We report on the Cu 1s resonant inelastic X-ray scattering (RIXS) of Cu-O one-dimensional (1D) strongly correlated insulator systems with contrasting atomic arrangements, namely edge-sharing CuGeO 3 and corner-sharing Sr 2 CuO 3 . Owing to good statistics of the high-resolution RIXS data, so far unresolved fine structures are revealed. Detailed photon-energy and momentum dependence of the RIXS spectra in comparison with theoretical calculations has clarified the natures of the low-energy charge excitations and hybridization of the electronic states.PACS Numbers: 78.70.Ck, 71.27.+a, 75.10.Pq Resonant inelastic X-ray scattering (RIXS) is a powerful tool to probe the momentum dependence of low-energy excitations in solids. 1,2 This technique is intriguing to clarify bulk electronic states of strongly correlated insulators, which are under a keen general interest in decades. 3,4,5 For metallic systems, highresolution angle-resolved photoemission (ARPES) is promising to detect their occupied states. Nowadays both surface-sensitive low-energy 6 and bulk-sensitive high-energy 7,8 ARPES measurements are feasible. Compared to ARPES, RIXS is really bulk sensitive and applicable to insulators with high resistivity, where the electron correlation is even stronger. 1,2,5,9 However, high energy resolution RIXS is rather demanding because of their poor count rate. For this purpose, high photon flux in a small spot size and a highly efficient analyzer crystal are required.Here we report photon-energy (hν) and momentum (Δk) dependence of the Cu 1s RIXS with good statistics for two contrasting Cu-O 1D insulating systems CuGeO 3 10 and Sr 2 CuO 3 2 with dominantly divalent Cu. As shown in Fig. 1c, CuGeO 3 has a single chain with the edge-sharing CuO 2 plane configuration with the Cu-O-Cu angle (θ) of 99˚, where the Cu-Cu chain axis is taken as the x-axis and the CuO 2 plane corresponds to the x-y plane. The 3d xy orbital is unoccupied because it has the highest energy among the whole d orbitals according to an extended d-p model calculation. 11,12 The transfer energy between the neighboring Cu 3d sites via O 2p sites is thought to be very small because of the orthogonality of the Cu 3d xy orbitals on the neighboring sites coupled to the O 2p orbitals in the edge-sharing CuGeO 3 . On the other hand, Sr 2 CuO 3 has a single Cu-O chain with the corner-sharing configuration as shown in Fig. 2b. The transfer energy is thought to be large in this case, in which the Cu 3d hole is thought to be in the 3d x 2 -y 2 state. Therefore very different behavior of charge dynamics is expected in these systems.RIXS experiment was performed at BL19LXU of SPring-8 with a 27m long X-ray linear undulator. By use of two channel cut crystal monochromators, the resolution of the incident hν was better than 300 meV. A horizontal focusing was better than 100 µm on the sample. The instrument with 1m Rowland circle was used for the measurement. The total resolution of 400 meV (full width at half maximum) was achieved by using a spherically bent Si(553) ana...