A persistent kink in the pressure dependence of the "hidden order" (HO) transition temperature of URu2−xRexSi2 is observed at a critical pressure Pc=15 kbar for 0 ≤ x ≤ 0.08. In URu2Si2, the kink at Pc is accompanied by the destruction of superconductivity; a change in the magnitude of a spin excitation gap, determined from electrical resistivity measurements; and a complete gapping of a portion of the Fermi surface (FS), inferred from a change in scattering and the competition between the HO state and superconductivity for FS fraction.PACS numbers: 75.30.Mb, 74.70.Tx, 81.30.Bx, 74.62.Fj Since its discovery over 20 years ago [1,2,3], the moderately heavy fermion compound URu 2 Si 2 has been the focus of many theoretical and experimental efforts designed to determine the elusive, hidden order parameter associated with the phase transition occurring at T 0 ≈ 17.5 K. The transition into this "hidden order" (HO) state is characterized by large anomalies (typical of magnetic ordering) in specific heat, electrical resistivity, thermal conductivity, and magnetization measurements [1,2,3,4,5,6,7]; however, only a small antiferromagnetic moment, insufficient to adequately explain the entropy released during the transition, was detected in low-temperature neutron diffraction experiments [8]. In addition to the puzzling order parameter of the HO state, URu 2 Si 2 undergoes a transition into an unconventional superconducting (SC) state, which coexists with weak antiferromagnetism (AFM), at T c ≈ 1.5 K. The potential interplay between the two ordered phases of URu 2 Si 2 as well as the nature of the HO state are underlying problems to our fundamental understanding of the properties of this compound.In an effort to explain the observed properties of URu 2 Si 2 , several microscopic models have been proposed [9,10,11,12,13,14,15]. In addition to the theoretical pursuits, many varied experimental techniques have been employed to confirm and/or constrain the proposed models; however, the experimental results fail to converge upon an encompassing microscopic description of the ordered states of URu 2 Si 2 , but do provide valuable insight when contextually analyzed. Low-temperature neutron diffraction measurements as a function of magnetic field provide evidence that the order parameter of the HO state must break time-reversal symmetry [16], and recent inelastic neutron scattering measurements reveal gapped spin excitations at incommensurate wavevectors [17]. Thermal transport measurements are consistent with the opening of a gap at the Fermi surface (FS), as previously suggested by optical conductivity and specific heat studies [3,18], depleting carriers and reducing electron-phonon scattering [5,6]. These exemplary measurements tend to converge upon a description of the HO state invoking the presence of a FS instability such as a spin density wave (SDW), further suggested by high-field measurements intimating the itinerant nature of the HO state [19].The application of pressure to URu 2 Si 2 further convolutes the discussion...