Abstract
The quantum Fourier transform (QFT) is a fundamental component in various quantum algorithms, including Shor’s factoring algorithm and the Harrow-Hassidim-Lloyd (HHL) algorithm for solving systems of linear equations. Efficient implementation of the QFT is essential for the practical realization of large-scale quantum algorithms, especially in fault-tolerant quantum computing. In fault-tolerant implementations, the Clifford + T gate library is the standard choice for building quantum circuits. As the most resource-intensive component within this framework, the T gate’s associated cost poses a significant challenge to the efficient implementation of the QFT and its dependent algorithms. While approximate QFT (AQFT) circuits reduce this cost, state-of-the-art implementations still require a T-count of and a T-depth of. Although these results represent a notable achievement, the associated resource cost remains a primary bottleneck for practical, large-scale quantum algorithms, motivating further optimization. To address this bottleneck, this paper introduces two novel -qubit AQFT circuits with an approximation error of. Our first design, AQFT Circuit 1, halves the T-count to by constructing inverse phase gradient transformation (PGT) circuits without using additional non-Clifford gates and by implementing the inverse PGTs using quantum adders. Our second design, AQFT Circuit 2, reduces the T-depth to through parallelization of the inverse PGTs that add only additional T gates. For both AQFT circuits, the state-of-the-art linear-depth quantum adder is employed. We demonstrate that employing the linear-depth quantum adder provides advantages over the currently known logarithmic-depth quantum adder, not only in terms of T-count but also in T-depth optimization for the AQFT, particularly within the range, which encompasses practical system sizes.
| Original language | English |
|---|---|
| Article number | 37199 |
| Journal | Scientific Reports |
| Volume | 15 |
| Issue number | 1 |
| DOIs | |
| State | Published - Dec 2025 |
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