We study the transport through a quantum dot subject to a randomly fluctuating potential, generated by a sequence of pulses in the gate voltage with the help of the autoregressive model. We find that the tunneling current is multistable when the fluctuating potential with a finite correlation time is applied before the non-equilibrium steady state is built up. The non-equilibrium stationary current is heavily dependent on the history of the fluctuating potential during the transient period if the potential has a finite correlation time. Furthermore, the averaged current over the path of the fluctuating potential is a function of its strength and correlation time. Our work therefore provides a robust theoretical proposal for the controlling of the non-equilibrium stationary current through a quantum dot in a randomly fluctuating potential.Introduction.-The study of the electronic transport in mesoscopic systems is one of today's most active research areas in condensed matter physics. A typical currentcarrying system comprises of two electron reservoirs of different temperatures or chemical potentials, between which the electrons continuously flow [1]. Whether the stationary current is uniquely determined by the temperatures and chemical potentials of the reservoirs is a fundamental problem in the quantum transport [2][3][4][5][6][7][8].One of the simplest models that can carry a nonequilibrium stationary current is the resonant level model, typically describing the coherent transport through a nanostructure [9], e.g., a quantum dot made from the semiconductor heterostructure. In the wide band limit, the tunneling current I as a function of the voltage bias V is well known to be I = (Γ/π) arctan[V /(2Γ)] at zero temperature [10], independent of the initial conditions, where Γ denotes the level broadening. In recent years, the transport through nanostructures subject to time-dependent potentials, called the driven quantum transport, attracted much attention [11][12][13][14][15][16][17][18][19][20][21]. In these studies, a deterministic driving, especially a time-periodic one, is used, in which the Keldysh formalism, the Floquet approach, or the transfer matrix approach can be applied (see Ref. [12] for a review of methods). However, little is known about the non-equilibrium stationary current when the level position of a quantum dot fluctuates randomly in time, which can be caused by the interactions between the electrons in the dot and the phonons in the environment [22] or by a manually generated fluctuating potential.The effect of the electron-phonon interaction on the electron transport has been discussed recently by several authors [6][7][8]23], while there is still controversy on the existence of the multistability of the stationary currents.