surface, have attracted tremendous interests in wide variety of applications such as self-cleaning, [2,3] chemical shielding, [4] corrosion resistance, [5] water energy harvesting, [6][7][8][9] membrane separation, [10] and lab-on-chip devices. [11,12] As such, superomniphobic surfaces have been fabricated on numerous substrates such as metals, polymers, glass, and paper. [13][14][15][16][17][18][19][20][21][22][23][24] Among these, paper-based superomniphobic surfaces are of great importance because paper is flexible, inexpensive, lightweight, breathable, and recyclable. However, prior reports [25][26][27][28][29][30][31] that relied on tuning the inherent heterogenous texture of papers to achieve superomniphobicity have failed to demonstrate low roll-off angle (or low contact angle hysteresis, indicative of negligible solidliquid adhesion) with low surface tension liquids. [32] To overcome this issue, in this work, we developed a superomniphobic paper through a simple technique of growing nanofilaments on the microfibers of the paper. Unlike prior work, [16,21,[33][34][35] our superomniphobic paper displays very low roll-off angle, indicative of ultra-high droplet mobility, even with low surface tension liquids (e.g., n-hexadecane). Further, the required hierarchical texture is formed using a grow-from approach on inherent microfibers of the paper, without noticeably altering the microscale features (i.e., diameter and distance of the microfibers). We also developed a facile method to control the motion and adhesion of the droplets on the superomniphobic paper. Utilizing the liquid mobility in a controlled manner on our superomniphobic papers, we fabricated a simple on-paper pH sensor. We envision that due to simple fabrication technique, flexibility, lightweight, breathability, selective permeability, and ultra-high droplet mobility, our superomniphobic papers will have numerous applications including lab-on-paper devices, water-oil separation, and devices (e.g., water drones and microrobots) with enhanced weight-bearing capacity.When a liquid droplet contacts a nontextured (i.e., smooth) solid surface, it displays an equilibrium (or Young's) contact angle θ Y at triple-phase contact line. [36] Whereas, if the droplet contacts a textured solid surface, it displays an apparent contact angle θ * and adopts either the Wenzel (or fully wetted) state [37] or the Cassie-Baxter state [38] to minimize its overall free energy. In the Cassie-Baxter state, which is preferred for designing super-repellent surfaces, an air layer is trapped between the surface texture and the contacting liquid droplet.