The quantum anomalous Hall (QAH) effect is a quintessential consequence of non-zero Berry curvature in momentum-space. The QAH insulator harbors dissipation-free chiral edge states in the absence of an external magnetic field. On the other hand, the topological Hall (TH) effect, a transport hallmark of the chiral spin textures, is a consequence of realspace Berry curvature. While both the QAH and TH effects have been reported separately, their coexistence, a manifestation of entangled chiral edge states and chiral spin textures, has not been reported. Here, by inserting a TI layer between two magnetic TI layers to form a sandwich heterostructure, we realized a concurrence of the TH effect and the QAH effect through electric field gating. The TH effect is probed by bulk carriers, while the QAH effect is characterized by chiral edge states. The appearance of TH effect in the QAH insulating regime is the consequence of chiral magnetic domain walls that result from the gate-induced Dzyaloshinskii-Moriya interaction and occur during the magnetization reversal process in the magnetic TI sandwich samples. The coexistence of chiral edge states and chiral spin textures potentially provides a unique platform for proof-of-concept dissipationless spintextured spintronic applications. Electronic band structures of nontrivial topology in momentum-space and magnetic chiral spin textures in real-space have attracted enormous attention in the past decade since they harbor elegant Berry curvature physics 1, 2, 3 . The intrinsic anomalous Hall (AH) effect is such an example: it is induced by the Berry curvature in momentum-space in ferromagnetic (FM) materials 4 and can even be quantized under certain circumstances, leading to the quantum anomalous Hall (QAH)effect. The QAH effect has been theoretically proposed 5, 6, 7, 8 and experimentally realized 9,10,11,12,13 in magnetically doped topological insulator (TI) films. On the other hand, chiral spin textures (e.g. skyrmions) provide another example of nontrivial topology, but in real-space. It has been shown that chiral spin textures can also induce a Hall current: this is known as the topological Hall (TH) effect and is generally regarded as the transport signature of non-zero spin chirality 3 . The TH effect has been experimentally observed in many metallic systems, such as MnSi 14, 15 , MnGe 16 , FeGe 17 , and SrIrO3/SrRuO3 interface 18,19 as well as magnetically doped TI films and heterostructures 20, 21 . The TH effect in these systems is usually observed accompanied by the AH effect. However, there is no conclusive evidence to date that the AH effect found in these metallic systems to be intrinsic, i.e., exclusively induced by the momentum-space Berry curvature 4 .The QAH and TH effects have been separately observed in magnetically doped TI 9, 10, 20, 21 , with distinctly different sample geometries. The QAH effect can be realized only in the insulating regime of a magnetic TI 9,10,11,12,13 while the TH effect is usually seen in metallic systems 20, 21 .In this Article, we re...