An N-D Technique for Coherent Wave Doa Estimation

J. Byrne, D. Cyganski, R. Vaz, C. R. Wright
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引用次数: 2

Abstract

of propagation. The signal phase difference between any two adjacent sensors in radians Dimensional Direction of Arrival (N-D DOA) estimated by measuring the phase difference technique is based between the signal values at each sensor, or mulation was motivated by previous work in tained in a “snapshot” of data from all the sensors. which the Cram& Rao Bound (CRB) for coherent wave N-D DOA was developed. Means formance for low SNR are also presented. rithm which is Our target application [3] generates a set of values corresponding to samples from an N-dimensional lattice of senIntroduction sors, the plane wave frequency components of The DOA problem involves estimation of which are the parameters revealing the object plane wave frequency components from data identity and pose. This motivates an extencollected by a uniformly spaced grid of sension of the DOA algorithm to N-D. sors. One and two-dimensional versions of There are a variety of techniques for perthe DOA problem arise in sonar and radar forming 1D DOA estimation, c.f. [4, 5 , 61; direction finding and target tracking applicaone such method, the state space technique, tions [l, 21; the need for an N-D DOA techwas chosen for this extension to N-D. The nique arises in a recently developed object state space DOA method involves determirecognition algorithm [3]. Figure 1 shows a nation of a system, the impulse response of plane wave impinging at an angle t9 on a 1which would produce the sensor data. Once D array of linearly spaced sensors. The dissuch a system is found, we may perform an tance between each sensor is I , The waveeigenvalue decomposition of the system malength of the plane wave is X = c/fo, where trix in order to determine the modes of the c is the speed of propagation of the wave system. These modes are the estimated freand fo is its spatial frequency. The plane quency components of the plane wave along wave is constant along a front perpendicuthe direction of the array of sensors. Given lar to the vectors that indicate the direction the distance 1 between each sensor, we can In this paper, we describe a to the Nis (2T1 sin e)/X. Thus the parameter 8 can be The N-D On a state ‘pace and its forequivalently by estimating the frequency confor improving the N-D DOA estimation perThe model based object recognition alga-
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相干波Doa估计的N-D技术
的传播。通过测量相位差技术估计的任意两个相邻传感器之间的弧度尺寸到达方向(N-D DOA)的信号相位差是基于每个传感器的信号值之间的,或者模拟是由先前的工作驱动的,包含所有传感器数据的“快照”。提出了相干波N-D DOA的cram&rao界(CRB)。同时给出了低信噪比下的均值性能。我们的目标应用[3]从传感器的n维晶格中生成一组与样本相对应的值,DOA问题涉及对其进行估计,这些参数是从数据身份和姿态中揭示目标平面波频率成分的参数。这激发了一种由均匀间隔网格感知的DOA算法扩展到N-D。传感器适用。在声纳和雷达形成1D DOA估计时出现的DOA问题有各种各样的技术,c.f. [4,5,61;测向和目标跟踪应用于这种方法,即状态空间技术[1,21];需要一个N-D的DOA技术选择了这个扩展到N-D。该方法出现在最近开发的对象状态空间DOA方法中,涉及确定性识别算法[3]。图1显示了一个系统的状态,平面波以1的角度撞击1的脉冲响应将产生传感器数据。一旦D阵列线性间隔传感器。对于这样一个系统,我们可以执行每个传感器之间的距离为I,将系统的平面波长度分解为X = c/fo,其中trix为确定模态,c为该系统的传播速度。这些模态是估计频率,0是它的空间频率。平面波沿波的平面频率分量沿传感器阵列的前方垂直方向是恒定的。给定指示每个传感器之间距离1方向的向量,我们可以在本文中,我们将a描述为Nis (2T1 sin e)/X。因此,参数8可以是一个状态的N-D速度,通过估计频率控制来提高基于模型的目标识别算法的N-D DOA估计
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Hopfield Network Approach to Beamforrning in Spread Spectrum Communication A Comparative Study of Statistical and Neural DOA Estimation Techniques A New Cumulant Based Phase Estimation Nonminimum-phase Systems By Allpass Study of the Couple (Reflection Coefficient, K-Nn Rule) An N-D Technique for Coherent Wave Doa Estimation
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