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基于因果检验的非线性系统的预测试验

张绿夷 王革丽 谭桂容 吴越

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基于因果检验的非线性系统的预测试验

张绿夷, 王革丽, 谭桂容, 吴越

Experimental study on prediction of nonlinear system based on causality test

Zhang Lü-Yi, Wang Ge-Li, Tan Gui-Rong, Wu Yue
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  • 非线性、非平稳系统的预测是一个具有重要科学意义的研究课题. 最近一些工作已将收敛交叉映射算法(convergent cross mapping, CCM)用于检验变量之间的因果关系, 由于在CCM算法中, 相空间中相互靠近的点在时间上具有相似的发展趋势和运动轨迹, 因此该方法可以尝试应用于非线性、非平稳系统的预测试验研究中. 鉴于此, 本文将CCM算法分别应用于Lorenz系统和实际气候时间序列的预测中, 并检测不同相空间重构方法对预测效果的影响. 主要结果如下: 1)不论是理想Lorenz模型还是实际气候序列, 对于单变量、多变量和多视角嵌入法3种重构相空间方法而言, 多视角嵌入法对变量的预测效果最好, 表明对于给定长度的时间序列, 重构相空间中包含的信息越多, 其预测能力越强; 2)将NAM (northern hemisphere annular mode)加入SAT (surface air temperature)的重构相空间中可以改善SAT的预测效果. 在使用单变量、多变量和多视角嵌入法进行预测时, 利用复杂系统中变量中共有信息的特性, 在时间序列长度一定的情况下, 可以利用动力系统的复杂性来增加系统内的信息. 基于因果检验的预测建模方法, 通过挖掘数据中定量信息的提取, 对非线性、非平稳系统预测技巧的改进提供了一个新颖的思路.
    The prediction of nonlinear and non-stationary systems is a research topic of great scientific significance. In some recent work the convergent cross mapping (CCM) algorithm is used to detect the causal relationship between variables. In the CCM algorithm, the points close to each other in the phase space have similar trends and trajectories in time. Therefore, this method can be applied to the prediction of experimental researches of nonlinear and non-stationary systems. Therefore, in this paper the CCM algorithm is applied to the prediction of the Lorenz system and the actual climate time series, and the effects of different phase space reconstruction methods on the prediction skill are investigated. The preliminary results are as follows. 1) No matter whether the ideal Lorenz model or the actual climate series, of the three reconstruction phase space methods of univariate, multivariate, and multiview embedding method, the multiview embedding method is the best predictive skill, indicating that for a given length of time series, the more the information contained in the reconstructed phase space, the stronger its predictive ability is. 2) Adding the data of NAM (northern hemisphere annular mode) to the reconstructed phase space of SAT (surface air temperature) can improve the prediction effect on prediction of SAT. Using the univariable, multivariable, and multiview embedding method for implementing prediction, the characteristics of common information in the complex system are considered. On condition that the length of the time series is fixed, the complexity of the dynamic system can be used to increase the information of the system. Based on causality detection, through the extraction of quantitative information of data, a novel idea for the improvement of predictive skills in nonlinear and non-stationary systems can be obtained.
      通信作者: 王革丽, wgl@mail.iap.ac.cn
    • 基金项目: 国家自然科学基金 (批准号: 42075054)资助的课题
      Corresponding author: Wang Ge-Li, wgl@mail.iap.ac.cn
    • Funds: Project supported by the National Natural Science Foundation of China (Grant No. 42075054)
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    丁瑞强, 李建平 2009 气象学报 67 241Google Scholar

    Ding R Q, Li J P 2009 Acta Meteor Sin. 67 241Google Scholar

    [3]

    Li H R, Jin F F, Song L C 2017 J. Meteorol. Res. 31 204Google Scholar

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    丁一汇 2004 气象 30 11Google Scholar

    Ding Y H 2004 Meteor. Mon. 30 11Google Scholar

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    徐邦琪, 臧钰歆, 朱志伟 2020 大气科学学报 43 212

    Hsu P C, Zang Y X, Zhu Z W 2020 Trans. Atmos. Sci. 43 212

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    杨培才, 卞建春, 王革丽, 周秀骥 2003 科学通报 48 1470Google Scholar

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    Farmer J D, Sidorowich J 1987 Phys. Rev. Lett. 59 845Google Scholar

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    Yang P C, Zhou X J, Bian J C 2000 J. Geophys. Res. 105 12253Google Scholar

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    Wang G L, Yang P C, Lv D R 2004 Adv. Atmos. Sci. 21 296Google Scholar

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    潘昕浓, 王革丽, 杨培才 2017 物理学报 66 080501Google Scholar

    Pan X N, Wang G L, Yang P C 2017 Acta Phys. Sin. 66 080501Google Scholar

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    陈潇潇, 王革丽, 金莲姬 2015 中国环境科学 35 694

    Chen X X, Wang G L, Jin L J 2015 China Environ. Sci. 35 694

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    杨培才, 周秀骥 2005 气象学报 63 556Google Scholar

    Yang P C, Zhou X J 2005 Acta Meteor. Sin. 63 556Google Scholar

    [16]

    Verdes P F, Granitto P M, Navone H D, Ceccatto H A 2001 Phys. Rev. Lett. 87 124101Google Scholar

    [17]

    Wiskott L 2003 Neural Comput. 15 2147Google Scholar

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    Verdes P F 2007 Phys. Rev. Lett. 99 1

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    Gunturkun U 2010 Phys. D. 239 1095Google Scholar

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    Granger C W J 1969 Econometrica 37 424Google Scholar

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    Barnett L, Barrett A B, Seth A K 2009 Phys. Rev. Lett. 103 238701Google Scholar

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    Bressler, Steven L, Seth A K 2011 NeuroImage 58 323Google Scholar

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    Sugihara G, May R M, Ye H 2012 Science 338 496Google Scholar

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    Deyle E R, Maher M C, Hernandez R D 2016 PNAS 113 13081Google Scholar

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    Runge J, Bathiany S, Bollt E 2019 Nat. Commun. 10 2553Google Scholar

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    Sugihara G 1994 Philos. Trans. Royal Soc. 348 477

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    Dixon P A, Milicich M J, Sugihara G 1999 Science 283 1528Google Scholar

    [33]

    Ye H, Sugihara G 2016 Science 335 922

    [34]

    Lorenz E N 1963 J. Atmos. Sci. 20 130Google Scholar

  • 图 1  最佳嵌入维数E的选取

    Fig. 1.  Selection of the best embedding dimension E.

    图 2  (a)单变量嵌入法预测结果; (b)多变量嵌入法预测结果; (c)多视角嵌入法预测结果; (d)三种嵌入法预测结果的平均绝对误差比较

    Fig. 2.  Forecast results: (a) Univariate embedding; (b) multivariate embedding; (c) multiview embedding; (d) average absolute error of the prediction results of the three embedding methods.

    图 3  三种嵌入方法预测能力随步长的变化 (a)单变量嵌入法; (b)多变量嵌入法; (c)多视角嵌入法

    Fig. 3.  The prediction ability of three embedding methods varies with step size: (a)Univariate embedding; (b) multivariate embedding; (c) multiview embedding;.

    图 4  (a)单变量嵌入法和在目标变量中加入NAM信号后的预测结果; (b)多变量嵌入法的预测结果(黑色圆圈代表仅利用SAT序列进行预测, 红色三角代表加入NAM信号后)

    Fig. 4.  (a) Univariate embedding method and prediction result after adding NAM signal to the target variable; (b) prediction result of multivariate embedding method (black circle represents prediction using only SAT sequence, red triangle represents after adding NAM signal).

    图 5  仅用东北亚地区冬季SAT重构相空间, (a)—(d)分别表示k取40, 41, 42, 43的预测结果

    Fig. 5.  Only using Northeast Asia winter surface air temperature reconstruct the phase space: (a)–(d) represent the prediction results of k taking 40, 41, 42, 43 respectively.

    图 6  仅将2月的NAM信号加入SAT的重构相空间中, (a)—(d)分别表示k取30, 36, 31, 34的预测结果

    Fig. 6.  Only adding the NAM signal in February to the reconstructed phase space of the SAT: (a)–(d) represent the prediction results of k taking 30, 36, 31, and 34, respectively.

    图 7  将12月至次年2月的NAM信号加入SAT的重构相空间中, (a)—(d)分别表示当k取38, 39, 36, 37时的预测结果

    Fig. 7.  Adding the NAM signals from December to next February to the reconstructed phase space of the SAT: (a)–(d) show the prediction results when k takes 38, 39, 36, and 37, respectively.

    表 1  多种嵌入方法的预测结果

    Table 1.  Predicted results of multiple embedding methods.

    Embedding methodReconstructing phase space with SAT only Adding NAM to SAT to reconstruct the phase space
    ρMAERMSEρMAERMSE
    Univariate0.121.061.30 0.180.971.18
    Multivariate0.151.021.270.260.951.12
    Multi-angle0.660.620.750.790.590.66
    下载: 导出CSV
  • [1]

    魏凤英 2006 应用气象学报 6 736Google Scholar

    Wei F Y 2006 J. Appl. Meteor. Sci. 6 736Google Scholar

    [2]

    丁瑞强, 李建平 2009 气象学报 67 241Google Scholar

    Ding R Q, Li J P 2009 Acta Meteor Sin. 67 241Google Scholar

    [3]

    Li H R, Jin F F, Song L C 2017 J. Meteorol. Res. 31 204Google Scholar

    [4]

    丁一汇 2004 气象 30 11Google Scholar

    Ding Y H 2004 Meteor. Mon. 30 11Google Scholar

    [5]

    徐邦琪, 臧钰歆, 朱志伟 2020 大气科学学报 43 212

    Hsu P C, Zang Y X, Zhu Z W 2020 Trans. Atmos. Sci. 43 212

    [6]

    杨培才, 卞建春, 王革丽, 周秀骥 2003 科学通报 48 1470Google Scholar

    Yang P C, Bian J C, Wang G L, Zhou X J 2003 Chin. Sci. Bull. 48 1470Google Scholar

    [7]

    Packard N H, Crutchfield J P, Farmer J D, Shaw R S 1980 Phys. Rev. Lett. 45 712Google Scholar

    [8]

    Takens F 1981 Lect. Notes Math. 898 366

    [9]

    Farmer J D, Sidorowich J 1987 Phys. Rev. Lett. 59 845Google Scholar

    [10]

    Casdagli M 1989 Phys. D 35 335Google Scholar

    [11]

    Yang P C, Zhou X J, Bian J C 2000 J. Geophys. Res. 105 12253Google Scholar

    [12]

    Wang G L, Yang P C, Lv D R 2004 Adv. Atmos. Sci. 21 296Google Scholar

    [13]

    潘昕浓, 王革丽, 杨培才 2017 物理学报 66 080501Google Scholar

    Pan X N, Wang G L, Yang P C 2017 Acta Phys. Sin. 66 080501Google Scholar

    [14]

    陈潇潇, 王革丽, 金莲姬 2015 中国环境科学 35 694

    Chen X X, Wang G L, Jin L J 2015 China Environ. Sci. 35 694

    [15]

    杨培才, 周秀骥 2005 气象学报 63 556Google Scholar

    Yang P C, Zhou X J 2005 Acta Meteor. Sin. 63 556Google Scholar

    [16]

    Verdes P F, Granitto P M, Navone H D, Ceccatto H A 2001 Phys. Rev. Lett. 87 124101Google Scholar

    [17]

    Wiskott L 2003 Neural Comput. 15 2147Google Scholar

    [18]

    Verdes P F 2007 Phys. Rev. Lett. 99 1

    [19]

    Gunturkun U 2010 Phys. D. 239 1095Google Scholar

    [20]

    Wiener N (Beckenbach E F Ed.) 1956 Modern Mathermatics for Engineers p165

    [21]

    Granger C W J 1969 Econometrica 37 424Google Scholar

    [22]

    Barnett L, Barrett A B, Seth A K 2009 Phys. Rev. Lett. 103 238701Google Scholar

    [23]

    Bressler, Steven L, Seth A K 2011 NeuroImage 58 323Google Scholar

    [24]

    Sugihara G, May R M, Ye H 2012 Science 338 496Google Scholar

    [25]

    Deyle E R, Maher M C, Hernandez R D 2016 PNAS 113 13081Google Scholar

    [26]

    Runge J, Bathiany S, Bollt E 2019 Nat. Commun. 10 2553Google Scholar

    [27]

    Tsonis A A, Deyle E R, May R M 2015 PNAS 112 3253Google Scholar

    [28]

    Zhang N N, Wang G L, Tsonis A A 2019 Climate DyNAMics 52 3175Google Scholar

    [29]

    Sugihara G, May R M 1990 Nature 344 734Google Scholar

    [30]

    Dixon P A, Milicich M J, Sugihara G 2001 Nonlinear Dynamics and Statistics (Boston: Birkhauser) p339

    [31]

    Sugihara G 1994 Philos. Trans. Royal Soc. 348 477

    [32]

    Dixon P A, Milicich M J, Sugihara G 1999 Science 283 1528Google Scholar

    [33]

    Ye H, Sugihara G 2016 Science 335 922

    [34]

    Lorenz E N 1963 J. Atmos. Sci. 20 130Google Scholar

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出版历程
  • 收稿日期:  2021-10-08
  • 修回日期:  2021-12-20
  • 上网日期:  2022-01-26
  • 刊出日期:  2022-04-20

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