TABLE V.
Measured A-scan SNRa | Measured image SNRa | Measured SNR gain from beamforming | Theoretical SNR gain from beamforming | |
---|---|---|---|---|
Flash | 14 | 34 | 53 | 54 |
CPA | 14 | 35 | 54 | 54 |
SPA-0 | −19b | 19 | 38 | 36 |
SPA-W | −19b | 18 | 37 | 35 |
SPA-H | −6b | 33 | 52 | 54 |
SPA-HW | −6b | 34 | 53 | 53 |
CPA = classic phased array; SPA-0 = basic synthetic phased array (SPA) without aperture weighting or multi-element firing; SPA-W = SPA with aperture weighting; SPA-H = SPA with Hadamard coding; SPA-HW = SPA with both Hadamard coding and aperture weighting.
For SNR measurements, we defined a signal window and a noise window on the A-scan or on the reconstructed image. The signal window enclosed the echo signal from the on-axis target at 13 mm depth, and the noise window was defined outside the echo signal window where the signal power is due to electronic noise alone. The signal and the noise amplitudes were then measured by calculating the rms of the A-scan or the image amplitude in the signal and the noise windows, respectively.
SNR values smaller than 0 dB were measured after averaging over multiple data sets.