Weyl semimetal phase in the non-centrosymmetric compound TaAs

Nature Physics Springer Nature 11:9 (2015) 728-732

Authors:

LX Yang, ZK Liu, Y Sun, H Peng, HF Yang, T Zhang, B Zhou, Y Zhang, YF Guo, M Rahn, D Prabhakaran, Z Hussain, S-K Mo, C Felser, B Yan, YL Chen

Evidence of quantum dimer excitations in Sr3Ir2O7

Physical Review B American Physical Society (APS) 92:2 (2015) 024405

Authors:

M Moretti Sala, V Schnells, S Boseggia, L Simonelli, A Al-Zein, JG Vale, L Paolasini, EC Hunter, RS Perry, D Prabhakaran, AT Boothroyd, M Krisch, G Monaco, HM Rønnow, DF McMorrow, F Mila

Importance of XY anisotropy in Sr2IrO4 revealed by magnetic critical scattering experiments

Physical Review B American Physical Society (APS) 92:2 (2015) 020406

Authors:

JG Vale, S Boseggia, HC Walker, R Springell, Z Feng, EC Hunter, RS Perry, D Prabhakaran, AT Boothroyd, SP Collins, HM Rønnow, DF McMorrow

Crystal field states of Tb3+ in the pyrochlore spin liquid Tb2Ti2O7 from neutron spectroscopy

Physical Review B American Physical Society (APS) 91:22 (2015) 224430

Authors:

AJ Princep, HC Walker, DT Adroja, D Prabhakaran, AT Boothroyd

Linear magnetoresistance caused by mobility fluctuations in n-doped Cd(3)As(2).

Physical review letters 114:11 (2015) 117201

Authors:

A Narayanan, MD Watson, SF Blake, N Bruyant, L Drigo, YL Chen, D Prabhakaran, B Yan, C Felser, T Kong, PC Canfield, AI Coldea

Abstract:

Cd(3)As(2) is a candidate three-dimensional Dirac semimetal which has exceedingly high mobility and nonsaturating linear magnetoresistance that may be relevant for future practical applications. We report magnetotransport and tunnel diode oscillation measurements on Cd(3)As(2), in magnetic fields up to 65 T and temperatures between 1.5 and 300 K. We find that the nonsaturating linear magnetoresistance persists up to 65 T and it is likely caused by disorder effects, as it scales with the high mobility rather than directly linked to Fermi surface changes even when approaching the quantum limit. From the observed quantum oscillations, we determine the bulk three-dimensional Fermi surface having signatures of Dirac behavior with a nontrivial Berry phase shift, very light effective quasiparticle masses, and clear deviations from the band-structure predictions. In very high fields we also detect signatures of large Zeeman spin splitting (g∼16).