SynopsisWe present a study of the vibrationally resolved B 1s photoionization cross section of the BF 3 mo lecule. A co mb ination of h igh-resolution photoelectron spectroscopy measurements and of state-of-the-art calcu lations shows the evolution of the photon energy dependence of the cross section from a co mplete trapping of the photoelectron wave (lo w energ ies) to oscillat ions due to intramolecular scattering [1,2]. These diffract ion pa tterns allow to access structural information of both the neutral mo lecule and the core -hole species generated upon photoabsoption [3].The advent of third-generation synchrotron radiation facilities, in combination with high energy-resolution detection techniques , has opened the way for the investigation of vibrationally-resolved inner-shell photoionization in small molecules, where an electron is emitted from a 1s orbital of a first-row atom. We present a study on B 1s photoionization of BF 3 , comparing experimental results with full firstprinciple calculations and showing that the most relevant features can be understood by means of simple models.In order to calculate vibrationally-resolved cross sections, we have evaluated (bound and continuum) electronic wave functions using the static-exchange and the time-dependent DFT methods [4], developed by Decleva and colla borators, for different molecular geometries along the totally symmetric stretching mode. This mode is the most affected by the structural rearrangement accompanying core ionization [1,2]. Our theoretical results are in good agreement with experimental measurements from SOLEIL synchrotron and, at high energies, qualitatively agree with a first-Born approximation model.We have found that the relative cross sections show clear oscillations in the high-energy region as a function of photoelectron mome ntum which are due to an intramolecular scattering mechanism: in its way out of the molecule, the photoelectron is diffracted by the surrounding atomic centers, encoding the geometry of the molecule [1,2,3]. Very close to the photoionization threshold a complete trapping of the photoelectron is observed, manifesting itself as an emission angle dependent shape resonance feature [1,2].