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Theoretical physicists working at a blackboard collaboration pod in the Beecroft building.
Credit: Jack Hobhouse

Shivaji Sondhi

Wykeham Professor of Physics

Sub department

  • Rudolf Peierls Centre for Theoretical Physics
shivaji.sondhi@physics.ox.ac.uk
Rudolf Peierls Centre for Theoretical Physics, room 60.04
  • About
  • Publications

Digital Herd Immunity and COVID-19

Authors:

Vir B Bulchandani, Saumya Shivam, Sanjay Moudgalya, SL Sondhi

Jamming Dynamics of Hardcore Spins

Authors:

Shivaji Sondhi, Benedikt Placke, Grace M Sommers, Roderich Moessner

Quantum oscillations in the zeroth Landau Level and the serpentine Landau fan

Physical Review Letters American Physical Society

Authors:

T Devakul, Yves H Kwan, SL Sondhi, SA Parameswaran

Abstract:

We identify an unusual mechanism for quantum oscillations in nodal semimetals, driven by a single pair of Landau levels periodically closing their gap at the Fermi energy as a magnetic field is varied. These `zero Landau level' quantum oscillations (ZQOs) appear in the nodal limit where the zero-field Fermi volume vanishes, and have distinctive periodicity and temperature dependence. We link the Landau spectrum of a two-dimensional (2D) nodal semimetal to the Rabi model, and show by exact solution that across the entire Landau fan, pairs of opposite-parity Landau levels are intertwined in a `serpentine' manner. We propose 2D surfaces of topological crystalline insulators as natural settings for ZQOs, and comment on implications for anomaly physics in 3D nodal semimetals.

Theory of competing excitonic orders in insulating WTe$_2$ monolayers

Physical Review B: Condensed Matter and Materials Physics American Physical Society

Authors:

Yves H Kwan, T Devakul, Shivaji Sondhi, Sa Parameswaran

Abstract:

We develop a theory of the excitonic phase recently proposed as the zero-field insulating state observed near charge neutrality in monolayer WTe$_2$. Using a Hartree-Fock approximation, we numerically identify two distinct gapped excitonic phases: a spin density wave state for weak but non-zero interaction strength $U_0$, and spin spiral order at larger $U_0$, separated by a narrow window of trivial insulator. We introduce a simplified model capturing essential features of the WTe$_2$ band structure, in which the two phases may be viewed as distinct valley ferromagnetic orders. We link the competition between the two phases to the orbital structure of the electronic wavefunctions at the Fermi surface and hence its proximity to the underlying gapped Dirac point in WTe$_2$. We briefly discuss collective modes of the two excitonic states, and comment on implications for experiments.

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