| Literature DB >> 30249974 |
Yarong Luo1, Chi Guo2, Jiansheng Zheng3, Shengyong You4.
Abstract
A non-linear filtering algorithm based on the alpha-divergence is proposed, which uses the exponential family distribution to approximate the actual state distribution and the alpha-divergence to measure the approximation degree between the two distributions; thus, it provides more choices for similarity measurement by adjusting the value of α during the updating process of the equation of state and the measurement equation in the non-linear dynamic systems. Firstly, an α -mixed probability density function that satisfies the normalization condition is defined, and the properties of the mean and variance are analyzed when the probability density functions p ( x ) and q ( x ) are one-dimensional normal distributions. Secondly, the sufficient condition of the alpha-divergence taking the minimum value is proven, that is when α ≥ 1 , the natural statistical vector's expectations of the exponential family distribution are equal to the natural statistical vector's expectations of the α -mixed probability state density function. Finally, the conclusion is applied to non-linear filtering, and the non-linear filtering algorithm based on alpha-divergence minimization is proposed, providing more non-linear processing strategies for non-linear filtering. Furthermore, the algorithm's validity is verified by the experimental results, and a better filtering effect is achieved for non-linear filtering by adjusting the value of α .Keywords: Kullback–Leibler divergence; alpha-divergence; exponential family distribution; non-linear filtering
Year: 2018 PMID: 30249974 PMCID: PMC6209919 DOI: 10.3390/s18103217
Source DB: PubMed Journal: Sensors (Basel) ISSN: 1424-8220 Impact factor: 3.576
Figure 1Hidden Markov Model (HMM).
The monotonicity of the mean and the variance of the -mixed probability density function.
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Figure 2The monotonicity of the mean and the variance with respect to .
Figure 3State estimation comparison of different non-linear filtering methods.
Figure 4RMS comparison at different times.
Average errors of experiments.
| 1 | 2 | 3 | 4 | 5 | 6 | 7 | |
|---|---|---|---|---|---|---|---|
| EKF | 1.6414 | 1.8434 | 1.8245 | 1.7749 | 1.6666 | 1.3255 | ⋯ |
| UKF | 1.5400 | 1.7703 | 1.6688 | 1.6387 | 1.6241 | 1.2243 | ⋯ |
| AKF | 1.4819 | 1.5921 | 1.4710 | 1.4694 | 1.4389 | 1.1222 | ⋯ |
Influence of the variance Q of state equation noise on experimental error.
| Q | 0.05 | 0.1 | 1 | 10 |
|---|---|---|---|---|
| EKF | 0.2256 | 0.2950 | 0.7288 | 1.7827 |
| UKF | 0.2222 | 0.3002 | 0.7396 | 1.6222 |
| AKF | 0.2167 | 0.2767 | 0.7144 | 1.5244 |
Figure 5The error changes as changes.