With a dramatically increasing demand for electric vehicles (EVs), a driving range of minimum 300 miles is a must to satisfy the market requirement. Such a demand has motivated enormous efforts focused on the development of high-Ni layered oxide cathodes (LiNi1 −xMxO2 with M = Mn and Co and (1 − x) > 0.9). However, degradation of the electrode–electrolyte interphase, which is a major cause for poor cycle life, remains as a critical problem that hinders their widespread application, especially when the voltage exceeds the HOMO (highest occupied molecular orbital, ≈ 4.3 V vs. Li/Li+) of the organic carbonate electrolytes used. Specifically, the parasitic electrolyte decomposition occurs on the charged cathode surface, resulting in the formation of cathode–electrolyte interphase (CEI) with complicated surface chemistry. Moreover, the surface degradation on cathode usually involves active mass dissolution, which is a common phenomenon in various cathodes. Subsequently, the dissolved transition-metal ions reach the anode side through chemical crossover and poison the anode–electrolyte interphase (AEI) on the graphite surface. Thus, understanding the chemical and electrochemical reactions between the electrode and electrolyte, which influences the composition, microstructure, and chemical properties of the formed electrolyte–electrolyte interphases (EEIs), is crucial to establishing high-energy-density Li-ion batteries with long, stable service life. Herein, with an ultrahigh-Ni layered oxide (LiNi0.94Co0.06O2) as a model cathode and lithium bis(oxalate) borate (LiBOB) as a model electrolyte additive, the EEI chemical and physical property changes on both the cathode and anode are elucidated. Moreover, the layered architecture of the CEI and AEI at the nanometer scale is revealed by time-of-flight secondary ion mass spectrometry (TOF-SIMS) and the correlation between CEI and AEI properties is illustrated. On a chemical perspective, the tuned EEIs are configured with B x O y species and less ethylene carbonate/LiPF6 decomposition products, which endows the CEI with extreme robustness against electrochemical abuse and better Li-ion diffusivity within both the CEI and AEI. Moreover, it reveals that the modification of the surface chemistry on the cathode side would beneficially change the physical stacking behavior of components on the AEI. AEI is reconstructed from a thick “three-layer” architecture (F-enriched exterior layer, O-dominating intermediate layer, and Li-containing interior layer) to a thin “two-layer” architecture (O-enriched exterior layer and Li-dominating interior layer), benefiting from the B x O y enrichment within the EEI. As a result, superior electrochemical performance is achieved by manipulating the electrode surface chemistry even under a moderately high operating voltage (4.4 V vs Li/Li+), and the capacity retention is greatly increased from 61 to 80% after 500 cycles in a full cell assembled with graphite anode. Figure 1