From NaGa(IO<sub>3</sub>)<sub>3</sub>F to NaGa(IO<sub>3</sub>)<sub>2</sub>F<sub>2</sub> and NaGa(IO<sub>3</sub>)<sub>4</sub>: The Effects of Chemical Substitution
between F<sup>–</sup> Anions and IO<sub>3</sub><sup>–</sup> Groups on the Structures
and Properties of Gallium Iodates
Introducing F<sup>–</sup> anions
or substituting
F<sup>–</sup> anions with IO<sub>3</sub><sup>–</sup> groups has been proven
to be ideal strategies for designing novel noncentrosymmetric (NCS)
and polar materials, yet systematic investigation into the effect
of F<sup>–</sup> anions or the substitution of IO<sub>3</sub><sup>–</sup> for F<sup>–</sup> anions on structures
and properties remains rarely explored. Herein, two new gallium iodates,
NaGa(IO<sub>3</sub>)<sub>2</sub>F<sub>2</sub> (<b>1</b>) and
NaGa(IO<sub>3</sub>)<sub>4</sub> (<b>2</b>), were successfully
designed and synthesized based on NaGa(IO<sub>3</sub>)<sub>3</sub>F by introducing more F<sup>–</sup> anions and replacing F<sup>–</sup> anions with IO<sub>3</sub> groups, respectively. Structurally,
in compound <b>1</b>, the adjacent [GaF<sub>3</sub>(IO<sub>3</sub>)<sub>3</sub>]<sup>3–</sup> polyanions are connected in an
antiparallel manner, resulting in a complete cancellation of local
polarity. While in compound <b>2</b>, all IO<sub>3</sub> groups
in 2D [Ga(IO<sub>3</sub>)<sub>4</sub>]<sub>∞</sub><sup>–</sup> layers are aligned, leading to large macroscopic polarization. Additionally,
chemical substitution also results in a qualitative improvement in
the functional properties of compound <b>2</b>. It possesses
strong SHG response (12 × KDP @1064 nm) and broad optical transparency,
coupled with large birefringence (0.21 @1064 nm), showcasing its promise
as a promising nonlinear optical (NLO) crystal. The effects of chemical
substitution between F<sup>–</sup> anions and IO<sub>3</sub><sup>–</sup> groups on the structures and properties are discussed
in detail.