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Quantum Multigrid Algorithm for Finite Element Problems

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arxiv 2404.07466 v1 pith:LA2VW3WL submitted 2024-04-11 quant-ph cs.NAmath.NA

classification quant-phcs.NAmath.NA
keywords quantumfinalmultigridsequenceexponentiallinearsolutionstate
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Quantum linear system algorithms (QLSAs) can provide exponential speedups for the solution of linear systems, but the growth of the condition number for finite element problems can eliminate the exponential speedup. QLSAs are also incapable of using an initial guess of a solution to improve upon it. To circumvent these issues, we present a Quantum Multigrid Algorithm (qMG) for the iterative solution of linear systems by applying the sequence of multigrid operations on a quantum state. Given an initial guess with error e_0, qMG can produce a vector encoding the entire sequence of multigrid iterates with the final iterate having a relative error e'=e/e_0, as a subspace of the final quantum state, with exponential advantage in O( poly log (N/e') ) time using O( poly log (N/e') ) qubits. Although extracting the final iterate from the sequence is efficient, extracting the sequence of iterates from the final quantum state can be inefficient. We provide an analysis of the complexity of the method along with numerical analysis.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. An Implementation of the Finite Element Method in Hybrid Classical/Quantum Computers

    quant-ph 2024-11 conditional novelty 6.0 of 10

    A variational quantum linear solver is coupled to finite element discretizations by an element-wise unitary decomposition, verified on 1D heat problems up to 7 qubits but with strong scaling barriers.

  2. Addressing the Readout Problem in Quantum Differential Equation Algorithms with Quantum Scientific Machine Learning

    quant-ph 2024-11 conditional novelty 5.0 of 10

    Quantum neural networks can classify shock and turbulent flow solutions encoded as quantum states, with accuracy strongly dependent on Fourier versus real-space basis choice.

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