Apr 24, 2024
11:15am - 11:30am
Terrace Suite 2, Level 4, Summit
Volodymyr Buturlim1,Xiaxin Ding1,Sabin Regmi1,Chris Marianetti2,Michael Manley3,Jason Jeffries4,Krzysztof Gofryk1
Idaho National Laboratory1,Columbia University2,Oak Ridge National Laboratory3,Lawrence Livermore National Laboratory4
Volodymyr Buturlim1,Xiaxin Ding1,Sabin Regmi1,Chris Marianetti2,Michael Manley3,Jason Jeffries4,Krzysztof Gofryk1
Idaho National Laboratory1,Columbia University2,Oak Ridge National Laboratory3,Lawrence Livermore National Laboratory4
Uranium is one of the only elemental metals in which charge density waves have been observed (the phases are labeled α<sub>1</sub>, α<sub>2</sub>, and α<sub>3</sub>). The first transition takes place at 43 K (α<sub>1</sub>), the second at 38 K (α<sub>2</sub>), and the last one stabilizes below 25 K (α<sub>3</sub>). The structure below the transition is complex, consisting of small displacements of the atoms along all three of the orthorhombic axes. Despite the large experimental and theoretical effort, the nature of these transitions is still elusive, but it is believed to be associated with the unique coupling of 5f states, residing in the vicinity of the Fermi level, and the lattice vibrations. Here we present detailed experimental and theoretical studies of low-temperature thermal, thermodynamic, and electronic transport properties of the high-quality single crystals of α-U, across the CDW transitions.<br/><br/>*<i>V.B. acknowledges the support from Idaho National Laboratory’s Laboratory Directed Research and Development (LDRD) program under DOE Idaho Operations Office Contract DE-AC07-05ID14517. K.G. acknowledges support from the Division of Materials Science and Engineering, Office of Basic Energy Sciences, Office of Science of the U. S. Department of Energy (U.S. DOE).</i>