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CMP
Credit: Jack Hobhouse

Dr Benjamin Huddart

PDRA

Research theme

  • Quantum materials

Sub department

  • Condensed Matter Physics

Research groups

  • Muons and magnets
benjamin.huddart@physics.ox.ac.uk
Clarendon Laboratory, room 106
  • About
  • Publications

Magnetic structure and crystal field states of antiferromagnetic CeNiGe$_3$: Neutron scattering and $\mu$SR investigations

(2024)

Authors:

A Kataria, R Kumar, DT Adroja, C Ritter, VK Anand, AD Hillier, BM Huddart, T Lancaster, S Rols, MM Koza, Sean Langridge, A Sundaresan

Weyl fermion excitations in the ideal Weyl semimetal CuTlSe2

Physical Review Research American Physical Society 6:3 (2024) 033229

Authors:

CN Wang, D Tay, QX Dong, Z Okvátovity, Benjamin M Huddart, CY Ma, K Yokoyama, L Yu, T Lancaster, GF Chen, H-R Ott, T Shiroka

Abstract:

An ideal Weyl semimetal is characterized by a dispersion in which only Weyl cones intersect the Fermi level, with low-energy behavior being governed by Weyl fermions. Although ideal Weyl semimetals have long been anticipated, only a few are realized in nonmagnetic materials. In this study, we confirm the presence of Weyl-fermion excitations in the ideal Weyl semimetal CuTlSe2 via a combination of magnetoresistance, Hall-effect, magnetic-susceptibility, nuclear magnetic resonance (NMR), and muon-spin relaxation (µ⁢SR) experiments. Magnetoresistance measurements reveal a negative longitudinal magnetoresistance (LMR), which scales as 𝐵2, while Hall-effect results indicate a predominant contribution from Weyl fermions with a hole-type charge. Magnetic susceptibility and µ⁢SR measurements indicate the lack of any intrinsic spontaneous magnetic moments down to base temperature. Finally, the NMR results can be modeled by a two-component effective Hamiltonian, which reproduces well the temperature-dependent 63Cu NMR (𝑇1⁢𝑇)−1 factor, shown to scale as 𝑇2 below 100 K and as 𝑇1 above 100 K. Overall, we find that the extremely low concentration (1017cm−3) of carriers in CuTlSe2 originates from an ideal nonmagnetic Weyl semimetallic state, persisting up to a thermal excitation energy of 9 meV (100 K), above which trivial electronic bands close to 𝐸F take over. Our findings highlight CuTlSe2 as a new member of the intriguing class of Weyl semimetals.

Muon spectroscopy investigation of anomalous dynamic magnetism in NiI$_2$

(2024)

Authors:

TL Breeze, BM Huddart, A Hernández-Melían, NP Bentley, DA Mayoh, GDA Wood, G Balakrishnan, J Wilkinson, FL Pratt, SJ Clark, T Lancaster

Low-temperature spin dynamics and absence of magnetic order in layered $\alpha$-RuI$_3$

(2024)

Authors:

Hank CH Wu, Benjamin M Huddart, Francis L Pratt, Danrui Ni, Robert J Cava, Stephen J Blundell

Demonstration of controlled skyrmion injection across a thickness step

Nano Letters American Chemical Society 24:22 (2024) 6813-6820

Authors:

Matthew T Littlehales, Samuel H Moody, Luke A Turnbull, Benjamin M Huddart, Ben A Brereton, Geetha Balakrishnan, Raymond Fan, Paul Steadman, Peter D Hatton, Murray N Wilson

Abstract:

Spintronic devices incorporating magnetic skyrmions have attracted significant interest recently. Such devices traditionally focus on controlling magnetic textures in 2D thin films. However, enhanced performance of spintronic properties through the exploitation of higher dimensionalities motivates the investigation of variable-thickness skyrmion devices. We report the demonstration of a skyrmion injection mechanism that utilizes charge currents to drive skyrmions across a thickness step and, consequently, a metastability barrier. Our measurements show that under certain temperature and field conditions skyrmions can be reversibly injected from a thin region of an FeGe lamella, where they exist as an equilibrium state, into a thicker region, where they can only persist as a metastable state. This injection is achieved with a current density of 3 × 108 A m–2, nearly 3 orders of magnitude lower than required to move magnetic domain walls. This highlights the possibility to use such an element as a skyrmion source/drain within future spintronic devices.

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