Free choice of splitting ratio is one of the main properties of a power splitter required in integrated photonics, but conventional multimode interference (MMI) power splitters can only obtain a few discrete ratios. This Letter presents both numerical and experimental results of an arbitrary-ratio 1 × 2 MMI power splitter, which is constructed by simply breaking the symmetry of the multimode region. In the new device, the power splitting ratio can be adjusted continuously from 100∶0 to 50∶50, while the dimension of the multimode section stays in the range of 1.5 × 1.8-2.8 μm. The experimental data also indicate that the proposed arbitrary-ratio splitter keeps the original advantages of MMI devices, such as low excess loss, weak wavelength dependence, and large fabrication tolerance. [5,6], and ladder-type optical filters [7]. However, the conventional MMI power splitter with two output ports can only obtain splitting ratios of 100∶0, 85∶15, 72∶28, and 50∶50 through adjusting the position of input and output ports [8,9]. Several methods have been reported aiming at an arbitrary-ratio MMI power splitter, such as butterfly-like MMI splitters [10], bent MMI splitters [11,12], MMI with computer-generated planar holograms [13,14], cascaded MMI couplers with unequal width [15][16][17], MMI splitter with cladding-filled gap [18], and multiple-arm MZI consisting of an active phase-shifting region placed between two MMI couplers [19]. However, all these methods suffer from relatively complex structures and large footprints. In this Letter, we propose and experimentally demonstrate a compact arbitrary-ratio 1 × 2 power splitter based on a simple asymmetric MMI structure. The schematic of the conventional symmetric 1 × 2 MMI power splitter is shown in Fig. 1(a). TE-polarized light is, through the single-mode input waveguide (WG in ), transmitted to the multimode region, where MMI is excited. Then, the light is tapered into two single-mode output waveguides (WG up and WG bot ) symmetrically at the first two-fold image distance. Due to the structural symmetry, the splitter only allows uniform split of the incident light into two output waveguides, as indicated in the energy flux density Even though these corners contain little optical field, removing one of them will break the symmetry of interference, in accordance with the self-imaging principle [20]. Such asymmetric MMI, excited by asymmetric perturbation in the multimode region, will have a significantly different optical field distribution.The proposed asymmetric MMI power splitter is shown in Fig. 1(b). Compared to the conventional symmetric power splitter, the only difference is that the symmetry of the multimode region is broken by removing its bottom left corner (marked with a red dashed rectangle). Such a minor structural change causes a dramatic redistribution of the optical field [ Figs. 1(e), 1(f), 1(i), and 1(j)]. If the output waveguides are also located at the position of the first two-fold image, the power output from WG up will be greater than that from WG ...