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 (ACS) (2024)

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

Dichotomous dynamics of magnetic monopole fluids.

Proceedings of the National Academy of Sciences of the United States of America Proceedings of the National Academy of Sciences 121:21 (2024) e2320384121-e2320384121

Authors:

Chun-Chih Hsu, Hiroto Takahashi, Fabian Jerzembeck, Jahnatta Dasini, Chaia Carroll, Ritika Dusad, Jonathan Ward, Catherine Dawson, Sudarshan Sharma, Graeme M Luke, Stephen J Blundell, Claudio Castelnovo, Jonathan N Hallén, Roderich Moessner, JC Séamus Davis

Abstract:

A recent advance in the study of emergent magnetic monopoles was the discovery that monopole motion is restricted to dynamical fractal trajectories [J. N. Hallén <i>et al.</i>, <i>Science</i> <b>378</b>, 1218 (2022)], thus explaining the characteristics of magnetic monopole noise spectra [R. Dusad <i>et al., Nature</i> <b>571</b>, 234 (2019); A. M. Samarakoon <i>et al.</i>, <i>Proc. Natl. Acad. Sci. U.S.A.</i> <b>119</b>, e2117453119 (2022)]. Here, we apply this novel theory to explore the dynamics of field-driven monopole currents, finding them composed of two quite distinct transport processes: initially swift fractal rearrangements of local monopole configurations followed by conventional monopole diffusion. This theory also predicts a characteristic frequency dependence of the dissipative loss angle for AC field-driven currents. To explore these novel perspectives on monopole transport, we introduce simultaneous monopole current control and measurement techniques using SQUID-based monopole current sensors. For the canonical material Dy<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub>, we measure [Formula: see text], the time dependence of magnetic flux threading the sample when a net monopole current [Formula: see text] is generated by applying an external magnetic field [Formula: see text] These experiments find a sharp dichotomy of monopole currents, separated by their distinct relaxation time constants before and after <i>t</i> ~[Formula: see text] from monopole current initiation. Application of sinusoidal magnetic fields [Formula: see text] generates oscillating monopole currents whose loss angle [Formula: see text] exhibits a characteristic transition at frequency [Formula: see text] over the same temperature range. Finally, the magnetic noise power is also dichotomic, diminishing sharply after <i>t</i> ~[Formula: see text]. This complex phenomenology represents an unprecedented form of dynamical heterogeneity generated by the interplay of fractionalization and local spin configurational symmetry.

Field-orientation-dependent magnetic phases in GdRu$_2$Si$_2$ probed with muon-spin spectroscopy

(2024)

Authors:

BM Huddart, A Hernández-Melián, GDA Wood, DA Mayoh, M Gomilšek, Z Guguchia, C Wang, SJ Blundell, G Balakrishnan, T Lancaster

Magnetostriction-driven muon localization in an antiferromagnetic oxide

Physical Review Letters American Physical Society 132:4 (2024) 046701

Authors:

Pietro Bonfà, Ifeanyi John Onuorah, Franz Lang, Iurii Timrov, Lorenzo Monacelli, Chennan Wang, Xiao Sun, Oleg Petracic, Giovanni Pizzi, Nicola Marzari, Stephen J Blundell, Roberto De Renzi

Abstract:

Magnetostriction results from the coupling between magnetic and elastic degrees of freedom. Though it is associated with a relatively small energy, we show that it plays an important role in determining the site of an implanted muon, so that the energetically favorable site can switch on crossing a magnetic phase transition. This surprising effect is demonstrated in the cubic rocksalt antiferromagnet MnO which undergoes a magnetostriction-driven rhombohedral distortion at the Néel temperature T_{N}=118  K. Above T_{N}, the muon becomes delocalized around a network of equivalent sites, but below T_{N} the distortion lifts the degeneracy between these equivalent sites. Our first-principles simulations based on Hubbard-corrected density-functional theory and molecular dynamics are consistent with the experimental data and help to resolve a long-standing puzzle regarding muon data on MnO, as well as having wider applicability to other magnetic oxides.