The Moho discontinuity represents a petrological boundary separating the Earth's silicic crust from the ultramafic mantle. It is the strongest seismic discontinuity within the Earth's outermost cold shell and even within the whole solid Earth except for the core-mantle boundary. The P-wave velocity contrast across the Moho in continental region can reach ∼20% in the IASP91 model (Kennett & Engdahl, 1991) or ∼15% in the CM95 model (Christensen & Mooney, 1995;Rabbel et al., 2013). Thus, seismic waves derived from the Moho discontinuity, which follow the first arrivals, usually dominate the early portion of a seismogram and serve as an important toolkit to decipher crustal structures (Grad & Tiira, 2009).Both active source surveys and passive seismic studies use Moho-related phases to constrain crustal structures. Active source surveys exploit local Moho-reflected waves PmP and Moho-refracted waves Pn (with frequency typically centered at ∼10 Hz) to investigate the Moho topography and crustal volumetric structure (Grad & Tiira, 2009;Mooney, 2010;Wright et al., 2013). Passive seismic studies sometimes use local Moho-reflected waves PmP or teleseismic Moho-converted waves Ps to image the crustal structure (Figure 1). Local PmP waves