-1354 transmission graph would require 1,710 qubits under an unpartitioned edge encoding<ref:2610.10772#pg4>. Spectral partitioning at ps = 50 instead produces 41 subgraphs for distributed execution<ref:2610.10772#pg9>. The partition bound ps counts edges (qubits)<ref:2610.10772#pg9>. Logical two-qubit depth reflects the maximum degree of interacting edge pairs, which governs transpiled depth on heavy-hex hardware<ref:2610.10772#pg6>. The partition bound ps counts edges (qubits)<ref:2610.10772#pg9>.
Stitching and Feasibility Repair
Raw stitched candidates frequently violate matching feasibility due to two distinct sources of collisions: intra-partition collisions and boundary collisions<ref:2610.10772#pg6>. Feasibility repair resolves these conflicts via a greedy pruning pass over the candidate edge set E˜, which sorts edges by current residual weights and accepts an edge if both endpoints are currently unoccupied<ref:2610.10772#pg6>. Unselected edges (xj = 0) are never introduced, ensuring repair acts strictly as a conflict-resolution filter on the quantum candidate rather than an augmenting heuristic<ref:2610.10772#pg6>.
Classical Update and Hardware Execution
E-FCFW updates the nonnegative weights subject to its cardinality bound and removes zero-weight matchings<ref:2610.10772#pg4>. The loop stops at the target error, a relative improvement plateau, or the iteration limit<ref:2610.10772#pg9>. Algorithm 1 gives the full workflow<ref:2610.10772#pg9>. Qoro’s scheduler orders circuits by size and packs them into execution rounds with a shared shot count<ref:2610.10772#pg10>. The observed PEGASE execution-time reduction is approximately 3×<ref:2610.10772#pg10>.
Parameter Calibration and Sampling Budgets
Offline training uses small prototypes with similar topology, degree distribution, and edge-weight encoding to the target family<ref:2610.10772#pg9>. Angles are calibrated offline and transferred across related subgraphs instead of being optimized at each E-FCFW iteration<ref:2610.10772#pg4>. For the PEGASE bus test case, the calibration landscape is evaluated on a representative 49-qubit partition with Maestro at bond dimension 128<ref:2610.10772#pg10>. The marked minimum near (γ0, β0) = (2.49, 0.16) supplies fixed execution angles for the PEGASE-1354 transmission graph experiments<ref:2610.
Improvements for AI systems
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The improved system can perform large-scale network scheduling and energy trading by solving Minimum Birkhoff Decomposition (MBD) problems with sparse approximations, as demonstrated by
retaining 50 to 75 matchings
in preliminary work on MBD track up to 4,096 variables. -
The system will achieve significant throughput speedups in hardware execution because
spatial circuit packing reduces hardware execution time by approximately a factor of three,
allowing independent subproblems to be executed concurrently on quantum processors. -
The AI can maintain high candidate quality during distributed optimization by utilizing
repaired QAOA samples
which achievelower residual decomposition error than both simulated annealing and uniform random sampling baselines.
-
The system will scale beyond the width of a single processor by employing a workflow that combines
spectral partitioning, spatial circuit packing, and classical feasibility repair,
providing anexecutable path for deploying gate-based quantum sampling on thousand-variable constrained optimization problems on current hardware.
Abstract
The Minimum Birkhoff Decomposition (MBD) seeks a sparse weighted sum of matchings and is a challenging optimization problem with applications in network scheduling and energy trading. We scale a quantum-assisted decomposition method by combining single-layer QAOA sampling with Extended Fully-Corrective Frank-Wolfe (E-FCFW) optimization, spectral graph partitioning, and greedy feasibility repair. We demonstrate the pipeline on the 1,354-node PEGASE bus test case (representing a 1,354-bus transmission grid with 1,710 transmission lines), whose 1,710 edges define a native 1,710-variable matching optimization problem requiring 1,710 qubits in the unpartitioned encoding. Partitioning enables distributed execution on IBM superconducting quantum processors. The best reported hardware result uses a 50-qubit partition bound, while reducing partitions to 20 qubits degrades convergence in the partition-size comparison. Larger partitions are more demanding for matrix product state (MPS) simulation, and bond-dimension tests show that truncating quantum correlations reduces candidate quality. The results therefore motivate retaining a substantive quantum sampling task within each partition as the overall problem scales. On the PEGASE-1354 benchmark, repaired QAOA samples achieve lower residual decomposition error than both simulated annealing and uniform random sampling baselines, while spatial circuit packing reduces hardware execution time by approximately a factor of three. These results demonstrate that combining spectral partitioning, spatial circuit packing, and classical feasibility repair provides an executable path for deploying gate-based quantum sampling on thousand-variable constrained optimization problems on current hardware.
Sources
- Boosting Sparsity in Graph Decompositions with QAOA Sampling
- Quantum Supremacy through the Quantum Approximate Optimization Algorithm
- A Multilevel Approach For Solving Large-Scale QUBO Problems With Noisy Hybrid Quantum Approximate Optimization
- Maestro: Intelligent Execution for Quantum Circuit Simulation
- Fast, accurate, high-resolution simulation of large-scale Fermi-Hubbard models on a digital quantum processor
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