Corona Virus Information Updated July 15, 2020

Long considered unachievable, magnetic monopoles have been realized in bulk crystals in recent years as ensembles containing equal numbers of monopoles and antimonopoles. In this form, exciting fundamental questions about the existence, properties, and dynamics of individual magnetic monopoles remain unanswered or inaccessible.

 

Pyrochlore_icespin

Figure: (a) 3D snapshot of the monopole distribution generated by Monte Carlo simulation of a pyrochlore/spin-ice/pyrochlore sandwich. (b) Schematic representation of the monopole gas stabilized at the interfaces between spin-ice and antiferromagnetic pyrochlore compounds. Magnetic monopoles are shown in green (orange=3 spins in, white=1 spin out).

To address these issues, PARADIM’s in-house research team has identified a strategy to form a two-dimensional magnetic monopole gas in a material called spin-ice (R2Ti2O7, R=Ho, Dy) that is sandwiched by the structurally matching pyrochlore compound R2Ir2O7. In this structure, Monte Carlo simulations suggest that the net magnetic charge and the density of monopoles can be controlled by an external field. The proposed two-dimensional monopole gas could enable entirely new classes of experiments and devices based on magnetic monopoles, akin to two-dimensional electron gases in semiconductor heterostructures.

L. Miao et al. Nature Communications 11 (2020) 1341. https://doi.org/10.1038/s41467-020-15213-z

Technical Background: Similar to electrons in a metal, magnetic monopoles in spin-ice compounds are believed to be unconfined and to interact via a magnetic analogue of Coulomb’s law and to form magnetic currents in magnetic fields. Unlike semiconductors and two-dimensional electron gases, however, where the charge degree of freedom can be actively controlled by chemical doping, interface modulation, and electrostatic gating, there is currently no analogue of these effects for emergent magnetic monopoles. To date, all experimental investigations have been restricted to bulk spin-ice systems with equally populated monopoles and antimonopoles.

The address these issues, PARADIM’s in-house research team has identified a strategy to form a two-dimensional magnetic monopole gas (2DMG) with a net magnetic charge at the heterointerface between a spin ice (R2Ti2O7) (R=Ho, Dy) and isostructural antiferromagnet (R2Ir2O7) in the pyrochlore family. At the boundary, the exchange field between the iridate and the spin ice has a non-zero flux flowing toward/away from the spin ice, resulting in a charged 2DMG in the adjacent layers of the spin ice. The boundary conditions are reminiscent of the polar discontinuity at the interface between LaAlO3 and SrTiO3, which hosts a two-dimensional electron gas [1,2] and inspired by recent theoretical proposals suggesting the surface crystallization of magnetic monopole and antimonopoles at the material/vacuum interface of spin-ice thin films [3,4]. The heterostructure proposed by L. Miao et al. represents an example of a magnetically charged monopole system, providing a unique opportunity to investigate properties and dynamics of magnetic monopoles.

 

The work was conducted by the PARADIM in-house research team at Cornell University together with a collaborator at Binghamton University.

 

Full reference: Ludi Miao, Yonghun Lee, Antonio B. Mei, Michael J. Lawler, and Kyle M. Shen, “Two-dimensional magnetic monopole gas in an oxide heterostructure,” Nature Communications 11 (2020) 1341. https://doi.org/10.1038/s41467-020-15213-z

 

Further Reading:

  1. A. Ohtomo and H. Y. Hwang, “A High-Mobility Electron Gas at the LaAlO3/SrTiO3 Heterointerface,” Nature 427(2004) 423–426.
  2. N. Nakagawa, H. Y. Hwang, and D. A. Muller, “Why Some Interfaces Cannot be Sharp,” Nature Materials 5(2006) 204–209.
  3. L.D.C. Jaubert, T. Lin, T.S. Opel, P.C.W. Holdsworth, and M.J.P. Gingras, “Spin ice thin film: Surface ordering, emergent square ice, and strain effects,” Phys. Rev. Lett. 118 (2017) 207206.
  4. E. Lantagne-Hurtubise, J.G. Rau, and M.J.P. Gingras, “Spin-ice thin films: Large-N Theory and Monte Carlo Simulations,” Phys. Rev. X 8 (2018) 021053.