Hena Das
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Hena Das has a total of 123 co-authors. Here are the top co-authors by number of shared publications:
- Masaki Azuma
Kanagawa Institute of Industrial Science and Technology, 705-1 Shimoimaizumi, Ebina, Kanagawa 243-0435, Japan
11 shared publications - Takumi Nishikubo
Kanagawa Institute of Industrial Science and Technology, Ebina, Japan
7 shared publications - Kei Shigematsu
Materials and Structures Laboratory, Institute of Integrated Research, Institute of Science Tokyo, 4259 Nagatsuta, Midori-ku, Yokohama, Kanagawa 226-8501, Japan
6 shared publications - Yuki Sakai
Kanagawa Institute of Industrial Science and Technology, Ebina, Japan
5 shared publications - Masayuki Fukuda
Materials and Structures Laboratory, Institute of Integrated Research, Institute of Science Tokyo, Yokohama, Japan
4 shared publications Tetsu Watanuki
Synchrotron Radiation Research Center, National Institutes for Quantum Science and Technology (QST), Sayo, Japan
4 shared publications
Latest Publications
- 28 November 2025
- Published by American Chemical Society (ACS) in Journal of the American Chemical Society
- Vol. 147 (49) , 44845-44851
Achieving Canted-Spin Weak Ferromagnetism and Negative Thermal Expansion in A- and B-Site-Substituted Bismuth Ferrite
BiFeO3 is the most intensively investigated multiferroic material. It has a cycloidal spin modulation superimposed on G-type antiferromagnetic ordering of Fe3+ (S = 5/2), which prohibits the appearance of a net magnetization. We found that the simultaneous substitution of Ru4+ or Ir4+ for Fe3+ and Ca2+ for Bi3+ suppressed the cycloidal modulation and induced canted weak ferromagnetism at room temperature, while preserving the polar rhombohedral crystal structure. Moreover, the A- and B-site substitutions substantially lowered the ferroelectric transition temperature and resulted in a 1.77% volumetric negative thermal expansion around room temperature. These findings open an avenue for designing new BiFeO3-based functional materials.
- 28 November 2025
- Published by American Chemical Society (ACS) in Journal of the American Chemical Society
- Vol. 147 (49) , 44845-44851
Achieving Canted-Spin Weak Ferromagnetism and Negative Thermal Expansion in A- and B-Site-Substituted Bismuth Ferrite
BiFeO3 is the most intensively investigated multiferroic material. It has a cycloidal spin modulation superimposed on G-type antiferromagnetic ordering of Fe3+ (S = 5/2), which prohibits the appearance of a net magnetization. We found that the simultaneous substitution of Ru4+ or Ir4+ for Fe3+ and Ca2+ for Bi3+ suppressed the cycloidal modulation and induced canted weak ferromagnetism at room temperature, while preserving the polar rhombohedral crystal structure. Moreover, the A- and B-site substitutions substantially lowered the ferroelectric transition temperature and resulted in a 1.77% volumetric negative thermal expansion around room temperature. These findings open an avenue for designing new BiFeO3-based functional materials.
- Open Access
- 19 March 2025
- Published by Springer Nature in Nature Communications
- Vol. 16 (1) , 1
Author Correction: Pressure-induced charge amorphisation in BiNiO3
- 19 March 2025
- Published by Springer Nature in Nature Communications
- Vol. 16 (1) , 1
Open AccessAuthor Correction: Pressure-induced charge amorphisation in BiNiO3
- Open Access
- 5 March 2025
- Published by Springer Nature in Nature Communications
- Vol. 16 (1) , 1-7
Pressure-induced charge amorphisation in BiNiO3
The order or disorder of electrons is fundamental to materials properties and also provides simple analogues to the different states of matter. A charge ordered (CO) insulating state, analogous to a crystalline solid, is observed in many mixed valence materials. On heating, this melts to a charge liquid (metallic) phase, often with interesting associated physics and functions such as the Verwey transition of Fe3O4, colossal magnetoresistances in manganites (e.g., La0.5Ca0.5MnO3), and superconductivity in K-doped BaBiO3. Here we report the observation of pressure induced charge amorphisation in a crystalline material. BiNiO3 has charge distribution Bi3+ 0.5Bi5+ 0.5Ni2+O3 with long range order of the Bi3+ and Bi5+ states at ambient pressure, but adopts another, structurally crystalline, but charge glassy, insulating phase at pressures of 4–5 GPa and temperatures below 200 K, before metallization above 6 GPa. This is analogous to the much-studied pressure induced amorphisations of many crystalline materials and melting is even observed at accessible pressure/temperature. BiNiO3 provides fundamental insights to the study of amorphisation using charge states rather than atoms or molecules.
- 5 March 2025
- Published by Springer Nature in Nature Communications
- Vol. 16 (1) , 1-7
Open AccessPressure-induced charge amorphisation in BiNiO3
The order or disorder of electrons is fundamental to materials properties and also provides simple analogues to the different states of matter. A charge ordered (CO) insulating state, analogous to a crystalline solid, is observed in many mixed valence materials. On heating, this melts to a charge liquid (metallic) phase, often with interesting associated physics and functions such as the Verwey transition of Fe3O4, colossal magnetoresistances in manganites (e.g., La0.5Ca0.5MnO3), and superconductivity in K-doped BaBiO3. Here we report the observation of pressure induced charge amorphisation in a crystalline material. BiNiO3 has charge distribution Bi3+ 0.5Bi5+ 0.5Ni2+O3 with long range order of the Bi3+ and Bi5+ states at ambient pressure, but adopts another, structurally crystalline, but charge glassy, insulating phase at pressures of 4–5 GPa and temperatures below 200 K, before metallization above 6 GPa. This is analogous to the much-studied pressure induced amorphisations of many crystalline materials and melting is even observed at accessible pressure/temperature. BiNiO3 provides fundamental insights to the study of amorphisation using charge states rather than atoms or molecules.
- Open Access
Pressure-Induced YbFe2O4-Type to Spinel Structural Change of InGaMgO4
Spinel-type InGaMgO4 with a = 8.56615(3) Å was prepared by treating layered YbFe2O4-type InGaMgO4 at 6 GPa and 1473 K. DFT calculation and Rietveld analysis of synchrotron X-ray powder diffraction data revealed the inverse spinel structure with In3+:Ga3+/Mg2+ = 0.726:0.274 in the tetrahedral site and 0.137:0.863 in the octahedral site. InGaMgO4 spinel is an insulator with an experimental band gap of 2.80 eV, and the attempt at hole doping by post-annealing in a reducing atmosphere to introduce an oxygen defect was unsuccessful. This is the first report of the bulk synthesis of AB2O4 compounds with both YbFe2O4 and spinel polymorphs.
Open AccessPressure-Induced YbFe2O4-Type to Spinel Structural Change of InGaMgO4
Spinel-type InGaMgO4 with a = 8.56615(3) Å was prepared by treating layered YbFe2O4-type InGaMgO4 at 6 GPa and 1473 K. DFT calculation and Rietveld analysis of synchrotron X-ray powder diffraction data revealed the inverse spinel structure with In3+:Ga3+/Mg2+ = 0.726:0.274 in the tetrahedral site and 0.137:0.863 in the octahedral site. InGaMgO4 spinel is an insulator with an experimental band gap of 2.80 eV, and the attempt at hole doping by post-annealing in a reducing atmosphere to introduce an oxygen defect was unsuccessful. This is the first report of the bulk synthesis of AB2O4 compounds with both YbFe2O4 and spinel polymorphs.
- 16 July 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (2) , 024422
High-spin as a trigger of weak ferromagnetism in Co-substitutedElectric field control of magnetization is expected to be utilized for energy-efficient nonvolatile magnetic memory application. -substituted (BFCO) exhibits both ferroelectric polarization () and the spin canting induced weakly ferromagnetic moment () perpendicular to each other at room temperature. Magnetization reversal by electric field was observed in a BFCO thin film. In our previous theoretical calculation, spin canted collinear structure having a weak ferromagnetic moment was stabilized when high-spin was substituted in . To confirm the presence of high-spin in BFCO, the pressured-induced spin-state transition of was investigated by first-principles calculations and Co synchrotron x-ray emission spectroscopy. We investigated the spin state of during the pressure-induced structural transition from to Pnma. As a result, a pressure-induced transition from high-spin to low-spin was predicted. Moreover, the presence of high-spin at ambient pressure was confirmed in by observing the decrease of peaks of Co x-ray emission spectra under pressure. This study provides evidence that the weak ferromagnetism of BFCO is attributed to high-spin and provides insight that may help to enhance weak magnetization by substitution of other elements.- 16 July 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (2) , 024422
High-spin as a trigger of weak ferromagnetism in Co-substitutedElectric field control of magnetization is expected to be utilized for energy-efficient nonvolatile magnetic memory application. -substituted (BFCO) exhibits both ferroelectric polarization () and the spin canting induced weakly ferromagnetic moment () perpendicular to each other at room temperature. Magnetization reversal by electric field was observed in a BFCO thin film. In our previous theoretical calculation, spin canted collinear structure having a weak ferromagnetic moment was stabilized when high-spin was substituted in . To confirm the presence of high-spin in BFCO, the pressured-induced spin-state transition of was investigated by first-principles calculations and Co synchrotron x-ray emission spectroscopy. We investigated the spin state of during the pressure-induced structural transition from to Pnma. As a result, a pressure-induced transition from high-spin to low-spin was predicted. Moreover, the presence of high-spin at ambient pressure was confirmed in by observing the decrease of peaks of Co x-ray emission spectra under pressure. This study provides evidence that the weak ferromagnetism of BFCO is attributed to high-spin and provides insight that may help to enhance weak magnetization by substitution of other elements.- Open Access
- 17 June 2024
- Published by AIP Publishing in Applied Physics Letters
- Vol. 124 (25)
Magnetoelectric coupling at the domain level in polycrystalline hexagonal ErMnO3
We explore the impact of a magnetic field on the ferroelectric domain pattern in polycrystalline hexagonal ErMnO3 at cryogenic temperatures. Utilizing piezoelectric force microscopy measurements at 1.65 K, we observe modifications of the topologically protected ferroelectric domain structure induced by the magnetic field. These alterations likely result from strain induced by the magnetic field, facilitated by intergranular coupling in polycrystalline multiferroic ErMnO3. Our findings give insights into the interplay between electric and magnetic properties at the domain scale and represent a so far unexplored pathway for manipulating topologically protected ferroelectric vortex patterns in hexagonal manganites.
- 17 June 2024
- Published by AIP Publishing in Applied Physics Letters
- Vol. 124 (25)
Open AccessMagnetoelectric coupling at the domain level in polycrystalline hexagonal ErMnO3
We explore the impact of a magnetic field on the ferroelectric domain pattern in polycrystalline hexagonal ErMnO3 at cryogenic temperatures. Utilizing piezoelectric force microscopy measurements at 1.65 K, we observe modifications of the topologically protected ferroelectric domain structure induced by the magnetic field. These alterations likely result from strain induced by the magnetic field, facilitated by intergranular coupling in polycrystalline multiferroic ErMnO3. Our findings give insights into the interplay between electric and magnetic properties at the domain scale and represent a so far unexplored pathway for manipulating topologically protected ferroelectric vortex patterns in hexagonal manganites.
- 10 February 2024
- Published by American Chemical Society (ACS) in Chemistry of Materials
- Vol. 36 (4) , 1899-1907
Pressure Induced Amorphization of Pb2+ and Pb4+ in Perovskite PbFeO3
- 10 February 2024
- Published by American Chemical Society (ACS) in Chemistry of Materials
- Vol. 36 (4) , 1899-1907
Pressure Induced Amorphization of Pb2+ and Pb4+ in Perovskite PbFeO3
- Open Access
- 6 January 2023
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 5 (1) , 013007
Coupling between improper ferroelectricity and ferrimagnetism in the hexagonal ferriteHere, we propose an idea to realize noncollinear ferrimagnetic orders with a considerably high magnetization and their coupling with an improper ferroelectric (FE) order in hexagonal type systems which exhibit interesting topological orders. These magnetic and magnetoelectric phenomena are driven by the antisymmetric Dzyaloshinskii-Moriya interactions between the magnetic ions and their coupling with the ferroelectricity. The proposed two-sublattice magnetic system, generated by a specific charge-ordered state, forms multiple energetically close, noncollinear ferrimagnetic orders. This offers a platform to manipulate the microscopic magnetic interactions and to trigger spin-reorientation (SR) transitions by various efficient means. The two-sublattice structure was realized in the hexagonal phase of doped with electrons. The proposed electron-doped systems are expected to exhibit switchable electric polarization (), considerably high magnetization (), and magnetic transition near room temperature (). Based on the coupling between the magnetic interactions and the FE primary order parameter observed in this system, microscopic mechanisms to achieve electric field induced SR transitions and switching of the direction of are discussed.- 6 January 2023
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 5 (1) , 013007
Open AccessCoupling between improper ferroelectricity and ferrimagnetism in the hexagonal ferriteHere, we propose an idea to realize noncollinear ferrimagnetic orders with a considerably high magnetization and their coupling with an improper ferroelectric (FE) order in hexagonal type systems which exhibit interesting topological orders. These magnetic and magnetoelectric phenomena are driven by the antisymmetric Dzyaloshinskii-Moriya interactions between the magnetic ions and their coupling with the ferroelectricity. The proposed two-sublattice magnetic system, generated by a specific charge-ordered state, forms multiple energetically close, noncollinear ferrimagnetic orders. This offers a platform to manipulate the microscopic magnetic interactions and to trigger spin-reorientation (SR) transitions by various efficient means. The two-sublattice structure was realized in the hexagonal phase of doped with electrons. The proposed electron-doped systems are expected to exhibit switchable electric polarization (), considerably high magnetization (), and magnetic transition near room temperature (). Based on the coupling between the magnetic interactions and the FE primary order parameter observed in this system, microscopic mechanisms to achieve electric field induced SR transitions and switching of the direction of are discussed. - 1 June 2022
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 6 (6) , 064401
Exploring the correlation between the spin-state configuration and the magnetic order in Co-substitutedCo-substituted systems exhibit both ferroelectric and antiferromagnetic (AFM) orders with a considerably high electric polarization and a modestly canted magnetization and a cross coupling between them at room temperature. In the present study, employing first-principles calculations and Monte Carlo simulations, we unravel the microscopic interactions that contribute to stabilize this particular canted AFM order with . Our results propose a correlation between the spin-state configuration of the trivalent ions and the energetics associated with the magnetic orders. Because of the complex interplay between the Hund's coupling and crystal field splitting , the trivalent ions are known to exhibit three spin configurations, namely low spin (LS), intermediate spin (IS), and high spin (HS). We observe electron correlation induced LS HS state transition, which implies a close competition among these spin states in the polar structure. Moreover, our detailed analysis points towards the formation of heterogeneous spin-state configuration at room temperature. While the LS state configuration was not observed to exhibit any particular tendency to stabilize the canted AFM phase, the HS state tends to strongly favor the formation of this desired magnetic order. On the other hand, interestingly, the formation of finite fraction of the IS state can contribute to enhance the magnitude of . Our investigation is expected to initiate further quest for appropriate magnetic substitutes to ensure enhanced functionalities of the system.- 1 June 2022
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 6 (6) , 064401
Exploring the correlation between the spin-state configuration and the magnetic order in Co-substitutedCo-substituted systems exhibit both ferroelectric and antiferromagnetic (AFM) orders with a considerably high electric polarization and a modestly canted magnetization and a cross coupling between them at room temperature. In the present study, employing first-principles calculations and Monte Carlo simulations, we unravel the microscopic interactions that contribute to stabilize this particular canted AFM order with . Our results propose a correlation between the spin-state configuration of the trivalent ions and the energetics associated with the magnetic orders. Because of the complex interplay between the Hund's coupling and crystal field splitting , the trivalent ions are known to exhibit three spin configurations, namely low spin (LS), intermediate spin (IS), and high spin (HS). We observe electron correlation induced LS HS state transition, which implies a close competition among these spin states in the polar structure. Moreover, our detailed analysis points towards the formation of heterogeneous spin-state configuration at room temperature. While the LS state configuration was not observed to exhibit any particular tendency to stabilize the canted AFM phase, the HS state tends to strongly favor the formation of this desired magnetic order. On the other hand, interestingly, the formation of finite fraction of the IS state can contribute to enhance the magnitude of . Our investigation is expected to initiate further quest for appropriate magnetic substitutes to ensure enhanced functionalities of the system.- 27 December 2021
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 5 (12) , 124416
Exploring the possible origin of the spin reorientation transition inSpin reorientation transitions and other related magnetic phenomena, which owe their origin to the complex interplay between multiple magnetic sublattices, have long attracted scientific attention both from the perspective of fundamental curiosity and technological applications. In this study, combining first principles calculations together with finite temperature Monte Carlo simulations, we explore the possible origins of reorientation transition of Cr spins in . We construct a specific magnetic model, consisting of symmetric superexchange interactions between magnetic ions, as well as their magnetic anisotropy. We show that the observed spin reorientation in arises out of a delicate balance between magnetic exchange interactions, single ion anisotropy of Nd spins, and single ion anisotropy of Cr spins. Moreover, though our model does not take into consideration the effect of antisymmetric and anisotropic-symmetric magnetic exchanges, the qualitative as well as quantitative agreement of the theoretically derived and the experimentally observed spin-reorientation transition in confirms the merit of our proposed microscopic model. Our results also propose a hitherto unobserved collective magnetic ordering in the Nd sublattice, which is challenging to detect as it is an extreme low temperature phenomena, which therefore calls for further investigations.- 27 December 2021
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 5 (12) , 124416
Exploring the possible origin of the spin reorientation transition inSpin reorientation transitions and other related magnetic phenomena, which owe their origin to the complex interplay between multiple magnetic sublattices, have long attracted scientific attention both from the perspective of fundamental curiosity and technological applications. In this study, combining first principles calculations together with finite temperature Monte Carlo simulations, we explore the possible origins of reorientation transition of Cr spins in . We construct a specific magnetic model, consisting of symmetric superexchange interactions between magnetic ions, as well as their magnetic anisotropy. We show that the observed spin reorientation in arises out of a delicate balance between magnetic exchange interactions, single ion anisotropy of Nd spins, and single ion anisotropy of Cr spins. Moreover, though our model does not take into consideration the effect of antisymmetric and anisotropic-symmetric magnetic exchanges, the qualitative as well as quantitative agreement of the theoretically derived and the experimentally observed spin-reorientation transition in confirms the merit of our proposed microscopic model. Our results also propose a hitherto unobserved collective magnetic ordering in the Nd sublattice, which is challenging to detect as it is an extreme low temperature phenomena, which therefore calls for further investigations.