An Implementation of the Finite Element Method in Hybrid Classical/Quantum Computers
- URL: http://arxiv.org/abs/2411.09038v1
- Date: Wed, 13 Nov 2024 21:32:30 GMT
- Title: An Implementation of the Finite Element Method in Hybrid Classical/Quantum Computers
- Authors: Abhishek Arora, Benjamin M. Ward, Caglar Oskay,
- Abstract summary: The Quantum Finite Element Method (Q-FEM) is developed for use in noisy intermediate-scale quantum computers.
Q-FEM keeps the structure of the finite element discretization intact allowing for the use of variable element lengths and material coefficients.
Numerical verification studies demonstrate that Q-FEM is effective in converging to the correct solution for a variety of problems.
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- Abstract: This manuscript presents the Quantum Finite Element Method (Q-FEM) developed for use in noisy intermediate-scale quantum (NISQ) computers, and employs the variational quantum linear solver (VQLS) algorithm. The proposed method leverages the classical FEM procedure to perform the unitary decomposition of the stiffness matrix and employs generator functions to design explicit quantum circuits corresponding to the unitaries. Q-FEM keeps the structure of the finite element discretization intact allowing for the use of variable element lengths and material coefficients in FEM discretization. The proposed method is tested on a steady-state heat equation discretized using linear and quadratic shape functions. Numerical verification studies demonstrate that Q-FEM is effective in converging to the correct solution for a variety of problems and model discretizations, including with different element lengths, variable coefficients, and different boundary conditions. The formalism developed herein is general and can be extended to problems with higher dimensions. However, numerical examples also demonstrate that the number of parameters for the variational ansatz scale exponentially with the number of qubits to increase the odds of convergence, and deterioration of system conditioning with problem size results in barren plateaus, and hence convergence difficulties.
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