TiSe2is an exciting material because it can be tuned between superconducting and charge density wave (CDW) transitions. In the monolayer limit, TiSe2exhibits a sizable energy gap in the CDW phase that makes it a promising quantum material. It is shown that interfacing a single layer of TiSe2with dissimilar van der Waals materials enables control of its properties. Using angle‐resolved photoemission spectroscopy, the energy gap opening is analyzed as a function of temperature for TiSe2monolayers supported on different van der Waals substrates. A substantial increase in the CDW transition temperature of ≈45 K is observed on MoS2compared to graphite (highly oriented pyrolytic graphite) substrates. This control of the CDW in monolayer TiSe2is suggested to arise from varying charge screening of the unconventional CDW of TiSe2by the substrate. In addition, the suppression of CDW order and a complete closing of the energy gap by electron doping of monolayer TiSe2is demonstrated. Regulating the many‐body physics phenomena in monolayer TiSe2lays the foundation of modifying TiSe2in, for example, artificial van der Waals heterostructures and thus creates a new approach for utilizing the quantum states of TiSe2in device applications.
Revealing the order parameter dynamics of 1T-TiSe$$_2$$ following optical excitation
Abstract The formation of a charge density wave state is characterized by an order parameter. The way it is established provides unique information on both the role that correlation plays in driving the charge density wave formation and the mechanism behind its formation. Here we use time and angle resolved photoelectron spectroscopy to optically perturb the charge-density phase in 1T-TiSe $$_2$$ 2 and follow the recovery of its order parameter as a function of energy, momentum and excitation density. Our results reveal that two distinct orders contribute to the gap formation, a CDW order and pseudogap-like order, manifested by an overall robustness to optical excitation. A detailed analysis of the magnitude of the the gap as a function of excitation density and delay time reveals the excitonic long-range nature of the CDW gap and the short-range Jahn–Teller character of the pseudogap order. In contrast to the gap, the intensity of the folded Se $$_{4p}$$ 4 p * band can only give access to the excitonic order. These results provide new information into the the long standing debate on the origin of the gap in TiSe $$_2$$ 2 and place it in the same context of other quantum materials where a pseudogap phase appears to be a precursor of long-range order.
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- NSF-PAR ID:
- 10376460
- Date Published:
- Journal Name:
- Scientific Reports
- Volume:
- 12
- Issue:
- 1
- ISSN:
- 2045-2322
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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- Free Publicly Accessible Full Text
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Accepted Manuscript1.0
- Journal Article:
- https://doi.org/10.1038/s41598-022-19319-w
