Metal-insulator transition effect on Graphene/VO2 heterostructure via temperature-dependent Raman spectroscopy and resistivity measurement
Issued Date
2024-12-01
Resource Type
eISSN
20452322
Scopus ID
2-s2.0-85185948215
Journal Title
Scientific Reports
Volume
14
Issue
1
Rights Holder(s)
SCOPUS
Bibliographic Citation
Scientific Reports Vol.14 No.1 (2024)
Suggested Citation
Lerttraikul K., Rattanasakuldilok W., Pakornchote T., Bovornratanaraks T., Klanurak I., Taychatanapat T., Srathongsian L., Seriwatanachai C., Kanjanaboos P., Chatraphorn S., Kittiwatanakul S. Metal-insulator transition effect on Graphene/VO2 heterostructure via temperature-dependent Raman spectroscopy and resistivity measurement. Scientific Reports Vol.14 No.1 (2024). doi:10.1038/s41598-024-54844-w Retrieved from: https://repository.li.mahidol.ac.th/handle/20.500.14594/97456
Title
Metal-insulator transition effect on Graphene/VO2 heterostructure via temperature-dependent Raman spectroscopy and resistivity measurement
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Abstract
High-quality VO2 films were fabricated on top of c-Al2O3 substrates using Reactive Bias Target Ion Beam Deposition (RBTIBD) and the studies of graphene/VO2 heterostructure were conducted. Graphene layers were placed on top of ∼ 50 and ∼ 100 nm VO2. The graphene layers were introduced using mechanical exfoliate and CVD graphene wet-transfer method to prevent the worsening crystallinity of VO2, to avoid the strain effect from lattice mismatch and to study how VO2 can affect the graphene layer. Slight increases in graphene/VO2 TMIT compared to pure VO2 by ∼ 1.9 ∘C and ∼ 3.8 ∘C for CVD graphene on 100 and 50 nm VO2, respectively, were observed in temperature-dependent resistivity measurements. As the strain effect from lattice mismatch was minimized in our samples, the increase in TMIT may originate from a large difference in the thermal conductivity between graphene and VO2. Temperature-dependent Raman spectroscopy measurements were also performed on all samples, and the G-peak splitting into two peaks, G+ and G-, were observed on graphene/VO2 (100 nm) samples. The G-peak splitting is a reversible process and may originates from in-plane asymmetric tensile strain applied under the graphene layer due to the VO2 phase transition mechanism. The 2D-peak measurements also show large blue-shifts around 13 cm-1 at room temperature and slightly red-shifts trend as temperature increases for 100 nm VO2 samples. Other electronic interactions between graphene and VO2 are expected as evidenced by 2D-peak characteristic observed in Raman measurements. These findings may provide a better understanding of graphene/VO2 and introduce some new applications that utilize the controllable structural properties of graphene via the VO2 phase transition.