In this work, the high-temperature and high-pressure ferroelectric, structural, and electrical transport properties for CuInP2Se6 upon compression and decompression under different hydrostatic environments were comprehensively studied via Raman spectroscopy, electrical conductivity, and high-resolution transmission electron microscopy observations. Upon non-hydrostatic pressurization, CuInP2Se6 experienced two successive phase transitions at 5.4 and 14.1 GPa originating from the rapid compression of van der Waals gaps and the local structure variation of Se-P-Se bonds, followed by a metallization at 25.1 GPa. Furthermore, a ∼2.0 GPa pressure hysteresis was detected for the emergence of electronic transformation in CuInP2Se6 under hydrostatic conditions owing to the influence of hydrostaticity. Upon decompression, the phase transition of CuInP2Se6 was demonstrated to be reversible with considerable pressure hysteresis under different hydrostatic environments. In addition, the positive sinusoidal voltage-dependent electrical current relations with the nonlinearity factors of ∼1.0 manifested the Ohmic response of CuInP2Se6 under high pressure conditions. Meantime, the disappearance of the P1 Raman peak and the discontinuities in Raman shifts and full width at half-maximums offered robust evidence on the occurrence of ferroelectric crossover in CuInP2Se6. It is the first time that the phase boundary from the mixed antiferroelectric and ferroelectric (FE) orderings into the FE state of CuInP2Se6 is well established [i.e., TC (K) = 165.5 P (GPa) + 292.1] under the conditions of 298-873 K and 0.4-40.3 GPa. Our findings shed light on the ferroelectricity, crystalline structure, and electrical configuration of CuInP2Se6 under extreme conditions, which is of paramount significance to the fundamental research and potential applications for other metallic thio(seleno)phosphates.
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http://dx.doi.org/10.1063/5.0251653 | DOI Listing |
J Chem Phys
March 2025
Laboratory of Optoelectronic Materials and Devices, School of Materials Science and Engineering, Guizhou Minzu University, Guiyang 550025, China.
In this work, the high-temperature and high-pressure ferroelectric, structural, and electrical transport properties for CuInP2Se6 upon compression and decompression under different hydrostatic environments were comprehensively studied via Raman spectroscopy, electrical conductivity, and high-resolution transmission electron microscopy observations. Upon non-hydrostatic pressurization, CuInP2Se6 experienced two successive phase transitions at 5.4 and 14.
View Article and Find Full Text PDFNanomaterials (Basel)
July 2022
School of Mechanics, Civil Engineering and Architecture, Northwestern Polytechnical University, Xi'an 710072, China.
Two-dimensional (2D) transition metal dichalcogenides endow individually addressable valleys in momentum space at the K and K' points in the first Brillouin zone due to the breaking of inversion symmetry and the effect of spin-orbit coupling. However, the application of 2H-VS monolayer in valleytronics is limited due to the valence band maximum (VBM) located at the Γ point. Here, by involving the 2D ferroelectric (FE) CuInPSe (CIPSe), the ferrovalley polarization, electronic structure, and magnetic properties of 2D 2H-VS/CIPSe heterostructures with different stacking patterns and FE polarizations have been investigated by using first-principles calculations.
View Article and Find Full Text PDFACS Nano
February 2022
Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United States.
Antiferroelectric (AFE) materials, in which alternating dipole moments cancel out to a zero net macroscopic polarization, can be used for high-density energy storage and memory applications. The AFE phase can exist in bulk CuInPSe, CuBiPS, and a few other transition-metal thiophosphates below 200 K. The required low temperature poses challenges for practical applications.
View Article and Find Full Text PDFNat Commun
July 2020
The Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, TN, 37831, USA.
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