量子神经网络通过测量诱导非线性,同时学习守恒与耗散动力学。
Quantum Port-Hamiltonian Neural Networks: Learning Conservative and Dissipative Dynamics via Measurement-Induced Nonlinearity

- 用量子线路实现哈密顿与耗散结构,通过测量引入非线性
- 单振子系统能量单调下降,网络结构下92%-98%能量衰减
- 适合研究量子控制、物理信息神经网络的科研人员
我们提出量子端口-哈密顿神经网络(Q-pHNN),一种参数化量子电路,以保持结构的方式学习经典动力学。该框架基于同构哈密顿映射(IHM):反对称互联矩阵\(\mathbf{J}\)对应于酉门演化,半正定耗散矩阵\(\mathbf{R}\)由中电路测量结合经典反馈实现的测量诱导非线性(MINL)表示。能量守恒与被动性通过构造强制实现,而非依赖惩罚项;耗散成为内在量子效应:能量通过测量行为逸出。我们构建三种架构:量子哈密顿神经网络(通过参数移位法提取哈密顿方程)、通过MINL耗散的Q-pHNN,以及将双通道提升至$N$节点耦合相量网络的拓扑纠缠量子图神经网络。模拟中,所有模型均训练成功,对称积分器下相对能量漂移为1.35%,单振子MINL电路达到100%能量单调性,环形、星形和链状网络在$N\in\{3,6,9\}$时相空间能量衰减率达92--98%。在IBM Heron处理器上,训练后的能面及其参数移位梯度与模拟值一致,误差主要来自读出噪声而非门保真度;耗散通道原生执行,但在当前深度下无法分离测量反作用影响。
原文摘要 · Abstract (English)
We introduce Quantum Port-Hamiltonian Neural Networks (Q-pHNNs), parameterised quantum circuits that learn classical dynamics in a structure-preserving manner. The framework rests on the Isomorphic Hamiltonian Mapping (IHM): the skew-symmetric interconnection matrix $\mathbf{J}$ corresponds to unitary gate evolution, and the positive-semidefinite dissipation matrix $\mathbf{R}$ to Measurement-Induced NonLinearity (MINL), realised by mid-circuit measurement with classical feedforward. Conservation and passivity are then enforced by construction rather than by penalty terms, and dissipation becomes an intrinsically quantum effect: energy leaves through the act of measurement. We instantiate the IHM in three architectures: a Quantum HNN that extracts Hamilton's equations via the Parameter-Shift Rule; a Q-pHNN that dissipates through MINL; and a topology-entangled Quantum Graph Neural Network lifting both channels to $N$-node coupled-phasor networks. In simulation, where every model here was trained, we obtain $1.35\%$ relative energy drift under a symplectic integrator, $100\%$ energy monotonicity for the single-oscillator MINL circuit, and $92$--$98\%$ phase-space energy decay across ring, star and chain networks at $N\in\{3,6,9\}$. On an IBM Heron processor the trained energy surface and its parameter-shift gradients reproduce their simulated values, with an error budget dominated by readout rather than gate infidelity; the dissipative channel executes natively, but its decay is not separable from measurement back-action at these depths.
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