We consider analytically current-driven dynamics of magnetic Néel walls in heavy metal/ ferromagnetic metal/oxide trilayers where strong spin-orbit coupling and interfacial Dzyaloshinskii-Moriya interaction (i-DMI) coexist. We show that field-like spin-orbit torque (FL-SOT) with effective field along´n J(n being the interface normal andĴ being the charge current direction) and i-DMI induced torque can both lead to Walker breakdown suppression meanwhile leaving the wall mobility (velocity versus current density) unchanged. However, i-DMI itself can not induce the 'universal absence of Walker breakdown' (UAWB) while FL-SOT exceeding a certain threshold can. Finitelyenlarged Walker limits before UAWB are theoretically calculated and well explain existing data. In addition, change in wall mobility and even its sign-inversion can be understood only if the antidamping-like SOT is appended. For Néel walls in ferromagnetic-metal layer with both perpendicular and in-plane anisotropies, we have calculated the respective modifications of wall mobility under the coexistence of spin-transfer torque, SOTs and i-DMI. Analytics shows that in trilayers with perpendicular anisotropy strong enough spin Hall angle and appropriate sign of i-DMI parameter can lead to sign-inversion in wall mobility even under small enough current density, while in those with in-plane anisotropy this only occurs for current density in a specific range.Over the past decade, in heavy metal/ferromagnetic metal/oxide (HM/FMM/Oxide) trilayers, axial domain wall propagation in FMM layer with perpendicular magnetic anisotropy (PMA) or in-plane magnetic anisotropy (IPMA) driven by axial currents are experimentally observed [25][26][27][28][29][30][31][32][33][34][35][36][37][38][39][40][41]. In certain case (Pt Co AlO x ), walls can move at a high velocity up to 400 m s -1 when current density is around -10 A cm 8 2 [37]. More interestingly, walls with certain polarity can even move in the direction of charge current [33][34][35][36][37][38][39][40][41], which is also confirmed by numerical simulations [42][43][44][45]. To understand these findings, spin-orbit torques (SOTs) from strong spin-orbit coupling (SOC) in these trilayers are proposed [46][47][48][49][50][51][52][53][54][55][56][57][58][59]. SupposeĴ is the charge current direction and n is interface normal. Mathematically, SOTs can be decomposed into two perpendicular components: (a) µ´(ˆ) m J n which is odd in magnetization direction m and usually referred to as field-like (FL) torque; (b) µ´´[ (ˆ)] m m J n which is even in m and usually called anti-damping-like (ADL) torque. Physically, two typical mechanisms are of most importance: the 'spin Hall torques' from the spin Hall effect (SHE) [60] in HM layer and the 'Rashba torques' from the structure inversion asymmetry (SIA) at the HM/ FMM interface. In early literatures, ADL-SOTs are believed to stem mostly from bulk SHE while field-like spinorbit torques (FL-SOTs) are mainly attributed to interfacial Rashba SOC. However, recent works based on scatt...