SearcharxivSearch

arXiv subjects

Ruairidh Sutcliffe

Publications and source records attributed to Ruairidh Sutcliffe.

6 recordsLinked to original sources

Pseudo-chiral phonon splitting from octupolar magnetic order

Motivated by the recent discovery of anomalously large magnetic response of chiral phonons in dipolar magnets, we explore an extension to study Einstein quantum phonon modes coupled to multipolar moments. We consider the case of non-Kramers $Γ_3$ doublets which encapsulate quadrupolar and Ising octupolar degrees of freedom, and which feature a symmetry-allowed linear coupling between local quadrupolar moments and Raman active $E_g$ phonon modes $(d_{x^2-y^2},d_{3z^2-r^2})$. We show that either octupolar or quadrupolar ordering leads to degeneracy breaking of the $E_g$ phonon doublet, with ferro-octupolar order favoring pseudo-chiral phonon eigenmodes with a detectable energy splitting. We describe this physics using a path integral approach in the limit where `fast' phonon modes sense the `slow' pseudospins as a static background which we average over using Monte Carlo simulations. We discuss implications for materials such as Ba$_2$CaOsO$_6$ and PrV$_2$Al$_{20}$ where Raman spectroscopy of phonons could be used as a potential probe of hidden octupolar order. Our work extends the important concept of chiral phonons to a large class of multipolar magnets.

cond-mat.str-el

Jahn-Teller effect in $j = 3/2$ Mott insulators: Ground states and thermal fluctuations

The interplay of strong atomic spin-orbit coupling with Jahn-Teller (JT) lattice distortions is an important theme in quantum materials hosting heavy atoms. A prototypical example of such a system is a degenerate $j = 3/2$ multiplet coupled to local phonon modes. Here, we study the multipolar ground states of this system as realized in Mott insulators, explore its thermal phase diagram via an $SU(4)$ spin Monte Carlo approach coupled to JT phonons, and study the temperature dependent splittings of the $j = 3/2$ multiplet as relevant to spectroscopic probes. Our work sheds light on coexisting distinct multipolar orders engendered by phonon coupling, role of thermal JT fluctuations, and the entropy of the coupled multipole-phonon system. We discuss broad implications for double perovskites $\rm Ba_2MgReO_6$, $\rm Ba_2NaOsO_6$ and lacunar spinels such as $\rm GaTa_4Se_8$ and $\rm GaNb_4Se_8$.

cond-mat.str-el

Phonon-driven multipolar dynamics in a spin-orbit coupled Mott insulator

Motivated by advances in pump-probe experiments and light-driven phenomena, we theoretically study the impact of pumped and driven phonons in Mott insulators which host multipole moments, thus going beyond conventional dipolar magnetism. As a case study, we examine pseudospin-1/2 Mott insulators hosting quadrupolar and octupolar moments, and investigate the effect of resonantly exciting ${\cal E}_g$ phonon modes which couple linearly to the quadrupoles. We show that this leads to multipolar precession, with the back action resulting in chiral phonon dynamics below the octupolar phase transition. We further explore the impact of a coherent two-phonon Floquet drive, showing that it can be used to `train' octupolar order or even switch its sign on ultrafast timescales. Our results are obtained combining a generalized Monte Carlo code incorporating phonons with molecular dynamics simulations which numerically integrate the coupled spin-phonon equations of motion. Our work shows how phonon-driven dynamics can be used to probe and control hidden orders in solids.

cond-mat.str-el

$SU(N)$ spin-phonon simulations of Floquet dynamics in spin $S > 1/2$ Mott insulators

The dynamics of magnetic moments coupled to phonons is of great interest for understanding spin transport in solids as well as for our ability to control magnetism via tailored phonon modes. For spin $S > 1/2$, spin-orbit coupling permits an unusual linear coupling of phonons to quadrupolar moments, so that phonons act as a dynamical transverse field for the spins. Here, we develop a generalized $SU(N)$ spin-phonon Monte Carlo and molecular dynamics technique to simulate the equilibrium and nonequilibrium properties of such spin-orbital-phonon coupled Mott insulators, and apply it to a spin-1 model with competing XY antiferromagnet (AFM) and quadrupolar paramagnet (QPM) phases which is relevant to the Mott insulator $\rm{Ba_2FeSi_2O_7}$. We uncover a rich variety of dynamical phenomena in this system induced by linear or chiral phonon drives, including the generation of a uniform magnetization in the QPM and AFM, strengthening of Néel order and gapping of the AFM Nambu-Goldstone mode by Floquet-Ising anisotropy, a non-equilibrium QPM to AFM transition, and creation of Floquet copies of transverse and longitudinal spin waves. Our work is relevant for driven spin-1 magnets, such as $\rm{Ba_2FeSi_2O_7}$, and we highlight broader implications for nonequilibrium multipolar magnetism.

cond-mat.str-el

Modified large-$N$ approach to gapless spin liquids, magnetic orders, and dynamics: Application to triangular lattice antiferromagnets

Recent work has shown that the triangular lattice spin-$1/2$ $J_1$-$J_2$ Heisenberg and XXZ antiferromagnets may exhibit coplanar or supersolid orders proximate to a gapless Dirac spin liquid phase. We explore a distinct $SU(2N)\!\!\times\!\!SU(M)$ fermionic parton approach, complemented by variational Monte Carlo calculations for the spin-$1/2$ model, to study the phase diagram of these models. We also calculate their dynamical spin response including parton interactions within a random phase approximation, and discuss implications for neutron scattering on triangular lattice cobaltates Ba$_3$CoSb$_2$O$_9$, Na$_2$BaCo(PO$_4$)$_2$, K$_2$Co(SeO$_3$)$_2$, Rb$_2$Co(SeO$_3$)$_2$, and Yb-based magnet KYbSe$_2$.

cond-mat.str-el

Thermal Conductivity of Square Ice

We investigate thermal transport in square ice, a two-dimensional analogue of spin ice, exploring the role played by emergent magnetic monopoles in transporting energy. Using kinetic Monte Carlo simulations based on energy preserving extensions of single-spin-flip dynamics, we explicitly compute the (longitudinal) thermal conductivity, $κ$, over a broad range of temperatures. We use two methods to determine $κ$: a measurement of the energy current between thermal baths at the boundaries, and the Green-Kubo formula, yielding quantitatively consistent values for the thermal conductivity. We interpret these results in terms of transport of energy by diffusion of magnetic monopoles. We relate the thermal diffusivity, $κ/C$ where $C$ is the heat capacity, to the diffusion constant of an isolated monopole, showing that the subdiffusive monopole implies $κ/C$ vanishes at zero temperature. Finally, we discuss the implications of these results for thermal transport in three-dimensional spin ice, in spin ice materials such as Dy$_2$Ti$_2$O$_7$ and Ho$_2$Ti$_2$O$_7$, and outline some open questions for thermal transport in highly frustrated magnets.

cond-mat.str-el