Since the India-Eurasia collision during 65-50 Ma (Ding et al., 2017;Hu et al., 2015), continuous plate convergence has caused uplift and outward expansion of the Tibetan Plateau. Several models have been proposed to explain how such a broad and high plateau formed and persisted, including the viscous thin sheet model (England & Houseman, 1986), deforming viscous lithospheric mantle model (Clark, 2012), lower crustal flow model (Clark & Royden, 2000), and removal of the lithospheric mantle model (Molnar et al., 1993). These models hold distinctively different views on the relationship between surface deformation and underlying dynamic processes, ranging from the coupled (Clark, 2012;England & Houseman, 1986) to decoupled (Clark & Royden, 2000;Molnar et al., 1993). The essential of these debates concerns whether observed surface deformation alone is sufficient to estimate dynamics state below the upper crust and changes in crustal thickness (Flesch & Bendick, 2012). Thus, the investigation on how surface deformation links to underlying geodynamic processes is crucial for understanding the growth of Tibet.One way to assess the relationships of surface deformation with underlying dynamic process is to analyze the surface deformation and exhumation pattern in conjunction with deep structures (e.g., Sobel et al., 2013;Tan et al., 2019). The East Kunlun Shan (EKLS) extends over 1,200 km in near E-W direction in northern Tibet (Figure 1a). This mountain range not only occupies the margin of the low-relief Tibet (Figure 1a and Figure S1 in Supporting Information S1), but also marks the boundary of the weak crust beneath the interior Tibet (Figure 1b;