lanthanum aluminate-strontium titanate interface

The interface between lanthanum aluminate (LaAlO₃) and strontium titanate (SrTiO₃) is a notable materials interface because it exhibits properties not found in its constituent materials. Individually, LaAlO₃ and SrTiO₃ are non-magnetic insulators, yet LaAlO₃/SrTiO₃ interfaces can exhibit electrical metallic conductivity, superconductivity, ferromagnetism, large negative in-plane magnetoresistance, and giant persistent photoconductivity. The study of how these properties emerge at the LaAlO₃/SrTiO₃ interface is a growing area of research in condensed matter physics.

Emergent properties

Conductivity

Under the right conditions, the LaAlO₃/SrTiO₃ interface is electrically conductive, like a metal. The angular dependence of Shubnikov–de Haas oscillations indicates that the conductivity is two-dimensional, leading many researchers to refer to it as a two-dimensional electron gas (2DEG). Two-dimensional does not mean that the conductivity has zero thickness, but rather that the electrons are confined to only move in two directions. It is also sometimes called a two-dimensional electron liquid (2DEL) to emphasize the importance of inter-electron interactions.

Conditions necessary for conductivity

Not all LaAlO₃/SrTiO₃ interfaces are conductive. Typically, conductivity is achieved only when:

*The LaAlO₃/SrTiO₃ interface is along the 001,110 and 111 crystallographic direction
*The LaAlO₃ and SrTiO₃ are crystalline and epitaxial
*The SrTiO₃ side of the interface is TiO₂-terminated (causing the LaAlO₃ side of the interface to be LaO-terminated)
*The LaAlO₃ layer is at least 4 unit cells thick
Conductivity can also be achieved when the SrTiO₃ is doped with oxygen vacancies; however, in that case, the interface is technically LaAlO₃/SrTiO_3−x instead of LaAlO₃/SrTiO₃.

Hypotheses for conductivity

The source of conductivity at the LaAlO₃/SrTiO₃ interface has been debated for years. SrTiO₃ is a wide-band gap semiconductor that can be doped n-type in a variety of ways. Clarifying the mechanism behind the conductivity is a major goal of current research. Four leading hypotheses are:

*Polar gating
*Oxygen vacancies
*Intermixing
*Structural distortions

= Polar gating

=

Polar gating was the first mechanism used to explain the conductivity at LaAlO₃/SrTiO₃ interfaces. It postulates that the LaAlO₃, which is polar in the 001 direction (with alternating sheets of positive and negative charge), acts as an electrostatic gate on the semiconducting SrTiO₃. When the LaAlO₃ layer grows thicker than three unit cells, its valence band energy rises above the Fermi level, causing holes (or positively charged oxygen vacancies ) to form on the outer surface of the LaAlO₃. The positive charge on the surface of the LaAlO₃ attracts negative charge to nearby available states. In the case of the LaAlO₃/SrTiO₃ interface, this means electrons accumulate in the surface of the SrTiO₃, in the Ti d bands.

The strengths of the polar gating hypothesis are that it explains why conductivity requires a critical thickness of four unit cells of LaAlO₃ and that it explains why conductivity requires the SrTiO₃ to be TiO₂-terminated. The polar gating hypothesis also explains why alloying the LaAlO₃ increases the critical thickness for conductivity.

One weakness of the hypothesis is that it predicts that the LaAlO₃ films should exhibit a built-in electric field; so far, x-ray photoemission experiments and other experiments have shown little to no built-in field in the LaAlO₃ films. The polar gating hypothesis also cannot explain why Ti³⁺ is detected when the LaAlO₃ films are thinner than the critical thickness for conductivity.

The polar gating hypothesis is sometimes called the polar catastrophe hypothesis, alluding to the counterfactual scenario where electrons don't accumulate at the interface and instead voltage in the LaAlO₃ builds up forever. The hypothesis has also been called the electronic reconstruction hypothesis, highlighting the fact that electrons, not ions, move to compensate the building voltage.

= Oxygen vacancies

=

Another hypothesis is that the conductivity comes from free electrons left by oxygen vacancies in the SrTiO₃. SrTiO₃ is known to be easily doped by oxygen vacancies, so this was initially considered a promising hypothesis. However, electron energy loss spectroscopy measurements have bounded the density of oxygen vacancies well below the density necessary to supply the measured free electron densities.
Another proposed possibility is that oxygen vacancies in the surface of the LaAlO₃ are remotely doping the SrTiO₃. Under generic growth conditions, multiple mechanisms can coexist. A systematic study across a wide growth parameter space demonstrated different roles played by oxygen vacancy formation and the polar gating at different interfaces. An obvious difference between oxygen vacancies and polar gating in creating the interface conductivity is that the carriers from oxygen vacancies are thermally activated as the donor level of oxygen vacancies is usually separated from the SrTiO₃ conduction band, consequently exhibiting the carrier freeze-out effect at low temperatures; in contrast, the carriers originating from the polar gating are transferred into the SrTiO₃ conduction band (Ti 3d orbitals) and are therefore degenerate.

= Intermixing

=

Lanthanum is a known dopant in SrTiO₃, so it has been suggested that La from the LaAlO₃ mixes into the SrTiO₃ and dopes it n-type. Multiple studies have shown that intermixing takes place at the interface; however, it is not clear whether there is enough intermixing to provide all of the free carriers. For example, a flipped interface between a SrTiO₃ film and a LaAlO₃ substrate is insulating.

= Structural distortions

=

A fourth hypothesis is that the LaAlO₃ crystal structure undergoes octahedral rotations in response to the strain from the SrTiO₃. These octahedral rotations in the LaAlO₃ induce octahedral rotations in the SrTiO₃, increasing the Ti d-band width enough so that electrons are no longer localized.

Superconductivity

Superconductivity was first observed in LaAlO₃/SrTiO₃ interfaces in 2007, with a critical temperature of ~200 mK. Like the conductivity, the superconductivity appears to be two-dimensional.

Ferromagnetism

Hints of ferromagnetism in LaAlO₃/SrTiO₃ were first seen in 2007, when Dutch researchers observed hysteresis in the magnetoresistance of LaAlO₃/SrTiO₃. Follow up measurements with torque magnetometry indicated that the magnetism in LaAlO₃/SrTiO₃ persisted all the way to room temperature. In 2011, researchers at Stanford University used a scanning SQUID to directly image the ferromagnetism, and found that it occurred in heterogeneous patches. Like the conductivity in LaAlO₃/SrTiO₃, the magnetism only appeared when the LaAlO₃ films were thicker than a few unit cells. However, unlike conductivity, magnetism was seen at SrO-terminated surfaces as well as TiO₂-terminated surfaces.

The discovery of ferromagnetism in a materials system that also superconducts spurred a flurry of research and debate, because ferromagnetism and superconductivity almost never coexist together. Ferromagnetism requires electron spins to align, while superconductivity typically requires electron spins to anti-align.

Magnetoresistance

Magnetoresistance measurements are a major experimental tool used to understand the electronic properties of materials. The magnetoresistance of LaAlO₃/SrTiO₃ interfaces has been used to reveal the 2D nature of conduction, carrier concentrations (through the hall effect), electron mobilities, and more.

Field applied out-of-plane

At low magnetic field, the magnetoresistance of LaAlO₃/SrTiO₃ is parabolic versus field, as expected for an ordinary metal. However, at higher fields, the magnetoresistance appears to become linear versus field. Linear magnetoresistance can have many causes, but so far there is no scientific consensus on the cause of linear magnetoresistance in LaAlO₃/SrTiO₃ interfaces. Linear magnetoresistance has also been measured in pure SrTiO₃ crystals, so it may be unrelated to the emergent properties of the interface.

Field applied in-plane

At low temperature (T < 30 K), the LaAlO₃/SrTiO₃ interface exhibits negative in-plane magnetoresistance, sometimes as large as -90%. The large negative in-plane magnetoresistance has been ascribed to the interface's enhanced spin-orbit interaction.

Electron gas distribution at the LaAlO₃/SrTiO₃ interface

Experimentally, the charge density profile of the electron gas at the LaAlO₃/SrTiO₃ interface has a strongly asymmetric shape with a rapid initial decay over the first 2 nm and a pronounced tail that extends to about 11 nm. A wide variety of theoretical calculations support this result. Importantly, to get electron distribution one have to take into account field-dependent dielectric constant of SrTiO₃.

Comparison to other 2D electron gases

The 2D electron gas that arises at the LaAlO₃/SrTiO₃ interface is notable for two main reasons. First, it has very high carrier concentration, on the order of 10¹³ cm⁻². Second, if the polar gating hypothesis is true, the 2D electron gas has the potential to be totally free of disorder, unlike other 2D electron gases that require doping or gating to form. However, so far researchers have been unable to synthesize interfaces that realize the promise of low disorder.

Synthesis methods

Most LaAlO₃/SrTiO₃ interfaces are synthesized using pulsed laser deposition. A high-power laser ablates a LaAlO₃ target, and the plume of ejected material is deposited onto a heated SrTiO₃ substrate. Typical conditions used are:

*Laser wavelength of 248 nm
*Laser fluence of 0.5 J/cm² to 2 J/cm²
*Substrate temperature of 600 °C to 850 °C
*Background oxygen pressure of 10⁻⁵ Torr to 10⁻³ Torr

Some LaAlO₃/SrTiO₃ interfaces have also been synthesized by molecular beam epitaxy, sputtering, and atomic layer deposition.

Similar interfaces

To better understand in the LaAlO₃/SrTiO₃ interface, researchers have synthesized a number of analogous interfaces between other polar perovskite films and SrTiO₃. Some of these analogues have properties similar to LaAlO₃/SrTiO₃, but some do not.

Conductive interfaces

*GdTiO₃/SrTiO₃
*LaTiO₃/SrTiO₃
*LaVO₃/SrTiO₃
*LaGaO₃/SrTiO₃
*PrAlO₃/SrTiO₃
*NdAlO₃/SrTiO₃
*NdGaO₃/SrTiO₃
*GdAlO₃/SrTiO₃
*Nd_0.35Sr_0.65MnO₃/SrTiO₃
*Al₂O₃/SrTiO₃
*amorphous-YAlO₃/SrTiO₃
*La_0.5Al_0.5Sr_0.5Ti_0.5O₃/SrTiO₃
*DyScO₃/SrTiO₃
*KTaO₃/SrTiO₃
*CaZrO₃/SrTiO₃

Insulating interfaces

*LaCrO₃/SrTiO₃
*LaMnO₃/SrTiO₃
*La₂O₃/SrTiO₃
*Y₂O₃/SrTiO₃
*LaYO₃/SrTiO₃
*EuAlO₃/SrTiO₃
*BiMnO₃/SrTiO₃

Applications

As of 2015, there are no commercial applications of the LaAlO₃/SrTiO₃ interface. However, speculative applications have been suggested, including field-effect devices, sensors, photodetectors, and thermoelectrics;
related LaVO₃/SrTiO₃ is a functional solar cell albeit hitherto with a low efficiency.

References

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External links

Materials science: Enter the oxides

Condensed matter physics
Materials science
Perovskites