We report a study of the quantum Hall states (QHSs) sequence of holes in mono-and bilayer WSe2. The QHSs sequence transitions between predominantly even and predominantly odd filling factors as the hole density is tuned in the range 1.6 â 12 Ă 10 12 cm â2 . The QHSs sequence is insensitive to the transverse electric field, and tilted magnetic field measurements reveal an insensitivity of the QHSs sequence to the in-plane magnetic field, evincing that the hole spin is locked perpendicular to the WSe2 plane. These observations imply that the QHSs sequence is controlled by the Zeemanto-cyclotron energy ratio, which remains constant as a function of perpendicular magnetic field at a fixed carrier density, but changes as a function of density due to strong electron-electron interaction.The strong spin-orbit coupling and broken inversion symmetry in 2H transition metal dichalcogenide (TMD) monolayers leads to coupled spin and valley degrees of freedom [1]. Breaking the time reversal symmetry by applying a perpendicular magnetic field further lifts the valley degeneracy, thanks to the spin (valley) Zeeman effect [2,3]. Insights into the Zeeman effect, a fundamental property of TMDs, have been provided by magnetooptical measurements of TMD monolayers, which report the exciton g-factors from luminescence shifts in perpendicular magnetic fields [4,5]. While magnetotransport measurements have been traditionally used to determine the effective g-factor (g * ) in several two-dimensional electron systems (2DESs) [6][7][8], the lack of reliable low temperature Ohmic contacts, combined with a moderate mobility, have hampered a similar progress in TMDs. Recent advances in sample fabrication have now facilitated more detailed studies of the electron physics in TMDs [9][10][11]. Tungsten diselenide (WSe 2 ) is of particular interest because of a large spin-orbit splitting in the valence band [12], high-mobility [10], and low temperature Ohmic contacts [13].In this work, we report on the magnetotransport of holes in mono-and bilayer WSe 2 in the quantum Hall regime. An examination of the Shubnikov-de Haas (SdH) oscillations, and the quantum Hall states (QHSs) sequence reveals interesting carrier density-dependent transitions between predominantly even and predominantly odd filling factors (FFs) as the hole density is tuned. Measurements in tilted magnetic fields reveal an insensitivity of the QHSs sequence to the in-plane magnetic field, indicating that the hole spin is locked perpendicular to the WSe 2 plane. The QHSs sequence is also found to be insensitive to the applied transverse electric field. These observations can be explained by a Zeeman-tocyclotron energy ratio which remains constant as a function of perpendicular magnetic field at a fixed carrier density, but changes as a function of density because of strong electron-electron interaction.Figure 1(a) shows the schematic cross section, and Fig. 1(b) the optical micrograph of an hBN encapsulated WSe 2 sample with bottom Pt contacts, and separate local top-and back-gates. ...