Enhancing the Harrow-Hassidim-Lloyd (HHL) algorithm in systems with large condition numbers

• URL: http://arxiv.org/abs/2407.21641v3
• Date: Wed, 9 Oct 2024 04:46:09 GMT
• Title: Enhancing the Harrow-Hassidim-Lloyd (HHL) algorithm in systems with large condition numbers
• Authors: Peniel Bertrand Tsemo, Akshaya Jayashankar, K. Sugisaki, Nishanth Baskaran, Sayan Chakraborty, V. S. Prasannaa,
• Abstract summary: We demonstrate the ability of Psi-HHL to handle situations involving large $mathcalkappa$ matrices. We consider matrices up to size $256 times 256$ that reach $mathcalkappa$ of about 466.
• Score: 0.0
• License: http://creativecommons.org/licenses/by/4.0/
• Abstract: Although the Harrow-Hassidim-Lloyd (HHL) algorithm offers an exponential speedup in system size for treating linear equations of the form $A\vec{x}=\vec{b}$ on quantum computers when compared to their traditional counterparts, it faces a challenge related to the condition number ($\mathcal{\kappa}$) scaling of the $A$ matrix. In this work, we address the issue by introducing the post-selection-improved HHL (Psi-HHL) approach that involves a simple yet effective modification of the HHL algorithm to extract a feature of $|x\rangle$, and which leads to achieving optimal behaviour in $\mathcal{\kappa}$ (linear scaling) for large condition number situations. This has the important practical implication of having to use substantially fewer shots relative to the traditional HHL algorithm. We carry out two sets of simulations, where we go up to 26-qubit calculations, to demonstrate the ability of Psi-HHL to handle situations involving large $\mathcal{\kappa}$ matrices via: (a) a set of toy matrices, for which we go up to size $64 \times 64$ and $\mathcal{\kappa}$ values of up to $\approx$ 1 million, and (b) a deep-dive into quantum chemistry, where we consider matrices up to size $256 \times 256$ that reach $\mathcal{\kappa}$ of about 466. The molecular systems that we consider are Li$_{\mathrm{2}}$, RbH, and CsH. Although the feature of $|x\rangle$ considered in our examples is an overlap between the input and output states of the HHL algorithm, our approach is general and can be applied in principle to any transition matrix element involving $|x\rangle$.

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