“…Phase manipulation of electromagnetic (EM) waves has been widely applied in imaging, materials science, and communications. [1][2][3][4][5][6][7][8][9] Such as, dispersive phase control is DOI: 10.1002/adom.202301258 applied to wave-cloaking at the terahertz band, [4] an optical metabroadcasting communication system is proposed by employing the phase-modulated metasurface, [9] Traditionally, phase was controlled via wavevector methods such as lens-shaping, [10] impedance-analysis, [11] and the Huygens principle, [12] Recently, based on the Pancharatnam-Berry (P-B) phase, [13] of spin angular momentum (SAM), the rotation phase of circularly-polarized (CP) waves is characterized and applied in metasurface research, which has been a focused topic of EM research, [14][15][16][17][18] However, these phase modulation methods exist some limitations, such as, i) They are limited to phase-angle dimensionality, and ii) The rotation phase is inapplicable to linearly-polarized (LP) waves. Furthermore, magnitude and phase were generally deemed as two distinct characters, so that they should be controlled separately.…”