Recently, investigation of metasurface has been extended to nonreciprocity through breaking time-reversal symmetry. Among a number of magnetless strategies, nonlinearity is an important nonreciprocal principle amenable to the metasurface. As passive analog-based devices, most of the existing nonlinear nonreciprocal metasurfaces are inherently characterized by the relatively unchangeable performance, sharp frequency response, and hysteresis loops. Here, an analog-digital-analog mechanism is proposed to realize the nonlinear nonreciprocity, which provides a digitally reconfigurable solution for a family of nonreciprocal performance within a shared hardware architecture. This concept is validated by a metasurface prototype with the integration of a digital module at microwave frequencies. Based on the proposed mechanism, the properties can be customized as demanded, ranging from a normal reciprocal response to a variety of nonreciprocal functions, including electromagnetic (EM) diode and EM unidirectional limiting functions, which have been experimentally demonstrated with direction reversibility and threshold tunability. The proposed metasurface is also underpinned by the nonhysteretic performance and wide operating bandwidth, thereby potentially making it an inexpensive and stable candidate for advanced manipulations of EM waves.A normal transparent metasurface, if not particularly designed, is restricted to the time-reversal symmetry. It means that its transmission properties remain the same if the sign of the time variable is flipped. It is equivalent to the "reciprocity," which means that the received-transmitted field ratios are identical when the sources and detectors are exchanged. [14] In other words, the transmission rates experienced by EM waves propagating through the metasurface from opposite sides are identical. Breaking the time-reversal symmetry or reciprocity is significant in some scenarios where transmission asymmetry is in demand. A conventional method for this purpose is to use gyrotropic materials in the presence of a static magnetic field, [15,16] but it is nonamenable to metasurfaces due to the shortcomings like bulky size, large weight, and significant loss of the system. [17] Therefore, a large number of investigations were conducted for magnetless nonreciprocal metasurfaces. Besides the popular timemodulation methods, [17][18][19][20] nonreciprocal metasurfaces were realized by loading artificial subwavelength structures with unidirectional active elements, such as field-effect transistor [21,22] and amplifier, [23,24] which mimicked the Faraday rotation without ferromagnetic materials or magnetic fields. A threelayer surface-circuit-surface configuration integrated with transistor-based amplifiers was proposed to achieve a nonreciprocal metasurface for linear-polarized waves. [25] In addition, a spatially dispersive metasurface was found to be self-biased by transverse momentum of the incident wave front, leading to nonreciprocal phenomena. [26] Apart from the above linear methodologies, ...