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A drift homotopy implicit particle filter method for nonlinear filtering problems

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  • In this paper, we develop a drift homotopy implicit particle filter method. The methodology of our approach is to adopt the concept of drift homotopy in the resampling procedure of the particle filter method for solving the nonlinear filtering problem, and we introduce an implicit particle filter method to improve the efficiency of the drift homotopy resampling procedure. Numerical experiments are carried out to demonstrate the effectiveness and efficiency of our drift homotopy implicit particle filter.

    Mathematics Subject Classification: 60G35, 62M20, 93E11.

    Citation:

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  • Figure 1.  Double well potential case 1: $ \alpha = 1 $, $ \sigma = 1.5 $, $ R = 1.5 $

    Figure 2.  Double well potential case 2: $ \alpha = 1 $, $ \sigma = 1 $, $ R = 1 $ with state switch

    Figure 3.  Double well potential case 3: $ \alpha = 10 $, $ \sigma = 1 $, $ R = 2 $ with state switch

    Figure 4.  Tracking performance for $ 4000 $ steps

    Figure 5.  Tracking errors for $ 4000 $ steps

    Figure 6.  Tracking performance with rapid change in the state

    Figure 7.  Tracking errors with rapid change in the state

    Figure 8.  Mean square errors with respect to observation gaps

    Table 1.   

    Algorithm: Drift homotopy implicit particle filter (DHIPF)
    Initialize the particle cloud $ \{x_0^{(i)}\}_{i=1}^{N_p} $, the number of drift homotopy levels $ L $ with the intermediate drift function $ b $ and the constant sequence $ \{\beta_l\}_{l=0}^{L} $, and the reference random variable $ \xi $ for the implicit particle filter procedure.
    while $ n =0, 1, 2, \cdots $, do
        for: particles $ i = 1, 2, \cdots, N_p $,
            for: drift homotopy levels $ l = 0, 1, 2, \cdots, L-1 $,
                -: Construct the drift homotopy dynamics (10);
                -: Solve for $ \psi_{l}^{n+1, i} $ in the equation (17) with the initial guess $ \hat{x}_{n+1, l}^{(i)} $;
                -: Generate the sample $ \hat{x}_{n+1, l+1}^{(i)} $ through $ \exp\big(- \frac{\xi^{T} \xi}{2}\big) J_{\psi_l^{n+1, i}}^{-1} $;
            end for
        end for
      The particles $ \{x_{n+1}^{(i)}\}_{i = 1}^{N_p} : = \{\hat{x}_{n+1, L}^{(i)}\}_{i = 1}^{N_p} $ provide an empirical distribution for the filtering density $ p(X_{n+1} | Y_{1:n+1}) $
    end while
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    Table 2.  Example 1. Performance comparison for Case 1

    APF EnKF IPF DHPF DHIPF
    CPU Time $ 9.703 $ $ 0.365625 $ $ 0.0938 $ $ 48.563 $ $ \bf{0.312} $
    MSE $ 2.03 E-3 $ $ 5.22 E-3 $ $ 1.10 E-3 $ $ 5.92 E-4 $ $ \bf{4.60 E-4} $
     | Show Table
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    Table 3.  Example 1. Performance comparison for Case 2

    APF EnKF IPF DHPF DHIPF
    CPU Time $ 9.391 $ $ 0.578 $ $ 0.109 $ $ 43.344 $ $ \bf{0.297} $
    MSE $ 6.29 E-1 $ $ 1.36 $ $ 5.28 E-3 $ $ 1.78 E-3 $ $ \bf{1.08 E-3} $
     | Show Table
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    Table 4.  Example 1. Performance comparison for Case 3

    APF EnKF IPF DHPF DHIPF
    CPU Time $ 9.563 $ $ 0.453 $ $ 0.156 $ $ 50.188 $ $ \bf{0.422} $
    MSE $ 1.80 $ $ 1.99 $ $ 5.02 E-3 $ $ 1.35 E-2 $ $ \bf{1.59 E-3} $
     | Show Table
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