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qSHIFT presents a significant advancement in quantum simulation by offering a protocol that improves gate complexity scaling without increasing quantum circuit depth or requiring ancillary qubits. While it introduces higher classical computational costs, the method maintains compatibility with elementary gate sets and shallow circuits essential for early fault-tolerant devices. This work directly addresses the need for efficient hybrid coherent algorithms where classical resources complement limited quantum coherence times.
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qSHIFT: An Adaptive Sampling Protocol for Higher-Order Quantum Simulation

arXiv2 min read

arXiv:2604.26263v3 Announce Type: replace Abstract: Early fault-tolerant quantum computers are expected to support reliable but depth-limited quantum circuits, while classical computational resources remain available. These conditions have motivated hybrid coherent algorithms which use quantum simulation as a central algorithmic primitive. This trend calls for quantum-simulation methods that operate with shallow circuits and admit systematic improvements in gate-complexity scaling. Here, we introduce qSHIFT, an adaptive sampling protocol for simulating a Hamiltonian $H=\sum_{i=1}^{L}h_iH_i$. qSHIFT achieves gate complexity $\mathcal{O}_r\left((\lambda t)^{1+1/r}/\varepsilon^{1/r}\right)$, where $r$ is an algorithmic parameter, $\lambda=\sum_i |h_i|$ and $\varepsilon$ denotes the target precision. Relative to qDRIFT, increasing $r$ systematically improves the gate complexity for a given target precision without incurring extra quantum cost. Unlike Trotterization, the number of sampled gates is nominally independent of $L$. qSHIFT retains the elementary gate set of qDRIFT and, unlike qSWIFT, requires neither ancillary qubits nor controlled operations. The improved gate complexity scaling is obtained at the cost of a classical calculation involving $L^r$ coefficients at each adaptive sampling round.

Abstract:Early fault-tolerant quantum computers are expected to support reliable but depth-limited quantum circuits, while classical computational resources remain available. These conditions have motivated hybrid coherent algorithms which use quantum simulation as a central algorithmic primitive. This trend calls for quantum-simulation methods that operate with shallow circuits and admit systematic improvements in gate-complexity scaling. Here, we introduce qSHIFT, an adaptive sampling protocol for simulating a Hamiltonian $H=\sum_{i=1}^{L}h_iH_i$. qSHIFT achieves gate complexity $\mathcal{O}_r\left((\lambda t)^{1+1/r}/\varepsilon^{1/r}\right)$, where $r$ is an algorithmic parameter, $\lambda=\sum_i |h_i|$ and $\varepsilon$ denotes the target precision. Relative to qDRIFT, increasing $r$ systematically improves the gate complexity for a given target precision without incurring extra quantum cost. Unlike Trotterization, the number of sampled gates is nominally independent of $L$. qSHIFT retains the elementary gate set of qDRIFT and, unlike qSWIFT, requires neither ancillary qubits nor controlled operations. The improved gate complexity scaling is obtained at the cost of a classical calculation involving $L^r$ coefficients at each adaptive sampling round.

arXiv:2604.26263 [quant-ph]

(or arXiv:2604.26263v3 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2604.26263 Focus to learn more arXiv-issued DOI via DataCite

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Full text under the publisher's open licence · 247 words

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