The X-site ion in organic-inorganic hybrid ABX 3 perovskites (OHPs) varies from halide ion to bridging linkers like HCOO À ,N 3 À ,NO 2 À ,and CN À .However,nonitrite-based OHP ferroelectrics have been reported so far.N ow,b ased on non-ferroelectric [(CH 3 ) 4 N][Ni(NO 2 ) 3 ], through the combined methodologies of quasi-spherical shape,h ydrogen bonding functionality,a nd H/F substitution, we have successfully synthesized an OHP ferroelectric, [FMeTP][Ni(NO 2 ) 3 ] (FMeTP = N-fluoromethyl tropine). As an unprecedented nitrite-based OHP ferroelectric,t he well-designed [FMeTP]-[Ni(NO 2 ) 3 ]u ndergoes the ferroelectric phase transition at 400 Kwith an Aizu notation of 6/mmmFm, showing multiaxial ferroelectric characteristics.T his work is ag reat step towards not only enriching the molecular ferroelectric families but also accelerating the potential practical applications.Molecular ferroelectrics with cheap,l ightweight, flexible, wearable,a nd environmentally benign characteristics have been amajor research topic in the past decades owing to the potential applications in data storage,p iezoelectric sensors, actuators,a nd nonlinear optical devices. [1] It is their intrinsic structure-property flexibility that brings forth particular interest for molecular design towards new materials with satisfactory ferroelectric performance near or even above room temperature. [2] Nevertheless,d iscovering ar eliable method to control the ordered organization of molecules into apolar lattice and thereby modulate ferroelectricity is an imminent ongoing challenge.R ecently,s everal design strategies involving the selection of molecular building blocks have been developed. [1b,c] Fore xample,t he Zn 2+ /Dy 3+ Schiff base antenna complex and the lower-symmetric quasi-spherical cations modified from the spherical [(CH 3 ) 4 N] + ,1 ,4diazabicyclo[2.2.2]octonium (dabco), or quinuclidinium were found to be promising for constructing molecular ferroelectrics with high Curie point (T c ). [3] Accordingly,w eh ave obtained several outstanding organic-inorganic hybrid perovskite (OHP) ferroelectrics with ageneral formula ABX 3 (A is an organic cation, Bi sametal, and Xi susually halides), such as [(CH 3 ) 3 NCH 2 Cl]MCl 3 (M = Mn, Cd) and [MeHdab-co]RbI 3 ,where the structural transitions arise mainly from the dynamic motions of the A-site moieties. [3b, 4] Remarkably,b y extending the X-site from monatomic anions to bridging linkers like HCOO À , [5] N 3 À , [6] NO 2 À , [7] and CN À , [8] aw ide range of larger and longer organic cations can be accommodated for enriching the OHP families and inducing abundant properties such as ferromagnetism and antiferromagnetism. Fort he classical pseudohalide NO 2 À ,o nly two kinds of inorganic ferroelectrics have been reported, NaNO 2 and MCd(NO 2 ) 3 (M = NH 4 ,K,Rb, Cs,Tl), [9] whereas there are no nitrite-based ferroelectrics in the OHPs.I nt his way,t he earlier work of non-ferroelectric [(CH 3 ) 4 N][Ni(NO 2 ) 3 ], adopting at rigonal centrosymmetric space group P3 m1a t room temper...