“…The transfer function of a noncollinear AOSF in this diffraction geometry has the O-type topology, and the radius of the phase-matching locus increases with the ultrasound frequency. Accurate analysis shows that the annular transfer function near the NPM diffraction geometry is slightly asymmetric, and the transfer function center shifts with the ultrasound frequency [2,3]. With respect to Equations ( 7) and ( 11), the resulting two-dimensional transfer function will be expressed as T 1 (θ, ϕ; f , Q, ∆φ), where θ and ϕ are the plane-wave direction angles, while f , Q, and ∆φ are the problem parameters corresponding to the ultrasound frequency, normalized amplitude, and the phase delay between the transducer sections.…”