Giant anomalous Hall effect in a ferromagnetic kagome-lattice semimetal (2024)

  • Nagaosa, N., Sinova, J., Onoda, S., MacDonald, A. H. & Ong, N. P. Anomalous Hall effect. Rev. Mod. Phys. 82, 1539–1592 (2010).

    Article ADS Google Scholar

  • Fang, Z. et al. The anomalous Hall effect and magnetic monopoles in momentum space. Science 302, 92–95 (2003).

    Article ADS Google Scholar

  • Haldane, F. D. M. Berry curvature on the Fermi surface: Anomalous Hall effect as a topological Fermi-liquid property. Phys. Rev. Lett. 93, 206602 (2004).

    Article ADS Google Scholar

  • Xiao, D., Chang, M. C. & Niu, Q. Berry phase effects on electronic properties. Rev. Mod. Phys. 82, 1959–2007 (2010).

    Article ADS MathSciNet Google Scholar

  • Nakatsuji, S., Kiyohara, N. & Higo, T. Large anomalous Hall effect in a non-collinear antiferromagnet at room temperature. Nature 527, 212–215 (2015).

    Article ADS Google Scholar

  • Weng, H. M., Fang, C., Fang, Z., Bernevig, B. A. & Dai, X. Weyl semimetal phase in noncentrosymmetric transition-metal monophosphides. Phys. Rev. X 5, 011029 (2015).

    Google Scholar

  • Yan, B. & Felser, C. Topological materials: Weyl semimetals. Annu. Rev. Condens. Matter Phys. 8, 337–354 (2017).

    Article ADS Google Scholar

  • Weng, H. M., Yu, R., Hu, X., Dai, X. & Fang, Z. Quantum anomalous Hall effect and related topological electronic states. Adv. Phys. 64, 227–282 (2015).

    Article ADS Google Scholar

  • Liu, C.-X., Zhang, S.-C. & Qi, X.-L. The quantum anomalous Hall effect: Theory and experiment. Annu. Rev. Condens. Matter Phys. 7, 301–321 (2016).

    Article ADS Google Scholar

  • Yu, R. et al. Quantized anomalous Hall effect in magnetic topological insulators. Science 329, 61–64 (2010).

    Article ADS Google Scholar

  • Chang, C.-Z. et al. Experimental observation of the quantum anomalous Hall effect in a magnetic topological insulator. Science 340, 167–170 (2013).

    Article ADS Google Scholar

  • Fang, C., Gilbert, M. J. & Bernevig, B. A. Large-Chern-number quantum anomalous Hall effect in thin-film topological crystalline insulators. Phys. Rev. Lett. 112, 046801 (2014).

    Article ADS Google Scholar

  • Kou, X. et al. Scale-invariant quantum anomalous Hall effect in magnetic topological insulators beyond the two-dimensional limit. Phys. Rev. Lett. 113, 137201 (2014).

    Article ADS Google Scholar

  • Burkov, A. A. & Balents, L. Weyl semimetal in a topological insulator multilayer. Phys. Rev. Lett. 107, 127205 (2011).

    Article ADS Google Scholar

  • Zyuzin, A. A., Wu, S. & Burkov, A. A. Weyl semimetal with broken time reversal and inversion symmetries. Phys. Rev. B 85, 165110 (2012).

    Article ADS Google Scholar

  • Wang, X., Vanderbilt, D., Yates, J. R. & Souza, I. Fermi-surface calculation of the anomalous Hall conductivity. Phys. Rev. B 76, 195109 (2007).

    Article ADS Google Scholar

  • Burkov, A. A. Anomalous Hall effect in Weyl metals. Phys. Rev. Lett. 113, 187202 (2014).

    Article ADS Google Scholar

  • Wan, X. G., Turner, A. M., Vishwanath, A. & Savrasov, S. Y. Topological semimetal and Fermi-arc surface states in the electronic structure of pyrochlore iridates. Phys. Rev. B 83, 205101 (2011).

    Article ADS Google Scholar

  • Xu, G., Weng, H. M., Wang, Z. J., Dai, X. & Fang, Z. Chern semimetal and the quantized anomalous Hall effect in HgCr2Se4. Phys. Rev. Lett. 107, 186806 (2011).

    Article ADS Google Scholar

  • Kübler, J. & Felser, C. Weyl points in the ferromagnetic Heusler compound Co2MnAl. Europhys. Lett. 114, 47005 (2016).

    Article ADS Google Scholar

  • Wang, Z. J. et al. Time-reversal-breaking Weyl fermions in magnetic Heusler alloys. Phys. Rev. Lett. 117, 236401 (2016).

    Article ADS Google Scholar

  • Chang, G. Q. et al. Room-temperature magnetic topological Weyl fermion and nodal line semimetal states in half-metallic Heusler Co2TiX (X = Si, Ge, or Sn). Sci. Rep. 6, 38839 (2016).

    Article ADS Google Scholar

  • Suzuki, T. et al. Large anomalous Hall effect in a half-Heusler antiferromagnet. Nat. Phys. 12, 1119–1123 (2016).

    Article Google Scholar

  • Ohgushi, K., Murakami, S. & Nagaosa, N. Spin anisotropy and quantum Hall effect in the kagome lattice: Chiral spin state based on a ferromagnet. Phys. Rev. B 62, R6065–R6068 (2000).

    Article ADS Google Scholar

  • Xu, G., Lian, B. & Zhang, S.-C. Intrinsic quantum anomalous Hall effect in the Kagome lattice Cs2LiMn3F12. Phys. Rev. Lett. 115, 186802 (2015).

    Article ADS Google Scholar

  • Ye, L. et al. Massive Dirac fermions in a ferromagnetic kagome metal. Nature 555, 638–642 (2018).

    Article ADS Google Scholar

  • Weihrich, R., Anusca, I. & Zabel, M. Half-antiperovskites: Structure and type-antitype relations of Shandites M3/2AS (M = Co, Ni; A = In, Sn). Z. Anorg. Allg. Chem. 631, 1463–1470 (2005).

    Article Google Scholar

  • Weihrich, R. & Anusca, I. Half antiperovskites. III - Crystallographic and electronic structure effects in Sn2-xInxCo3S2. Z. Anorg. Allg. Chem. 632, 1531–1537 (2006).

    Article Google Scholar

  • Vaqueiro, P. & Sobany, G. G. A powder neutron diffraction study of the metallic ferromagnet Co3Sn2S2. Solid State Sci. 11, 513–518 (2009).

    Article ADS Google Scholar

  • Schnelle, W. et al. Ferromagnetic ordering and half-metallic state of Sn2Co3S2 with the Shandite-type structure. Phys. Rev. B 88, 144404 (2013).

    Article ADS Google Scholar

  • Dedkov, Y. S., Holder, M., Molodtsov, S. L. & Rosner, H. Electronic structure of shandite Co3Sn2S2. J. Phys. Conf. Ser. 100, 072011 (2008).

    Article Google Scholar

  • Holder, M. et al. Photoemission study of electronic structure of the half-metallic ferromagnet Co3Sn2S2. Phys. Rev. B 79, 205116 (2009).

    Article ADS Google Scholar

  • Ali, M. N. et al. Large, non-saturating magnetoresistance in WTe2. Nature 514, 205–208 (2014).

    Article ADS Google Scholar

  • Kumar, N. et al. Extremely high magnetoresistance and conductivity in the type-II Weyl semimetals WP2 and MoP2. Nat. Commun. 8, 1642 (2017).

    Article ADS Google Scholar

  • Ziman, J. M. Electrons and Phonons: Theory of Transport Phenomena in Solids (Oxford Univ. Press, Oxford, 1960).

  • Xu, Q. et al. Topological surface Fermi arcs in the magnetic Weyl semimetal Co3Sn2S2. Phys. Rev. B 97, 235416 (2018).

    Article ADS Google Scholar

  • Nielsen, H. B. & Ninomiya, M. The Adler–Bell–Jackiw anomaly and Weyl fermions in a crystal. Phys. Lett. B 130, 389–396 (1983).

    Article ADS MathSciNet Google Scholar

  • Son, D. T. & Spivak, B. Z. Chiral anomaly and classical negative magnetoresistance of Weyl metals. Phys. Rev. B 88, 104412 (2013).

    Article ADS Google Scholar

  • Onoda, S., Sugimoto, N. & Nagaosa, N. Intrinsic versus extrinsic anomalous Hall effect in ferromagnets. Phys. Rev. Lett. 97, 126602 (2006).

    Article ADS Google Scholar

  • Miyasato, T. et al. Crossover behavior of the anomalous Hall effect and anomalous Nernst effect in itinerant ferromagnets. Phys. Rev. Lett. 99, 086602 (2007).

    Article ADS Google Scholar

  • Yue, D. & Jin, X. Towards a better understanding of the anomalous Hall effect. J. Phys. Soc. Jpn 86, 011006 (2016).

    Article ADS Google Scholar

  • Gantmakher, V. F. The experimental study of electron–phonon scattering in metals. Rep. Prog. Phys. 37, 317–362 (1974).

    Article ADS Google Scholar

  • Checkelsky, J. G. et al. Trajectory of the anomalous Hall effect towards the quantized state in a ferromagnetic topological insulator. Nat. Phys. 10, 731–736 (2014).

    Article Google Scholar

  • Samarth, N. Quantum materials discovery from a synthesis perspective. Nat. Mater. 16, 1068–1076 (2017).

    Article ADS Google Scholar

  • Chan, C.-K., Lee, P. A., Burch, K. S., Han, J. H. & Ran, Y. When chiral photons meet chiral fermions: Photoinduced anomalous Hall effects in Weyl semimetals. Phys. Rev. Lett. 116, 026805 (2016).

    Article ADS Google Scholar

  • Ikhlas, M. et al. Large anomalous Nernst effect at room temperature in a chiral antiferromagnet. Nat. Phys. 13, 1085–1090 (2017).

    Article Google Scholar

  • Rajamathi, C. R. et al. Weyl semimetals as hydrogen evolution catalysts. Adv. Mater. 29, 1606202 (2017).

    Article Google Scholar

  • Yang, B.-J., Moon, E.-G., Isobe, H., & Nagaosa, N. Quantum criticality of topological phase transitions in three-dimensional interacting electronic systems. Nat. Phys. 10, 774–778 (2014).

    Article Google Scholar

  • Kurebayashi, D. & Nomura, K. Voltage-driven magnetization switching and spin pumping in Weyl semimetals. Phys. Rev. Appl. 6, 044013 (2016).

    Article ADS Google Scholar

  • Tokura, Y., Kawasaki, M. & Nagaosa, N. Emergent functions of quantum materials. Nat. Phys. 13, 1056–1068 (2017).

    Article Google Scholar

  • Kresse, G. & Furthmüller, J. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. Phys. Rev. B 54, 11169–11186 (1996).

    Article ADS Google Scholar

  • Perdew, J. P., Burke, K. & Ernzerhof, M. Generalized gradient approximation made simple. Phys. Rev. Lett. 77, 3865–3868 (1996).

    Article ADS Google Scholar

  • Mostofi, A. A. et al. wannier90: A tool for obtaining maximally-localised Wannier functions. Comput. Phys. Commun. 178, 685–699 (2008).

    Article ADS Google Scholar

  • Giant anomalous Hall effect in a ferromagnetic kagome-lattice semimetal (2024)

    FAQs

    What is the ferromagnetic Kagome lattice? ›

    In solid-state physics, the kagome metal or kagome magnet is a type of ferromagnetic quantum material. The atomic lattice in a kagome magnet has layered overlapping triangles and large hexagonal voids, akin to the kagome pattern in traditional Japanese basket-weaving.

    What is the ferromagnetic quantum anomalous hall effect? ›

    The quantum anomalous Hall effect (QAHE), featured by a quantized Hall conductance at zero magnetic field and the topologically protected chiral edge states, has been widely studied in recent years [1–3].

    What is the anomalous hall effect in a collinear antiferromagnet? ›

    To date, an anomalous Hall current in collinear antiferromagnets has been experimentally identified only as a consequence of canting of the magnetic moments by an applied magnetic field, or due to a field-induced spin-flip transition into a ferromagnetic state6,25,26.

    What is the anomalous hall effect in magnetization? ›

    When magnetic field is applied to a metal in which current is flowing, a transverse electrical current appears. This is the so-called classical Hall effect. In some magnetic materials a transverse current appears even in absence of external magnetic field, an effect known as the anomalous Hall effect (AHE)1.

    What is a kagome lattice? ›

    The Kagome lattice consists of corner-sharing triangles and is characterised by a large degree of geometric frustration, which becomes visible for instance in an antiferromagnetic Heisenberg model: while two of the three spins can be antiparallel, the third one is frustrated—both possible configurations will always ...

    What are the materials in kagome lattice? ›

    Here, there are mainly two categories of kagome materials: magnetic kagome materials and nonmagnetic ones. On one hand, magnetic kagome materials mainly focus on the 3d transition-metal-based kagome systems, including Fe3Sn2, Co3Sn2S2, YMn6Sn6, FeSn, and CoSn.

    What is Hall effect in ferromagnetic materials? ›

    Synopsis. Apart from the normal Hall voltage a magnetized ferromagnetic material usually shows a relatively large extra voltage in the same direction, which can be found by linear extrapolation to B=O. It is shown that this spontaneous Hall effect cannot exist in a perfectly periodic lattice.

    What is the anomalous effect? ›

    The anomalous photovoltaic effect (APE) is a type of a photovoltaic effect which occurs in certain semiconductors and insulators. The "anomalous" refers to those cases where the photovoltage (i.e., the open-circuit voltage caused by the light) is larger than the band gap of the corresponding semiconductor.

    What is the quantum anomalous Hall effect? ›

    The integer quantum anomalous Hall (QAH) effect is a lattice analogue of the quantum Hall effect at zero magnetic field1,2,3. This phenomenon occurs in systems with topologically non-trivial bands and spontaneous time-reversal symmetry breaking.

    What is the difference between Hall effect and anomalous Hall effect? ›

    The Hall effect is a very powerful tool for characterizing materials. In addition to the ordinary Hall effect (OHE) that is present in semiconductors and metals, there is an additional voltage proportional to the magnetization1 called the anomalous Hall effect (AHE) in magnetic materials.

    What is the physics behind the Hall effect? ›

    The Hall effect is the deflection of electrons (holes) in an n-type (p-type) semiconductor with current flowing perpendicular to a magnetic field. The deflection of these charged carriers sets up a voltage, called the Hall voltage, whose polarity depends on the effective charge of the carrier.

    What does the Hall effect depend on? ›

    The sign of the Hall coefficient is determined by the polarity of the charge carriers: a negative sign implies carriers with a negative charge ("normal Hall effect"), and a positive sign indicates carriers with a positive charge ("anomalous Hall effect").

    What is the equation for the anomalous Hall effect? ›

    As discussed in the introduction, the Hall resistivity of a ferromagnet is described by ρxy = RoB + Rs4πM, where the second term is the anomalous contribution to the Hall resistivity.

    What is the quantum anomalous hall effect in topological insulators? ›

    The quantum Hall (QH) effect, quantized Hall resistance combined with zero longitudinal resistance, is the characteristic experimental fingerprint of Chern insulators - topologically non-trivial states of two-dimensional matter with broken time-reversal symmetry.

    What is the Hall effect of magnetization? ›

    When a magnetic field is applied to a flowing current, it creates a weak but measurable voltage. This is the Hall effect. This movement of electrons results in a weak but measurable potential difference, or voltage, perpendicular both to the current flow and the applied magnetic field.

    What is the Bravais lattice of Kagome? ›

    The kagome lattice is a triangular Bravais lattice with a 3-point basis labelled l = 1, 2, 3; a1 = ˆ x and a2 = (ˆ x + √ 3ˆy3ˆy)/2 are the basis vectors. In the metallic kagome lattice F e3Sn2, spin-orbit coupling arises from the electric field due to the Sn ion at the center of the hexagon.

    What is superconductivity in kagome lattice? ›

    It has been argued that the kagome lattice can host a variety of unconventional pairing superconducting states, including the d + id chiral superconductor (SC) [26–28] and f-wave spin-triplet SC [29], among others. However, superconducting kagome materials are rare in nature.

    What is ferromagnetic crystal? ›

    Ferromagnet crystals have the magnetic moments from all their constituent ions aligned in the same direction; the magnetic moment of the crystal is the summation of the individual moments of the ions. There must be a magnetic force between the different ions that causes them to cooperatively align their moments.

    What is the magnetic lattice structure? ›

    The magnetic structure is an incommensurate modulated 2D structure with q = 0.4 along the c-axis (Selte et al., 1972). Rodriguez et al. (2011) reported results from neutron powder diffraction (NPD) studies of FeAs, yielding an incommensurate modulated spin structure with q = 0.395 along the c-axis at 4 K.

    Top Articles
    Andrea Contreras Yuma Az
    Noma Snow Thrower 8Hp 27 Price
    neither of the twins was arrested,传说中的800句记7000词
    Skyward Houston County
    J & D E-Gitarre 905 HSS Bat Mark Goth Black bei uns günstig einkaufen
    Meer klaarheid bij toewijzing rechter
    Obituaries
    Best Cheap Action Camera
    Atrium Shift Select
    Dark Souls 2 Soft Cap
    Blue Ridge Now Mugshots Hendersonville Nc
    No Strings Attached 123Movies
    Swedestats
    使用 RHEL 8 时的注意事项 | Red Hat Product Documentation
    Nhl Tankathon Mock Draft
    Transactions (zipForm Edition) | Lone Wolf | Real Estate Forms Software
    Ivegore Machete Mutolation
    Exl8000 Generator Battery
    Cain Toyota Vehicles
    Rs3 Ushabti
    Which Sentence is Punctuated Correctly?
    Jeff Nippard Push Pull Program Pdf
    6 Most Trusted Pheromone perfumes of 2024 for Winning Over Women
    Buhl Park Summer Concert Series 2023 Schedule
    Chelsea Hardie Leaked
    Miles City Montana Craigslist
    Mastering Serpentine Belt Replacement: A Step-by-Step Guide | The Motor Guy
    DIY Building Plans for a Picnic Table
    Scat Ladyboy
    Wisconsin Volleyball Team Leaked Uncovered
    Shiftwizard Login Johnston
    Google Jobs Denver
    That1Iggirl Mega
    KM to M (Kilometer to Meter) Converter, 1 km is 1000 m
    Google Chrome-webbrowser
    Www Craigslist Com Brooklyn
    Bones And All Showtimes Near Johnstown Movieplex
    What Is Kik and Why Do Teenagers Love It?
    Thelemagick Library - The New Comment to Liber AL vel Legis
    Former Employees
    Nami Op.gg
    M&T Bank
    Portal Pacjenta LUX MED
    Reilly Auto Parts Store Hours
    Tlc Africa Deaths 2021
    Backpage New York | massage in New York, New York
    Dicks Mear Me
    Craigslist Sparta Nj
    Rocket Bot Royale Unblocked Games 66
    Tommy Gold Lpsg
    Ff14 Palebloom Kudzu Cloth
    Latest Posts
    Article information

    Author: Aracelis Kilback

    Last Updated:

    Views: 5473

    Rating: 4.3 / 5 (44 voted)

    Reviews: 91% of readers found this page helpful

    Author information

    Name: Aracelis Kilback

    Birthday: 1994-11-22

    Address: Apt. 895 30151 Green Plain, Lake Mariela, RI 98141

    Phone: +5992291857476

    Job: Legal Officer

    Hobby: LARPing, role-playing games, Slacklining, Reading, Inline skating, Brazilian jiu-jitsu, Dance

    Introduction: My name is Aracelis Kilback, I am a nice, gentle, agreeable, joyous, attractive, combative, gifted person who loves writing and wants to share my knowledge and understanding with you.