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Research PaperResearchia:202607.15076

Expressibility and trainability of a two-dimensional pairwise quantum-circuit ansatz

Shuai Zhang

Abstract

Parameterized quantum circuits~(PQCs) constitute a central building block of variational quantum algorithms~(VQAs) and quantum machine learning~(QML) methods. Existing ansatz designs often adopt hardware-agnostic or simplified 1D chain/ring entanglement patterns. However, as quantum hardware continues to develop, native 2D connectivity patterns, such as planar superconducting-qubit architectures, are becoming increasingly important. Inspired by this hardware structure, we construct a native 2D p...

Submitted: July 15, 2026Subjects: Quantum Physics; Quantum Computing

Description / Details

Parameterized quantum circuits~(PQCs) constitute a central building block of variational quantum algorithms~(VQAs) and quantum machine learning~(QML) methods. Existing ansatz designs often adopt hardware-agnostic or simplified 1D chain/ring entanglement patterns. However, as quantum hardware continues to develop, native 2D connectivity patterns, such as planar superconducting-qubit architectures, are becoming increasingly important. Inspired by this hardware structure, we construct a native 2D pairwise ansatz and compare its expressibility and trainability with representative 1D ansatze at identical layer depths, despite their different circuit depths. For the fixed 16-qubit system, the 2D ansatz has the smallest KL divergence at L=1L=1 and 22, and its second-order frame potential approaches the theoretical lower bound more rapidly at shallow layer counts than the frame potentials of the three 1D ansatze. We also evaluate the gradient variance of the Pauli-ZZ-string expectation value ⟨Z0βŠ—β‹―βŠ—Z15⟩\langle Z_0\otimes\cdots\otimes Z_{15}\rangle with respect to the first RyR_y angle. For this Pauli-ZZ string and fixed parameter, the gradient variance is smaller for the 2D circuit at L=1L=1--44. The differences narrow at L=5L=5, and the four ansatze yield statistically compatible variances at L=6L=6.


Source: arXiv:2607.12996v1 - http://arxiv.org/abs/2607.12996v1 PDF: https://arxiv.org/pdf/2607.12996v1 Original Link: http://arxiv.org/abs/2607.12996v1

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Date:
Jul 15, 2026
Topic:
Quantum Computing
Area:
Quantum Physics
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