Using high resolution angle-resolved photoemission spectroscopy, we systematically investigate the electronic structure of T d -WTe 2 , which has attracted substantial research attention due to its diverse and fascinating properties, especially the predicted type-II topological Weyl semimetal (TWS) phase. The observed significant lattice contraction and the fact that our ARPES measurements are well reproduced by our ab initio calculations under reduced lattice constants support the theoretical prediction of a type-II TWS phase in T d -WTe 2 at temperatures below 10 K. We also investigate the evolution of the electronic structure of T d -WTe 2 and realize two-stage Lifshitz transitions induced by temperature regulation and surface modification, respectively. Our results not only shed light on the understanding of the electronic structure of T d -WTe 2 , but also provide a promising method to manipulate the electronic structures and physical properties of the type-II TWS T d -XTe 2 .Topological Weyl semimetals (TWSs) are characterized by the existence of bulk Weyl fermions and topological surface Fermiarcs connecting each pair of Weyl points (WPs) of opposite chirality. [1] Upon their discovery, TWSs have evoked enormous research interests due to their intriguing physical properties and broad application potential. [1][2][3][4][5][6][7][8][9] Soon after the establishment of the TWS phase in the transition metal mono-pnictide (TMMP) family, [10][11][12][13][14][15][16][17] the type-II TWS phase was theoretically proposed in T d -XTe 2 (X ¼ W, Mo) that violates the Lorentz symmetry, [18] thus the strongly tilted bulk Weyl cones introduce non-vanishing bulk (both electron and hole) Fermi pockets on the Fermi surface (FS). [18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35] Compared to the complicated distribution of 24 Weyl fermions in the TMMPs and their three-dimensional (3D) crystal structures, [10][11][12][13][14][15] T d -XTe 2 not only has much more concise distribution of Weyl fermions, but also crystallizes into layered structure, thus providing a more promising material basis to design, process, and fabricate TWS-based electronic and spintronic devices.Besides being recognized as type-II TWSs, T d -XTe 2 materials are well known to possess other rich and intriguing physical properties, such as quantum spin Hall effect, [36][37][38] nonsaturating magnetoresistance, [39,40] strong spin-orbit