Piezoelectric charge coefficient (d33) and piezoelectric voltage coefficient (g33) are the two most critical parameters that define output performance of piezoelectric nanogenerators (PNGs). Herein, we propose a vacancy-ordered double perovskite of TMCM2SnCl6 (where TMCM is trimethylchloromethyl ammonium) with a large d33 of 137 pC/N and g33 of 980 ×10 -3 V•m/N. The 5 Piezoelectric nanogenerators (PNGs) have been emerging as a promising power source for self-1 powered electronics owing to their direct power conversion from mechanical to electrical energy. [1][2][3][4][5] To maximize the output power of PNGs, both the d33 and g33 of the piezoelectric host are 3 important, which determines the output current (Isc=(d33×ΔF)/Δt, where ΔF is the applied force and Δt is the time) and voltage (Voc=g33×ΔP×L, where ΔP is the applied pressure and L is the original film thickness), respectively. [6][7][8][9] In the past decade, a wide range of piezoelectric materials, targeting high g33 or d33, have been synthesized for the efficient PNGs. For example, the organic polyvinylidene fluoride (PVDF) possesses a high g33 (~286 ×10 -3 V•m/N), leading to a high output piezoelectric voltage. Unfortunately, the resultant current is limited due to its relatively-low d33 (~30 pC/N). [10][11][12][13] Conversely, inorganic perovskite oxide ceramics, including PbZrxTi1-xO3 (PZT) and BaTiO3 (BTO), exhibit a high d33 (>100 pC/N) but their g33 is rather low (~20 ×10 -3 V•m/N). [14][15][16][17][18] Considering the relation between d33 and g33 (g33=d33/(ε0×εr)), where εr is material relative 12