TY - JOUR
T1 - The bichromatic intensity correlation of radiation reflected off a randomly irregular surface
AU - Frankenthal, Shimshon
PY - 1990/6
Y1 - 1990/6
N2 - When phase information is absent (incoherent detection), the basic statistical entity relevant to data processing is the bichromatic four-point coherence. Using the strength and size parameters Φ 2and A, an integral expression for this quantity is formulated and evaluated for a high-frequency signal scattered by a phase screen that represents the randomly reflecting ocean cover (or, alternatively, a randomly refracting thin layer). The evaluation is illustrated by a treatment of the monochromatic mean-square intensity (I2), then applied to the bichromatic intensity correlation (I1I2). Viewed as a function of the frequency-independent parameter ⋏Φ, (I2) rises from 1 to 2, passing through a maximum which scales as log k (the wavenumber) at some intermediate value of ⋏Φ that depends only on the form of the screen statistics. By constrast, (I1I2) saturates at 1. Moreover, even when ⋏Φ is large, the second and fourth coherence moments are found to be consistent with the assumption that the bichromatic signal possesses joint normal statistics only within a narrow range of frequency separations (~O(1/Φ)), which nonetheless encompasses the coherent bandwidth (~O(1/⋏Φ 2)).
AB - When phase information is absent (incoherent detection), the basic statistical entity relevant to data processing is the bichromatic four-point coherence. Using the strength and size parameters Φ 2and A, an integral expression for this quantity is formulated and evaluated for a high-frequency signal scattered by a phase screen that represents the randomly reflecting ocean cover (or, alternatively, a randomly refracting thin layer). The evaluation is illustrated by a treatment of the monochromatic mean-square intensity (I2), then applied to the bichromatic intensity correlation (I1I2). Viewed as a function of the frequency-independent parameter ⋏Φ, (I2) rises from 1 to 2, passing through a maximum which scales as log k (the wavenumber) at some intermediate value of ⋏Φ that depends only on the form of the screen statistics. By constrast, (I1I2) saturates at 1. Moreover, even when ⋏Φ is large, the second and fourth coherence moments are found to be consistent with the assumption that the bichromatic signal possesses joint normal statistics only within a narrow range of frequency separations (~O(1/Φ)), which nonetheless encompasses the coherent bandwidth (~O(1/⋏Φ 2)).
UR - http://www.scopus.com/inward/record.url?scp=0025171060&partnerID=8YFLogxK
U2 - 10.1121/1.399093
DO - 10.1121/1.399093
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AN - SCOPUS:0025171060
SN - 0001-4966
VL - 87
SP - 2467
EP - 2476
JO - Journal of the Acoustical Society of America
JF - Journal of the Acoustical Society of America
IS - 6
ER -