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arXiv:2610.32968

Distributed Quantum-Centric Supercomputing with Multi-Layered Generative Learning for Intermolecular Interactions

Chayan Patra, Prayas Ghosh, Adwait Patkhedkar, Rahul Maitra

quant-phSubmitted Oct 23, 2026• Announced Oct 26, 2026• 0 citations
arXivHTMLPDF

Abstract

Quantum-centric supercomputing (QCSC) approaches, such as sample-based quantum diagonalization (SQD), combine quantum processors with high-performance computers (HPC), offering a promising route toward solving challenging electronic structure problems. However, implementation of QCSC approaches to large active space calculations is constrained by the associated number of qubits, deep quantum circuits, sampling cost, and large-scale Hamiltonian diagonalization. To overcome these limitations, we introduce a distributed QCSC framework that decomposes complex molecular problems into parallel sub-problems requiring fewer qubits, shallower circuits, and reduced shot budgets. A physically motivated, two-step aggregation scheme then reconstructs the global solution: first, a computational bit assignment strategy optimizes a cost function to appropriately map local bit indices to global ones, yielding a mapped tensor product state (MTPS); second, an inter-fragment correlation recovery module restores missing cross-fragment interactions. Herein, we employ a multi-layered generative machine learning architecture, starting with utilizing the recently proposed physics-informed generative SQD (PIGen-SQD) as a distributed QCSC solver, followed by a secondary generative module to model configuration distributions and identify dominant sectors of the global Hilbert space. For water and formamide dimers, our method achieves up to $95\%$ reduction in the diagonalization dimension while enhancing energy accuracy by an order of magnitude over conventional SQD. Furthermore, application to the water hexamer ($\mathrm{(H_2O)_6}$) cage successfully decomposes a 120-qubit problem into six 20-qubit monomeric subsystems, and stitches the monomers under a dimeric approximation, demonstrating excellent agreement with the reference classical methods.

AI Summary

The paper asks whether sample-based quantum diagonalization (SQD) can treat molecular assemblies using quantum samples only from smaller fragments, while reconstructing inter-fragment correlations classically. It introduces PIGen-SQD(MAPS), combining fragment molecular orbital (FMO) partitioning with parallel fragment solvers that use hardware samples, perturbatively selected determinants, and restricted Boltzmann machines (RBMs). An orbital-overlap- and energy-based linear assignment maps fragment occupation bitstrings into the supersystem basis. Their mapped products are augmented with cross-fragment single excitations, CISD configurations, and perturbative triples, then refined through a second RBM-driven selection/diagonalization loop. An alternative uses SQD’s S-CORE recovery initialized with the same mapped space. Tests use IBM Heron R3 samples and classical electronic-structure references for water and formamide dimers in a 6-31G basis. Relative to conventional full-dimer SQD, the reported improvements reach a $95\%$ reduction in diagonalization dimension and roughly an order of magnitude lower energy error. PIGen-SQD(MAPS) gives approximately $0.4\,\mathrm{m}E_h$ errors against heat-bath CI across the studied separation curves. For a water hexamer, sampling is restricted to six 20-spin-orbital monomers; classical recovery treats 15 fragment pairs. The resulting FMO-2 energy differs from the FMO-2 heat-bath-CI reference by $0.915\,\mathrm{m}E_h$, rather than benchmarking an unfragmented 120-qubit solution. The framework assumes predominantly local correlation and weaker inter-fragment coupling. Fragmentation and many-body expansion order are user choices; including larger fragment combinations increases classical cost. Recovery also depends on initialization, configuration thresholds, and sampling quality.

Little sign of AI-generated textIncrementalOverclaimsMissing comparisonStrong assumptions

Error found: The claimed initialization-only comparison between SQD and S-CORE(MTPS) also changes samples per batch from 1,000 to 10,000, so it cannot isolate the benefit of MTPS initialization. The paper asserts a combinatorial shot requirement without specifying distributional or recovery-accuracy assumptions, although useful configuration sampling need not require shots proportional to the ambient Hilbert-space dimension.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

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The paper asks whether sample-based quantum diagonalization (SQD) can treat molecular assemblies using quantum samples only from smaller fragments, while reconstructing inter-fragment correlations classically. It introduces PIGen-SQD(MAPS), combining fragment molecular orbital (FMO) partitioning with parallel fragment solvers that use hardware samples, perturbatively selected determinants, and restricted Boltzmann machines (RBMs). An orbital-overlap- and energy-based linear assignment maps fragment occupation bitstrings into the supersystem basis. Their mapped products are augmented with cross-fragment single excitations, CISD configurations, and perturbative triples, then refined through a second RBM-driven selection/diagonalization loop. An alternative uses SQD’s S-CORE recovery initialized with the same mapped space.
Tests use IBM Heron R3 samples and classical electronic-structure references for water and formamide dimers in a 6-31G basis. Relative to conventional full-dimer SQD, the reported improvements reach a 95%95\%95% reduction in diagonalization dimension and roughly an order of magnitude lower energy error. PIGen-SQD(MAPS) gives approximately 0.4 mEh0.4\,\mathrm{m}E_h0.4mEh​ errors against heat-bath CI across the studied separation curves. For a water hexamer, sampling is restricted to six 20-spin-orbital monomers; classical recovery treats 15 fragment pairs. The resulting FMO-2 energy differs from the FMO-2 heat-bath-CI reference by 0.915 mEh0.915\,\mathrm{m}E_h0.915mEh​, rather than benchmarking an unfragmented 120-qubit solution.
The framework assumes predominantly local correlation and weaker inter-fragment coupling. Fragmentation and many-body expansion order are user choices; including larger fragment combinations increases classical cost. Recovery also depends on initialization, configuration thresholds, and sampling quality.
Abstract Quantum centric supercomputing (QCSC) framework, such as sample-based quantum diagonalization (SQD) holds immense promise toward achieving practical quantum utility to solve classically hard sampling problems in quantum chemistry. QCSC leverages quantum computers to perform the classically intractable task of sampling the dominant fermionic configurations from the Hilbert space that have substantial support to a target state, followed by Hamiltonian diagonalization on a classical processor. However, noisy quantum hardware produces erroneous samples upon measurements, making robust and efficient configuration-recovery strategies essential for scalable QCSC pipelines. Toward this, in this work, we introduce PIGen-SQD, an efficiently designed QCSC workflow that utilizes the capability of generative machine learning (ML) along with physics-informed configuration screening via implicit low-rank tensor decompositions for accurate fermionic state reconstruction. The physics-informed pruning is based on a class of efficient perturbative measures that, in conjunction with samples drawn from quantum hardware, provide a substantial overlap with the target state. This distribution induces an anchoring effect on the generative ML models to stochastically explore only the dominant sector of the Hilbert space for effective identification of additional important configurations in a self-consistent manner. Our numerical experiments performed on IBM Heron R2 and R3 quantum processors with up to 58 qubit experiments demonstrate this synergistic workflow produces compact, high-fidelity subspaces that substantially reduce diagonalization cost while maintaining chemical accuracy under strong electronic correlations. With such a concerted integration of classical many-body intuitions, generative ML and quantum computers as a sampling engine, PIGen-SQD offers a promising pathway toward accurate and systematically improvable quantum simulations on utility-scale quantum hardware.
Quantum centric supercomputing (QCSC) framework, such as sample-based quantum diagonalization (SQD) holds immense promise toward achieving practical quantum utility to solve challenging problems. QCSC leverages quantum computers to perform the classically intractable task of sampling the dominant fermionic configurations from the Hilbert space that have substantial support to a target state, followed by Hamiltonian diagonalization on a classical processor. However, noisy quantum hardware produces erroneous samples upon measurements, making robust and efficient configuration-recovery strategies essential for a scalable QCSC pipeline. Toward this, in this work, we introduce PIGen-SQD, an efficiently designed QCSC workflow that utilizes the capability of generative machine learning (ML) along with physics-informed configuration screening via implicit low-rank tensor decompositions for accurate fermionic state reconstruction. The physics-informed pruning is based on a class of efficient perturbative measures that, in conjunction with hardware samples, provide a substantial overlap with the target state. This distribution induces an anchoring effect on the generative ML models to stochastically explore only the dominant sector of the Hilbert space for effective identification of additional important configurations in a self-consistent manner. Our numerical experiments performed on IBM Heron R2 quantum processors demonstrate this synergistic workflow produces compact, high-fidelity subspaces that substantially reduce diagonalization cost while maintaining chemical accuracy under strong electronic correlations. By embedding classical many body intuitions directly into the generative ML model, PIGen-SQD advances the robustness and scalability of QCSC algorithms, offering a promising pathway toward chemically reliable quantum simulations on utility-scale quantum hardware.
Sample-based quantum diagonalization (SQD) has emerged as a promising route for quantum-centric supercomputing, relying on classical diagonalization of the molecular Hamiltonian within a hardware-sampled determinant subspace. However, its accuracy degrades in strongly correlated regimes where the relevant determinant space exceeds what finite-shot sampling can capture. In this work, we introduce Quantum Wavefunction Augmentation via Variational Autoencoders (Q-WAVE), a hybrid method that combines determinants sampled via SqDRIFT Krylov circuits and configuration interaction singles and doubles (CISD) determinants with generative machine learning. Using a custom βββ-annealed variational autoencoder (VAE) model, Q-WAVE iteratively expands this basis toward the variational ground state. The VAE learns the wavefunction's primary support structure from the combined hardware and CISD seed in a continuous latent space, generating new dominant determinants beyond any fixed excitation hierarchy. The resulting compact wavefunction exceeds what can be extracted from raw hardware samples alone. We demonstrate sub-millihartree accuracy compared to full configuration interaction for H2O\text{H}_2\text{O}H2​O and N2\text{N}_2N2​ dissociation. Finally, we establish Q-WAVE's scalability on a 52-qubit ethylene system (achieving sub-millihartree accuracy versus CCSD(T)) and a highly correlated 60-qubit Cr2\text{Cr}_2Cr2​ stress test that attains chemical accuracy upon a final perturbative correction.
Abstract We present the first quantum-centric simulations of noncovalent interactions using a supramolecular approach. We simulate the potential energy surfaces (PES) of the water and methane dimers, featuring hydrophilic and hydrophobic interactions, respectively, with a sample-based quantum diagonalization (SQD) approach. Our simulations on quantum processors, using 27- and 36-qubit circuits, are in remarkable agreement with classical methods, deviating from complete active space configuration interaction (CASCI) and coupled-cluster singles, doubles, and perturbative triples (CCSD(T)) within 1 kcal/mol in the equilibrium regions of the PES. Finally, we test the capacity limits of the quantum methods for capturing hydrophobic interactions with an experiment on 54 qubits. These results mark significant progress in the application of quantum computing to chemical problems, paving the way for more accurate modeling of noncovalent interactions in complex systems critical to the biological, chemical and pharmaceutical sciences.
Computing ground-state properties of molecules is a promising application for quantum computers operating in concert with classical high-performance computing resources. Quantum embedding methods are a family of algorithms particularly suited to these computational platforms: they combine high-level calculations on active regions of a molecule with low-level calculations on the surrounding environment, thereby avoiding expensive high-level full-molecule calculations and allowing to distribute computational cost across multiple and heterogeneous computing units. Here, we present the first density matrix embedding theory (DMET) simulations performed in combination with the sample-based quantum diagonalization (SQD) method. We employ the DMET-SQD formalism to compute the ground-state energy of a ring of 18 hydrogen atoms, and the relative energies of the chair, half-chair, twist-boat, and boat conformers of cyclohexane. The full-molecule 41- and 89-qubit simulations are decomposed into 27- and 32-qubit active-region simulations, that we carry out on the ibm_cleveland device, obtaining results in agreement with reference classical methods. Our DMET-SQD calculations mark a tangible progress in the size of active regions that can be accurately tackled by near-term quantum computers, and are an early demonstration of the potential for quantum-centric simulations to accurately treat the electronic structure of large molecules, with the ultimate goal of tackling systems such as peptides and proteins.
Quantum computers offer the potential to simulate chemical systems beyond the capabilities of classical computers. However, current quantum computing approaches to ab initio molecular dynamics (AIMD) and vibrational analysis largely rely on the Variational Quantum Eigensolver (VQE), whose circuit depth, iterative optimization, and measurement overhead hinder the practical simulation of molecular systems. Here, we extend Sample-based Quantum Diagonalization (SQD), a quantum sampling-based electronic-structure method, to AIMD and vibrational analysis on noisy quantum hardware. The resulting framework enables nuclear forces and Hessians to be derived from quantum-computed electronic energies, facilitating molecular dynamics and characterization of potential energy surfaces. We demonstrate the approach using diverse molecular processes, including H2 bond vibration, the proton-exchange reaction (H+ + H2), the bimolecular nucleophilic substitution (SN2) reaction (Cl- + CH3Cl), and proton-transfer dynamics between two water molecules involving transient formation of the Zundel cation (H2O···H+···OH2). Across these systems, SQD-AIMD trajectories and vibrational frequencies obtained with noisy quantum hardware/noise-models show excellent agreement with classical reference calculations and substantially improved accuracy relative to previously reported VQE-based simulations. Importantly, the SQD-based approach eliminates costly variational optimization and significantly reduces measurement requirements relative to VQE, enabling AIMD simulations spanning approximately 500 timesteps (∼200 fs), substantially longer than previously reported AIMD simulations on quantum hardware. These results establish SQD-AIMD and SQD-vibrational analysis as practical and scalable frameworks for simulating chemical reaction dynamics and elucidating reaction mechanisms on near-term quantum hardware, extending quantum computing applications beyond static electronic structure calculations.