electrical control of the respective materials' SHG properties. Highly interesting as efficient large bandgap SHG materials are borates like KBBF, i.e., KBe 2 BO 3 F 2 , providing a layered structure. [10] According to these the coplanar configuration of the non-centrosymmetric building units promotes birefringence and SHG. Moreover, the weak ionic interactions mediated via K + -F − contacts between adjacent [Be 2 BO 3 F 2 ] layers strengthen its layer habit further. Recently, with Cs 3 Zn 6 B 9 O 21 (CZB) [11] within the same family of compounds another highly promising borate was presented, both of special interest because of their large bandgap allowing SHG also in the UV regime. A close relative to KBBF is Sr 2 Be 2 B 2 O 7 (SBBO), [12] comprising [Be 2 (BO 3 ) 2 O] layers. Both materials contain beryllium which is not favored in applications due to the high toxicity of Be 2+ ions.Fluorooxoborates should comprise sufficiently large bandgaps in the UV as well as preferential formation of non-centrosymmetric structures, thus making them ideal candidates for SHG materials in the UV. Beyond that, they normally combine the birefringence promoting triangular BO 3 or tetrahedral BO 3 F moieties providing terminal fluorine atoms with a proclivity for weak coordination. [13][14][15][16][17][18][19][20][21][22][23][24][25][26] Recent calculations [27] as well our own results [28] confirm these considerations and suggest a boost for NLO materials based on so-called fluorooxoborates.Apparently, nature normally strives for high symmetry, and therefore-from a solid state chemists point of viewnon-centrosymmetric structures are facilitated by the presence of suited basic building blocks like the mentioned triangular or tetrahedral ones. But frequently, also these are arranged centrosymmetrically in a crystal structure. Our approach therefore uses as second driving force the choice of such basic building Herein, the crystal structure as well as second-harmonic-generation (SHG), thermal and spectroscopic properties of Sn[B 2 O 3 F 2 ] (TFB = tin-fluorooxoborate) are presented. TFB adopts a novel non-centrosymmetric crystal structure, which is determined by single-crystal X-ray diffraction (XRD) (P31m, Z = 1, a = 4.5072(2) Å, c = 4.7624(3) Å) and comprises [B 2 O 3 F 2 ] 2− layers consisting solely of BO 3 F tetrahedra; the covalent BF bonds are unequivocally localized via solid-state NMR spectroscopy as well as density functional theory (DFT) calculations. TFB is insensitive to air and moisture, shows a stronger SHG intensity than K[H 2 PO 4 ] (KDP) and a bandgap of ≈5 eV. The thermal decomposition yields two new borate fluorides.