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Two-dimensional electron gas with six-fold symmetry at the (111) surface of KTaO3

Scientific Reports volume 4, Article number: 3586 (2014) | Download Citation

Abstract

Two-dimensional electron gases (2DEGs) at transition-metal oxide (TMO) interfaces, and boundary states in topological insulators, are being intensively investigated. The former system harbors superconductivity, large magneto-resistance, and ferromagnetism. In the latter, honeycomb-lattice geometry plus bulk spin-orbit interactions lead to topologically protected spin-polarized bands. 2DEGs in TMOs with a honeycomb-like structure could yield new states of matter, but they had not been experimentally realized, yet. We successfully created a 2DEG at the (111) surface of KTaO3, a strong insulator with large spin-orbit coupling. Its confined states form a network of weakly-dispersing electronic gutters with 6-fold symmetry, a topology novel to all known oxide-based 2DEGs. If those pertain to just one Ta-(111) bilayer, model calculations predict that it can be a topological metal. Our findings demonstrate that completely new electronic states, with symmetries not realized in the bulk, can be tailored in oxide surfaces, promising for TMO-based devices.

Introduction

The realization of 2DEGs at surfaces or interfaces of transition-metal oxides is a field of bursting activity1,2,3,4,5,6,7,8,9,10,11,12,13. These materials are usually correlated-electron systems presenting a wealth of unique properties, such as high-temperature superconductivity, colossal magnetoresistance, metal-to-insulator transitions, or multiferroic behaviour. In the search for new functionalities and future electronic device applications, a crucial challenge is to find original ways to design the oxide-based 2DEGs, so as to endow them with the exotic physics of their parent compounds, and to tailor novel states of matter.

Research in non-trivial topological edge states is also a very active field14,15,16,17,18,19. The possibility of realizing these in oxide-based 2DEGs, raised in several recent theoretical works20,21,22,23,24, is attracting much interest. A practical proposal was based on a key insight: that the cubic ABO3 perovskite structure, common to many correlated oxides, realizes a honeycomb lattice when a bilayer along the [111] direction is considered20,23,24. Such artificial structure could, in principle, be digitally engineered as a sandwich between two oxide insulators20. However, this approach currently remains a technological challenge.

Here we take an alternative route towards the same goal. Beyond the realization of 2DEGS at LaAlO3/SrTiO3 interfaces oriented along [001]1, and lately [110] and [111] cristallographic directions25,26, it was recently discovered that 2DEGs can be simply obtained at the vacuum-cleaved (001) surface of insulating ABO3 perovskites10,11,12,13 opening an exciting perspective to create novel 2DEGs at the surface of correlated oxides. Following this methodology, here we demonstrate that the Fermi sea of the 2DEG can be crafted by properly choosing the cleaving plane of the perovskite crystal. Specifically, we obtain a 2DEG at the (111) surface of the strong spin-orbit coupled insulator KTaO3 (KTO), and determine directly its electronic structure using angle-resolved photoemission spectroscopy (ARPES). We observe an open Fermi surface of 6-fold symmetry with weakly dispersing branches, which is unique among all other previously known oxide-based 2DEGs. Using model calculations we show that it originates from electron hopping between consecutive layers of Ta atoms along the [111] direction. Furthermore, by analyzing the symmetries of this electronic structure, we demonstrate that confining this novel 2DEG to a bilayer of Ta atoms, hence a honeycomb lattice, will lead to a topological metal.

Results

Basic considerations: structure of KTaO3 along the [111] direction

Figure 1(a) presents the crystal structure of KTaO3. Along the [111] direction, the system has 3-fold symmetry, as any cubic system, and consists of alternating layers of Ta and KO3. There are three different Ta-(111) layers per unit cell, labelled Ta-I, Ta-II and Ta-III. Figure 1(b) shows the Ta atoms in the 3D structure seen from the [111] direction. Arrows represent the lattice vectors of a 2D unit cell in the (111) plane, which corresponds to a centered hexagonal network with 6-fold symmetry. When only two layers are considered (Ta-I and Ta-II, for example), the lattice formed by nearest neighbors is a honeycomb lattice (thick black lines), similar to the bi-layer structure proposed in Ref. 20. As we shall see later, our ARPES data are consistent with the formation of a 2DEG with the periodicity and the symmetry of an unresconstructed (111) plane.

Figure 1: KTaO3 crystal in real space: schematics of the structure along the [111] direction.
Figure 1

(a) Crystal structure of KTaO3. Dashed triangles indicate the three Ta-(111) layers in the unit cell, labeled Ta-I, Ta-II and Ta-III. Ta atoms lying in the same (111) plane have the same shading color (green, blue or red). Note that Ta atoms in consecutive Ta-(111) layers are nearest neighbors. (b) View along the [111] direction of the Ta atoms alone. Lines connecting Ta atoms represent the edges of the 3D unit cell. Thick black lines connect nearest neighbors in layers Ta-I and Ta-II, forming a honeycomb lattice. Curved double arrows represent electron hopping between nearest neighbors. Straight black arrows are the lattice vectors of a 2D unit cell in the (111) plane. Such 2D unit cell is independent of the number of Ta-layers considered.

Experimental electronic structure

Figure 2(a) shows the Fermi surface (color map) of the 2DEG measured at the (111) surface of transparent and bulk insulating KTO, pictured in Fig. 2(b). Experimental details of the extraction of this Fermi surface are given in the Supplementary Material. The black hexagons in figure 2(a) represent the Brillouin zone of the unreconstructed (111) surface. Note that the observed Fermi surface has a well defined 6-fold symmetry and a periodicity corresponding to that of the unreconstructed KTO-(111) layers. By Bloch theorem, we infer that the 2DEG is formed by itinerant conduction electrons experiencing an in-plane potential compatible with unreconstructed (111) layers. In turn, this strongly suggests that, while one might expect that the highly-polar KTO-(111) surface reconstructs, the observed 2DEG is formed by electrons confined in unreconstructed subsurface layers.

Figure 2: Electronic structure of the 2DEG at the (111) surface of bulk insulating KTaO3.
Figure 2

(a) Fermi surface in the (111) plane, obtained from the superposition of ARPES maps measured at = 96 eV and = 50 eV, and integrated over [−50, +5] meV around EF. Black hexagons correspond to the surface Brillouin zones. (b) Picture of a measured sample of KTaO3 before fracturing in vacuum. (c) Energy-momentum intensity map of the band structure in the direction, measured along the dashed green line in panel (a). The red dashed lines are parabolic fits to the dispersion. (d) Stack of MDCs for the intensity map in (c). Each MDC was integrated over ±20 meV around its corresponding energy. Thicker lines represent the MDCs at EF and at the bottom of the bands. Dashed lines are guides to the eye for the peaks of the two observed bands. (e) Stack of EDCs along , dashed red arrow in panel (a). The positions of the peaks at E ~ −260 meV correspond to the bottom of the parabolic electron bands, like those of panel (c), forming the quasi-non-dispersive ‘gutters’. Data of (c), (d) and (e) were measured at = 96 eV.

More specifically, the Fermi surface of Fig. 2(a) consists of 6 branches extending out from to the six points. From the area enclosed by this Fermi surface, we obtain a carrier density n2D ~ 1014 cm−2. The observation of such a large Fermi surface fully supports the quasi-2D (i.e., confined) character of the electron gas. Indeed, if the Fermi surface was a cross-section of an hypothetical 3D Fermi surface, the ensuing electron density would be, by simple scaling, . For such density, only one order of magnitude smaller than that of pure gold, the sample would be highly conducting and its aspect would be mirror-like, in stark contrast with the transparent character of the bulk crystal shown in figure 2(b), indicative of an insulating state.

Different energy-momentum intensity maps across the Fermi sea provide valuable complementary information about the 2DEG at the (111) surface of KTO. Figures 2(c, d) show the dispersion along the direction, dashed green line in figure 2(a), in the form of, respectively, intensity map and stack of momentum distribution curves (MDCs). This dispersion indicates that the Fermi surface branches are formed by electron-like bands coming close to each other near . The effective mass of these electron-like bands, deduced from a parabolic fit (red dashed lines), is (me is the free electron mass). Furthermore, as shown by the stack of energy distribution curves (EDCs) in figure 2 (e), the bottom of each of these electron bands is essentially non-dispersive along the direction. Accordingly, the Fermi surface forms a star with six open branches, each branch being composed of two quasi-parallel sheets. In other words, the electronic structure of the 2DEG at the (111) surface of KTO consists of a network of weakly dispersing “electron gutters”.

Since we observe only the first subband (E1) of the 2DEG, we can only estimate an upper limit for the extension L of the 2DEG. We make the reasonable assumptions that E1 ≈ −V0, where V0 is the depth of the confining potential well, and that the next quantum level (E2) of the same nature as the measured subband lies at an energy E2E1V0, at or above EF. The result, detailed in the Supplementary Material, is L < 16 Å, or equivalently, L < 7 Ta-layers along (111).

Note, from figures 2(c–e), that there is an intense background below E = −260 meV trailing behind the bands forming the 2DEG. The most likely origin of this background is inelastic scattering of the electrons off impurities or disorder. This can be either in-plane scattering, which will broaden the spectral lines, or scattering of the electron on its way out of the surface during the photoemission process. For instance, we expect that the fractured native surface will be rugged, and will contain a large density of vacancies. Thus, a large number of photo-emitted electrons will loose some kinetic energy, due to inelastic scattering, on their way out of the solid. All these electrons will contribute to an intense inelastic background trailing behind the broadened parabolic quasi-particle peak. As this background is extrinsic to the electronic structure, it has no effect on the quasi-particle spectral function, in agreement with the observation, noted earlier, that the experimental effective mass of the 2DEG's band is essentially the same as the one given by non-correlated tight-binding calculations (Supplementary Material and Ref. 13).

Discussion

The observed electronic structure can be understood in terms of electron hopping between neighbouring Ta layers. To see how, we modeled the 2DEG using a tight binding (TB) hamiltonian on a Ta-(111) bilayer with the hopping parameters determined from our previous study of KTO-(001)13 –see details in the Supplementary Material. Indeed, as schematically indicated by the double arrows in figure 1(b), and in Ref. 20, the largest hopping occurs between the Ta atoms of consecutive (111) layers, as they correspond to nearest neighbors along [001] in the cubic 3D lattice. In figure 3(a) we compare the experimental ARPES Fermi surface to the calculated Fermi surface. We observe that the model correctly gives the band-structure of the weakly dispersing electron gutters. The comparison between the data and calculations close to the point is more difficult due to the experimental resolution. We checked that including extra Ta layers or considering the hopping of electrons between Ta atoms on the same (111) layer, which are next-nearest neighbors, will mainly change the computed band-structure around the point, but not the structure of the gutters, so that the comparison above remains valid.

Figure 3: Comparison of experimental and tight-binding Fermi surfaces of the 2DEG at the (111) surface of KTaO3.
Figure 3

(a) Experimental Fermi momenta from the original data after symmetrization (blue open circles) compared to the Fermi surface from a two-layer tight-binding calculation (red lines). The Fermi momenta were determined from the peak positions of the MDCs at EF, using Lorenzian fits. The inner quasi-circular Fermi surface found in the calculations, of radius ~ 0.15 Å−1, is difficult to compare with the data, due to the experimental resolution. (b) Directional paths, in real space, created by the different t2g orbitals, dxy, dzx and dyz, on a (111) bilayer of Ta atoms. The orange solid lines illustrate hopping channels created by the dxy orbitals, while dashed green and violet lines illustrate the channels created by the dzx and dyz orbitals, respectively.

The weakly dispersing gutters along the lines are the most salient feature of the observed Fermi surface. They can be intuitively understood from the directional overlaps between t2g orbitals in neighboring Ta sites, which give rise to large nearest-neighbor hopping amplitudes along the [001] (and equivalent) directions. When seen from the [111] direction, these appear as directional zig-zag chains at 120° from each other, as depicted in Fig. 3(b) for two consecutive Ta (111) layers. Each set of parallel hopping chains on the 2D lattice will lead to open weakly dispersing Fermi sheets in reciprocal space, i.e., to the observed gutters.

Our results demonstrate that a 2DEG with hexagonal symmetry can be easily created at the (111) surface of KTO. As an outlook for near-future investigations, an exciting feature arises when such a 2DEG is confined to a Ta-(111) bilayer, which forms a honeycomb lattice –as seen from the lattice formed by layers Ta-I and Ta-II in figure 1(b). In this case, following Ref. 27, one can demonstrate (details in the Supplementary Material) that the electron wave-function of the ground state has an odd parity at one of the points (and its time-reversal partner), but an even parity at all other points, implying a non trivial topological index Z2 = 1. In this case, the 2DEG at the KTO (111) surface would correspond to a topological 2D metal, similar to some of the non-trivial states predicted in Ref. 20, with the 2DEG itself corresponding to the “bulk” states, and the non-trivial states appearing at the 1D edges of the sample.

From a broader perspective, our results show that different surface orientations can be used to tailor Fermi seas and to radically change the microscopic state, hence the physical properties, of oxide perovskite-based 2DEGs. Of particular interest is the prospect for engineering 2DEGs of strongly correlated insulators on honeycomb lattice-structures, which could lead to correlated topological and edge-states with new physical properties not shown by semiconducting topological insulators. Thus, in perspective, our results provide some initial bridges between the fields of topological matter, correlated electrons and oxide electronics.

Methods

The angle resolved photoemission spectroscopy (ARPES) experiments were done at the Synchrotron Radiation Center (SRC, University of Wisconsin, Madison) and at the Synchrotron SOLEIL (France), using linearly polarized photons in the energy range 20–100 eV and Scienta R4000 detectors with vertical slits (henceforth the ky direction). The momentum and energy resolutions were 0.25° and 15 meV, respectively. The mean diameter of the incident photon beam was smaller than 50 μm (SOLEIL) and about 150 μm (SRC).

The samples studied were undoped transparent high-grade laser crystals of KTaO3 (SurfaceNet, GmbH), of purity 99,9995%, grown by a modified top seeded solution growth (TSSG) using KO2 as solvent. The estimated amount of oxygen vacancies is less than 10 ppm, being mostly concentrated in the seeding area, which was not used for the final cut crystals. Similarly, the estimated amount of defects is less than 100 cm−3.

The crystals were mounted with and fractured in-situ along the (111) surface at 25 K (SRC) and 10 K (SOLEIL), in pressure lower than 6 × 10−11 Torr. The fractured surfaces had homogeneous electron photo-emittance over a large area.

The results have been reproduced in 6 different cleaves.

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Acknowledgements

We thank R. Weht, J. Guevara, G. Montambaux, F. Piéchon, J.-N. Fuchs and M.-O. Goerbig for discussions. A.F.S.-S. and M.G. acknowledge support from the Institut Universitaire de France. This work was supported by the ANR (project LACUNES) and the LabEX PALM (project ELECTROX).

Author information

Affiliations

  1. CSNSM, Université Paris-Sud and CNRS/IN2P3, Bâtiments 104 et 108, 91405 Orsay cedex, France

    • C. Bareille
    • , F. Fortuna
    • , T. C. Rödel
    •  & A. F. Santander-Syro
  2. Universität Würzburg, Experimentelle Physik VII, Am Hubland, 97074 Würzburg, Germany

    • T. C. Rödel
  3. Synchrotron SOLEIL, L'Orme des Merisiers, Saint-Aubin-BP48, 91192 Gif-sur-Yvette, France

    • F. Bertran
    • , A. Taleb-Ibrahimi
    •  & P. Le Fèvre
  4. Laboratoire de Physique des Solides, Université Paris-Sud and CNRS, Bâtiment 510, 91405 Orsay, France

    • M. Gabay
    • , O. Hijano Cubelos
    •  & M. J. Rozenberg
  5. Unité Mixte de Physique CNRS/Thales, Campus de l'Ecole Polytechnique, 1 Av. A. Fresnel, 91767 Palaiseau, France and Université Paris-Sud, 91405 Orsay, France

    • M. Bibes
    •  & A. Barthélémy
  6. Institut d'Electronique Fondamentale, Université Paris-Sud and CNRS, Bâtiment 220, 91405 Orsay, France

    • T. Maroutian
    •  & P. Lecoeur

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Contributions

Project conception: A.F.S.-S.; ARPES measurements: C.B., T.R., F.F., F.B. and A.F.S.-S.; infrastructure for ARPES experiments at Soleil: F.B., A.T.I. and P.L.F.; sample characterizations: M.B., A.B., T.M. and P.L.; data analysis, interpretation, calculations: C.B., A.F.S.-S., M.G., O.H.C. and M.J.R.; writing of the manuscript: A.F.S.-S., with input from C.B., M.G. and M.J.R. All authors discussed extensively the results and the manuscript.

Competing interests

The authors declare no competing financial interests.

Corresponding author

Correspondence to A. F. Santander-Syro.

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https://doi.org/10.1038/srep03586

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