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    Melting point depression of the charge density wave in 1T−TiSe2 due to size effects

    Saif Siddique1,2,*, Mehrdad T. Kiani1,3,*, Omri Lesser4, Stephen D. Funni1, Nishkarsh Agarwal5, Maya Gates6, Miti Shah5, William Millsaps5, Suk Hyun Sung7 et al.

    Noah Schnitzer1,2, Lopa Bhatt8, David A. Muller2,8, Robert Hovden5, Ismail El Baggari7,9, Eun-Ah Kim4, and Judy J. Cha1,†

    • *These authors contributed equally to this work.
    • †Contact author: jc476@cornell.edu

    Phys. Rev. B 113, 224106 – Published 5 June, 2026

    DOI: https://doi.org/10.1103/3dm3-g29b

    Abstract

    In correlated electronic states, observation of size-dependent nucleation and melting is rarely reported, likely due to the extremely small length scales necessary to observe such effects for electronic states. Here, using 1T−TiSe2 nanoflakes as a prototypical two-dimensional charge density wave (CDW) system, we perform in situ cryogenic electron microscopy with temperature down to 20 K and observe size-dependent melting of CDWs. Specifically, we observe a melting point depression of CDW for 1T−TiSe2 flakes with lateral sizes less than 100 nm. By fitting experimental data to a Ginzburg-Landau model, we estimate a zero-temperature correlation length of 10–50 nm, which matches the reported CDW domain size for 1T−TiSe2. As the flake size approaches the correlation length, the divergence of the CDW correlation length near the transition is cut off by the finite flake size, limiting long-range order and thereby lowering the transition temperature. For very small flakes whose size is close to the correlation length, we also observe absence of long-range CDW, as predicted by the model.

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