Although, as part of a general phenomenon, the piezoelectric response of Ba(Ti 1-y M y )O 3 (M= Zr, Sn, Hf) increases in the vicinity of the orthorhombic (Amm2) -tetragonal (P4mm) and orthorhombic (Amm2)-rhombohedral (R3m) polymorphic phase boundaries, experiments in the last few years have shown that the same phase boundaries show significantly enhanced weakfield piezo-properties in the Ca-modified variants of these ferroelectric alloys, i.e., (Ba,Ca)(Ti, M)O 3 . So far there is a lack of clarity with regard to the unique feature(s) which Ca modification brings about that enables this significant enhancement. Here, we examine this issue from a structural standpoint with M = Sn as a case study. We carried out a comprehensive comparative structural, ferroelectric and piezoelectric analysis of the Amm2 phase in the immediate vicinity of the P4mm -Amm2 phase boundaries of (i) Ca-modified Ba(Ti,Sn)O 3 , as per the nominal formula (1-x)BaTi 0.88 Sn 0.12 O 3 -(x)Ba 0.7 Ca 0.3 TiO 3 and (ii) without Ca modification, i.e. Ba(Ti 1-y Sn y )O 3 . We found that the spontaneous lattice strain of the Amm2 phase is noticieably smaller in the Ca-modified counterpart. Interestingly, this happens alongwith an improved spontaneous polarization by enhancing the covalent character of the Ti-O bond.Our study suggests that the unique role of Ca-modification lies in its ability to induce these seemingly contrasting features (reduction in spontaneous lattice strain but increase the polarization). *