In this study, we investigated the resistive switching (RS) behavior of Pt/Nb-doped SrTiO 3 (Pt/Nb:STO) single-crystal junctions in air and vacuum. We performed steady-state electrical characterizations: the direct current (DC) current-voltage relationship and relaxation current-time dependence under an applied voltage step. The ideality factor of the junction suggested the existence of interface states and tunneling current. We observed that the relaxation current followed the Curie-von Schweidler law; electrical conduction was dominated by a space-charge-limited current based on charge recombination at the interface states. The dynamic electric response was obtained using an alternating current (AC) conductance technique. The carrier lifetime at the interface traps was largely dependent on the resistance state and the ambient environment. Thus, surface potential modification by charge capture/release at the interface traps played a crucial role in the RS of our junctions. Additionally, the ambient effect showed that oxygen desorption (adsorption) at the Nb:STO surface increased (decreased) the interface state density. Finally, an RS model based on interface states in Pt/Nb:STO was proposed.Many investigations have studied the resistive switching (RS) phenomena of thin-film and single-crystal metal oxides. 1-17 Schottky junctions composed of conducting electrodes and Nb-doped SrTiO 3 (Nb:STO) single crystals often exhibit strong rectifying transport characteristics, accompanied by a large hysteresis, i.e., bistable RS nature, without the need for any initial forming process. 8-17 Such single-crystal-based systems have less ambiguity in their transport properties, whereas thin films (mostly polycrystalline) present complications originating from the samples' microstructure and chemical imperfections. 1-7 Several models have been put forward to explain the RS memory effects. Coupled electron-ion dynamics is believed to play a key role in many of these models. As widely accepted, the migration of oxygen vacancies under the influence of an electric field is similar to the behavior of mobile dopants, in that the local conductivity and potential profile at the interface are affected, resulting in the formation of bi-stable resistance states. The resulting vacancy clusters often form localized conducting paths to induce RS (i.e., 'conducting filaments'). 1-6 Fujii et al. 8 discussed variations in the Schottky barrier height (SBH) from charge carriers trapped at interface states as the origin of RS. Shang et al. 9 reported little change in the SBH; however, the resistance states of their RS junctions were affected by trap-assisted tunneling. Lee et al. 10 reported that local barrier height fluctuations depend on the resistance state; however, the mean SBH is nearly constant, as indicated by internal photoemission spectra. Li et al. 11 claimed that SBH inhomogeneity and deep levels in the depletion layer play a crucial role in RS. Recently, Buzio et al. 12 and our research group 13 examined the effect of ambient condit...