We have successfully observed linear dichroism in angle-resolved Yb 3+ 3d 5/2 core-level photoemission spectra for YbB12 in cubic symmetry. Its anisotropic 4f charge distribution due to the crystal-field splitting is responsible for the linear dichroism, which has been verified by spectral simulations using ionic calculations with the full multiplet theory for a single-site Yb 3+ ion in cubic symmetry. The observed linear dichroism as well as the polarization-dependent spectra in two different photoelectron directions for YbB12 are quantitatively reproduced by theoretical analysis for the Γ8 ground state, indicating the Γ8 ground-state symmetry for the Yb 3+ ions mixed with the Yb 2+ state.Rare-earth-based strongly correlated electron systems show various interesting phenomena such as competition between magnetism and unconventional superconductivity, charge and/or multipole ordering, and the formation of a narrow (∼meV) gap at low temperatures. Among them, YbB 12 is known as a Kondo semiconductor [1][2][3][4][5], which has been recently recognized as a candidate for topological insulators [6], as intensively discussed for another Kondo semiconductor, SmB 6 [7-9]. The mean valence of YbB 12 has been estimated as ∼2.9+ by bulksensitive 3d core-level hard X-ray photoemission (HAX-PES) spectroscopy [10]. To discuss the mechanisms of the gap opening at low temperatures [5,[11][12][13][14][15][16] Generally, it is difficult to experimentally determine the 4f ground-state symmetry. Inelastic neutron scattering is useful, but other excitations such as phonon excitations often hamper the observation of magnetic 4f −4f excitations. Linear dichroism (LD) in 3d−to−4f soft Xray absorption spectroscopy (XAS) for single crystals is powerful owing to the dipole selection rules, as reported for Ce compounds [19][20][21][22]. However, it is not applicable to compounds in cubic symmetry, in which there is no anisotropic axis relative to the electric field of the incident light. On the other hand, the selection rules work also in the photoemission process while the excited electron energy is much higher than that in the absorption. Furthermore, there is another controllable measurement parameter in photoemission, called the "photoelectron detection direction" relative to the single-crystalline axis, in addition to the polarization direction of the excitation light. Indeed, by using LD in 3d core-level HAXPES spectra, the Yb 3+ 4f ground state has been determined for tetragonal YbCu 2 Si 2 and YbRh 2 Si 2 [23]. LD in the core-level HAXPES for cubic Yb compounds is also expected to be observed, as discussed below.In the case of Yb 3+ ions in tetragonal symmetry, the eightfold degenerate J = 7/2 state splits into four dou-