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SUMMARY:Seminar By Despina Louca, Univ. of Virginia
DTSTAMP:20190205T174230Z
DESCRIPTION:Title: Topological phase transitions in MoTe2 Weyl semimetal\NHost: Dragana Popvic\NAbstract: A Weyl (semi)metal is a new topological state of matter that hosts the condensed matter equivalent of relativistic Weyl fermions. Weyl fermions exist as low-energy electronic excitations at Weyl nodes in three-dimensional momentum space, producing exotic physical properties such as unique surface Fermi arcs and negative magnetoresistance. The topological Weyl state can be realized by breaking either time-reversal or lattice inversion symmetry. A candidate topological Weyl semimetal is the quasi two-dimensional transition metal dichalcogenide MoTe2. The transition to the non-trivial topologically protected crystal state occurs upon cooling from the high temperature 1T′ monoclinic phase to the low temperature orthorhombic Td phase. The transition is driven by c-axis layer stacking order around 250 K [9-12]. Upon cooling to the non-centrosymmetric Td phase, Weyl quasiparticles are expected at characteristic electron and hole band crossings in momentum space. Furthermore, MoTe2 is a candidate topological superconductor in the orthorhombic phase at ambient pressure. In the superconducting state, Fermi arcs are proposed to still exist. The application of pressure can dramatically enhance the superconducting transition temperature from 0.25 up to ~8 K as well as extend the superconducting state over a wide pressure range. Recent studies suggested that while in the superconducting state, a phase transition occurs from the orthorhombic Td back to the monoclinic 1T′ phase under pressure. Using single crystal neutron diffraction, the pressure-temperature phase diagram is mapped out and combined with band structure calculations, we elucidate the effects of pressure on the electronic band structure topology. The results provide evidence for a topological state, beyond the Td-1T' boundary with applied pressure.\NFor more information please contact Aisha Qureshi
X-ALT-DESC;FMTTYPE=text/html:**Title**: Topological phase transitions in MoTe_{2} Weyl semimetal

**Host**: Dragana Popvic

**Abstract**: A Weyl (semi)metal is a new topological state of matter that hosts the condensed matter equivalent of relativistic Weyl fermions. Weyl fermions exist as low-energy electronic excitations at Weyl nodes in three-dimensional momentum space, producing exotic physical properties such as unique surface Fermi arcs and negative magnetoresistance. The topological Weyl state can be realized by breaking either time-reversal or lattice inversion symmetry. A candidate topological Weyl semimetal is the quasi two-dimensional transition metal dichalcogenide MoTe_{2}. The transition to the non-trivial topologically protected crystal state occurs upon cooling from the high temperature 1T′ monoclinic phase to the low temperature orthorhombic Td phase. The transition is driven by c-axis layer stacking order around 250 K [9-12]. Upon cooling to the non-centrosymmetric T_{d} phase, Weyl quasiparticles are expected at characteristic electron and hole band crossings in momentum space. Furthermore, MoTe_{2} is a candidate topological superconductor in the orthorhombic phase at ambient pressure. In the superconducting state, Fermi arcs are proposed to still exist. The application of pressure can dramatically enhance the superconducting transition temperature from 0.25 up to ~8 K as well as extend the superconducting state over a wide pressure range. Recent studies suggested that while in the superconducting state, a phase transition occurs from the orthorhombic T_{d} back to the monoclinic 1T′ phase under pressure. Using single crystal neutron diffraction, the *pressure-temperature* phase diagram is mapped out and combined with band structure calculations, we elucidate the effects of pressure on the electronic band structure topology. The results provide evidence for a topological state, beyond the T_{d}-1T' boundary with applied pressure.

For more information please contact Aisha Qureshi

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