The opposing effects of high pressure (in the GPa range) and the Jahn-Teller distortion led to many intriguing phenomena which are still not well understood. Here we report a combined experimental-theoretical study on the high-pressure behavior of an archetypical Jahn-Teller system, copper difluoride (CuF 2). At ambient conditions this compound adopts a distorted rutile structure of P2 1 /c symmetry. Raman scattering measurements performed up to 29 GPa indicate that CuF 2 undergoes a phase transition at 9 GPa. We assign the novel high-pressure phase to a distorted fluorite structure of Pbca symmetry, iso-structural with the ambient-pressure structure of AgF 2. Density functional theory calculations indicate that the Pbca structure should transform to a non-centrosymmetric Pca2 1 polymorph above 30 GPa, which, in turn, should be replaced by a cotunnite phase (Pnma symmetry) at 72 GPa. The elongated octahedral coordination of the Cu 2+ cation persists up to the Pca2 1-Pnma transition upon which it is replaced by a capped trigonal prism geometry, still bearing signs of a Jahn-Teller distortion. The high-pressure phase transitions of CuF 2 resembles those found for difluorides of transition metals of similar radius (MgF 2 , ZnF 2 , CoF 2), although with a much wider stability range of the fluorite-type structures, and lower dimensionality of the high-pressure polymorphs. Our calculations indicate no region of stability of a nanotubular polymorph observed for the related AgF 2 system.