4.7 Article

Correlated nanoelectronics and the second quantum revolution

Journal

APL MATERIALS
Volume 10, Issue 11, Pages -

Publisher

AIP Publishing
DOI: 10.1063/5.0111221

Keywords

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Funding

  1. NSF [PHY-1913034]
  2. ONR [N00014-20-1-2481, N00014-21-1-2537]
  3. DOE [DE-SC0022277]
  4. U.S. Department of Energy (DOE) [DE-SC0022277] Funding Source: U.S. Department of Energy (DOE)

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The field of correlated nanoelectronics combines correlated oxide electronics and semiconductor nanoelectronics. By controlling complex material properties at nanoscale dimensions, quantum technologies for computation, simulation, and sensing can be developed. Heterostructures and nanostructures formed at the interface between LaAlO3 and SrTiO3 exhibit unique behavior that can be controlled using reversible methods such as conductive atomic force microscope lithography and ultra-low-voltage electron beam lithography.
The growing field of correlated nanoelectronics exists at the intersection of two established fields: correlated oxide electronics and semiconductor nanoelectronics. The development of quantum technologies that exploit quantum coherence and entanglement for the purposes of computation, simulation, and sensing will require complex material properties to be controlled at nanoscale dimensions. Heterostructures and nanostructures formed at the interface between LaAlO3 and SrTiO3 exhibit striking behavior that arises from the ability to program the conductive behavior at extreme nanoscale dimensions. The active electronic layer, SrTiO3, exhibits a wide range of gate-tunable phenomena such as ferroelectricity, ferroelasticity, magnetism, superconductivity, and spin-orbit coupling, all of which can be controlled at the nanoscale using two reversible methods: conductive atomic force microscope lithography and ultra-low-voltage electron beam lithography. Mesoscopic devices such as single-electron transistors and quasi-one-dimensional electron waveguides can be sketched using these techniques, and the properties of these devices differ significantly from those created from traditional semiconductors, such as Si or GaAs. The strongly correlated nature of the SrTiO3 system is evident from superconducting behavior as well as a state in which electrons are paired outside the superconducting state. A highly exotic phase was discovered in which a degenerate quantum liquid is formed from bound states of n = 2, 3, 4, horizontal ellipsis electrons. Further development of correlated nanoelectronics based on the LaAlO3/SrTiO3 system can potentially lead to a general platform for quantum simulation as well as a pathway for the development of highly entangled states of multiple photons.

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