Arzhang Ardavan Clarendon Laboratory, University of Oxford, England
Date: August 17th, 2021
Time: GMT 8:00 / KST 17:00
Venue: Online (ZOOM)
Electric field control of spins in piezoelectrics, ferroelectrics, and molecules Magnetic fields are challenging to localise to short length scales because their sources are electrical currents. Conversely, electric fields can be applied using electrostatic gates on scales limited only by lithography. This has important consequences for the design of spin-based information technologies: while the Zeeman interaction with a magnetic field provides a convenient tool for manipulating spins, it is difficult to achieve local control of individual spins on the length scale anticipated for useful quantum technologies. This motivates the study of electric field control of spin Hamiltonians .
Mn2+ defects in ZnO exhibit extremely long spin coherence times and a small axial zero-field splitting. Their environment is inversion-symmetry-broken, and the zero-field splitting shows a linear dependence on an externally applied electric field. This control over the spin Hamiltonian offers a route to controlling the phase of superpositions of spin states using d.c. electric field pulses, and to driving spin transitions using microwave electric fields . An analogous sensitivity to external electric fields is exhibited by Fe3+ defect spins in the archetypal ferroelectric PbTiO3. The Fe spin anisotropy axis is set by the ferroelectric order, so the spin Hamiltonian is controllable by manipulating the ferroelectric polarization direction .
Electric fields may couple to spins in molecular magnets by a range of mechanisms , including via intramolecular exchange interactions or hyperfine interactions, as well as through anisotropy terms. Through chemical design it is possible to optimise the conditions for molecular spin-electric coupling, yielding systems showing strong effects .
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