Light-induced switching and manipulation of the magnetization in magneto-optical (MO) materials has enjoyed continuous growing interests due to its potential alluring applications, such as all-optical magnetic recording/storage, [1][2][3][4] magnetic resonance microscopy, [5,6] atom trapping, [7,8] and magnetic holography, [9,10] among other feats. In particular, according to the prediction by International Data Corporation, the total data amount generated globally will reach up to 160ZB (1ZB ¼ 10 12 GB) by the year 2025. [11,12] Such a vast quantity of data elicits an urge to develop bran-new magnetization-based storage technologies. In these contexts, the inverse Faraday effect (IFE) first pioneered in the 1960s has revived as a mainstream leading mechanism giving insights into diverse optomagnetic phenomena, [13][14][15] principally because the light fields tailored either by amplitude/ phase/polarization modulator or by spin/ orbital angular momentum generator could couple strongly with the engineered magnetic systems. [16][17][18][19][20][21] Whereupon a variety of light-triggered subdiffraction-scale versatile magnetization fields with tunable polarization orientations and exotic spatial textures can be achieved by leveraging the canonical IFE, which holds the key for most applications, especially for high-density and low-energy consumption optomagnetic storage. Unlike the circularly polarized beam excitation, [22,23] the well-engineered vectorial beams under tight focusing are able to produce not only purely longitudinal subdiffractionlimited magnetization but also high-purity transverse magnetization, [24,25] which would foster vast opportunities for