Quasiparticle Breakdown and Spin Hamiltonian of the Frustrated Quantum Pyrochlore $Yb_{2}Ti_{2}O_{7}$ in a Magnetic Field

Physical Review Letters American Physical Society 119:5 (2017) 057203

Authors:

JD Thompson, PA McClarty, D Prabhakaran, I Cabrera, T Guidi, Radu Coldea

Abstract:

The frustrated pyrochlore magnet $Yb_{2}Ti_{2}O_{7}$ has the remarkable property that it orders magnetically but has no propagating magnons over wide regions of the Brillouin zone. Here we use inelastic neutron scattering to follow how the spectrum evolves in cubic-axis magnetic fields. At high fields we observe, in addition to dispersive magnons, a two-magnon continuum, which grows in intensity upon reducing the field and overlaps with the one-magnon states at intermediate fields leading to strong renormalization of the dispersion relations, and magnon decays. Using heat capacity measurements we find that the low- and high-field regions are smoothly connected with no sharp phase transition, with the spin gap increasing monotonically in field. Through fits to an extensive data set of dispersion relations combined with magnetization measurements, we reevaluate the spin Hamiltonian, finding dominant quantum exchange terms, which we propose are responsible for the anomalously strong fluctuations and quasiparticle breakdown effects observed at low fields.

Observation of nodal line in non-symmorphic topological semimetal InBi

New Journal of Physics IOP Publishing 19:065007 (2017) 1-8

Authors:

Sandy A Ekahana, S-C Wu, J Jiang, K Okawa, Dharmalingam Prabhakaran, C-C Hwang, S-K Mo, T Sasagawa, C Felser, B Yan, Z Liu, Yulin Chen

Abstract:

Topological nodal semimetal (TNS), characterized by its touching conduction and valence bands, is a newly discovered state of quantum matter which exhibits various exotic physical phenomena. Recently, a new type of TNS called topological nodal line semimetal (TNLS) is predicted where its conduction and valence band form a degenerate one-dimension line which is further protected by its crystal symmetry. In this work, we systematically investigated the bulk and surface electronic structure of the non-symmorphic, TNLS in InBi (which is also a type II Dirac semimetal) with strong spin-orbit coupling by using angle resolved photoemission spectroscopy. By tracking the crossing points of the bulk bands at the Brillouin zone boundary, we discovered the nodal-line feature along the kz direction, in agreement with the ab initio calculations and confirmed it to be a new compound in the TNLS family. Our discovery provides a new material platform for the study of these exotic topological quantum phases and paves the way for possible future applications.

Crystal growth of pyrochlore rare-earth stannates

JOURNAL OF CRYSTAL GROWTH 468 (2017) 335-339

Authors:

D Prabhakaran, S Wang, AT Boothroyd

Topological triplon modes and bound states in a Shastry–Sutherland magnet

Nature Physics Springer Nature 13:8 (2017) 736-741

Authors:

PA McClarty, F Krüger, T Guidi, SF Parker, K Refson, AW Parker, D Prabhakaran, Radu Coldea

Abstract:

The twin discoveries of the quantum Hall effect1, in the 1980s, and of topological band insulators2, in the 2000s, were landmarks in physics that enriched our view of the electronic properties of solids. In a nutshell, these discoveries have tau ght us that quantum mechanical wavefunctions in crystalline solids may carry nontrivial topological invariants which have ramifications for the observable physics. One of the side effects of the recent topological insulator revolution has been that such physics is much more widespread than was appreciated ten years ago. For example, while topological insulators were originally studied in the context of electron wavefunctions, recent work has initiated a hunt for topological insulators in bosonic systems: in photonic crystals3-6, in the vibrational modes of crystals7, and in the excitations of ordered magnets8. Using inelastic neutron scattering along with theoretical calculations, we demonstrate that, in a weak magnetic field, the dimerized quantum magnet SrCu 2 (BO 3 ) 2 is a bosonic topological insulator with topologically protected chiral edge modes of triplon excitations.

Doping dependence of collective spin and orbital excitations in the Spin-1 quantum antiferromagnet La₂₋ₓSrₓNiO₄ oObserved by X rays.

Physical Review Letters American Physical Society 118:15 (2017) 156402

Authors:

Gilberto Fabbris, Derek Meyers, Lei Xu, Vamshi M Katukuri, Liviu Hozoi, Xuerong Liu, Z-Y Chen, Jun Okamoto, Thorsten Schmitt, Anne-Christine Uldry, Bernhard Delley, Gen D Gu, Dharmalingam Prabhakaran, Andrew Boothroyd, Jeroen van den Brink, DJ Huang, Mark PM Dean

Abstract:

We report the first empirical demonstration that resonant inelastic x-ray scattering (RIXS) is sensitive to collective magnetic excitations in S=1 systems by probing the Ni L₃ edge of La₂₋ₓSrₓNiO₄ (x=0, 0.33, 0.45). The magnetic excitation peak is asymmetric, indicating the presence of single and multi-spin-flip excitations. As the hole doping level is increased, the zone boundary magnon energy is suppressed at a much larger rate than that in hole doped cuprates. Based on the analysis of the orbital and charge excitations observed by RIXS, we argue that this difference is related to the orbital character of the doped holes in these two families. This work establishes RIXS as a probe of fundamental magnetic interactions in nickelates opening the way towards studies of heterostructures and ultrafast pump-probe experiments.