Specific heat of CeRhIn5:: Pressure-driven evolution of the ground state from antiferromagnetism to superconductivity -: art. no. 224509

Resistivity measurements on CeRhIn5 have suggested an unusual "first-order-like" transition from antiferromagnetism to superconductivity at a critical pressure P-c, similar to15 kbar: At pressures below P-c the magnetic ordering temperature is approximately independent of pressure. At P-c antiferromagnetism disappears abruptly and is replaced by superconductivity, with a critical temperature that is also approximately independent of pressure. Here we report measurements of the low-temperature specific heat of CeRhIn5 at pressures to 21 kbar, and for 21 kbar in magnetic fields to 70 kOe. They confirm, by measurement of a bulk thermodynamic property, the unusual relation between magnetism and superconductivity, and permit an estimate of the discontinuity in entropy at P-c. They also give insight into the natures of the antiferromagnetic and superconducting states and their changes with pressure: With increasing pressure the zero-field specific-heat anomaly changes from one typical of antiferromagnetic ordering at ambient pressure to one more characteristic of the formation of a Kondo singlet ground state at 21 kbar. The change in general shape of the anomaly is gradual, but at P-c, where the data suggest a weak thermodynamic first-order transition, there is a discontinuous change from an antiferromagnetic ground state to a superconducting ground state. Below P-c the quasiparticle density of states increases and the spin-wave stiffness decreases with increasing pressure. At P-c the low-energy magnetic excitations disappear and are replaced by excitations that are characteristic of superconductivity with line nodes in the energy gap. The quasiparticle density of states is continuous at P-c, but decreases with increasing pressure, to zero at 21 kbar. These features suggest the possibility of superconductivity with d-wave pairing and, at intermediate pressures, "extended gaplessness." At 21 kbar except for the line nodes, the Fermi surface is fully gapped. The specific-heat data also show the existence of a second-order transition in the 11-12-kbar region, where features in the magnetic susceptibility and resistivity have been observed.