Metallicity at interphase boundaries due to polar catastrophe induced by charge density discontinuity
Source abstract
Abstract
The electronic properties of interphase boundaries are of basic importance for most materials, particularly when those properties deviate strongly from the bulk behavior. We introduce a mechanism that can result in metallicity at stoichiometric interphase boundaries between semiconductors based on the idea of polar catastrophe, which is usually considered only in the context of heterostructures. To this end, we perform ab initio calculations within density functional theory to investigate the electronic states at stoichiometric SnO/SnO2 (110) interphase boundaries. In this system, one would not expect polar catastrophe to have a role according to state-of-the-art theory because the interface lacks formal charge discontinuity. However, we observe the formation of a hole gas between the semiconductors SnO and SnO2. To explain these findings, we provide a generalized theory based on the idea that the charge density discontinuity between SnO and SnO2, a consequence of lattice mismatch, drives a polar catastrophe scenario. As a result, SnO/SnO2 (110) interphase boundaries can develop metallicity depending on the grain size. The concept of metallicity due to polar catastrophe induced by charge density discontinuity is of general validity and applies to many interphase boundaries with lattice mismatch. Tin oxide semiconductors can turn metallic at customized interfaces between two crystal phases, a theoretical study has found. Inspired by recent discoveries of surprisingly conductive regions formed when different insulators are sandwiched together, Udo Schwingenschlögl and two colleagues from KAUST in Saudi Arabia investigated whether similar properties could emerge at phase boundaries inside tin oxide materials. Density functional calculations of tin monoxide-dioxide interfaces indicate that certain polar arrangements generate desirable, high-mobility quantum gases even though the two sides of the boundary have the same formal charge – typically, abrupt charge changes are needed to create two-dimensional metallic states. The team proposed that this unexpected behavior arises from charge density discontinuities due to the mismatched lattices of tin monoxide and dioxide. We introduce a mechanism that can result in metallicity at stoichiometric interphase boundaries between semiconductors, based on the idea of polar catastrophe induced by charge density discontinuity. As an example, we demonstrate metallicity at the stoichiometric (110) interphase boundary of the semiconductors SnO and SnO2. The proposed mechanism is of general validity and expected to have an important role at interphase boundaries between polar materials.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Electronic and Structural Properties of Oxides · ZnO doping and properties · Gas Sensing Nanomaterials and Sensors
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (39)
Show source-provided references
1. Batzill, M. & Diebold, U. The surface and materials science of tin oxide. Prog. Surf. Sci. 79, 47–154 (2005).10.1016/j.progsurf.2005.09.002 ↗
2. Caraveo-Frescas, J. A., Nayak, P. K., Al-Jawhari, H. A., Granato, D. B., Schwingenschlögl, U. & Alshareef, H. N. Record mobility in transparent p-type tin monoxide films and devices by phase engineering. ACS Nano 7, 5160–5167 (2013).10.1021/nn400852r ↗
3. Shanmugasundaram, A., Basak, P., Satyanarayana, L. & Manorama, S. V. Hierarchical SnO/SnO2 nanocomposites: formation of in situ p-n junctions and enhanced H2 sensing. Sens. Actuators B 185, 265–273 (2013).10.1016/j.snb.2013.04.097 ↗
4. Chakhalian, J., Millis, A. J. & Rondinelli, J. Whither the oxide interface. Nat. Mater. 11, 92–94 (2012).10.1038/nmat3225 ↗
5. Yu, P., Chu, Y. H. & Ramesh, R. Oxide interfaces: pathways to novel phenomena. Mater. Today 15, 320–327 (2012).10.1016/S1369-7021(12)70137-2 ↗
6. Ohtomo, A. & Hwang, H. Y. A high-mobility electron gas at the LaAlO3/SrTiO3 heterointerface. Nature 427, 423–426 (2004).10.1038/nature02308 ↗
7. Zhong, Z., Xu, P. X. & Kelly, P. J. Polarity-induced oxygen vacancies at LaAlO3/SrTiO3 interfaces. Phys. Rev. B 82, 165127 (2010).10.1103/PhysRevB.82.165127 ↗
8. Perna, P., Maccariello, D., Radovic, M., Scotti di Uccio, U., Pallecchi, I., Codda, M., Marré, D., Cantoni, C., Gazquez, J., Varela, M., Pennycook, S. J. & Granozio, F. M. Conducting interfaces between band insulating oxides: the LaGaO3/SrTiO3 heterostructure. Appl. Phys. Lett. 97, 152111 (2010).10.1063/1.3496440 ↗
9. Moetakef, P., Cain, T. A., Ouellette, D. G., Zhang, J. Y., Klenov, D. O., Janotti, A., Van de Walle, C. G., Rajan, S., Allen, S. J. & Stemmer, S. Electrostatic carrier doping of GdTiO3/SrTiO3 interfaces. Appl. Phys. Lett. 99, 232116 (2011).10.1063/1.3669402 ↗
10. Biscaras, J., Bergeal, N., Hurand, S., Grossetête, C., Rastogi, A., Budhani, R. C., LeBoeuf, D., Proust, C. & Lesueur, J. Two-dimensional superconducting phase in LaTiO3/SrTiO3 heterostructures induced by high-mobility carrier doping. Phys. Rev. Lett. 108, 247004 (2012).10.1103/PhysRevLett.108.247004 ↗
11. Xu, P., Phelan, D., Jeong, S. J., Mkhoyan, K. A. & Jalan, B. Stoichiometry-driven metal-to-insulator transition in NdTiO3/SrTiO3 heterostructures. Appl. Phys. Lett. 104, 082109 (2014).10.1063/1.4866867 ↗
12. Hotta, Y., Susaki, T. & Hwang, H. Y. Polar discontinuity doping of the LaVO3/SrTiO3 interface. Phys. Rev. Lett. 99, 236805 (2007).10.1103/PhysRevLett.99.236805 ↗
13. Narkilahti, J., Plekh, M., Levoska, J. & Tyunina, M. Anomalous growth and properties of SrTiO3-NaNbO3 superlattices. Phys. Rev. B 79, 014106 (2009).10.1103/PhysRevB.79.014106 ↗
14. Park, M. S., Rhim, S. H. & Freeman, A. J. Charge compensation and mixed valency in LaAlO3/SrTiO3 heterointerfaces studied by the FLAPW method. Phys. Rev. B 74, 205416 (2006).10.1103/PhysRevB.74.205416 ↗
15. Choi, W. S., Kang, M. G., Do, Y. H., Jung, W. S., Ju, B. K., Yoon, S. J., Yoo, K. S. & Kang, C. Y. Oxygen vacancy effects of two-dimensional electron gas in SrTiO3/KNbO3 hetero structure. J. Sensor Sci. Technol. 22, 244–248 (2013).10.5369/JSST.2013.22.4.244 ↗
16. Zhang, L., Zhou, X. F., Wang, H. T., Xu, J. J., Li, J., Wang, E. G. & Wei, S. H. Origin of insulating behavior of the p-type LaAlO3/SrTiO3 interface: polarization-induced asymmetric distribution of oxygen vacancies. Phys. Rev. B 82, 125412 (2010).10.1103/PhysRevB.82.125412 ↗
17. Siemons, W., Koster, G., Yamamoto, H., Harrison, W. A., Lucovsky, G., Geballe, T. H., Blank, D. H. A. & Beasley, M. R. Origin of charge density at LaAlO3 on SrTiO3 heterointerfaces: possibility of intrinsic doping. Phys. Rev. Lett. 98, 196802 (2007).10.1103/PhysRevLett.98.196802 ↗
18. Thiel, S., Hammerl, G., Schmehl, A., Schneider, C. W. & Mannhart, J. Tunable quasi-two-dimensional electron gases in oxide heterostructures. Science 313, 1942–1945 (2016).10.1126/science.1131091 ↗
19. Pauli, S. A. & Willmott, P. R. Conducting interfaces between polar and non-polar insulating perovskites. J. Phys. Condens. Matter 20, 264012 (2008).10.1088/0953-8984/20/26/264012 ↗
20. Bristowe, N. C., Ghosez, P., Littlewood, P. B. & Artacho, E. The origin of two-dimensional electron gases at oxide interfaces: insights from theory. J. Phys. Condens. Matter 26, 143201 (2014).10.1088/0953-8984/26/14/143201 ↗
21. Mannhart, J., Blank, D. H. A., Hwang, H. Y., Millis, A. J. & Triscone, J. M. Two-dimensional electron gases at oxide interfaces. MRS Bull. 33, 1027–1034 (2008).10.1557/mrs2008.222 ↗
22. Nakagawa, N., Hwang, H. Y. & Muller, D. A. Why some interfaces cannot be sharp. Nat. Mater. 5, 204–209 (2006).10.1038/nmat1569 ↗
23. Popovic, Z. S., Satpathy, S. & Martin, R. M. Origin of the two-dimensional electron gas carrier density at the LaAlO3 on SrTiO3 interface. Phys. Rev. Lett. 101, 256801 (2008).10.1103/PhysRevLett.101.256801 ↗
24. Behtash, M., Nazir, S., Wang, Y. & Yang, K. Polarization effects on the interfacial conductivity in LaAlO3/SrTiO3 heterostructures: a first-principles study. Phys. Chem. Chem. Phys. 18, 6831–6838 (2016).10.1039/C5CP07581E ↗
25. Zhuang, H. L., Zhang, L., Xu, H., Kent, P. R. C., Ganesh, P. & Cooper, V. R. Tunable one-dimensional electron gas carrier densities at nanostructured oxide interfaces. Sci. Rep. 6, 25452 (2016).10.1038/srep25452 ↗
26. Jeon, S., Doak, P. W., Sumpter, B. G., Ganesh, P. & Maksymovych, P. Thermodynamic control of two-dimensional molecular ionic nanostructures on metal surfaces. ACS Nano 10, 7821–7829 (2016).10.1021/acsnano.6b03492 ↗
27. Kresse, G. & Joubert, D. From ultrasoft pseudopotentials to the projector augmented-wave method. Phys. Rev. B 59, 1758–1775 (1999).10.1103/PhysRevB.59.1758 ↗
28. Cossement, C., Darville, J., Gilles, J., Nagy, J. B., Fernandez, C. & Amoureux, J. Chemical shift anisotropy and indirect coupling in SnO2 and SnO. Magn. Reson. Chem. 30, 263–270 (1992).10.1002/mrc.1260300313 ↗
29. Lefebvre, I., Szymanski, M. A., Olivier-Fourcade, J. & Jumas, J. C. Electronic structure of tin monochalcogenides from SnO to SnTe. Phys. Rev. B 58, 1896–1906 (1998).10.1103/PhysRevB.58.1896 ↗
30. Behtash, M., Joo, P. H., Nazir, S. & Yang, K. Electronic structures and formation energies of pentavalent-ion-doped SnO2: first-principles hybrid functional calculations. J. Appl. Phys. 117, 175101 (2015).10.1063/1.4919422 ↗
31. Van de Walle, C. G. & Martin, R. M. Theoretical study of band offsets at semiconductor interfaces. Phys. Rev. B 35, 8154–8165 (1987).10.1103/PhysRevB.35.8154 ↗
32. Puthenkovilakam, R., Carter, E. A. & Chang, J. P. First-principles exploration of alternative gate dielectrics: electronic structure of ZrO2/Si and ZrSiO4/Si interfaces. Phys. Rev. B 69, 155329 (2004).10.1103/PhysRevB.69.155329 ↗
33. Quackenbush, N. F., Allen, J. P., Scanlon, D. O., Sallis, S., Hewlett, J. A., Nandur, A. S., Chen, B., Smith, K. E., Weiland, C., Fischer, D. A., Woicik, J. C., White, B. E., Watson, G. W. & Piper, L. F. J. Origin of the bipolar doping behavior of SnO from X-ray spectroscopy and density functional theory. Chem. Mater. 25, 3114–3123 (2013).10.1021/cm401343a ↗
34. Duan, Y. Electronic properties and stabilities of bulk and low-index surfaces of SnO in comparison with SnO2: a first-principles density functional approach with an empirical correction of van der Waals interactions. Phys. Rev. B 77, 045332 (2008).10.1103/PhysRevB.77.045332 ↗
35. Tasker, P. W. The stability of ionic crystal surfaces. J. Phys. C 12, 4977–4984 (1979).10.1088/0022-3719/12/22/036 ↗
36. Hong, S.-N., Kye, Y.-H., Yu, C.-J., Jong, U.-G., Ri, G.-C., Choe, C.-S., Kim, K.-H. & Han, J.-M. Ab anitio thermodynamic study of the SnO2(110) surface in an O2 and NO environment: a fundamental understanding of the gas sensing mechanism for NO and NO2 . Phys. Chem. Chem. Phys. 18, 31566–31578 (2016).10.1039/C6CP05433A ↗
37. Nazir, S., Singh, N. & Schwingenschlögl, U. Charge transfer mechanism for the formation of metallic states at the KTaO3/SrTiO3 interface. Phys. Rev. B 83, 113107 (2011).10.1103/PhysRevB.83.113107 ↗
38. Noguera, C. & Goniakowski, J. Oxide materials at the two-dimensional limit. Springer Ser. Mater. Sci. 234, 201–231 (2016).10.1007/978-3-319-28332-6_7 ↗
39. Mundy, J. A., Hikita, Y., Hidaka, T., Yajima, T., Higuchi, T., Hwang, H. Y., Muller, D. A. & Kourkoutis, L. F. Visualizing the interfacial evolution from charge compensation to metallic screening across the manganite metal–insulator transition. Nat. Commun. 5, 3464 (2014).10.1038/ncomms4464 ↗