## Abstract

Metallic LaAlO

_{3}/SrTiO_{3}(LAO/STO) interfaces attract enormous attention, but the relationship between the electron mobility and the sheet electron density,*n*, is poorly understood. Here, we derive a simple expression for the three-dimensional electron density near the interface,_{s}*n*, as a function of_{3D}*n*and find that the mobility for LAO/STO-based interfaces depends on_{s}*n*in the same way as it does for bulk doped STO. It is known that undoped bulk STO is strongly compensated with N similar or equal to 5 x 10_{3D}^{18}cm^{-3}background donors and acceptors. In intentionally doped bulk STO with a concentration of electrons*n*<_{3D}*N*, background impurities determine the electron scattering. Thus, when*n*<_{3D}*N*, it is natural to see in LAO/STO the same mobility as in the bulk. On the other hand, in the bulk samples with*n*>_{3D}*N*, the mobility collapses because scattering happens on*n*intentionally introduced donors. For LAO/STO, the polar catastrophe which provides electrons is not supposed to provide an equal number of random donors and thus the mobility should be larger. The fact that the mobility is still the same implies that for the LAO/STO, the polar catastrophe model should be revisited._{3D}Original language | English |
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Article number | 092106 |

Journal | Applied Physics Letters |

Volume | 111 |

Issue number | 9 |

Number of pages | 4 |

ISSN | 0003-6951 |

DOIs | |

Publication status | Published - 2017 |

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