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Badola S, Mukherjee S, Ghosh B, Sunil G, Vaitheeswaran G, Garcia-Castro AC, Saha S. Lattice dynamics across the ferroelastic phase transition in Ba 2ZnTeO 6: a Raman and first-principles study. Phys Chem Chem Phys 2022; 24:20152-20163. [PMID: 35993971 DOI: 10.1039/d2cp03137j] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/21/2022]
Abstract
Structural phase transitions drive several unconventional phenomena including some illustrious ferroic attributes which are relevant for technological advancements. On this note, we have investigated the ferroelastic structural transition of perovskite-type trigonal Ba2ZnTeO6 across Tc ∼ 150 K. With the help of Raman spectroscopy and density-functional theory (DFT)-based calculations, we report new intriguing observations associated with the phase transition in Ba2ZnTeO6. We observed the presence of a central peak (quasi-elastic Rayleigh profile), huge softening in the soft mode, hysteretic phonon behavior, and signatures of coexistent phases. The existence of a central peak in Ba2ZnTeO6 is manifested by a sharp rise in the intensity of the Rayleigh profile concomitant with the huge damping (or softening) of the soft mode (at ∼31 cm-1) near Tc, shedding light on the lattice dynamics during the phase transition. This is further corroborated by our phonon calculations that show that the soft mode (Eg) in the high-symmetry structure involving TeO6 octahedral rotation (with Ba and Zn translation) condenses into Ag and Bg modes in the C2/m low-symmetry phase. While most of the phonon bands split below Tc confirming the phase transition, we observed thermal hysteretic behavior of phonon modes, which signifies the first-order nature of the transition and the presence of coexisting phases as corroborated by our temperature-dependent X-ray diffraction and specific heat measurements.
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Affiliation(s)
- Shalini Badola
- Indian Institute of Science Education and Research Bhopal, Bhopal 462066, India.
| | - Supratik Mukherjee
- Advanced Centre of Research in High Energy Materials (ACRHEM), University of Hyderabad, Prof. C. R. Rao Road, Gachibowli, Hyderabad 500046, Telangana, India
| | - B Ghosh
- Indian Institute of Science Education and Research Bhopal, Bhopal 462066, India.
| | - Greeshma Sunil
- Indian Institute of Science Education and Research Bhopal, Bhopal 462066, India.
| | - G Vaitheeswaran
- School of Physics, University of Hyderabad, Prof. C. R. Rao Road, Gachibowli, Hyderabad 500046, Telangana, India
| | - A C Garcia-Castro
- School of Physics, Universidad Industrial de Santander, Calle 09 Carrera 27, Bucaramanga, Santander, 680002, Colombia
| | - Surajit Saha
- Indian Institute of Science Education and Research Bhopal, Bhopal 462066, India.
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Liu N, Holmes J, Bordenave N, Hemmer E. Microwave-assisted synthesis of NaMnF 3 particles with tuneable morphologies. Chem Commun (Camb) 2021; 57:11799-11802. [PMID: 34676854 DOI: 10.1039/d1cc04714k] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/05/2023]
Abstract
Here, the synthesis of sub-micron MMnF3 (M = Na or K) particles by a rapid microwave-assisted approach is reported. Adjustment of the Na+-to-Mn2+ ratio in the reaction mixture yielded tuneable morphologies, i.e., rods, ribbons, and plates. Relaxometric results indicated that poly(acrylic acid)-capped MMnF3 particles exhibited characteristic magnetic properties, which endows them with potential T1-weighted contrast agent capabilities.
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Affiliation(s)
- Nan Liu
- Department of Chemistry and Biomolecular Sciences, University of Ottawa, 10 Marie-Curie Private, Ottawa (ON) K1N 6N5, Canada.
| | - Jessica Holmes
- Department of Chemistry and Biomolecular Sciences, University of Ottawa, 10 Marie-Curie Private, Ottawa (ON) K1N 6N5, Canada.
| | - Nicolas Bordenave
- Department of Chemistry and Biomolecular Sciences, University of Ottawa, 10 Marie-Curie Private, Ottawa (ON) K1N 6N5, Canada. .,School of Nutrition Sciences, University of Ottawa, 451 Smyth Road, Ottawa (ON) K1H 8L1, Canada
| | - Eva Hemmer
- Department of Chemistry and Biomolecular Sciences, University of Ottawa, 10 Marie-Curie Private, Ottawa (ON) K1N 6N5, Canada. .,Centre for Advanced Materials Research (CAMaR), University of Ottawa, Ottawa (ON) K1N 6N5, Canada
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Gelves-Badillo JS, Romero AH, Garcia-Castro AC. Unveiling the mechanisms behind the ferroelectric response in the Sr(Nb,Ta)O 2N oxynitrides. Phys Chem Chem Phys 2021; 23:17142-17149. [PMID: 34179906 DOI: 10.1039/d1cp01716k] [Citation(s) in RCA: 3] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/21/2022]
Abstract
Oxynitride perovskites of the type ABO2N have attracted considerable attention thanks to their potential ferroelectric behavior and tunable bandgap energy, making them ideal candidates for photocatalysis processes. Therefore, in order to shed light on the origin of their ferroelectric response, here we report a complete analysis of the structural and vibrational properties of SrNbO2N and SrTaO2N oxynitrides. By employing first-principles calculations, we analyzed the symmetry in-equivalent structures considering the experimentally reported parent I4/mcm space group (with a phase a0a0c- in Glazer's notation). Based on the I4/mcm reference within the 20-atoms unit-cell, we found and studied the ensemble of structures where different octahedral anionic orderings are allowed by symmetry. Thus, by exploring the vibrational landscape of the cis- and trans-type configuration structures and supported by the ionic eigendisplacements and the Born effective charges, we explained the mechanism responsible for the appearance of stable ferroelectric phases in both anionic orderings. The latter goes from covalent-driven in the trans-type ordering to the geometrically-driven in the cis-type configuration. Finally, we found in both cases that the biaxial xy epitaxial strain considerably enhances such ferroelectric response.
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Affiliation(s)
- J S Gelves-Badillo
- School of Physics, Universidad Industrial de Santander, Carrera 27 Calle 09, 680002, Bucaramanga, Colombia.
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Xu X, Zhang H, Zhong Z, Zhang R, Yin L, Sun Y, Huang H, Lu Y, Lu Y, Zhou C, Ma Z, Shen L, Wang J, Guo J, Sun J, Sheng Z. Polar Rectification Effect in Electro-Fatigued SrTiO 3-Based Junctions. ACS APPLIED MATERIALS & INTERFACES 2020; 12:31645-31651. [PMID: 32551489 DOI: 10.1021/acsami.0c08418] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/11/2023]
Abstract
Rectifying semiconductor junctions are crucial to electronic devices. They convert alternating current into a direct one by allowing unidirectional charge flows. Analogous to the current-flow rectification for itinerary electrons, here, a polar rectification that is based on the localized oxygen vacancies (OVs) in a Ti/fatigued-SrTiO3 (fSTO) Schottky junction is first demonstrated. The fSTO with OVs is produced by an electrodegradation process. The different movabilities of localized OVs and itinerary electrons in the fSTO yield a unidirectional electric polarization at the interface of the junction under the coaction of external and built-in electric fields. Moreover, the fSTO displays a pre-ferroelectric state located between paraelectric and ferroelectric phases. The pre-ferroelectric state has three sub-states and can be easily driven into a ferroelectric state by an external electric field. These observations open up opportunities for potential polar devices and may underpin many useful polar-triggered electronic phenomena.
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Affiliation(s)
- Xueli Xu
- Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Science, Hefei 230031, China
- University of Science and Technology of China, Hefei, Anhui 230026, China
- Key Laboratory of Photovoltaic and Energy Conservation Materials, Institute of Applied Technology, Chinese Academy of Sciences, Hefei 230031, China
| | - Hui Zhang
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
- Fert Beijing Institute, School of Microelectronics, Beijing Advanced Innovation Center for Big Data and Brain Computing, Beihang University, Beijing 100191, China
| | - Zhicheng Zhong
- Key Laboratory of Magnetic Materials and Devices, Zhejiang Province Key Laboratory of Magnetic Materials and Application Technology, Ningbo Institute of Materials Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, China
| | - Ranran Zhang
- Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Science, Hefei 230031, China
| | - Lihua Yin
- Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China
| | - Yuping Sun
- Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China
| | - Haoliang Huang
- Anhui Laboratory of Advanced Photon Science and Technology, National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei 230026, P. R. China
| | - Yalin Lu
- Anhui Laboratory of Advanced Photon Science and Technology, National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei 230026, P. R. China
| | - Yi Lu
- Institute for Theoretical Physics, Heidelberg University, Philosophenweg 19, 69120 Heidelberg, Germany
| | - Chun Zhou
- Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Science, Hefei 230031, China
| | - Zongwei Ma
- Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Science, Hefei 230031, China
| | - Lei Shen
- Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Science, Hefei 230031, China
- University of Science and Technology of China, Hefei, Anhui 230026, China
| | - Junsong Wang
- Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Science, Hefei 230031, China
| | - Jiandong Guo
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
| | - Jirong Sun
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
| | - Zhigao Sheng
- Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Science, Hefei 230031, China
- Key Laboratory of Photovoltaic and Energy Conservation Materials, Institute of Applied Technology, Chinese Academy of Sciences, Hefei 230031, China
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Garcia-Castro AC, Ibarra-Hernandez W, Bousquet E, Romero AH. Direct Magnetization-Polarization Coupling in BaCuF_{4}. PHYSICAL REVIEW LETTERS 2018; 121:117601. [PMID: 30265112 DOI: 10.1103/physrevlett.121.117601] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/02/2018] [Revised: 08/04/2018] [Indexed: 06/08/2023]
Abstract
Herewith, first-principles calculations based on density functional theory are used to describe the ideal magnetization reversal through polarization switching in BaCuF_{4} which, according to our results, could be accomplished close to room temperature. We also show that this ideal coupling is driven by a single soft mode that combines both polarization, and octahedral rotation. The later being directly coupled to the weak ferromagnetism of BaCuF_{4}. This, added to its strong Jahn-Teller distortion and its orbital ordering, makes this material a very appealing prototype for crystals in the ABX_{4} family for multifunctional applications. The described mechanism behaves ideally as it couples the ferroelectric and the magnetic properties naturally and it has not been reported previously.
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Affiliation(s)
- A C Garcia-Castro
- Department of Physics, Universidad Industrial de Santander, Carrera 27 Calle 9, Bucaramanga, Colombia
- Physique Théorique des Matériaux, CESAM, Université de Liège, B-4000 Sart-Tilman, Belgium
| | - W Ibarra-Hernandez
- Department of Physics and Astronomy, West Virginia University, Morgantown, West Virginia WV-26506-6315, USA
- Facultad de Ingeniería-BUAP, Apartado Postal J-39, Puebla, Pue. 72570, Mexico
| | - Eric Bousquet
- Physique Théorique des Matériaux, CESAM, Université de Liège, B-4000 Sart-Tilman, Belgium
| | - Aldo H Romero
- Department of Physics and Astronomy, West Virginia University, Morgantown, West Virginia WV-26506-6315, USA
- Facultad de Ingeniería-BUAP, Apartado Postal J-39, Puebla, Pue. 72570, Mexico
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