faster writing speed, higher thermal stability, etc. while compared to their ferromagnetic counterparts. [20-23] One of the main obstacles impedes the development of AFM spin switching memory was the difficulty of reversing the Néel spin order due to the extraordinary large anisotropy field of AFM, which has been recently demonstrated to be eased by the current-induced spin-orbit torque. [24] For example, in the antiferromagnetic CuMnAs and Mn 2 Au, multistate electrical resistive switching has been achieved via the broken inversion symmetry-induced staggered spin-orbit torque. [25-29] The spin torque switching of AFM has soon been extended to the antiferromagnetic insulator (AFMI)/heavy metal (HM) bilayer systems such as NiO/Pt and α-Fe 2 O 3 /Pt in which the HM (Pt) is utilized to generate spin-orbit torque. [30-35] More remarkably, the current-induced multistate switching characteristic makes the AFM-based spintronic device appealing for neuromorphic computing as an artificial synapse, in the sense that one important prerequisite needs to be met in a synaptic device is to have a symmetric and linear relation between the device conductance and the number of input current pulses. [36] All these thrilling developments take along pressing need to establish the comprehensive understanding and fully control of the current-induced switching in AFM-based devices. However, intense debates are currently underway over the physical origin of the current-induced resistive switching in AFMI/Pt bilayers. The initial studies propose the scenario of Néel spin order switching to explain the switching of AFMI, which has been further backed up by the recent studies of imaging through X-ray magnetic linear dichroism [31,32] and longitudinal spin Seebeck effect. [33] On the other hand, other studies have found that the switching behavior in AFMI/Pt bilayers has nonmagnetic origins thus going beyond the scenario of Néel spin order switching. For example, Chiang's recent work on the NiO/Pt bilayer shows similar switching behaviors even without AFMI and suggests the Seebeck effect in Pt as an alternative explanation. [37] Moreover, Cheng et al. [34] and Zhang et al. [35] also reported nonmagnetic origin for the switching in the α-Fe 2 O 3 /Pt bilayers. All these works fuel raising concerns on the origin of resistive switching in AFMI/ Pt bilayers. New materials and mechanisms to retain electrically tunable resistance states are highly pursed to advance information technology. In this study, a novel scenario of current-induced planar resistive switching mediated by oxygen migration is unveiled in the NiO/Pt bilayers. Sawtooth-like switching is successfully realized in various crystalline NiO, and the switching amplitude monotonically increases with the Pt thickness. On the other hand, the critical switching current is found to be strongly correlated with the substrate thermal conductivity hence suggesting a thermal origin. By directly probing the Ni 2+ and O 2− distribution before and after switching via electron energy loss spectrum, ...