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322 Handbook on the Physics and Chemistry of Rare Earths FIG. 16 2.5 Pseudogap 2.4 20 10 0 123456 T (K) 2.0 CeRhIn5 Pressure induced superconductivity and destruction of antiferromagnetism in CeRhIn5 determined via resistivity with pressure increasing vertically from 0 to 21 kbars. From dr/dT, the antiferromagnetic transition temperature TN can be found, and the superconducting transition Tc occurs when r 1⁄4 0. According to Hegger, H., Petrovic, C., Moshopoulou, E.G., Hundley, M.F., Sarrao, J.L., Fisk, Z., Thompson, J.D., 2000. Pressure-induced superconductivity in quasi-2D CeRhIn5. Phys. Rev. Lett. 84 (21), 4986. 1.5 2.0 1.0 120 100 80 60 40 20 MO+ SC 1.6 1.8 PC1 Pc2 2.2 Magnetic field, temperature, and pressure phase diagram of CeRhIn5. The T1⁄40.65 K plane represents the extrapolated T1⁄40 QCP. Here, lines of phase transitions are expected between magnetically ordered (MO) to coexisting magnetic order with superconductivity (MO+SC) to a superconducting phase (SC), and finally a high field magnetic disordered state (MD). Note the tetracritical point at Pc2. According to Park, T., Ronning, F., Yuan, H.Q., Salamon, M.B., Movshovich, R., Sarrao, J.L., Thompson, J.D., 2006. Hidden magnetism and quantum criticality in the heavy fermion superconductor CeRhIn5. Nature 440 (7080), 65-68. FIG. 17 T = 0.65 K plane MO MD H (kOe) r (μΩ cm) SC T (K) MO SC P (GPa) H = 0 kOe planePDF Image | HANDBOOK ON THE PHYSICS AND CHEMISTRY OF RARE EARTHS
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