I. Introduction
Thanks to the two-way dynamic focusing, when combined with the same beamforming method, synthetic transmit aperture (STA) imaging can achieve comparatively high spatial (lateral) resolution and contrast resolution among all the imaging sequences [1]. In STA imaging, all the transducer elements are activated individually and sequentially to transmit spherical waves and to obtain low-quality images. Thereafter, transmit focusing can be resynthesized at all image points by coherently summing these images to obtain the final high-resolution STA image. However, owing to the limited energy transmitted by the individual element in each transmission, STA imaging severely suffers from the low signal-to-noise ratio (SNR) issue (especially in the deep region). In addition, as STA imaging requires activating all the elements sequentially, its frame rate (FR) is limited by a large number of transmissions.
Illustration of the range-null space decomposition.