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METALS, SUPERCONDUCTORS... 2009High field resistivity measurem<strong>en</strong>ts on single crystalline UPt 2 Si 2Tetragonal UPt 2 Si 2 has rec<strong>en</strong>tly be<strong>en</strong> characterized as amoderately mass <strong>en</strong>hanced antiferromagnet (T N = 32 K),which in various physical properties closely resembles thehidd<strong>en</strong> order material URu 2 Si 2 [Süllow et al., J. Phys. Soc.Jpn. 77, 024708 (2008); Johanns<strong>en</strong> et al., Phys. Rev. B 78,121103 (2008) ; Kim et al., Phys. Rev. Lett. 91, 256401(2003); Amitsuka et al., Physica B 177, 173 (1992) ].are clearly to be se<strong>en</strong>, supporting the notion of the similaritybetwe<strong>en</strong> the two systems. Pres<strong>en</strong>tly, high field magnetizationmeasurem<strong>en</strong>ts at 3 He temperatures are underway toext<strong>en</strong>d the determination of these phase boundaries to verylow temperatures.Similar to URu 2 Si 2 , high field phase transitions at low temperatureshave be<strong>en</strong> observed in UPt 2 Si 2 , that is in fieldsof 30 T to 45 T along the a direction and 20 T to 33 Talong c [Amitsuka]. Rec<strong>en</strong>t high field measurem<strong>en</strong>ts revealadditional structure in the magnetic phase diagram, emphasizingthe close resemblance to URu 2 Si 2 .Based on these findings, the goal of the pres<strong>en</strong>t set of experim<strong>en</strong>tswas to verify and more accurately define the highfield phase boundaries observed in previous resistivity andmagnetization measurem<strong>en</strong>ts. Therefore, high field resistivityexperim<strong>en</strong>ts at low temperatures along the crystallographica and c axes of UPt 2 Si 2 were initiated and carriedout.We have measured the high field resistivity along the crystallographica and c axes in field and temperature sweeps upto 28 T and 40 K. From our data we calculated the differ<strong>en</strong>tialresistivities ∂R/∂B and ∂R/∂T , in which the transitionsappear as local maxima (∂R/∂B) or minima (∂R/∂T ).In the temperature sweeps the transition to the antiferromagnetphase is clearly visible for both directions. In fieldsweeps with B applied along the a axis the high field phaseis not accessible but for B//c the phase boundary to thelowest high field phase occurring at ∼ 25 T below 18 K isvisible.Together with the data tak<strong>en</strong> previously, we construct themagnetic phase diagram of UPt 2 Si 2 , as shown in figure 86.In these diagrams, field induced phases similar to URu 2 Si 2Figure 86: Proposed magnetic phase diagrams for the crystallographica and c directions derived from previous and actual magnetizationand resistivity measurem<strong>en</strong>ts.I. SheikinD. Schulze Grachtrup, S. Süllow (TU Braunschweig, Institute for Physics of Cond<strong>en</strong>sed Matter, Braunschweig, Germany)64

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