Ocean Acoustical Services and Instrumentation Systems, Inc, 11006 Clara Barton Drive, Fairfax Station, Virginia 22039, USA.
J Acoust Soc Am. 2011 Apr;129(4):2026-41. doi: 10.1121/1.3557048.
A set of measures of coherence are defined and applied to the CALOPS experiment, conducted off the coast of Florida in the summer of 2007. A set of narrowband CW tones were transmitted from a towed source received on a 118-element bottom mounted horizontal line array (206 m aperture) with broadside oriented along the 250 m isobath. Two coherence measures are based upon the eigenvalue spread: the power factor and the eigenvalue ratio. This approach is not sensitive to array element error or model mismatch. Two measures are based upon phase residuals; these include the rms-phase error and the coherence function. Three measures are based upon power responses: beam width, array signal gain degradation, and array gain. These approaches have varying sensitivity to array location errors, model mismatch, signal-to-noise ratio, and the structure of the noise field. A Gaussian noise model is used to infer a coherence length from most of the coherence measures. The primary result is that coherence lengths increase with frequency and are on the order of 200 m, the length of the array. The frequency increased coherence length with frequency goes against conventional wisdom, which is to define the coherence length as a fixed number of wavelengths.
定义了一组相干性度量,并将其应用于 2007 年夏季在佛罗里达海岸进行的 CALOPS 实验。从拖曳源发射了一组窄带 CW 音调,在一个由 118 个底部安装的水平线阵(206 米孔径)接收,宽边沿 250 米等深线定向。有两种基于特征值扩展的相干性度量:功率因数和特征值比。这种方法对阵元误差或模型失配不敏感。两种基于相位残差的度量包括均方根相位误差和相干函数。三种基于功率响应的度量包括波束宽度、阵列信号增益降级和阵列增益。这些方法对阵列位置误差、模型失配、信噪比和噪声场的结构具有不同的敏感性。使用高斯噪声模型从大多数相干性度量中推断相干长度。主要结果是相干长度随频率增加,大约为 200 米,即阵列的长度。增加频率的相干长度与传统观点相悖,传统观点将相干长度定义为固定数量的波长。