Anuradha M. Vibhakar
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Research Interests
Anuradha M. Vibhakar has a total of 33 co-authors. Here are the top co-authors by number of shared publications:
- Alessandro Bombardi
Diamond Light Source
5 shared publications D. D. Khalyavin
ISIS Facility Rutherford Appleton Laboratory-STFC OX11 0QX Chilton Didcot United Kingdom
4 shared publications- Alexei A. Belik
National Institute for Materials Science
3 shared publications - Fabio Orlandi
ISIS Neutron and Muon Source
3 shared publications P. Manuel
ISIS Facility, Rutherford Appleton Laboratory-STFC, Chilton, Didcot OX11 0QX, United Kingdom
3 shared publicationsDmitry D. Khalyavin
ISIS Facility, Rutherford Appleton Laboratory-STFC, Chilton, Didcot, UK
2 shared publications
Latest Publications
- 6 March 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (9)
Coupled crystal and magnetic chiralities in NiCo 2 TeO 6 determined by polarized x-ray and neutron scattering
- 6 March 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (9)
Coupled crystal and magnetic chiralities in NiCo 2 TeO 6 determined by polarized x-ray and neutron scattering
- Open Access
- 30 September 2024
- Published by Springer Nature in Communications Physics
- Vol. 7 (1) , 1-8
Spontaneous reversal of spin chirality and competing phases in the topological magnet EuAl4
Materials exhibiting a spontaneous reversal of spin chirality have the potential to drive the widespread adoption of chiral magnets in spintronic devices. Unlike the majority of chiral magnets that require the application of an external field to reverse the spin chirality, we observe the spin chirality to spontaneously reverse in the topological magnet EuAl4. Using resonant elastic x-ray scattering we demonstrate that all four magnetic phases in EuAl4 are single-k, where the first two magnetic phases are characterized by spin density wave order and the last two by helical spin order. A single spin chirality was stabilised across the 1mm2 sample, and the reversal of spin chirality occurred whilst maintaining a helical magnetic structure. At the onset of the helical magnetism, the crystal symmetry lowers to a chiral monoclinic space group, explaining the asymmetry in the chiral spin order, and establishing a mechanism by which the spin chirality could reverse via magnetostructural coupling.
- 30 September 2024
- Published by Springer Nature in Communications Physics
- Vol. 7 (1) , 1-8
Open AccessSpontaneous reversal of spin chirality and competing phases in the topological magnet EuAl4
Materials exhibiting a spontaneous reversal of spin chirality have the potential to drive the widespread adoption of chiral magnets in spintronic devices. Unlike the majority of chiral magnets that require the application of an external field to reverse the spin chirality, we observe the spin chirality to spontaneously reverse in the topological magnet EuAl4. Using resonant elastic x-ray scattering we demonstrate that all four magnetic phases in EuAl4 are single-k, where the first two magnetic phases are characterized by spin density wave order and the last two by helical spin order. A single spin chirality was stabilised across the 1mm2 sample, and the reversal of spin chirality occurred whilst maintaining a helical magnetic structure. At the onset of the helical magnetism, the crystal symmetry lowers to a chiral monoclinic space group, explaining the asymmetry in the chiral spin order, and establishing a mechanism by which the spin chirality could reverse via magnetostructural coupling.
- Open Access
- 11 June 2024
- Published by Springer Nature in Research Square
Spontaneous reversal of spin chirality and competing phases in the topological magnet EuAl4
Materials exhibiting a spontaneous reversal of spin chirality have the potential to drive the widespread adoption of chiral magnets in spintronic devices. Unlike the majority of chiral magnets that require the application of an external field to reverse the spin chirality, we observed the spin chirality to spontaneously reverse in the topological magnet EuAl4. Using resonant magnetic x-ray scattering we demonstrate that all four magnetic phases in EuAl4 are single-k, where the first two magnetic phases are characterized by spin density wave order and the last two by helical spin order. We show a single spin chirality was stabilised across the 1mm2 sample, and that the reversal of spin chirality occurred whilst maintaining a helical magnetic structure. At the onset of the helical magnetic order, the crystal symmetry lowers to a chiral monoclinic space group, explaining the asymmetry in the chiral spin order, and establishing a mechanism by which the spin chirality could reverse via magnetostructural coupling.
- 11 June 2024
- Published by Springer Nature in Research Square
Open AccessSpontaneous reversal of spin chirality and competing phases in the topological magnet EuAl4
Materials exhibiting a spontaneous reversal of spin chirality have the potential to drive the widespread adoption of chiral magnets in spintronic devices. Unlike the majority of chiral magnets that require the application of an external field to reverse the spin chirality, we observed the spin chirality to spontaneously reverse in the topological magnet EuAl4. Using resonant magnetic x-ray scattering we demonstrate that all four magnetic phases in EuAl4 are single-k, where the first two magnetic phases are characterized by spin density wave order and the last two by helical spin order. We show a single spin chirality was stabilised across the 1mm2 sample, and that the reversal of spin chirality occurred whilst maintaining a helical magnetic structure. At the onset of the helical magnetic order, the crystal symmetry lowers to a chiral monoclinic space group, explaining the asymmetry in the chiral spin order, and establishing a mechanism by which the spin chirality could reverse via magnetostructural coupling.
- Open Access
Spontaneous spin chirality reversal and competing phases in the topological magnet EuAl$_4$
We demonstrate the spontaneous reversal of spin chirality in a single crystal sample of the intermetallic magnet EuAl$_4$. We solve the nanoscopic nature of each of the four magnetically phases of EuAl$_4$ using resonant magnetic x-ray scattering, and demonstrate all four phases order with single-k incommensurate magnetic modulation vectors. Below 15.4 K the system forms a spin density modulated spin structure where the spins are orientated in the ab plane perpendicular to the orientation of the magnetic propagation vector. Below 13.2 K a second spin density wave orders with moments aligned parallel to the c-axis, such that the two spin density wave orders coexist. Below 12.2 K a magnetic helix of a single chirality is stabilised across the entire sample. Below 10 K the chirality of the magnetic helix reverses, and the sample remains a single chiral domain. Concomitant with the establishment of the helical magnetic ordering is the lowering of the crystal symmetry to monoclinic, as evidenced the formation of uniaxial charge and spin strip domains. A group theoretical analysis demonstrates that below 12.2 K the symmetry lowers to polar monoclinic, which is necessary to explain the observed asymmetry in the chiral states of the magnetic helix and the spin chiral reversal. We find that in every magnetically ordered phase of EuAl4 the in-plane moment is perpendicular to the orientation of the magnetic propagation vector, which we demonstrate is favoured by magnetic dipolar interactions.
Open AccessSpontaneous spin chirality reversal and competing phases in the topological magnet EuAl$_4$
We demonstrate the spontaneous reversal of spin chirality in a single crystal sample of the intermetallic magnet EuAl$_4$. We solve the nanoscopic nature of each of the four magnetically phases of EuAl$_4$ using resonant magnetic x-ray scattering, and demonstrate all four phases order with single-k incommensurate magnetic modulation vectors. Below 15.4 K the system forms a spin density modulated spin structure where the spins are orientated in the ab plane perpendicular to the orientation of the magnetic propagation vector. Below 13.2 K a second spin density wave orders with moments aligned parallel to the c-axis, such that the two spin density wave orders coexist. Below 12.2 K a magnetic helix of a single chirality is stabilised across the entire sample. Below 10 K the chirality of the magnetic helix reverses, and the sample remains a single chiral domain. Concomitant with the establishment of the helical magnetic ordering is the lowering of the crystal symmetry to monoclinic, as evidenced the formation of uniaxial charge and spin strip domains. A group theoretical analysis demonstrates that below 12.2 K the symmetry lowers to polar monoclinic, which is necessary to explain the observed asymmetry in the chiral states of the magnetic helix and the spin chiral reversal. We find that in every magnetically ordered phase of EuAl4 the in-plane moment is perpendicular to the orientation of the magnetic propagation vector, which we demonstrate is favoured by magnetic dipolar interactions.
- Open Access
- 22 September 2023
- Published by American Physical Society (APS) in Physical Review B
- Vol. 108 (10) , L100404
Competing charge and magnetic order in the candidate centrosymmetric skyrmion hostare centrosymmetric systems that have recently been identified as candidates to stabilize topologically nontrivial magnetic phases, such as skyrmion lattices. In this Letter, we present a high-resolution resonant x-ray and neutron scattering study on that provides new details of the complex coupling between the electronic ordering phenomena. Our results unambiguously demonstrate that the system orders to form a spin density wave with moments aligned perpendicular to the direction of the propagation vector below 19.5 K, and upon further cooling below 15 K, a cycloid with moments in the plane, in contrast to what has been reported in the literature. We show that concomitant with the onset of the spin density wave is the suppression of the charge density wave order, indicative of a coupling between the localized electrons and itinerant electron density. Furthermore, we demonstrate that the charge density wave order breaks the fourfold symmetry present in the crystal structure, thus declassifying these systems as square-net magnets.- 22 September 2023
- Published by American Physical Society (APS) in Physical Review B
- Vol. 108 (10) , L100404
Open AccessCompeting charge and magnetic order in the candidate centrosymmetric skyrmion hostare centrosymmetric systems that have recently been identified as candidates to stabilize topologically nontrivial magnetic phases, such as skyrmion lattices. In this Letter, we present a high-resolution resonant x-ray and neutron scattering study on that provides new details of the complex coupling between the electronic ordering phenomena. Our results unambiguously demonstrate that the system orders to form a spin density wave with moments aligned perpendicular to the direction of the propagation vector below 19.5 K, and upon further cooling below 15 K, a cycloid with moments in the plane, in contrast to what has been reported in the literature. We show that concomitant with the onset of the spin density wave is the suppression of the charge density wave order, indicative of a coupling between the localized electrons and itinerant electron density. Furthermore, we demonstrate that the charge density wave order breaks the fourfold symmetry present in the crystal structure, thus declassifying these systems as square-net magnets. - Open Access
- 3 August 2023
- Published by American Physical Society (APS) in Physical Review B
- Vol. 108 (5) , 054403
Magnetic inhomogeneities in the quadruple perovskite manganiteA combination of competing exchange interactions and substitutional disorder gives rise to magnetic inhomogeneities in the and 0.16 quadruple perovskite manganites. Our neutron powder scattering measurements show that both the and 0.16 samples separate into two distinct magnetic phases; below = 120 10 K the system undergoes a transition from a paramagnetic phase to a phase characterized by short-range antiferromagnetic clusters contained in a paramagnetic matrix, and below K the system is composed of well-correlated long-range collinear ferrimagnetic order, punctuated by short-range antiferromagnetic clusters. A sharp increase in the antiferromagnetic phase fraction is observed below K, concomitant with a decrease in the ferrimagnetic phase fraction. Our results demonstrate that the theoretically proposed antiferromagnetic phase is stabilized in the manganites in the presence of dominant exchange interactions, as predicted.- 3 August 2023
- Published by American Physical Society (APS) in Physical Review B
- Vol. 108 (5) , 054403
Open AccessMagnetic inhomogeneities in the quadruple perovskite manganiteA combination of competing exchange interactions and substitutional disorder gives rise to magnetic inhomogeneities in the and 0.16 quadruple perovskite manganites. Our neutron powder scattering measurements show that both the and 0.16 samples separate into two distinct magnetic phases; below = 120 10 K the system undergoes a transition from a paramagnetic phase to a phase characterized by short-range antiferromagnetic clusters contained in a paramagnetic matrix, and below K the system is composed of well-correlated long-range collinear ferrimagnetic order, punctuated by short-range antiferromagnetic clusters. A sharp increase in the antiferromagnetic phase fraction is observed below K, concomitant with a decrease in the ferrimagnetic phase fraction. Our results demonstrate that the theoretically proposed antiferromagnetic phase is stabilized in the manganites in the presence of dominant exchange interactions, as predicted. - 22 December 2020
- Published by American Physical Society (APS) in Physical Review B
- Vol. 102 (21) , 214428
Effects of magnetic dilution in the ferrimagnetic columnar ordered perovskitesPowder neutron-diffraction experiments have been employed to establish the effects of site-selective magnetic dilution in the -site columnar ordered quadruple perovskite manganites (, and ). We show that in all three compositions the Mn ions adopt a collinear ferrimagnetic structure below 27, 62, and 34 K, respectively. An unexpected increase in the ordering temperature was observed between the and samples, which indicates a considerable departure from mean-field behavior. This result is corroborated by large reductions in the theoretical ground-state magnetic moments observed across the series, which indicate the presence of spin fluctuations and/or disorder. We show that long-range magnetic order in the sample, which occurs below the percolation threshold for B-B exchange, can only be understood to arise if it is mediated via both A-B and B-B exchange, hence confirming the importance of A-B exchange interactions in these materials. Finally, we show that site-selective magnetic dilution enables the tuning of a ferrimagnetic compensation point and the introduction of temperature-induced magnetization reversal.- 22 December 2020
- Published by American Physical Society (APS) in Physical Review B
- Vol. 102 (21) , 214428
Effects of magnetic dilution in the ferrimagnetic columnar ordered perovskitesPowder neutron-diffraction experiments have been employed to establish the effects of site-selective magnetic dilution in the -site columnar ordered quadruple perovskite manganites (, and ). We show that in all three compositions the Mn ions adopt a collinear ferrimagnetic structure below 27, 62, and 34 K, respectively. An unexpected increase in the ordering temperature was observed between the and samples, which indicates a considerable departure from mean-field behavior. This result is corroborated by large reductions in the theoretical ground-state magnetic moments observed across the series, which indicate the presence of spin fluctuations and/or disorder. We show that long-range magnetic order in the sample, which occurs below the percolation threshold for B-B exchange, can only be understood to arise if it is mediated via both A-B and B-B exchange, hence confirming the importance of A-B exchange interactions in these materials. Finally, we show that site-selective magnetic dilution enables the tuning of a ferrimagnetic compensation point and the introduction of temperature-induced magnetization reversal.- 23 March 2020
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 124 (12) , 127201
Spontaneous Rotation of Ferrimagnetism Driven by Antiferromagnetic Spin Canting
Spin-reorientation phase transitions that involve the rotation of a crystal’s magnetization have been well characterized in distorted-perovskite oxides such as orthoferrites. In these systems spin reorientation occurs due to competing rare-earth and transition metal anisotropies coupled via exchange. Here, we demonstrate an alternative paradigm for spin reorientation in distorted perovskites. We show that the ( or Dy) triple -site columnar-ordered quadruple perovskites have three ordered magnetic phases and up to two spin-reorientation phase transitions. Unlike the spin-reorientation phenomena in other distorted perovskites, these transitions are independent of rare-earth magnetism, but are instead driven by an instability towards antiferromagnetic spin canting likely originating in frustrated Heisenberg exchange interactions, and the competition between Dzyaloshinskii-Moriya and single-ion anisotropies.- 23 March 2020
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 124 (12) , 127201
Spontaneous Rotation of Ferrimagnetism Driven by Antiferromagnetic Spin Canting
Spin-reorientation phase transitions that involve the rotation of a crystal’s magnetization have been well characterized in distorted-perovskite oxides such as orthoferrites. In these systems spin reorientation occurs due to competing rare-earth and transition metal anisotropies coupled via exchange. Here, we demonstrate an alternative paradigm for spin reorientation in distorted perovskites. We show that the ( or Dy) triple -site columnar-ordered quadruple perovskites have three ordered magnetic phases and up to two spin-reorientation phase transitions. Unlike the spin-reorientation phenomena in other distorted perovskites, these transitions are independent of rare-earth magnetism, but are instead driven by an instability towards antiferromagnetic spin canting likely originating in frustrated Heisenberg exchange interactions, and the competition between Dzyaloshinskii-Moriya and single-ion anisotropies.