High-field electrical transport and point-contact tunneling spectroscopy were used to investigate superconducting properties of the unique spinel oxide, LiTi 2 O 4−δ films with various oxygen content. We find that the upper critical field B c2 gradually increases as more oxygen impurities are brought into the samples by carefully tuning the deposition atmosphere. It is striking that although the superconducting transition temperature and energy gap are almost unchanged, an astonishing isotropic B c2 up to ∼ 26 Tesla is observed in oxygenrich sample, which is doubled compared to the anoxic sample and breaks the Pauli limit.Such anomalies of B c2 were rarely reported in other three dimensional superconductors.Combined with all the anomalies, three dimensional spin-orbit interaction induced by tiny oxygen impurities is naturally proposed to account for the remarkable enhancement of B c2 in oxygen-rich LiTi 2 O 4−δ films. Such mechanism could be general and therefore provides ideas for optimizing practical superconductors with higher B c2 .In this letter, we present systematic transport measurements and point-contact tunneling spectroscopy study of LiTi 2 O 4−δ films with various oxygen content. For oxygen-rich samples, a significantly enhanced B c2 up to 26 T at low temperatures is observed. Such doubled B c2 , compared with anoxic samples, is isotropic. Intriguingly, superconducting energy gap and T c are almost the same for all samples. Temperature-dependent B c2 can be well fitted by the Werthamer-Helfand-Hohenberg (WHH) theory considering spin paramagnetism and spin-orbit scattering[20], yet it leads to an underestimation of relaxation time for oxygen-rich samples. Here we consider the three dimensional spin-orbit interaction induced by oxygen impurities, which is beyond the WHH theory, thereby giving an universal understanding of the enhancement of B c2 and other anomalies.High-quality LiTi 2 O 4−δ thin films were epitaxially grown on MgAl 2 O 4 (001) substrates by pulsed laser deposition under various oxygen pressures from basic vacuum (< 1 × 10 −6 Torr) to ∼ 5 × 10 −6 Torr [19]. The temperature-and field-dependence of resistance were measured by a standard four-probe method in PPMS-16T, and steady high magnetic field facility with field up to 33 T. Point-contact measurements were performed by employing a homemade probe using Pt/Ir