Topological phase transitions and Berry-phase hysteresis in exchange-coupled nanomagnets

Authors

Ahsan Ullah, University of Nebraska - LincolnFollow
Xin Li, University of Nebraska-LincolnFollow
Yunlong Jin, University of Nebraska-Lincoln
Rabindra Pahari, University of Nebraska-Lincoln
Lanping Yue, University of Nebraska - LincolnFollow
Xiaoshan S. Xu, University of Nebraska-LincolnFollow
Balamurugan Balasubramanian,, University of Nebraska-Lincoln
David J. Sellmyer, University of Nebraska-Lincoln
Ralph Skomski, University of Nebraska-Lincoln

Date of this Version

10-25-2022

Citation

PHYSICAL REVIEW B 106, 134430 (2022). DOI: 10.1103/PhysRevB.106.134430

Comments

Used by permission.

Abstract

Topological phase in magnetic materials yields a quantized contribution to the Hall effect known as the topological Hall effect, which is often caused by skyrmions, with each skyrmion creating a magnetic flux quantum ±h/e. The control and understanding of topological properties in nanostructured materials is the subject of immense interest for both fundamental science and technological applications, especially in spintronics. In this work, the electron-transport properties and spin structure of exchange-coupled cobalt nanoparticles with an average particle size of 13.7 nm are studied experimentally and theoretically. Magnetic and Hall-effect measurements identify topological phase transitions in the exchange-coupled cobalt nanoparticles and were used to discover a qualitatively new type of hysteresis in the topological Hall effect—namely, Berry-phase hysteresis. Micromagnetic simulations reveal the origin of the topological Hall effect—namely, the chiral domains, with domain-wall chirality quantified by an integer skyrmion number. These spin structures are different from the skyrmions formed due to Dzyaloshinskii–Moriya interactions in B20 crystals and multilayered thin films, and caused by cooperative magnetization reversal in the exchange-coupled cobalt nanoparticles. An analytical model is developed to explain the underlying physics of Berry-phase hysteresis, which is strikingly different from the iconic magnetic hysteresis and constitutes one aspect of 21st-century reshaping of our view on nature at the borderline of physics, chemistry, mathematics, and materials science.