characteristics. Thus, tuning elements can be coordinated with the resonator. On the other hand, these methods do not work for the random laser system due to the absence of a periodic cavity. The simplicity and randomness set a hurdle for controlling random lasers. However, several approaches have been proposed to break through the bottlenecks. Here, we classify related studies into four main categories: wavelength manipulation, mode control, directional confinement, and threshold abatement. Wavelength manipulation is one of the most crucial parts of random lasers. There are two kinds of tuning designs, which are known as preprocess and postprocess, respectively. The tuning strategies of preprocess include modifying the absorption condition, [21,22] the size of scatterers, [23] and the geometry of photonic crystals. [24] Besides, external parameters such as optics, [25] electricity, [26] temperature, [27][28][29] and deformation, [30] can realize wavelength tunability after the fabrication of disordered nanostructures, so called postprocess. Further, people drive persistent endeavors to control the random lasing modes. Mode-locking and single-mode random lasers, the longstanding scientific goals, have been demonstrated by the pumping scheme, [31] Raman gain, [32] intentional defect sites, [33] and bioinspired photonic structure. [34] Modetransition can also be accomplished by altering the pumping condition, [35] modulating the concentration of gain media or scatterers, [36,37] and the mechanically induced reformation. [38] Although inherent angle-free emissions of random lasers are useful for some specific applications, a directional output is also highly desired. Several directional confinements have been introduced into random lasing systems such as low-dimensional cavities, [29,39] optical waveguides, [40,41] and customized pump profiles. [42] The strategies for lowering the lasing threshold have been extensively studied, e.g., optimization of the mean free path and particle size [43,44] or fine-tuning the concentration or refractive index between scattering and gain media. [45,46] In addition, fluorescence resonance energy transfer and surface plasmon resonance have also been highly addressed. [47][48][49] Here, a simple and straightforward design of magnetically controllable random lasers (MCRLs) is presented. Stilbene 420 laser dye, titanium dioxide nanoparticles (TiO 2 NPs), and ferrous ferric oxide nanoparticles (Fe 3 O 4 NPs) are chosen to compose the MCRLs. Stilbene 420 laser dye is selected from various laser dyes as the gain media because of its exceptional Toward practical applications of random lasers, controllability is a key factor. Here, magnetically controllable random lasers (MCRLs) are designed, fabricated, and demonstrated. Under a prescribed magnetic field, the MCRLs composed of stilbene 420 laser dye, TiO 2 nanoparticles, and Fe 3 O 4 nanoparticles possess magnetic controllability and switchability with good responsivity and durability. The applied magnetic field can be used to manipulate t...