Abstract
Understanding phonons in $\ensuremath{\alpha}\text{\ensuremath{-}}{\mathrm{RuCl}}_{3}$ is critical to analyze the controversy around the observation of the half-integer thermal quantum Hall effect. While many studies have focused on the magnetic excitations in $\ensuremath{\alpha}\text{\ensuremath{-}}{\mathrm{RuCl}}_{3}$, its vibrational excitation spectrum has remained relatively unexplored. We investigate the phonon structure of $\ensuremath{\alpha}\text{\ensuremath{-}}{\mathrm{RuCl}}_{3}$ via inelastic neutron-scattering experiments and density-functional-theory calculations. Our results show excellent agreement between experiment and first-principles calculations. After validating our theoretical model, we extrapolate the low-energy phonon properties. We find that the phonons in $\ensuremath{\alpha}\text{\ensuremath{-}}{\mathrm{RuCl}}_{3}$ that either propagate or vibrate in the out-of-plane direction have significantly reduced velocities and therefore have the potential to dominate the observability of the elusive half-integer plateaus in the thermal Hall conductance. In addition, we use low-energy interlayer phonons to resolve the low-temperature stacking structure of our large crystal of $\ensuremath{\alpha}\text{\ensuremath{-}}{\mathrm{RuCl}}_{3}$, which we find to be consistent with that of the $R\overline{3}$ space group, in agreement with neutron diffraction.
Highlights
In the Kitaev honeycomb model, strong bond-dependent interactions constrain the spins along the spin-orbital x, y, or z axis, leading to significant bond frustration [1]
The R factor that we obtained from the refinement for R3 ̄ is 0.0459, while attempts to index the majority of the peaks in other space-groups yielded an R factor of 0.1667 for C2/m and 0.2747 for P3112, even when twins were included
We have shown that in α-RuCl3 the phonon velocities, and the thermalization lengths, depend strongly on the polarization of the phonons and the direction of their momenta
Summary
In the Kitaev honeycomb model, strong bond-dependent interactions constrain the spins along the spin-orbital x, y, or z axis, leading to significant bond frustration [1]. This model can be exactly solved to reveal a Z2-type quantum spin liquid state in which there is no long-range magnetic order even down to zero Kelvin. One of the interesting properties of the Kitaev quantum spin liquid is that in zero field, spins can be shown to fractionalize into static and dynamic Majorana fermions, which leads to a spectrum of static Z2 gauge fluxes and itinerant Majorana fermions. It is being realized that phonons play a crucial role in the observability of the halfinteger plateaus [22,24,25]
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