However, limited by the finite periodic system, or fabrication errors, such as the roughness or the incline of the sidewall of holes in photonics devices, [7] radiative loss is hardly suppressed and only the quasi-BICs with finite radiative lifetime can be actually observed, exhibiting a Fano resonance in the scattering spectrum. [8] Such inevitable imperfections will hinder the development of high-Q on-chip photonic devices. [9,10] In recent years, merging BIC, as an efficient approach, is proposed to address this challenge, which originates from moving several BICs near the same spatial frequency in the momentum space. [11] The merging BICs can not only suppress the radiative losses of one eigenmode but also suppress surrounding resonances to achieve the high radiative Q-factor in a relatively broader range of spatial frequency, reducing the susceptibility of the structure, which makes them more robust to external perturbations. The numerical and experimental results of merging BIC at the Γ point on PC slabs were initially demonstrated in 2019, where the Q-factor was 12 times higher than the isolated BICs. [11,12] Following this design, an ultralow-threshold laser using merging BIC was proposed to explore its practical application in nanophotonics. [13] Besides, merging BIC at the off-Γ point was investigated in PC slab as well, which is constructed by a Friedrich-Wintgen BIC and an accidental BIC. [14] However, all the above approaches to generating merging BICs rely on controlling the geometric parameters of the structure including thickness or period, [11][12][13][14] which cannot dynamically tuned once the pattern is settled, thus limiting its reconfigurable performance of on-chip integrated photonic devices.