Dynamic phase transition into a mixed-CDW state in 1$T$-TaS$_2$ via a thermal quench
Ultrafast light-matter interaction has emerged as a new mechanism to exert control over the macroscopic properties of quantum materials toward novel functionality. To date, technological applications of these non-thermal phases are limited by their ultrashort lifetimes and low-ordering temperatures....
Saved in:
Main Authors | , , , , , , , , , , |
---|---|
Format | Journal Article |
Language | English |
Published |
10.07.2024
|
Subjects | |
Online Access | Get full text |
DOI | 10.48550/arxiv.2407.07953 |
Cover
Loading…
Summary: | Ultrafast light-matter interaction has emerged as a new mechanism to exert
control over the macroscopic properties of quantum materials toward novel
functionality. To date, technological applications of these non-thermal phases
are limited by their ultrashort lifetimes and low-ordering temperatures. Among
the most studied photoinduced metastable phases for their technological promise
is the hidden metallic charge density wave (H-CDW) in the model correlated CDW
compound 1$T$-TaS$_2$. Despite active study and engineering, the nature of the
photoinduced H-CDW remains the subject of debate and is only accessible at
cryogenic temperatures. Here, we stabilize the H-CDW phase at thermal
equilibrium up to near-room temperature by accessing an intermediate mixed CDW
order regime via thermal quenching. Using x-ray high dynamic range reciprocal
space mapping (HDRM) and scanning tunneling spectroscopy (STS), we reveal the
coexistence of commensurate (C) CDW and H-CDW domains below 180 K during
cooling and below 210 K during warming. Our findings show that each order
parameter breaks basal plane mirror symmetry with different chiral orientations
and induces out-of-plane unit cell tripling in the H-CDW phase. Despite
metallic domain walls and a finite density of states at zero bias observed via
STS, bulk resistance remains insulating due to CDW stacking disorder. This
study establishes the H-CDW as a thermally stable phase and introduces a new
mechanism for switchable metallic behavior in thin flakes of 1$T$-TaS$_2$ and
similar materials with competing order phases. |
---|---|
DOI: | 10.48550/arxiv.2407.07953 |