Dec 4, 2024
9:15am - 9:30am
Hynes, Level 2, Room 207
Nitish Mathur1,Guangming Cheng1,Fang Yuan1,Ratnadwip Singha1,2,Scott B. Lee1,Vincent M. Plisson3,Francisco Ballester4,Jiangchang Zheng5,Caiyun Chen5,Berthold Jäck5,Kenneth Burch3,Ion Errea4,Maia G. Vergniory4,6,Sanfeng Wu1,Nan Yao1,Leslie Schoop1
Princeton University1,Indian Institute of Technology Guwahati2,Boston College3,Donostia International Physics Center4,The Hong Kong University of Science and Technology5,Max Planck Institute for Chemical Physics of Solids6
Nitish Mathur1,Guangming Cheng1,Fang Yuan1,Ratnadwip Singha1,2,Scott B. Lee1,Vincent M. Plisson3,Francisco Ballester4,Jiangchang Zheng5,Caiyun Chen5,Berthold Jäck5,Kenneth Burch3,Ion Errea4,Maia G. Vergniory4,6,Sanfeng Wu1,Nan Yao1,Leslie Schoop1
Princeton University1,Indian Institute of Technology Guwahati2,Boston College3,Donostia International Physics Center4,The Hong Kong University of Science and Technology5,Max Planck Institute for Chemical Physics of Solids6
Charge density waves (CDWs) are emergent phenomena in quantum materials, characterized by periodic modulations in charge ordering. Recently, novel functionalities of CDW phases in van der Waals (vdW) materials, such as 1T-Ta(S,Se)<sub>2</sub>, have opened new prospects for engineering and exploring CDW-driven symmetry-breaking quantum phenomena near room temperature. However, there is a scarcity of two-dimensional (2D) materials that exhibit high-temperature CDW transitions and can be easily exfoliated to fabricate nanodevices. Here we report on TaCo<sub>2</sub>Te<sub>2</sub> (space group Pmna), a 2D van der Waals Peierls-distorted metal that exhibits a one-dimensional commensurate CDW (1D-C-CDW) phase at room temperature and a reversible CDW transition (T<sub>c</sub>) near 573 K. In-situ heating transmission electron microscopy (TEM) reveals irreversible hidden CDW ordering above T<sub>c</sub> in exfoliated nanoflakes and focused ion beam (FIB) fabricated lamellae (<100 nm) of TaCo<sub>2</sub>Te<sub>2</sub>, manifesting as ordered incommensurate (O-IC) CDW superlattice peaks. Interestingly, we also observed O-IC CDW ordering in TaNi<sub>2</sub>Te<sub>2</sub> (space group Pmna) nanoflakes, an undistorted version of TaCo<sub>2</sub>Te<sub>2</sub>, with a multi-q vector CDW ordering, in contrast to the 1D O-IC CDW ordering in TaCo<sub>2</sub>Te<sub>2</sub>. This irreversible O-IC CDW ordering is stable only in Ta(Co,Ni)<sub>2</sub>Te<sub>2</sub> nanoflakes, not in the bulk crystal. The presence of internal residual strain and soft phonon modes facilitates the nucleation of competing charge orderings in Ta(Co,Ni)<sub>2</sub>Te<sub>2</sub> nanoflakes at high temperatures and offers thermomechanical manipulation as a route to engineering CDW states at and above room temperature.