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(47)

Hence, Eq. (43) can be written as a product of the original signal amplified $M$ times and the beamforming function, i.e.,

$z\left(\stackrel{\to }{r},t\right)=Mf\left(t-\frac{r}{c}\right)BF\left(\mathbf{w},M\right)$ (48)

(48)

In order to study the relative effects of array spacing $d$, wavelength $\lambda$, and distance ...

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