Two-Dimensional Electron Gases at the Surface of Potassium Tantalate Ben Pound Electron Physics Group SURF Colloquium, August 8, 2014.

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Presentation transcript:

Two-Dimensional Electron Gases at the Surface of Potassium Tantalate Ben Pound Electron Physics Group SURF Colloquium, August 8, 2014

Outline  Semiconductor technology  Properties of perovskites  Some properties of KTaO 3 2

Transistor size is approaching its limit 3 90 nm 32 nm 1970’s: 10,000 nm Approximate feature size: Wikipedia, “Moore’s Law”

Two-dimensional electron gases give functionality to field-effect transistors 4 Wikipedia, “Lateral MOSFET”

Ionic Liquid Gate KTaO 3 5 A two-dimensional electron gas forms at the surface of KTaO 3 by applying an electric field Charge Separation < 1 nm! Huge electric fields! K. Ueno, Nature Nanotechnology 6, 408–412 (2011)

“2 Dimensional” Crystal Structure 6

Perovskite crystal structure is periodic in three dimensions 7

There are many different perovskites 8 Adapted by G. Khalsa from,Schlom, D.G. et al., J. Am. Ceram. Soc. 91, 2429 (2008).

Perovskites have many diverse properties 9 P. Zubko, et al. Annu. Rev. Condens. Matter Phys :141–65

Theoretical Model 10 Black Box -Lattice “spring constants” -Dielectric Screening -Bonding parameters -Electric Potential by layer -Lattice Displacements -Layer Charge Density

Screening reduces external electric fields in the interior of the material 11  When external electric fields are applied, electron clouds and nuclei move to reduce electric fields inside the material. Ionic Liquid KTaO 3 Gate

Screening in KTaO 3 is enhanced by atomic movement  High dielectric constant = high polarization Oxygen Tantalum Potassium

Screening in layered KTaO 3 13 Ionic Liquid Gate KTaO

Inelastic neutron scattering provides “spring constants” of the lattice 14  Phonon energy can be converted to a frequency  K depends on frequency, and on layer C. H. Perry, et al. Phys. Rev. B 39, 8666 (1989) Energy (meV) 0 qxqx

Capacitance measurements show how well KTaO 3 screens electric field  Dielectric constant changes with applied electric field 15 C. Ang, et al. Phys. Rev. B 64, (2001)

Combining inelastic neutron scattering and capacitance measurements gives Q 16 Displacement Energy

Theoretical Model 17 Black Box -Lattice “spring constants” -Bonding parameters -Dielectric Screening -Electric Potential by layer -Lattice Displacements -Layer Charge Density

Conclusions  Field-effect transistors made from perovskite materials are different than traditional silicon transistors  Lattice screening is very different – adds significant complication  Extracted information from literature about KTaO 3 to be inputs for a simple electrostatic model  Bonding parameters and “spring constants”  Dependence of dielectric constant on electric field  Born effective charge 18

Acknowledgements  SURF Program and SURF Directors  Mark Stiles (advisor)  Guru Khalsa (postdoctoral researcher) 19