Topological Quantum Matter Research Unit

Principal Investigator

PI Name Max Hirschberger
Degree Ph.D.
Title Unit Leader
Brief Resume
2011 Dipl. Phys., Department of Physics, Technical University of Munich, Munich, Germany
2017 Ph.D., Department of Physics, Princeton University, Princeton, NJ, USA
2017 Postdoctoral Researcher, RIKEN Center for Emergent Matter Science (CEMS)
2018 Alexander von Humboldt / JSPS Research Fellow and Visiting Researcher at RIKEN CEMS
2019 Project Lecturer, Quantum-Phase Electronics Center, School of Engineering, The University of Tokyo
2019 Unit Leader, Topological Quantum Matter Research Unit, RIKEN CEMS (-present)
2021 Associate Professor, Department of Applied Physics, School of Engineering, The University of Tokyo (-present)
2021 Project Associate Professor, Quantum-Phase Electronics Center, School of Engineering, The University of Tokyo (-present)

Outline

We study the interplay between magnetic order, in particular non-coplanar spin arrangements such as magnetic skyrmions, and the electronic band structure in solids. Particular emphasis is put on compounds with the potential to be grown in thin-film form and on realizing new types of protected surface states in correlated materials. Methods include materials search guided by density functional theory calculations, crystal synthesis using a variety of solid state techniques, and ultra-high resolution transport measurements (up to very high magnetic fields). We collaborate closely with other researchers at RIKEN and beyond to resolve the magnetic structure of new materials using scattering and imaging experiments.

Research Fields

Physics, Materials Science

Keywords

Strongly Correlated electron system
Magnetism
Skyrmion
Spin-orbit interaction
Emergent electromagnetism
Topological materials
Frustrated quantum magnets
Berry phase physics

Results

Non-coplanar helimagnetism in the layered van-der-Waals metal DyTe3

Van-der-Waals magnets with highly anisotropic chemical bonding can be exfoliated to realize ultrathin sheets or interfaces. With an eye towards future applications in twistronics, however, the lack of lattice-incommensurate helimagnets within this material class is a particular problem. Via polarized neutron scattering, we reveal the cycloidal, or conical, magnetic structure in DyTe3, and establish a spin Hamiltonian that captures the coupling of magnetic moments and an underlying charge density wave (CDW). Experimentally, we find two coupled order parameters: qAFM = (0 1 0.5) signifies uudd AFM coupling along the c-axis, while qcyc = (0 0 0.207) corresponds to a superimposed cycloidal component, indicating coupled charge and spin density wave orders. Furthermore, we identify a structural feature of this material class as a key driver of helimagnetism: The mixed covalent / metallic crystal field environment of Dy3+ ions both suppresses magnetic anisotropy and enables strong coupling between magnetic moments and the charge-density wave order. Our work paves the way for twistronics research, where helimagnetic layers can be combined to form complex spin textures on-demand.

Non-coplanar helimagnetism in the layered van-der-Waals metal DyTe3. a, Crystallographic unit cell with covalently bonded DyTe bilayers and metallic Te bilayers, with natural cleaving plane (dashed). b, Zigzag chain illustration of double-square net structure in DyTe3. The interactions J1, J2 connect nearest and next-nearest neighbours in the zigzag chain model, respectively. Conical, noncoplanar helimagnetism is resolved in the zero-field ground state by neutron scattering. The cone direction, parallel to the a-axis, alternates both between pairs of magnetic sites in a zigzag chain, and between stacked zigzag chains. This texture causes polarization along the b-axis, i.e. perpendicular to square net bilayers (yellow arrow). c, Experimental geometry for polarized neutron scattering from layered DyTe3 (grey plane, square net of Dy indicated). The scattering plane (blue) is spanned by wavevectors ki, kf of incoming and outgoing neutron beams, respectively. Separating spin-flip (SF, red) and non-spin flip (NSF, blue) scattering intensities at the detector, we identify conical magnetic order (top). d,e, Polarization analysis for the incommensurate cycloidal reflection qcyc: absence of spin flip (SF) intensity indicates absence of mb and mc, while non-spin flip (NSF) intensity reveals dominant ma. f, Magnetic susceptibility χ for H∥[101], overlaid with phase boundaries from specific heat (white open circles) and magnetization (black circles): I (conical ground state), II, III, IV, and V.

 

Skyrmions in a centrosymmetric breathing Kagome magnet

Non-coplanar magnetic order in solids gives rise to an emergent magnetic field, which is known to strongly affect the motion of charge carriers. The magnitude of the emergent magnetic field is enhanced when pushing non-coplanar spin textures to shorter and shorter length scales λ. We have recently explored the limit of ultra-short range spin texture formation (λ~2-3 nanometers) in intermetallic magnets, where we found giant topological Hall and Nernst effects from non-coplanar skyrmion spin vortices. Hexagonal Gd2PdSi3 and Gd3Ru4Al12 are centrosymmetric alloys which defy an important paradigm: typically, it is thought that Dzyaloshinskii-Moriya interactions arising exclusively in non-centrosymmetric material platforms are the key to skyrmion formation. Instead, competing interactions due to the high symmetry of the (hexagonal) lattice combine with Ruderman-Kittel-Kasuya-Yosida (RKKY) interactions between Gd3+ rare earth moments to create a curious non-coplanar ordering on very short length scales. For example, the existence of the skyrmion lattice in Gd3Ru4Al12 was confirmed by quantum beam (neutron & x-ray) scattering experiments as well as real-space imaging using Lorentz transmission electron microscopy (L-TEM), as shown in the figure. Future directions for skyrmions on centrosymmetric lattices are the exploration of new types of domains of left- and right-handed helicity, the coupling of the symmetry-breaking magnetic order to light, and the search for new types of magnetic vortex lattices, such as antiskyrmions or antiferromagnetically stacked skyrmions, due to the high level of spin-orientational degeneracy on the lattice. These exotic forms of magnetic order may be within reach in centrosymmetric magnets due to the flat energy landscape with many nearly degenerate magnetic states.

Figure

Skyrmion formation in the centrosymmetric hexagonal metal Gd3Ru4Al12. (a) The crystal structure hosts closely correlated spin-trimers of Gd3+ moments, which are connected by weaker next-nearest neighbor interactions. The rare earth sites in each plane form a distorted (‘breathing’) Kagome network. (b) Illustration of a two-dimensional cut of the skyrmion spin vortex, with each cone representing an individual magnetic moment on a Gd-site of the lattice. (c) Magnetic phase diagram for field aligned along the c-axis, where many magnetic phases are observed due to competing interactions. (d) Only in the skyrmion lattice phase (labeled ‘SkL’) we found a large topological Hall signal, marked by grey shaded areas. (e) Real space image of a thin plate of Gd3Ru4Al12 in phase SkL, where both the atomic lattice and the magnetic texture leave their fingerprints in the data. (f) Fourier transform of the data in panel (e), where reflections due to the atomic lattice and skyrmion spin textures are marked by red and yellow circles, respectively. Inset in (e) shows filtered data after removing intensity originating from the atomic lattice.

Members

Max Hirschberger

Unit Leader maximilian.hirschberger[at]riken.jp

Publications

  1. L. Spitz, T. Nomoto, S. Kitou, H. Nakao, A. Kikkawa, S. Francoual, Y. Taguchi, R. Arita, Y. Tokura, T.-h. Arima, and M. Hirschberger

    Entropy-Assisted Long-Period Stacking of Honeycomb Layers in an AIB2-Type Silicide

    J. Am. Chem. Soc. 144, 16866-16871 (2022)
  2. M. Hirschberger, L. Spitz, T. Nomoto, T. Kurumaji, S. Gao, J. Masell, T. Nakajima, A. Kikkawa, Y. Yamasaki, H. Sagayama, H. Nakao, Y. Taguchi, R. Arita, T.-h. Arima, and Y. Tokura

    Topological Nernst Effect of the Two-Dimensional Skyrmion Lattice

    Phys. Rev. Lett. 125, 076602 (2020)
  3. M. Hirschberger, T. Nakajima, S. Gao, L. Peng, A. Kikkawa, T. Kurumaji, M. Kriener, Y. Yamasaki, H. Sagayama, H. Nakao, K. Ohishi, K. Kakurai, Y. Taguchi, X. Yu, T.-h. Arima, and Y. Tokura

    Skyrmion phase and competing magnetic orders on a breathing kagome lattice

    Nat. Commun. 10, 5831 (2019)
  4. M. Hirschberger, S. Kushwaha, Z. Wang, Q. Gibson, S. Liang, C.A. Belvin, B.A. Bernevig, R.J. Cava, and N.P. Ong

    The chiral anomaly and thermopower of Weyl fermions in the half-Heusler GdPtBi

    Nat. Mater. 15, 1161–1165 (2016)
  5. M. Hirschberger, R. Chisnell, Y.S. Lee, and N.P. Ong

    Thermal Hall effect of spin excitations in a kagome magnet

    Phys. Rev. Lett. 115, 106603 (2015)

Articles

お問い合わせ

2-1 Hirosawa, Wako, Saitama
Frontier Research Building #208 351-0198 Japan

E-mail:
maximilian.hirschberger[at]riken.jp

Links