| − | 这里的<math>\mathbf{A}</math>便是我们拟合输出的结果。Champion, Brunton 和 Kutz等人表明<ref name=champion_2019>K. P. Champion, S. L. Brunton, and J. N. Kutz, Discovery of nonlinear multiscale systems: Sampling strategies and embeddings, SIAM J. Appl. Dyn. Syst., 18 (2019), pp. 312--333, https://doi.org/10.1137/18M1188227. (Cited on pp. 288, 289)</ref>,该[[线性系统]]捕捉了弱[[非线性系统]]的[[动力学]]。然而,对于[[混沌系统]],即使有近似Koopman不变的测量系统,在识别封闭的线性模型方面仍存在挑战。无论多么高维的线性模型,都无法捕捉多个[[不动点]]或具有正[[Lyapunov指数]]的[[混沌]]所特有的不可预测行为<ref name=Brunton_2016>S. L. Brunton, B. W. Brunton, J. L. Proctor, and J. N. Kutz, Koopman invariant subspaces and finite linear representations of nonlinear dynamical systems for control, PLoS ONE, 11 (2016), art. e0150171. (Cited on pp. 234, 247, 248, 254, 284, 285, 286, 288, 295, 308, 309, 312, 318)</ref>。与其为 <math>\mathbf{V}</math> 中的前 <math>r</math> 个变量构建一个封闭的线性模型,不如在前 <math>r-1</math> 个变量上构建一个线性模型,并将最后一个变量 <math>v_r</math> 强加为一个外力项<ref name=brunton_2017 />:
| + | 其中 <math>\mathbf{v}(t) = \begin{bmatrix} v_1(t) & v_2(t) & \cdots & v_{r}(t) \end{bmatrix}^T</math>便是来自奇异向量<math>\mathbf{V}</math> 的前 <math>r</math> 列。这里的<math>\mathbf{A}</math>便是我们拟合输出的结果。Champion, Brunton 和 Kutz等人表明<ref name=champion_2019>K. P. Champion, S. L. Brunton, and J. N. Kutz, Discovery of nonlinear multiscale systems: Sampling strategies and embeddings, SIAM J. Appl. Dyn. Syst., 18 (2019), pp. 312--333, https://doi.org/10.1137/18M1188227. (Cited on pp. 288, 289)</ref>,该[[线性系统]]捕捉了弱[[非线性系统]]的[[动力学]]。然而,对于[[混沌系统]],即使有近似Koopman不变的测量系统,在识别封闭的线性模型方面仍存在挑战。无论多么高维的线性模型,都无法捕捉多个[[不动点]]或具有正[[Lyapunov指数]]的[[混沌]]所特有的不可预测行为<ref name=Brunton_2016>S. L. Brunton, B. W. Brunton, J. L. Proctor, and J. N. Kutz, Koopman invariant subspaces and finite linear representations of nonlinear dynamical systems for control, PLoS ONE, 11 (2016), art. e0150171. (Cited on pp. 234, 247, 248, 254, 284, 285, 286, 288, 295, 308, 309, 312, 318)</ref>。与其为 <math>\mathbf{V}</math> 中的前 <math>r</math> 个变量构建一个封闭的线性模型,不如在前 <math>r-1</math> 个变量上构建一个线性模型,并将最后一个变量 <math>v_r</math> 强加为一个外力项<ref name=brunton_2017 />: |
| | Hankel矩阵在[[系统]]辨识中已使用了几十年,例如在[[ERA]]<ref>J. N. Juang and R. S. Pappa, An eigensystem realization algorithm for modal parameter identification and model reduction, J. Guidance Control Dynam., 8 (1985), pp. 620--627. (Cited on pp. 262, 289, 303)</ref>和奇异谱分析(singular spectrum analysis,SSA)<ref>R. W. Brockett, Optimal control of the Liouville equation, in Proceedings of the International Conference on Complex Geometry and Related Fields, AMS/IP Stud. Adv. Math. 39, AMS, 2007, pp. 23--35. (Cited on p. 300)</ref>中。这些早期算法是专门为线性[[系统]]开发的,尽管它们常被应用于弱[[非线性系统]],但当时尚不清楚如何解释由这些方法产生的模型和分解。 | | Hankel矩阵在[[系统]]辨识中已使用了几十年,例如在[[ERA]]<ref>J. N. Juang and R. S. Pappa, An eigensystem realization algorithm for modal parameter identification and model reduction, J. Guidance Control Dynam., 8 (1985), pp. 620--627. (Cited on pp. 262, 289, 303)</ref>和奇异谱分析(singular spectrum analysis,SSA)<ref>R. W. Brockett, Optimal control of the Liouville equation, in Proceedings of the International Conference on Complex Geometry and Related Fields, AMS/IP Stud. Adv. Math. 39, AMS, 2007, pp. 23--35. (Cited on p. 300)</ref>中。这些早期算法是专门为线性[[系统]]开发的,尽管它们常被应用于弱[[非线性系统]],但当时尚不清楚如何解释由这些方法产生的模型和分解。 |