Lifshitz transition represents a sudden reconstruction of Fermi surface structure, giving rise to anomalies in electronic properties of materials. Such a transition does not necessarily rely on symmetry-breaking and thus is topological. It holds a key to understand the origin of many exotic quantum phenomena, for example the mechanism of extremely large magnetoresistance (MR) in topological Dirac/Weyl semimetals. Here, we report studies of the angle-dependent MR (ADMR) and the thermoelectric effect in W 2 As 3 single crystal. The compound shows a large unsaturated MR (of about 70000% at 4.2 K and 53 T). The most striking finding is that the ADMR significantly deforms from the horizontal dumbbell-like shape above 40 K to the vertical lotus-like pattern below 30 K. The window of 30-40 K also corresponds substantial changes in Hall effect, thermopower and Nernst coefficient, implying an abrupt change of Fermi surface topology. Such a temperatureinduced Lifshitz transition results in a compensation of electron-hole transport and the large MR as well. We thus suggest that the similar method can be applicable in detecting a Fermi-surface change of a variety of quantum states when a direct Fermi-surface measurement is not possible. A Lifshitz transition means an abrupt change of the Fermi surface topology of metals without symmetry breaking[1], therefore, it is also termed as electronic topological transition. Conventional Lifshitz transition is quantum phase transition at zero temperature, driven by chemical doping, magnetic field, pressure or uniaxial stress, in the vicinity of which the topology of the Fermi surface deforms [2-5]. Indeed, such Lifshitz transition is associated with a variety of emergent quantum phenomena like van-Hove singulary, non-Fermi-liquid behavior, unconventional superconductivity et. al.. A recent famous example is Sr 2 RuO 4 , whose γ-Fermi sheet hits the edge of Brillouine zone and forms a van-Hove singularity under uniaxial stress. The critical transition temperature increases from ∼1.5 K up to ∼3.5 K [5], and meanwhile transport, magnetic and thermodynamic properties change correspondingly[6, 7]. Besides those quantum control parameters, temperature can be regarded as another driving force to induce a Lifshitz transition, because the chemical potential (µ F ) is temperature-dependence and its shift can modify the Fermi surface structure[8]. However, such realistic examples are rare [9-11] due to the stringent requirements: (i) small Fermi energy (ε F in the order of k B T 100 meV), so that the varying temperature can be influential to µ F with respect to ε F ; (ii) band structure near the Fermi energy displaying anomalous dispersion, so that the contoured Fermi surface experiences an abrupt change. Recently, a wide spectrum of topological semimetals have been extensively studied including Dirac semimetals (DSM)[12-14], Weyl semimetals (WSM)[15-20] as well as nodal-line semimetals[21-23]. These topological semimetals have bearing on a common feature: the extremely large magnetoresistance (...