The introduction of manganite buffer layers, La7/8Sr1/8MnO3 (LSMO) in particular, at the metallic interface between SrTiO3 (STO) and another band insulator suppresses the carrier density of the interfacial two-dimensional electron gas (2DEG) and improves significantly the electron mobility. However, the mechanisms underlying the extreme mobility enhancement remain elusive. Herein, we used 18 O isotope exchanged SrTi 18 O3 as substrates to create 2DEG at room temperature with and without the LSMO buffer layer. By mapping the oxygen profile across the interface between STO 18 and disordered LaAlO3 or yttria-stabilized zirconia (YSZ), we provide unambiguous evidence that redox reactions occur at oxide interfaces even grown at room temperature. Moreover, the manganite buffer layer not only suppresses the carrier density but also strongly suppresses the oxygen exchange dynamics of the STO substrate, which likely prevents the reduction of STO during the formation of the 2DEG. The underlying mechanism on the enhanced electron mobility at buffered oxide interfaces is also discussed.Strontium titanate, SrTiO3 (STO), is a representative perovskite-type oxide insulator with a band gap of 3.2 eV. Analogous to silicon for conventional semiconductor electronics, STO is the basis material for oxide electronics. It is by far one of the most widely used substrate materials for the growth of epitaxial oxide thin films due to its structural compatibility to both isostructural perovskites and non-isostructural spinels, fluorites, pyrochlores, and so on. Doped STO with oxygen vacancies or with substitutional elements such as La, Nb or Ta, in its own right, shows a wide range of interesting properties such as metallic conduction with high electron mobility [1] and superconductivity [2]. Besides, STO is also a model system for mixed ionic and electronic conductors at high temperatures, due to the presence of unintentional dopants (typically Fe, Al, and Mn) which act as acceptor type impurities [3]. In recent years, STO has attracted increasing attention for application in oxide electronics as active materials, particularly upon the discovery of a two-dimensional electron gas (2DEG) at the STO surface [4] or its interface with another band insulator, such as perovskite LaAlO3 (LAO) [5] or spinel γ-Al2O3 (GAO) [6].The 2DEG of STO interface to another oxide insulator has drawn extensive attention because of the emergent properties which are not observed in the bulk counterparts, such as 2D superconductivity [7,8], magnetism [9], quantum Hall effect [10], as well as light enhanced field effects [11]. On the