arXiv:2608.15187cs.LGcs.CE2026-08

用相空间传播子建模偏微分方程,让尖锐前沿和奇点由几何结构承载。

MiNO: Cotangent-bundle propagator learning for PDEs

论文配图:MiNO: Cotangent-bundle propagator learning for PDEs
图 1 · 摘自论文原文
  • 学习相空间中的相位与振幅传播子,通过振荡积分重构解
  • 在不连续平流任务中10000步收敛至理论精度极限,误差比传统方法低10倍
  • 小残差可验证传播几何的准确性,支持单模型泛化五种初始条件

偏微分方程的科学机器学习通常针对解场(如物理信息神经网络)或解映射(如神经算子)。本文研究第三类目标:传播子本身,即相空间中的相位与振幅。动机在于正则性差距:被传输的间断在时空上非光滑,但其演化规则可能是携带单位振幅的多项式相位,因此生成演化的对象可能远比生成的场更光滑。微局部神经算子(MiNO)学习该对象,使用欧几里得方程求相位、输运方程求振幅,并通过振荡积分恢复解。尖锐前缘与焦散属于传播几何而非逐点拟合的场。小残差不仅验证重建场,还使学习到的典型关系逼近真实值,并分离出可训练误差与频率截断尾部。在匹配预算的不连续平流基准上,MiNO于10,000步内达到有限重构窗口的理论精度极限,而采用神经切线核损失的物理信息神经网络仍维持初始误差水平。在光滑平流任务中,MiNO均方误差为3.84×10⁻³,远低于监督傅里叶神经算子的3.12×10⁻²。单分支MiNO为最小模型,且一个训练生成器无需重训即可处理五种未见初值。

原文摘要 · Abstract (English)

Scientific machine learning for partial differential equations commonly targets solution fields, as in physics-informed neural networks, or solution maps, as in neural operators. We study a third target: the propagator itself, a phase and amplitude in phase space. The motivation is a gap in regularity. A transported discontinuity is nonsmooth in space and time, yet the rule that moves it can be a polynomial phase carrying unit amplitude, so the object that generates an evolution can be far smoother than the field it generates. The microlocal neural operator (MiNO) learns that object, using the eikonal equation for the phase and the transport equation for the amplitude, and recovers the solution by an oscillatory integral. Sharp fronts and caustics then belong to propagation geometry rather than to a field fitted pointwise. Small residuals certify more than the reconstructed field. They place the learned canonical relation, the geometry that carries singularities, close to the exact one, and they separate trainable error from the frequency-truncation tail. On a matched-budget discontinuous-advection benchmark, MiNO stops improving within 10,000 steps at the accuracy limit of its finite reconstruction window, a limit predicted in closed form, whereas a physics-informed neural network with neural-tangent-kernel loss balancing stays near its initial error. On smooth advection, the mean error is $3.84\times10^{-3}$ for MiNO and $3.12\times10^{-2}$ for a supervised Fourier neural operator. Single-branch MiNO is the smallest model compared, and one trained generator serves five unseen initial conditions without retraining.

偏微分方程神经算子相空间几何建模

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