The second-order phase transition into a hidden order phase in URu 2 Si 2 goes along with an order parameter that is still a mystery, despite 30 years of research. However, it is understood that the symmetry of the order parameter must be related to the symmetry of the low-lying local electronic f-states. Here, we present results of a spectroscopic technique, namely core-level nonresonant inelastic X-ray scattering (NIXS). This method allows for the measurement of local high-multipole excitations and is bulk-sensitive. The observed anisotropy of the scattering function unambiguously shows that the 5f ground-state wave function is composed mainly of the Γ 1 with majority Jz = |4 + |−4 and/or Γ 2 singlet states. The incomplete dichroism indicates the possibility that quantum states of other irreducible representation are mixed into the ground state. strongly correlated electron systems | X-ray spectroscopy | crystal-electric field | heavy fermions | hidden order I n heavy fermion rare earth or actinide compounds, the f electrons are well localized at high temperatures, but as temperature is lowered, hybridization with conduction electrons becomes increasingly effective, resulting in a more itinerant f -electron character at low temperatures. These hybridized f electrons form narrow bands and have large effective masses. Quasiparticle interaction effects in these narrow bands are responsible for the many exciting phenomena present in heavy fermion compounds: multipolar order (1), unconventional superconductivity (2), or quantum criticality (3). The hidden order phase in URu2Si2 is one example of the exotic low-temperature phases found in this material class. URu2Si2 is a tetragonal heavy fermion compound that undergoes two phase transitions, the nonmagnetic hidden order (HO) transition at THO = 17.5 K, which involves an appreciable loss of entropy, and a superconducting transition at about 1.5 K (4-7). Below the HO transition, small-ordered magnetic moments were observed in the earlier studies but were determined later to belong to a parasitic minority phase. With applied pressure (p ≥ 0.7 GPa), the HO order is replaced by an antiferromagnetic phase with large-ordered moments (so-called LMAF -phase) (8). The order parameter of the HO phase has been the subject of intense investigations for more than 30 years but, so far, has remained hidden, which has been the inspiration for its name. This second-order transition into an electronically ordered state involves a reconstruction of the Fermi surface (9, 10) and a change of quasiparticle scattering rate (11). The Fermi surfaces of the HO and high-pressure LMAF phase are very similar (12).In URu2Si2 three-energy scales have been identified: a hybridization gap of ∆ hyb ≈ 13 meV [150 K] (13) that opens below 27 K, another gap that opens in the HO phase with ∆HO ≈ 4.1 meV [50 K] in the charge (9, 10, 14, 15) as well as spin channel (16,17), and a resonance mode that appears in the HO gap at ∼ =1.6 meV [18 K], also in both channels (18)(19)(20). Furthermore, with entering ...