momentum directions. In the presence of broken time-reversal symmetry (TRS) or space-inversion symmetry, Dirac semimetals evolve into Weyl semimetals and Dirac points split into pairs of Weyl points due to the lifted spin degeneracy. [8,9] For both the Dirac and Weyl semimetals, due to the coexistence of the conventional charge carriers and relativistic carriers, interesting transport phenomena can often be observed, for example, chiral anomaly [10][11][12] and ultrahigh carrier mobilities. [13] Accordingly, transport studies are viewed as an important way to explore the unique scattering mechanism of charge carriers in Dirac/Weyl semimetals. In addition, through transport quantum oscillations, one can get deep insights into the underlying band topology of Dirac/Weyl semimetals.In general, Weyl semimetals can be classified into two types: the standard type I which possesses a point-like Fermi surface, and the type II with strongly tilted Weyl cones induced by the broken Lorentz symmetry. [14] The Weyl points for type II Weyl semimetals appear only at the contact of electron and hole pockets. The qualitatively distinct band topology of type II Weyl semimetals can lead to marked differences in physical properties, such as the direction restricted chiral anomaly and exotic superconductivity. [15][16][17] To date, several noncentrosymmetric material systems, for example, the transition metal dichalcogenides T M X 2 (T M = W, Mo, etc.; X = Se, Te), [14,[18][19][20] the diphosphides (Mo, W)P 2 , [21] LaAlGe, [22] etc., have been considered to be type II Weyl semimetals, while most of them display complex band structures with multiple Weyl points, which adds difficulties in the conventional transport studies of these materials. Moreover, in many Weyl semimetals, the Weyl points are located deeply below the Fermi level, which often hinders the observation of intrinsic characteristics associated with the relativistic carriers.Very recently, ternary MTTe 4 (M = Nb or Ta; T = Ir or Rh) compounds were theoretically predicted as a new series of type II Weyl semimetals, [23,24] and verified experimentally in TaIrTe 4 . [25][26][27] In comparison with the previous type II Weyl semimetals, the angle-resolved photoemission spectroscopy (ARPES) data and band calculation of TaIrTe 4 suggests the existence of only four Weyl points, [24,26] which is the minimum number of Weyl points allowed for a time-reversal invariant Weyl semimetals, characterized by nodal points in the bulk and Fermi arc states on the surface, have recently attracted extensive attention due to their potential application as materials for low-energy-consumption electronics. The thermodynamic and transport properties of a theoretically predicted Weyl semimetal NbIrTe 4 is measured in high magnetic fields up to 35 T and low temperatures down to 0.4 K. Remarkably, NbIrTe 4 exhibits a nonsaturating transverse magnetoresistance that follows a power-law dependence in B. Low-field Hall measurements reveal that hole-like carriers dominate the transport for T > 80 K, while...