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摘要: 3D打印技术是一种新兴的增材制造技术，许多人认为是一项将要改变世界的“破坏性”技术，并声称该技术将引发新一轮工业革命.本文根据3D打印技术涉及的不同核心成型技术、材料和设备体积等，介绍了3D打印技术的不同分类，综述了主流3D打印过程控制技术，指出了3D打印技术的控制系统存在的问题并提出了产业化进程中的建议和意见.Abstract: 3D printing is a new add manufacturing technology, and many people think it is a "destructive" technology that will change the world, claim it will trigger a new round of industrial revolution. According to 3D printing technology involved in different core forming technologies, materials and equipment volumes, this paper introduces the different classifications of 3D printing technology, overviews the mainstream 3D printing technology control system, discusses the problems existing in the control system of 3D printing, and provides suggestions and advices for the process of industrialization.
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近年来, 基于随机有限集的多目标跟踪算法[1-2]引起了学者们的广泛关注.它从集值估计的角度来解决多目标跟踪问题, 避免了传统多目标跟踪算法中复杂的数据关联过程.众所周知, 数据关联一直是多目标跟踪问题的一个难点, 尤其是在目标个数较多且存在杂波的情况下, 关联过程将变得非常复杂.基于随机有限集的多目标跟踪算法利用随机有限集对多目标的状态和观测建模, 在贝叶斯滤波框架下通过递推后验多目标密度来解决多目标跟踪问题.该类算法主要包括概率假设密度(Probability hypothesis density, PHD)滤波器[3-5]、势概率假设密度(Cardinality PHD, CPHD)滤波器[6-7]和势均衡多目标多伯努利(Cardinality balanced multi-target multi-Bernoulli, CBMeMBer)滤波器[8].不同于PHD和CPHD滤波器递推多目标密度的强度和势分布估计, CBMeMBer滤波器直接近似递推后验多目标密度, 使得多目标跟踪问题的求解显得更为直观.随后, 学者们对CBMeMBer滤波器进行了深入地研究, 并取得了一些研究成果[9-13].
基于随机有限集的多目标跟踪算法主要包括高斯混合(Gaussian mixture, GM)和序贯蒙特卡洛(Sequential Monte Carlo, SMC)两种实现方法.这两种实现方法的前提条件是目标的状态和观测模型为隐马尔科夫模型(Hidden Markov model, HMM), 即目标的状态演化过程是一个马尔科夫过程, 而k时刻目标的量测只与当前时刻目标的状态有关.但在实际应用中, 目标模型不一定满足HMM隐含的马尔科夫假设和独立性假设条件.例如过程噪声与量测噪声相关或量测噪声为有色噪声的情况[14].文献[15-18]等提出一种比HMM更为一般化的Pairwise马尔科夫模型(Pairwise Markov model, PMM), 它将目标的状态和量测整体看作一个马尔科夫过程.与HMM的区别在于: 1)目标的状态不一定为马尔科夫过程; 2)目标的量测不仅与当前时刻的状态有关, 而且与该目标上一时刻的量测也有关系[15].因此, 在解决一些实际问题时采用PMM比采用HMM的效果更好.例如在分割问题中, 采用PMM代替HMM可以有效地降低误差率[19].
本文的研究目的是在PMM框架下利用随机有限集解决杂波环境下的多目标跟踪问题.文献[[20-21]已经给出了在PMM框架下的PHD滤波器及其GM实现.但是当目标数较多时, 该滤波器对目标个数的估计会出现欠估计的情况, 且估计精度和效率较差.本文给出了PMM框架下CBMeMBer滤波器的递推过程, 并给出它在线性高斯PMM条件下的GM实现.最后, 采用文献[21]提出的一种满足HMM局部物理特性的线性高斯PMM, 将本文所提算法与GM-PMM-PHD滤波器进行比较.实验结果表明, 本文所提算法对目标数的估计是无偏的, 不存在GM-PMM-PHD滤波器在目标数较多时出现欠估计的情况, 并且本文所提算法的估计精度和效率也优于GM-PMM-PHD滤波器.
1. HMM和PMM
1.1 HMM
在信号处理过程中, 一个重要问题是根据可观测的量测$y\!=\!{{\left\{ {{\mathit{\boldsymbol{y}}}_{k}} \right\}}_{k\in \rm{IN}}}$估计不可观测的状态$x\!=\!{{\left\{ {{\mathit{\boldsymbol{x}}}_{k}} \right\}}_{k\in \rm{IN}}}$, IN表示整数.在HMM中, 假设x为马尔科夫过程, 且k时刻的量测${{\mathit{\boldsymbol{y}}}_{k}}$只与当前时刻的状态${{\mathit{\boldsymbol{x}}}_{k}}$有关, 即[15]
\begin{equation}\label{} p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{0:k-1}} \right)=p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k-1}} \right) \end{equation}
(1) \begin{equation}\label{} p\left( {{\mathit{\boldsymbol{y}}}_{0:k}}|{{\mathit{\boldsymbol{x}}}_{0:k}} \right)=\prod\limits_{i=0}^{k}{p\left( {{\mathit{\boldsymbol{y}}}_{i}}|{{\mathit{\boldsymbol{x}}}_{0:k}} \right)} \end{equation}
(2) \begin{equation}\label{} p\left( {{\mathit{\boldsymbol{y}}}_{i}}|{{\mathit{\boldsymbol{x}}}_{0:k}} \right)=p\left( {{\mathit{\boldsymbol{y}}}_{i}}|{{\mathit{\boldsymbol{x}}}_{i}} \right), \quad 0\le i\le k \end{equation}
(3) $p\left( \cdot \right)$表示概率密度函数.状态${{\mathit{\boldsymbol{x}}}_{k}}$的后验概率密度$p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{y}}}_{0:k}} \right)$可由Bayes递推算法得到[22]:
\begin{equation}\label{} p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{y}}}_{0:k-1}} \right)=\!\int\!{p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k-1}} \right)p\left( {{\mathit{\boldsymbol{x}}}_{k-1}}|{{\mathit{\boldsymbol{y}}}_{0:k-1}} \right){\rm d}{{\mathit{\boldsymbol{x}}}_{k-1}}} \end{equation}
(4) \begin{equation}\label{} p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{y}}}_{0:k}} \right)\propto p\left( {{\mathit{\boldsymbol{y}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k}} \right)p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{y}}}_{0:k-1}} \right) \end{equation}
(5) 在实际应用中, 由于Bayes公式中存在积分运算, 通常不能得到它的解析解.为了使Bayes公式能够递推运算, 考虑如下线性HMM
\begin{equation}\label{} {{\mathit{\boldsymbol{x}}}_{k}}={{F}_{k}}{{\mathit{\boldsymbol{x}}}_{k-1}}+{{\mathit{\boldsymbol{u}}}_{k}} \end{equation}
(6) \begin{equation}\label{} {{\mathit{\boldsymbol{y}}}_{k}}={{H}_{k}}{{\mathit{\boldsymbol{x}}}_{k}}+{{\mathit{\boldsymbol{v}}}_{k}} \end{equation}
(7) ${{F}_{k}}$和${{H}_{k}}$分别表示状态转移矩阵和观测矩阵. ${{\mathit{\boldsymbol{u}}}_{k}}$和${{\mathit{\boldsymbol{v}}}_{k}}$分别表示零均值的过程噪声和量测噪声, 与初始状态${{\mathit{\boldsymbol{x}}}_{0}}$相互独立.若${{\mathit{\boldsymbol{v}}}_{k}}$、${{\mathit{\boldsymbol{u}}}_{k}}$和${{\mathit{\boldsymbol{x}}}_{0}}$均为高斯变量, 则状态${{\mathit{\boldsymbol{x}}}_{k}}$的后验概率密度$p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{y}}}_{0:k}} \right)$为高斯分布, 可以用它的均值和协方差描述.此时, $p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{y}}}_{0:k}} \right)$的Bayes递推过程退化为经典的卡尔曼滤波器[23].
1.2 PMM
在过程噪声与量测噪声相关或量测噪声为有色噪声的情况下, 目标模型不满足HMM隐含的马尔科夫假设和独立性假设条件.此时, 再利用HMM建模是不合适的.文献[15]提出一种比HMM更为一般化的PMM, 它将状态和量测整体$\varepsilon \!=\!\left( x, y \right)$看作马尔科夫过程, 即
\begin{equation}\label{} p\left( {{\mathit{\boldsymbol{\varepsilon }}}_{k}}|{{\mathit{\boldsymbol{\varepsilon }}}_{0:k-1}} \right)=p\left( {{\mathit{\boldsymbol{\varepsilon }} }_{k}}|{{\mathit{\boldsymbol{\varepsilon }} }_{k-1}} \right)=p\left( {{\mathit{\boldsymbol{x}}}_{k}}, {{\mathit{\boldsymbol{y}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k-1}}, {{\mathit{\boldsymbol{y}}}_{k-1}} \right) \end{equation}
(8) 可以有效地处理上述复杂的目标跟踪场景.
在PMM中, x不一定为马尔科夫过程, 且${{\mathit{\boldsymbol{y}}}_{k}}$不仅与当前时刻的状态${{\mathit{\boldsymbol{x}}}_{k}}$有关, 同时与${{\mathit{\boldsymbol{x}}}_{k-1}}$和${{\mathit{\boldsymbol{y}}}_{k-1}}$也有关系.当$p\left( {{\mathit{\boldsymbol{x}}}_{k}}, {{\mathit{\boldsymbol{y}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k-1}}, {{\mathit{\boldsymbol{y}}}_{k-1}} \right)$满足
\begin{equation}\label{} p\left( {{\mathit{\boldsymbol{x}}}_{k}}, {{\mathit{\boldsymbol{y}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k-1}}, {{\mathit{\boldsymbol{y}}}_{k-1}} \right)=p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k-1}} \right)p\left( {{\mathit{\boldsymbol{y}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k}} \right) \end{equation}
(9) 时, PMM就退化为HMM, 即HMM是PMM的一种特殊情况.在PMM框架下, 状态${{\mathit{\boldsymbol{x}}}_{k}}$的后验概率密度$p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{y}}}_{0:k}} \right)$的Bayes公式为[15]
\begin{equation}\label{} p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{y}}}_{0:k}} \right)\propto \int{p\left( {{\mathit{\boldsymbol{\varepsilon }}}_{k}}|{{\mathit{\boldsymbol{\varepsilon }} }_{k-1}} \right)p\left( {{\mathit{\boldsymbol{x}}}_{k-1}}|{{\mathit{\boldsymbol{y}}}_{0:k-1}} \right){\rm d}{{\mathit{\boldsymbol{x}}}_{k-1}}} \end{equation}
(10) 与HMM框架下的Bayes递推算法的不同之处在于它采用$p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k-1}}, {{\mathit{\boldsymbol{y}}}_{k-1}} \right)$和$p\left( {{\mathit{\boldsymbol{y}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k}}, {{\mathit{\boldsymbol{x}}}_{k-1}}, {{\mathit{\boldsymbol{y}}}_{k-1}} \right)$分别代替$p\left( {{\mathit{\boldsymbol{x}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k-1}} \right)$和$p\left( {{\mathit{\boldsymbol{y}}}_{k}}|{{\mathit{\boldsymbol{x}}}_{k}} \right)$.同样, 上式没有解析解.
在线性高斯条件下, PMM模型可以描述为
\begin{equation}\label{} \underbrace{\left[\begin{matrix} {{\mathit{\boldsymbol{x}}}_{k}} \\ {{\mathit{\boldsymbol{y}}}_{k}} \\ \end{matrix} \right]}_{{{\mathit{\boldsymbol{\varepsilon }}}_{k}}}=\underbrace{\left[\begin{matrix} F_{k}^{1}&F_{k}^{2} \\ H_{k}^{1}&H_{k}^{2} \\ \end{matrix} \right]}_{{{B}_{k}}}\underbrace{\left[\begin{matrix} {{\mathit{\boldsymbol{x}}}_{k-1}} \\ {{\mathit{\boldsymbol{y}}}_{k-1}} \\ \end{matrix} \right]}_{{{\mathit{\boldsymbol{\varepsilon }} }_{k-1}}}+{{\mathit{\boldsymbol{w}}}_{k}} \end{equation}
(11) 其中, ${{\left\{ {{\mathit{\boldsymbol{w}}}_{k}} \right\}}_{k\in \rm{IN}}}$表示零均值的高斯白噪声, 它的协方差为
\begin{equation}\label{} {\rm{E}}\left( {{\mathit{\boldsymbol{w}}}_{k}}\mathit{\boldsymbol{w}}_{k}^{\rm{T}} \right)={{\Sigma }_{k}}=\left[\begin{matrix} \Sigma _{k}^{11}&\Sigma _{k}^{12} \\ \Sigma _{k}^{21}&\Sigma _{k}^{22} \\ \end{matrix} \right] \end{equation}
(12) ${{\left\{ {{\mathit{\boldsymbol{w}}}_{k}} \right\}}_{k\in \rm{IN}}}$与初始状态${{\mathit{\boldsymbol{\varepsilon }}}_{0}}$相互独立. ${{\mathit{\boldsymbol{\varepsilon }} }_{0}}$服从正态分布N$\left( \cdot ;{{\mathit{\boldsymbol{m}}}_{0}}, {{P}_{0}} \right)$, ${{\mathit{\boldsymbol{m}}}_{0}}$和${{P}_{0}}$分别表示它的均值和协方差.文献[15]给出了在PMM框架下的卡尔曼滤波器.
2. PMM-CBMeMBer滤波器及其GM实现
文献[8]已经给出在HMM框架下CBMeMBer滤波器的递推过程, 这里不再赘述.下面将直接给出在PMM框架下CBMeMBer滤波器的递推过程, 以及它在线性高斯PMM条件下的GM实现.
2.1 PMM-CBMeMBer滤波器
k时刻监控区域内${{M}_{k}}$个目标的状态集合记为${{X}_{k}}\!\!=\!\!\left\{ \mathit{\boldsymbol{\varepsilon }} _{k}^{\left( i \right)} \right\}_{i=1}^{{{M}_{k}}}$, 其中${{\mathit{\boldsymbol{\varepsilon }}}_{k}}\!\!=\!\!{{\left[\mathit{\boldsymbol{x}}_{k}^{\rm{T}}, \mathit{\boldsymbol{y}}_{k}^{\rm{T}} \right]}^{\rm{T}}}$, ${\mathit{\boldsymbol{x}}_{k}}$和${\mathit{\boldsymbol{y}}_{k}}$分别表示目标的动力学状态和量测.在PMM框架下, $\varepsilon $是一个马尔科夫过程, 它的状态转移概率密度$p\left( {{\mathit{\boldsymbol{\varepsilon }} }_{k}}|{{\mathit{\boldsymbol{\varepsilon }} }_{k-1}} \right)$包含目标的动力学演化模型$p\left( {\mathit{\boldsymbol{x}}_{k}}|{\mathit{\boldsymbol{x}}_{k-1}}, {\mathit{\boldsymbol{y}}_{k-1}} \right)$和传感器的量测模型$p\left( {\mathit{\boldsymbol{y}}_{k}}|{\mathit{\boldsymbol{x}}_{k}}, {\mathit{\boldsymbol{x}}_{k-1}}, {\mathit{\boldsymbol{y}}_{k-1}} \right)$.根据目标的物理特性, 假设目标的存活概率仅与目标的动力学状态有关, 记为${{p}_{s, k}}\left( {\mathit{\boldsymbol{x}}_{k}} \right)$.
k时刻传感器的量测集合记为${{Z}_{k}}\!=\!\left\{ \mathit{\boldsymbol{z}}_{k}^{\left( i \right)} \right\}_{i=1}^{{{N}_{k}}}$, ${{N}_{k}}$表示量测的个数. ${{Z}_{k}}$由源于目标的量测和杂波量测构成, 两者不可区分.根据传感器的物理特性, 假设传感器的检测概率仅与目标的动力学状态有关, 记为${{p}_{d, k}}\left( {\mathit{\boldsymbol{x}}_{k}} \right)$.
在满足如下假设条件下:
1) ${\varepsilon}$为马尔科夫过程, 目标之间相互独立;
2) 新生目标为多伯努利随机有限集, 与存活目标相互独立;
3) 杂波量测与目标产生的量测相互独立, 杂波数服从泊松分布.
PMM-CBMeMBer滤波器的递推过程如下:
步骤1.预测步
假设$k-1$时刻后验多目标密度为多伯努利形式:
\begin{equation}\label{} {{\pi }_{k-1}}=\left\{ \left( r_{k-1}^{\left( i \right)}, p_{k-1}^{\left( i \right)} \right) \right\}_{i=1}^{{{M}_{k-1}}} \end{equation}
(13) $r_{k-1}^{\left( i \right)}\in \left[0, 1 \right]$, 表示$k-1$时刻第i个目标的存在概率, $p_{k-1}^{\left( i \right)}\left( {\mathit{\boldsymbol{\varepsilon }}_{i}} \right)$表示${\mathit{\boldsymbol{\varepsilon }}_{i}}$的概率密度, ${{M}_{k-1}}$表示$k-1$时刻可能出现的最大目标数.则预测多目标密度也为多伯努利形式:
\begin{equation}\label{} {{\pi }_{k|k-1}}\!\!=\!\!\left\{ \!\left( \!r_{P, k|k-1}^{\left( i \right)}, p_{P, k|k-1}^{\left( i \right)} \!\right) \!\right\}_{i=1}^{{{M}_{k-1}}}\!\!\bigcup\! \left\{ \!\left( \!r_{\Gamma, k}^{\left( i \right)}, p_{\Gamma, k}^{\left( i \right)} \!\right) \!\right\}_{i=1}^{{{M}_{\Gamma, k}}} \end{equation}
(14) 前一项表示存活目标的密度, 后一项表示k时刻新生目标的密度.
\begin{equation}\label{} r_{P, k|k-1}^{\left( i \right)}=r_{k-1}^{\left( i \right)}\left\langle p_{k-1}^{\left( i \right)}, {{p}_{s, k}} \right\rangle \end{equation}
(15) \begin{equation}\label{} p_{P, k|k-1}^{\left( i \right)}\left( \mathit{\boldsymbol{\varepsilon }} \right)=\frac{\left\langle {{p}_{k|k-1}}\left( \mathit{\boldsymbol{\varepsilon }} |\cdot \right), p_{k-1}^{\left( i \right)}{{p}_{s, k}} \right\rangle }{\left\langle p_{k-1}^{\left( i \right)}, {{p}_{s, k}} \right\rangle } \end{equation}
(16) $\left\langle \cdot, \cdot \right\rangle $表示内积运算, 如$\left\langle \alpha, \beta \right\rangle =\int{\alpha \left( x \right)\beta \left( x \right){\rm d}x}$.
步骤2.更新步
假设k时刻预测多目标密度为多伯努利形式
\begin{equation}\label{} {{\pi }_{k|k-1}}=\left\{ \left( r_{k|k-1}^{\left( i \right)}, p_{k|k-1}^{\left( i \right)} \right) \right\}_{i=1}^{{{M}_{k|k-1}}} \end{equation}
(17) 则后验多目标密度可由如下多伯努利形式近似
\begin{equation}\label{} {{\pi }_{k}}\!\approx \!\left\{ \!\left( r_{L, k}^{\left( i \right)}, p_{L, k}^{\left( i \right)} \right) \!\right\}_{i=1}^{{{M}_{k|k-1}}}\!\!\bigcup\! {{\left\{ \!\left( {{r}_{U, k}}\left( \mathit{\boldsymbol{z}} \right)\!, {{p}_{U, k}}\!\left( \cdot ;\mathit{\boldsymbol{z}} \right)\! \right) \!\right\}}_{\mathit{\boldsymbol{z}}\in {{Z}_{k}}}} \end{equation}
(18) 前一项表示漏检部分的多目标密度, 后一项表示量测更新部分的多目标密度.
\begin{equation}\label{} r_{L, k}^{\left( i \right)}=r_{k|k-1}^{\left( i \right)}\frac{1-\left\langle p_{k|k-1}^{\left( i \right)}, {{p}_{d, k}} \right\rangle }{1-r_{k|k-1}^{\left( i \right)}\left\langle p_{k|k-1}^{\left( i \right)}, {{p}_{d, k}} \right\rangle } \end{equation}
(19) \begin{equation}\label{} p_{L, k}^{\left( i \right)}\left( \mathit{\boldsymbol{\varepsilon }} \right)=p_{k|k-1}^{\left( i \right)}\left( \mathit{\boldsymbol{\varepsilon }} \right)\frac{1-{{p}_{d, k}}\left( \mathit{\boldsymbol{x}} \right)}{1-\left\langle p_{k|k-1}^{\left( i \right)}, {{p}_{d, k}} \right\rangle } \end{equation}
(20) \begin{equation}\label{} {{r}_{U, k}}\left( \mathit{\boldsymbol{z}} \right)\!=\!\frac{\sum\limits_{i=1}^{{{M}_{k|k-1}}}{\frac{r_{k|k-1}^{\left( i \right)}\left( 1-r_{k|k-1}^{\left( i \right)} \right)\left\langle p_{k|k-1}^{\left( i \right)}, {{\psi }_{k, \mathit{\boldsymbol{z}}}} \right\rangle }{{{\left( 1-r_{k|k-1}^{\left( i \right)}\left\langle p_{k|k-1}^{\left( i \right)}, {{p}_{d, k}} \right\rangle \right)}^{2}}}}}{{{\kappa }_{k}}\left( \mathit{\boldsymbol{z}} \right)\!+\!\sum\limits_{i=1}^{{{M}_{k|k-1}}}{\frac{r_{k|k-1}^{\left( i \right)}\left\langle p_{k|k-1}^{\left( i \right)}, {{\psi }_{k, \mathit{\boldsymbol{z}}}} \right\rangle }{1-r_{k|k-1}^{\left( i \right)}\left\langle p_{k|k-1}^{\left( i \right)}, {{p}_{d, k}} \right\rangle }}} \end{equation}
(21) \begin{equation}\label{} {{p}_{U, k}}\left( \mathit{\boldsymbol{\varepsilon }} ;\mathit{\boldsymbol{z}} \right)\!=\!\frac{\sum\limits_{i=1}^{{{M}_{k|k-1}}}{\frac{r_{k|k-1}^{\left( i \right)}}{1-r_{k|k-1}^{\left( i \right)}}p_{k|k-1}^{\left( i \right)}\left( \mathit{\boldsymbol{\varepsilon }} \right){{\psi }_{k, \mathit{\boldsymbol{z}}}}\left( \mathit{\boldsymbol{\varepsilon }} \right)}}{\sum\limits_{i=1}^{{{M}_{k|k-1}}}{\frac{r_{k|k-1}^{\left( i \right)}}{1-r_{k|k-1}^{\left( i \right)}}\left\langle p_{k|k-1}^{\left( i \right)}{{\psi }_{k, \mathit{\boldsymbol{z}}}} \right\rangle }} \end{equation}
(22) ${{\psi }_{k, \mathit{\boldsymbol{z}}}}\left( \mathit{\boldsymbol{\varepsilon }} \right)={{p}_{d, k}}\left( \mathit{\boldsymbol{x}} \right){g_k}\left( {\mathit{\boldsymbol{z}}|\mathit{\boldsymbol{x}}} \right)$
${{\kappa }_{k}}\left( \cdot \right)$表示k时刻杂波的强度, ${g_k}\left( {\mathit{\boldsymbol{z}}|\mathit{\boldsymbol{x}}} \right)$表示目标$\mathit{\boldsymbol{x}}$的似然函数.
在上述递推过程中, 若状态转移函数${{p}_{k|k-1}}$满足式(9), 并且新生目标模型满足:
\begin{equation}\label{} {{\gamma }_{\Gamma, k}}\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}} \right)={{g}_{k}}\left( \mathit{\boldsymbol{y}}|\mathit{\boldsymbol{x}} \right){{\tilde{\gamma }}_{\Gamma, k}}\left( \mathit{\boldsymbol{x}} \right) \end{equation}
(23) ${{\tilde{\gamma }}_{\Gamma, k}}\left( \mathit{\boldsymbol{x}} \right)$表示仅与目标动力学状态相关的新生目标密度函数.此时, PMM-CBMeMBer滤波算法就退化为HMM-CBMeMBer滤波算法.
2.2 PMM-CBMeMBer滤波器的GM实现
下面给出PMM-CBMeMBer滤波器在线性高斯条件下的GM实现.
在新生目标模型中, 若$p_{\Gamma, k}^{\left( i \right)}$为GM形式:
\begin{equation}\label{} p_{\Gamma, k}^{\left( i \right)}\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}} \right)\!=\!\sum\limits_{j=1}^{J_{\Gamma, k}^{\left( i \right)}}{\omega _{\Gamma, k}^{\left( i, j \right)}N\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}};\mathit{\boldsymbol{m}}_{\Gamma, k}^{\left( i, j \right)}, P_{\Gamma, k}^{\left( i, j \right)} \right)} \end{equation}
(24) 其中, $J_{\Gamma, k}^{\left( i \right)}$表示第i个目标对应的高斯项个数, $\omega _{\Gamma , k}^{\left( i, j \right)}$、$\mathit{\boldsymbol{m}}_{\Gamma, k}^{\left( i, j \right)}$和$P_{\Gamma, k}^{\left( i, j \right)}$分别表示第i个目标中第j个高斯项的权重、均值和协方差.则GM-PMM-CBMeMBer滤波器的递推过程如下:
步骤1.预测步
假设$k-1$时刻后验多目标密度
\begin{equation}\label{} {{\pi }_{k-1}}\!=\!\left\{\! \left( r_{k-1}^{1, \left( i \right)}, p_{k-1}^{1, \left( i \right)} \right)\! \right\}_{i=1}^{M_{k-1}^{1}}\!\bigcup\! \left\{\! \left( r_{k-1}^{2, \left( i \right)}, p_{k-1}^{2, \left( i \right)} \right)\! \right\}_{i=1}^{M_{k-1}^{2}} \end{equation}
(25) 已知, $p_{k-1}^{\ell, \left( i \right)}$, $\ell =\left\{ 1, 2 \right\}$, 为如下GM形式,
\begin{equation}\label{} p_{k-1}^{1, \left( i \right)}\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}} \right)=\sum\limits_{j=1}^{J_{k-1}^{1, \left( i \right)}}{\omega _{k-1}^{1, \left( i, j \right)}{\rm N}\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}};\mathit{\boldsymbol{m}}_{k-1}^{1, \left( i, j \right)}, P_{k-1}^{1, \left( i, j \right)} \right)} \end{equation}
(26) \begin{equation}\label{} p_{k-1}^{2, \left( i \right)}\!\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}} \right)\!=\!\!\sum\limits_{j=1}^{J_{k-1}^{2, \left( i \right)}}\!{\omega _{k-1}^{2, \left( i, j \right)}\!{\rm N}\!\!\left( \!\mathit{\boldsymbol{x}};\mathit{\boldsymbol{m}}_{k-1}^{2, \left( i, j \right)}\!, P_{k-1}^{2, \left( i, j \right)} \!\right)\!{{\delta }_{{{\mathit{\boldsymbol{z}}}^{\left( i \right)}}}}\!\left( \mathit{\boldsymbol{y}} \right)} \end{equation}
(27) ${{\delta }_{{{\mathit{\boldsymbol{z}}}^{\left( i \right)}}}}\!\left( \mathit{\boldsymbol{y}} \right)$为Dirac delta函数[2], ${{\mathit{\boldsymbol{z}}}^{\left( i \right)}}\in {{Z}_{k-1}}$, ${\mathit{\boldsymbol{y}}}$表示状态为${\mathit{\boldsymbol{x}}}$对应的量测.若${{\mathit{\boldsymbol{z}}}^{\left( i \right)}}=\mathit{\boldsymbol{y}}$, 说明${{\mathit{\boldsymbol{z}}}^{\left( i \right)}}$是由$\mathit{\boldsymbol{x}}$产生的量测; 否则, $\mathit{\boldsymbol{z}}^{\left( i \right)}$不是由${\mathit{\boldsymbol{x}}}$产生的量测.则预测多目标密度
\begin{align} {\pi _{k|k - 1}} \!=&\! \left\{ {\!\left( {r_{P, k|k - 1}^{1, \left( i \right)}, p_{P, k|k - 1}^{1, \left( i \right)}} \right)} \!\right\}_{i = 1}^{M_{k - 1}^1} \cup \nonumber\\ &\left\{ {\!\left( {r_{P, k|k - 1}^{2, \left( i \right)}, p_{P, k|k - 1}^{2, \left( i \right)}} \right)} \!\right\}_{i = 1}^{M_{k - 1}^2} \!\cup\!\nonumber\\ &\left\{ {\!\left( {r_{\Gamma, k}^{\left( i \right)}, p_{\Gamma, k}^{\left( i \right)}} \right)} \!\right\}_{i = 1}^{{M_{\Gamma, k}}} \end{align}
(28) 可由如下公式得到:
\begin{align} &r_{P, k|k-1}^{\ell, \left( i \right)}={{p}_{s, k}}r_{k-1}^{\ell , \left( i \right)}, \quad \ell =\left\{ 1, 2 \right\} \end{align}
(29) \begin{align} &p_{P, k|k-1}^{1, \left( i \right)}\!\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}} \right)\!=\nonumber\\ &\qquad\sum\limits_{j=1}^{J_{k-1}^{1, \left( i \right)}}\!\!{\omega _{k-1}^{1, \left( i, j \right)}\!{\rm N}\!\!\left(\! \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}};\mathit{\boldsymbol{m}}_{P, k|k-1}^{1, \left( i, j \right)}, P_{P, k|k-1}^{1, \left( i, j \right)} \!\right)}\end{align}
(30) \begin{align} &p_{P, k|k-1}^{2, \left( i \right)}\!\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}} \right)\!=\nonumber\\ &\qquad\sum\limits_{j=1}^{J_{k-1}^{2, \left( i \right)}}\!\!{\omega _{k-1}^{2, \left( i, j \right)}\!{\rm N}\!\!\left( \!\mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}};\mathit{\boldsymbol{m}}_{P, k|k-1}^{2, \left( i, j \right)}, P_{P, k|k-1}^{2, \left( i, j \right)} \!\right)} \end{align}
(31) 其中
\begin{equation}\label{} \mathit{\boldsymbol{m}}_{P, k|k-1}^{1, \left( i, j \right)}\!=\!{{B}_{k}}\mathit{\boldsymbol{m}}_{k-1}^{1, \left( i, j \right)}, \mathit{\boldsymbol{m}}_{P, k|k-1}^{2, \left( i, j \right)}\!=\!{{B}_{k}}\!\left[\begin{matrix} \mathit{\boldsymbol{m}}_{k-1}^{2, \left( i, j \right)} \\ {{\mathit{\boldsymbol{z}}}^{\left( i \right)}} \\ \end{matrix} \right] \end{equation}
(32) \begin{equation}\label{} P_{P, k|k-1}^{1, \left( i, j \right)}={{\Sigma }_{k}}+{{B}_{k}}P_{k-1}^{1, \left( i, j \right)}B_{k}^{\rm{T}} \end{equation}
(33) \begin{equation}\label{} P_{P, k|k-1}^{2, \left( i, j \right)}={{\Sigma }_{k}}+\left[\begin{matrix} F_{k}^{1} \\ H_{k}^{1} \\ \end{matrix} \right]P_{k-1}^{2, \left( i, j \right)}\left[\begin{matrix} {{\left( F_{k}^{1} \right)}^{\rm{T}}}&{{\left( H_{k}^{1} \right)}^{\rm{T}}} \\ \end{matrix} \right] \end{equation}
(34) 新生目标模型已知, $p_{\Gamma, k}^{\left( i \right)}$见式(24).
步骤2.更新步
在式(28)中, 由于组成预测多目标密度的三个部分形式相同, 令${{M}_{k|k-1}}=M_{k-1}^{1}+M_{k-1}^{2}+{{M}_{\Gamma, k}}$, 它们可以重写为
\begin{equation}\label{} {{\pi }_{k|k-1}}=\left\{ \left( r_{k|k-1}^{\left( i \right)}, p_{k|k-1}^{\left( i \right)} \right) \right\}_{i=1}^{{{M}_{k|k-1}}} \end{equation}
(35) \begin{equation}\label{} p_{k|k-1}^{\left( i \right)}\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}} \right)\!=\!\sum\limits_{j=1}^{J_{k|k-1}^{\left( i \right)}}\!{\omega _{k|k-1}^{\left( i, j \right)}{\rm N}\!\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}};\mathit{\boldsymbol{m}}_{k|k-1}^{\left( i, j \right)}, P_{k|k-1}^{\left( i, j \right)} \right)} \end{equation}
(36) \begin{equation}\label{} \mathit{\boldsymbol{m}}_{k|k-1}^{\left( i, j \right)}\!=\!\left[\begin{matrix} \mathit{\boldsymbol{m}}_{k|k-1}^{\mathit{\boldsymbol{x}}, \left( i, j \right)} \\ \mathit{\boldsymbol{m}}_{k|k-1}^{\mathit{\boldsymbol{y}}, \left( i, j \right)} \\ \end{matrix} \right]\!, P_{k|k-1}^{\left( i, j \right)}\!=\!\left[\begin{matrix} P_{k|k-1}^{\mathit{\boldsymbol{x}}, \left( i, j \right)} \!&\! P_{k|k-1}^{\mathit{\boldsymbol{xy}}, \left( i, j \right)} \\ P_{k|k-1}^{\mathit{\boldsymbol{yx}}, \left( i, j \right)} \!&\! P_{k|k-1}^{\mathit{\boldsymbol{y}}, \left( i, j \right)} \\ \end{matrix} \right] \end{equation}
(37) 则更新多目标密度
\begin{align} {{\pi }_{k}}\!=&\!\left\{ \!\left( r_{L, k}^{\left( i \right)}, p_{L, k}^{\left( i \right)} \right) \!\right\}_{i=1}^{{{M}_{k|k-1}}}\!\bigcup\!\nonumber\\&{{\left\{ \!\left( {{r}_{U, k}}\!\left( \mathit{\boldsymbol{z}} \right)\!, {{p}_{U, k}}\!\left( \cdot ;\mathit{\boldsymbol{z}} \right) \right) \!\right\}}_{\mathit{\boldsymbol{z}}\in {{Z}_{k}}}} \end{align}
(38) 可由如下公式得到:
\begin{equation}\label{} r_{L, k}^{\left( i \right)}=r_{k|k-1}^{\left( i \right)}\frac{1-{{p}_{d, k}}}{1-r_{k|k-1}^{\left( i \right)}{{p}_{d, k}}} \end{equation}
(39) \begin{equation}\label{} p_{L, k}^{\left( i \right)}\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}} \right)=p_{k|k-1}^{\left( i \right)}\left( \mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}} \right) \end{equation}
(40) \begin{equation}\label{} {{r}_{U, k}}\left( \mathit{\boldsymbol{z}} \right)=\frac{\sum\limits_{i=1}^{{{M}_{k|k-1}}}{\frac{r_{k|k-1}^{\left( i \right)}\left( 1-r_{k|k-1}^{\left( i \right)} \right)\rho _{U, k}^{\left( i \right)}\left( \mathit{\boldsymbol{z}} \right)}{{{\left( 1-r_{k|k-1}^{\left( i \right)}{{p}_{d, k}} \right)}^{2}}}}}{{{\kappa }_{k}}\left( \mathit{\boldsymbol{z}} \right)+\sum\limits_{i=1}^{{{M}_{k|k-1}}}{\frac{r_{k|k-1}^{\left( i \right)}\rho _{U, k}^{\left( i \right)}\left( \mathit{\boldsymbol{z}} \right)}{1-r_{k|k-1}^{\left( i \right)}{{p}_{d, k}}}}} \end{equation}
(41) \begin{equation}\label{} {p_{U, k}}\!\left( \!{\mathit{\boldsymbol{x}}, \mathit{\boldsymbol{y}};\mathit{\boldsymbol{z}}} \!\right)\! =\! \frac{{\sum\limits_{i = 1}^{{M_{k|k - 1}}}\! {\sum\limits_{j = 1}^{J_{k|k - 1}^{\left( i \right)}} \!\!{\omega _{U, k}^{\left( {i, j} \right)}\!\!\left( \mathit{\boldsymbol{z}} \right)\!{\rm N}\!\!\left( \! {\mathit{\boldsymbol{x}};\mathit{\boldsymbol{m}}_{U, k}^{\left( {i, j} \right)}\!, P_{U, k}^{\left( {i, j} \right)}} \!\right)} } }}{{\sum\limits_{i = 1}^{{M_{k|k - 1}}} {\sum\limits_{j = 1}^{J_{k|k - 1}^{\left( i \right)}} {\omega _{U, k}^{\left( {i, j} \right)}\left( \mathit{\boldsymbol{z}} \right)} } }} \end{equation}
(42) 其中
\begin{equation}\label{} \rho _{U, k}^{\left( i \right)}\left( \mathit{\boldsymbol{z}} \right)={{p}_{d, k}}\sum\limits_{j=1}^{J_{k|k-1}^{\left( i \right)}}{\omega _{k|k-1}^{\left( i, j \right)}q_{k}^{\left( i, j \right)}\left( \mathit{\boldsymbol{z}} \right)} \end{equation}
(43) \begin{equation}\label{} q_{k}^{\left( i, j \right)}\left( \mathit{\boldsymbol{z}} \right)={\rm N}\left( \mathit{\boldsymbol{z}};\mathit{\boldsymbol{m}}_{k|k-1}^{\mathit{\boldsymbol{y}}, \left( i, j \right)}, P_{k|k-1}^{\mathit{\boldsymbol{y}}, \left( i, j \right)} \right) \end{equation}
(44) \begin{equation}\label{} \omega _{U, k}^{\left( i, j \right)}\left( \mathit{\boldsymbol{z}} \right)=\frac{r_{k|k-1}^{\left( i \right)}}{1-r_{k|k-1}^{\left( i \right)}}{{p}_{d, k}}\omega _{k|k-1}^{\left( i, j \right)}q_{k}^{\left( i, j \right)}\left( \mathit{\boldsymbol{z}} \right) \end{equation}
(45) \begin{equation}\label{} \mathit{\boldsymbol{m}}_{U, k}^{\left( i, j \right)}\left( \mathit{\boldsymbol{z}} \right)=\mathit{\boldsymbol{m}}_{k|k-1}^{\mathit{\boldsymbol{x}}, \left( i, j \right)}+K_{U, k}^{\left( i, j \right)}\left( \mathit{\boldsymbol{z}}-\mathit{\boldsymbol{m}}_{k|k-1}^{\mathit{\boldsymbol{y}}, \left( i, j \right)} \right) \end{equation}
(46) \begin{equation}\label{} P_{U, k}^{\left( i, j \right)}=P_{k|k-1}^{\mathit{\boldsymbol{x}}, \left( i, j \right)}-K_{U, k}^{\left( i, j \right)}{{\left( P_{k|k-1}^{\mathit{\boldsymbol{xy}}, \left( i, j \right)} \right)}^{\rm{T}}} \end{equation}
(47) \begin{equation}\label{} K_{U, k}^{\left( i, j \right)}=P_{k|k-1}^{\mathit{\boldsymbol{xy}}, \left( i, j \right)}{{\left( P_{k|k-1}^{\mathit{\boldsymbol{y}}, \left( i, j \right)} \right)}^{-1}} \end{equation}
(48) 在更新步中, 漏检部分的状态包括动力学状态和相应的量测, 协方差也是动力学状态和量测整体的协方差; 量测更新部分给出了动力学状态的求解, 式(46)中的$\mathit{\boldsymbol{z}}$表示该动力学状态对应的量测, 式(47)为目标动力学状态的协方差, 不包括量测以及量测与动力学状态的协方差.即算法中漏检部分和量测更新部分对应的多目标密度的表示形式不同, 故在$k-1$时刻将多目标密度假设为相应的两部分.
根据GM-HMM-PHD滤波器得到的后验多目标强度的高斯项个数[5], 不难得到在不考虑衍生目标的情况下GM-HMM-CBMeMBer滤波器的后验多目标密度的高斯项个数为$\left(\! \sum\nolimits_{i=1}^{{{M}_{k-1}}}\!\!{J_{k-1}^{\left( i \right)}}\!+\!\sum\nolimits_{i=1}^{{{M}_{\Gamma, k}}}\!\!{J_{\Gamma , k}^{\left( i \right)}} \!\right)\!\left( \!1\!+\!\left| {{Z}_{k}} \right|\! \right)$, GM-PMM-CBMeMBer滤波器的后验多目标密度的高斯项个数为$\left( \! \sum\nolimits_{i=1}^{M_{k-1}^{1}}\!\!{J_{k-1}^{1, \left( i \right)}}\!+\!\sum\nolimits_{i=1}^{M_{k-1}^{2}}\!\!{J_{k-1}^{2, \left( i \right)}}\!+\!\sum\nolimits_{i=1}^{{{M}_{\Gamma , k}}}\!\!{J_{\Gamma, k}^{\left( i \right)}} \!\right)\!$ $(\! 1\!+\!| {{Z}_{k}} | \!)$.在相同场景下, GM-PMM-CBMeMBer滤波器和GM-HMM-CBMeMBer滤波器的计算复杂度为同一数量级.但由于GM-PMM-CBMeMBer滤波器状态维数的增加, 计算量会相应增大.
由于新生目标的出现和更新步中假设轨迹的平均化, 航迹个数和每条航迹对应的高斯项会逐渐增加, 需要采用剪切和合并技术[5]进行处理: 1)剪切.一是航迹的剪切, 去掉存在概率小于阈值为${{T}_{r}}$的航迹; 二是航迹对应的高斯项的剪切, 去掉权值小于阈值为${{T}_{\omega }}$的高斯项. 2)合并.在每条航迹中, 将距离小于阈值为U的高斯项进行合并.由于在后验多目标密度中漏检部分和量测更新部分对应的高斯项的形式不同, 在合并过程中需要加以区分.同时, 设定航迹数的最大值为${{M}_{\max }}$, 每条航迹对应的高斯项个数的最大值为${{J}_{\max }}$.最后, 对目标的状态进行提取.若航迹的存在概率大于给定阈值(如0.5), 则认为它是一个目标, 选择它对应的权值最大的高斯项作为目标的状态.
3. 仿真
3.1 一种满足HMM局部物理特性的PMM
文献[21]总结了过程噪声与量测噪声相关和量测噪声为有色噪声对应的PMM, 并提出一种满足HMM局部物理特性的PMM.为了与HMM框架下的CBMeMBer滤波器的性能进行比较, 本文采用上述满足HMM局部物理特性的PMM进行仿真实验.并将本文所提算法的跟踪性能与PHD滤波器[21]进行比较.下面首先给出该PMM的描述.
假设线性高斯HMM为
\begin{equation}\label{} p\left( {\mathit{\boldsymbol{x}}_{0}} \right)={\rm N}\left( {\mathit{\boldsymbol{x}}_{0}};{\mathit{\boldsymbol{m}}_{0}}, {{P}_{0}} \right) \end{equation}
(49) \begin{equation}\label{} {{f}_{k|k-1}}\left( {\mathit{\boldsymbol{x}}_{k}}|{\mathit{\boldsymbol{x}}_{k-1}} \right)={\rm N}\left( {\mathit{\boldsymbol{x}}_{k}};{{F}_{k}}{\mathit{\boldsymbol{x}}_{k-1}}, {{Q}_{k}} \right) \end{equation}
(50) \begin{equation}\label{} {{g}_{k}}\left( {\mathit{\boldsymbol{y}}_{k}}|{\mathit{\boldsymbol{x}}_{k}} \right)={\rm N}\left( {\mathit{\boldsymbol{y}}_{k}};{{H}_{k}}{\mathit{\boldsymbol{x}}_{k}}, {{R}_{k}} \right) \end{equation}
(51) 则满足$p\left( {\mathit{\boldsymbol{x}}_{k}}|{\mathit{\boldsymbol{x}}_{k-1}} \right)={{f}_{k|k-1}}\left( {\mathit{\boldsymbol{x}}_{k}}|{\mathit{\boldsymbol{x}}_{k-1}} \right)$, $p( {\mathit{\boldsymbol{y}}_{k}}|{\mathit{\boldsymbol{x}}_{k}})={{g}_{k}}\left( {\mathit{\boldsymbol{y}}_{k}}|{\mathit{\boldsymbol{x}}_{k}} \right)$, 且${{p}_{k|k-1}}=\left( {\mathit{\boldsymbol{x}}_{k}}, {\mathit{\boldsymbol{y}}_{k}}|{\mathit{\boldsymbol{x}}_{k-1}}, {\mathit{\boldsymbol{y}}_{k-1}} \right)$不依赖于参数$\left( {\mathit{\boldsymbol{m}}_{0}}, {{P}_{0}} \right)$的线性高斯PMM为
\begin{equation}\label{} p\left( {\mathit{\boldsymbol{\varepsilon }}_{0}} \right)\!=\!{\rm N}\left( {\mathit{\boldsymbol{\varepsilon }}_{0}};\left[\begin{matrix} {\mathit{\boldsymbol{m}}_{0}} \\ {{H}_{0}}{\mathit{\boldsymbol{m}}_{0}} \\ \end{matrix} \right]\!, \left[\begin{matrix} {{P}_{0}} \!&\! {{\left( {{H}_{0}}{{P}_{0}} \right)}^{\rm{T}}} \\ {{H}_{0}}{{P}_{0}}\! &\! {{R}_{0}}\!+\!{{H}_{0}}{{P}_{0}}H_{0}^{\rm{T}} \\ \end{matrix} \right] \right) \end{equation}
(52) \begin{equation}\label{} {{p}_{k|k-1}}\left( {\mathit{\boldsymbol{\varepsilon }}_{k}}|{\mathit{\boldsymbol{\varepsilon }}_{k-1}} \right)={\rm N}\left( {\mathit{\boldsymbol{\varepsilon }}_{k}};{{B}_{k}}{\mathit{\boldsymbol{\varepsilon }}_{k-1}}, {{\Sigma }_{k}} \right) \end{equation}
(53) 其中
\begin{equation}\label{} {{B}_{k}}=\left[\begin{matrix} {{F}_{k}}-F_{k}^{2}{{H}_{k-1}}&F_{k}^{2} \\ {{H}_{k}}{{F}_{k}}-H_{k}^{2}{{H}_{k-1}}&H_{k}^{2} \\ \end{matrix} \right] \end{equation}
(54) \begin{equation}\label{} {{\Sigma }_{k}}=\left[\begin{matrix} \Sigma _{k}^{11}&\Sigma _{k}^{12} \\ \Sigma _{k}^{21}&\Sigma _{k}^{22} \\ \end{matrix} \right] \end{equation}
(55) \begin{equation}\label{} \Sigma _{k}^{11}={{Q}_{k}}-F_{k}^{2}{{R}_{k-1}}{{\left( F_{k}^{2} \right)}^{\rm{T}}} \end{equation}
(56) \begin{equation}\label{} \Sigma _{k}^{21}={{\left( \Sigma _{k}^{12} \right)}^{\rm{T}}}={{H}_{k}}{{Q}_{k}}-H_{k}^{2}{{R}_{k-1}}{{\left( F_{k}^{2} \right)}^{\rm{T}}} \end{equation}
(57) \begin{equation}\label{} \Sigma _{k}^{22}={{R}_{k}}-H_{k}^{2}{{R}_{k-1}}{{\left( H_{k}^{2} \right)}^{\rm{T}}}+{{H}_{k}}{{Q}_{k}}H_{k}^{\rm{T}} \end{equation}
(58) 在满足${{\Sigma }_{k}}$为正定矩阵的情况下, $F_{k}^{2}$和$H_{k}^{2}$可以任意选取.
3.2 仿真分析
为了与PHD滤波器的跟踪性能进行比较, 依据文献[21]对上述PMM的参数进行设置.
\begin{equation}\label{} {{F}_{k}}=\left[\begin{matrix} 1&t&0&0 \\ 0&1&0&0 \\ 0&0&1&t \\ 0&0&0&1 \\ \end{matrix} \right], \quad {{H}_{k}}=\left[\begin{matrix} 1&0&0&0 \\ 0&0&1&0 \\ \end{matrix} \right] \end{equation}
(59) \begin{equation}\label{} {{Q}_{k}}=\left[\begin{matrix} 100&1&0&0 \\ 1&10&0&0 \\ 0&0&100&1 \\ 0&0&1&10 \\ \end{matrix} \right], \quad {{R}_{k}}=\left[\begin{matrix} {{10}^{2}}&0 \\ 0&{{10}^{2}} \\ \end{matrix} \right] \end{equation}
(60) \begin{equation}\label{} F_{k}^{2}=\left[\begin{matrix} a&0 \\ 0&0 \\ 0&b \\ 0&0 \\ \end{matrix} \right], \quad H_{k}^{2}=\left[\begin{matrix} c&0 \\ 0&d \\ \end{matrix} \right] \end{equation}
(61) 令$t=1$, $a=b=0.7$, $c=d=0.1$.仿真硬件环境为Matlab R2013b, Windows 10 64bit, Intel Core i5-4570 CPU 3.20GHz, RAM 4.00GB.
监控区域内有12个目标:目标1、2和3在$k=1$时出现, 4、5和6在$k=20$时出现, 7和8在$k=40$时出现, 9和10在$k=60$时出现, 11和12在$k=80$时出现, 而目标1和2在$k=70$时消失, 其他目标不消失.目标的状态为${\mathit{\boldsymbol{x}}_{k}}={{\left[ {{x}_{k}}, {{{\dot{x}}}_{k}}, {{y}_{k}}, {{{\dot{y}}}_{k}} \right]}^{\rm{T}}}$, ${{x}_{k}}$和${{y}_{k}}$表示二维笛卡尔坐标系下目标的位置, ${{\dot{x}}_{k}}$和${{\dot{y}}_{k}}$分别表示对应方向的速度.在监控区域$V=\left[-2000, ~2000 \right]\rm{m}\times \left[ -2000, ~2000 \right]m$中, 各采样时刻的杂波个数服从均值为20的泊松分布, 杂波量测在监控区域内均匀分布. 图 1是基于上述线性高斯PMM的目标运动轨迹, 红色三角形表示目标的初始位置.
CBMeMBer滤波器中新生目标的模型参数${{\pi }_{\Gamma }}\!\!=\!\!\left\{ \left( {{r}_{\Gamma }}, p_{\Gamma }^{\left( i \right)} \right) \right\}_{i=1}^{4}$设置如下:在HMM中, ${{r}_{\Gamma }}\!\!=\!\!0.01$, $p_{\Gamma }^{\left( i \right)}\left( x \right) \!\!=\!\!{\rm N}\left( \mathit{\boldsymbol{x}};\mathit{\boldsymbol{m}}_{\Gamma }^{\left( i \right)}, {{P}_{\Gamma }} \right)$, $\mathit{\boldsymbol{m}}_{\Gamma }^{\left( 1 \right)}\!\!=\!\!{{\left[0, 0, 0, 0 \right]}^{\rm{T}}}$, $\mathit{\boldsymbol{m}}_{\Gamma }^{\left( 2 \right)}\!\!=\!\!{{\left[400, 0, -600, 0 \right]}^{\rm{T}}}$, $\mathit{\boldsymbol{m}}_{\Gamma }^{\left( 3 \right)}\!\!=\!\!{{\left[-800, 0, -200, 0 \right]}^{\rm{T}}}$, $\mathit{\boldsymbol{m}}_{\Gamma }^{\left( 4 \right)}\!\!=\!\!{{\left[-200, 0, 800, 0 \right]}^{\rm{T}}}$, ${{P}_{\Gamma }}\!\!=\!\!\rm{diag}\left\{\!1000, 400, 1000, 400 \right\}$; 在PMM中, ${{r}_{\Gamma }}=0.01$,
$p_\Gamma ^{\left( i \right)}\left( \mathit{\boldsymbol{\varepsilon }} \right) = {\rm{N}}\left( {\mathit{\boldsymbol{\varepsilon }};\left[ {\begin{array}{*{20}{c}} {\mathit{\boldsymbol{m}}_\Gamma ^{\left( i \right)}}\\ {{H_k}\mathit{\boldsymbol{m}}_\Gamma ^{\left( i \right)}} \end{array}} \right],\left[ {\begin{array}{*{20}{c}} {{P_\Gamma }}&{{{\left( {{H_k}{P_\Gamma }} \right)}^{\rm{T}}}}\\ {{H_k}{P_\Gamma }}&{{R_k} + {H_k}{P_\Gamma }H_k^{\rm{T}}} \end{array}} \right]} \right)$
$i=\left\{ 1, \cdots, 4 \right\}$.目标的存活概率为${{p}_{s, k}}=0.98$, 传感器的检测概率为${{p}_{d, k}}=0.9$.在剪切和合并过程中, 设航迹存在概率的阈值为${{T}_{r}}={{10}^{-3}}$, 高斯项权值的阈值为${{T}_{\omega }}={{10}^{-5}}$, 合并阈值为$U=4\rm{m}$, 航迹的最大值为${{M}_{\max }}=100$, 每条航迹对应高斯项个数的最大值为${{J}_{\max }}=30$. PHD滤波器新生目标的模型参数见文献[21].
图 2给出了GM-PMM-CBMeMBer滤波器单次仿真的结果, 两个子图分别对应不同时刻X轴和Y轴的状态估计.整体来看, 所提算法可以比较准确地估计目标的状态.在某些时刻会出现虚假目标或目标跟踪丢失的情况, 但随着时间推移, 算法自身可以很快地进行修正.
本文采用OSPA (Optimal subpattern assignment)距离[24]评估算法的跟踪性能.设多目标真实状态的集合为$X=\left\{ {\mathit{\boldsymbol{x}}_{1}}, \cdots , {\mathit{\boldsymbol{x}}_{m}} \right\}$, 估计状态的集合为$\hat{X}=\left\{ {{{\hat{\mathit{\boldsymbol{x}}}}}_{1}}, \cdots, {{{\hat{\mathit{\boldsymbol{x}}}}}_{n}} \right\}$, 若$m\le n$, 则OSPA距离为
\begin{equation}\label{} \begin{array}{l} \bar d_p^{\left( c \right)}\left( {X, \hat X} \right) = \\ \quad {\left( {\frac{1}{n}\left( {\mathop {\min }\limits_{\pi \in {\Pi _n}} \sum\limits_{i = 1}^m {{d^{\left( c \right)}}{{\left( {{\mathit{\boldsymbol{x}}_i}, {{\hat {\mathit{\boldsymbol{x}}}}_{\pi \left( i \right)}}} \right)}^p} + {c^p}\left( {n - m} \right)} } \right)} \right)^{\frac{1}{p}}} \end{array} \end{equation}
(62) 其中, ${{d}^{\left( c \right)}}\left( {\mathit{\boldsymbol{x}}_{i}}, {{{\hat{\mathit{\boldsymbol{x}}}}}_{\pi \left( i \right)}} \right)=\min \left( c, \left\| \mathit{\boldsymbol{x}}-\hat{\mathit{\boldsymbol{x}}} \right\| \right)$, ${{\Pi }_{n}}$表示$\left\{ 1, \cdots, n \right\}$的所有排列集合.若$m>n$, 则$\bar d_p^{\left( c \right)}\left( {X, \hat X} \right) = \bar d_p^{\left( c \right)}\left( {\hat X, X} \right)$.令距离阶次$p=1$, 截断系数$c=20\rm {m}$.
本例做了500次蒙特卡洛(Monte carlo, MC)仿真实验, 分析结果如下:
1) 图 3为不同算法对目标数估计的均值和标准差.可以看出, 在PMM或HMM框架下, CBMeMBer滤波器对目标数的估计是无偏的, PHD滤波器随着目标数的增加, 会出现欠估计的情况.说明本文所提算法对目标数的估计优于PHD滤波器[21].相比不同框架下的CBMeMBer滤波器和PHD滤波器, 它们对目标数估计的统计特性非常接近.
2) 图 4为不同算法对应的OSPA距离.可以看出, CBMeMBer滤波器在PMM和HMM框架下的OSPA距离评价指标均优于PHD滤波器. CBMeMBer滤波器和PHD滤波器在PMM框架下的OSPA距离评价指标优于HMM框架下相应的OSPA距离评价指标.
3) 表 1为不同杂波环境下4种算法的性能比较.不同杂波环境下, CBMeMBer滤波器和PHD滤波器在PMM框架下的OSPA距离评价指标优于HMM框架下的OSPA距离评价指标, 但单步运行时间的均值会变大.由于GM-CBMeMBer滤波器是将每个目标的密度分别用GM表示, 而GM-PHD滤波器是将多目标密度的强度整体用GM表示.因此, 它们的高斯项个数不同, 比较运行时间也就没有意义.但从表 1可以看出, 相比GM-PMM-PHD滤波器, GM-PMM-CBMeMBer滤波器以更小的时间代价可以得到更优的OSPA距离评价指标.
表 1 不同杂波环境下的性能比较Table 1 Tracking performance verses clutter's number$\lambda $ 0 5 10 20 PMM-CBMeMBer OSPA(m) 15.173 15.196 15.202 15.390 时间(s) 0.0203 0.0221 0.0237 0.0244 HMM-CBMeMBer OSPA(m) 16.010 16.065 16.086 16.234 时间(s) 0.0179 0.0194 0.0211 0.0228 PMM-PHD OSPA(m) 15.631 15.654 15.698 15.739 时间(s) 0.0203 0.0280 0.0350 0.0476 HMM-PHD OSPA(m) 16.806 16.817 16.855 16.889 时间(s) 0.0084 0.0118 0.0132 0.0191 4. 结论
本文提出一种在PMM框架下的CBMeMBer滤波器, 并给出了它在线性高斯PMM条件下的GM实现.该算法放宽了HMM隐含的马尔科夫假设和独立性假设限制.在仿真实验中, 采用一种满足HMM局部物理特性的PMM, 将本文所提算法与文献[21]所提的GM-PMM-PHD滤波器进行比较, 仿真结果表明本文所提算法的跟踪性能优于GM-PMM-PHD滤波器.本文考虑的是PMM在线性高斯条件下的多目标跟踪问题, 而非线性条件下的多目标跟踪问题有待进一步研究.
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图 14 NIR图像在预热阶段中温区间
Fig. 14 Medium temperature range of NIR images at pre-heating phases
表 1 3D打印技术的分类
Table 1 The classification of 3D printing technology
成型方式（材料） 成型方式名称 3D打印成型技术 熔挤压（热塑性塑料） 熔融沉积成型技术 FDM熔融沉积成型技术 层压（纸、金属膜、塑料薄膜） 分层直接成型技术 LOM分层实体制造技术 粉末粘接（石膏、陶瓷粉末） 粉末粘接成型技术 3DP三维打印粘接成型技术 光聚合（液态光敏树脂） 光聚合成型技术 SLA立体光固化技术，DLP数字光处理技术PloyJet多头喷射技术 粉末烧结/熔融（金属、合金、热塑性、陶瓷等粉末） 激光粉末成型技术 SLS选择性激光烧结技术，DMLS直接金属激光烧结技术SLM选择性激光熔化成型技术，EBM电子束熔炼技术 
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表 2 参数V, N, ΔP1和喷嘴孔直径d0稳定喷射关系
Table 2 The stable jetting relations of the parameters V, N, ΔP1 and diameter d0 of the nozzle orifice
实例 流速V (mm/s) 功率N (kW) 压力ΔP1 (mbar) 直径知d0 (mm) 1 30 2.13 170 217 2 34 2.13 180 225 3 28 2.07 180 194 4 28 2.07 190 193 5 32 1.99 300 181 6 26 1.96 320 169 7 26 1.96 360 149 8 30 1.96 290 178
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表 3 已存在的混合路径算法和所提出算法的路径比较
Table 3 Comparison of the proposed method with the existing hybrid method
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表 4 振镜校正实验数据
Table 4 Vibrating mirror calibration experiment data
试验次数 1 2 3 4 5 6 7 第一次X 149.8 0 149.7 149.8 0 149.6 150.3 第一次Y 149.7 150 149.8 0 0 0 150.2 第二次X 150 0 150.2 150.1 0 150.2 149.7 第二次Y 150.2 149.9 150.1 0 0 0 149.8
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