Melting point depression of charge density wave in 1T-TiSe$_2$ due to size effects
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| Main Authors: | , , , , , , , , , , , , , , , |
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| Format: | Preprint |
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2025
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| _version_ | 1866908549506924544 |
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| author | Siddique, Saif Kiani, Mehrdad T. Lesser, Omri Funni, Stephen D. Agarwal, Nishkarsh Gates, Maya Shah, Miti Millsaps, William Sung, Suk Hyun Schnitzer, Noah Bhatt, Lopa Muller, David A. Hovden, Robert Baggari, Ismail El Kim, Eun-Ah Cha, Judy J. |
| author_facet | Siddique, Saif Kiani, Mehrdad T. Lesser, Omri Funni, Stephen D. Agarwal, Nishkarsh Gates, Maya Shah, Miti Millsaps, William Sung, Suk Hyun Schnitzer, Noah Bhatt, Lopa Muller, David A. Hovden, Robert Baggari, Ismail El Kim, Eun-Ah Cha, Judy J. |
| contents | Classical nucleation theory predicts size-dependent nucleation and melting due to surface and confinement effects at the nanoscale. 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-TiSe$_2$ nanoflakes as a prototypical two-dimensional (2D) charge density wave (CDW) system, we perform in-situ cryogenic electron microscopy with temperature down to 20 K and observe size-dependent nucleation and melting of CDWs. Specifically, we observe a melting point depression of CDW for 1T-TiSe$_2$ 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-TiSe$_2$. 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 CDWs, as predicted by the model. We thus show that an electronic phase transition follows classical nucleation theory. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2509_16730 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Melting point depression of charge density wave in 1T-TiSe$_2$ due to size effects Siddique, Saif Kiani, Mehrdad T. Lesser, Omri Funni, Stephen D. Agarwal, Nishkarsh Gates, Maya Shah, Miti Millsaps, William Sung, Suk Hyun Schnitzer, Noah Bhatt, Lopa Muller, David A. Hovden, Robert Baggari, Ismail El Kim, Eun-Ah Cha, Judy J. Materials Science Classical nucleation theory predicts size-dependent nucleation and melting due to surface and confinement effects at the nanoscale. 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-TiSe$_2$ nanoflakes as a prototypical two-dimensional (2D) charge density wave (CDW) system, we perform in-situ cryogenic electron microscopy with temperature down to 20 K and observe size-dependent nucleation and melting of CDWs. Specifically, we observe a melting point depression of CDW for 1T-TiSe$_2$ 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-TiSe$_2$. 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 CDWs, as predicted by the model. We thus show that an electronic phase transition follows classical nucleation theory. |
| title | Melting point depression of charge density wave in 1T-TiSe$_2$ due to size effects |
| topic | Materials Science |
| url | https://arxiv.org/abs/2509.16730 |