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Table · dataset · 2026

Phase Selectivity in Borate Flux Synthesis Using Refractory Additives

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Here, we report a novel approach to borate flux synthesis in which refractory oxide additives alter reaction phase outcome.

Description

In the absence of refractory additives, reactions of copper oxide and boron oxide flux yielded single crystals of the previously reported Cu<sub>15</sub>(BO<sub>3</sub>)<sub>6</sub>(B<sub>2</sub>O<sub>5</sub>)<sub>2</sub>O<sub>2</sub> (Cu<sub>3</sub>B<sub>2</sub>O<sub>6</sub>), containing solely trigonal planar-coordinated borate monomers and dimers.

Addition of TiO<sub>2</sub> led to the discovery of a novel structural prototype Cu<sub>7–<i>x</i>+<i>y</i></sub>Ti<sub><i>x</i></sub>(BO<sub>3</sub>)(B<sub>2</sub>O<sub>5</sub>)(B<sub>3</sub>O<sub>7</sub>)O (Cu<sub>7–<i>x</i>+<i>y</i></sub>Ti<sub><i>x</i></sub>B<sub>6</sub>O<sub>16</sub>), which crystallizes in space group <i>P</i>1̅, with <i>a</i> = 3.31989(4) Å, <i>b</i> = 10.54906(13) Å, <i>c</i> = 17.9143(2) Å, α = 75.5076(10)°, β = 88.8619(10)°, and γ = 86.7381(10)° for <i>x</i> = 0.276(7), <i>y</i> = 0.0135(15).

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It consists of quasi-2D layers of Cu<sup>2+</sup> cations enclosing trigonal planar borate monomers, dimers, and the uncommon (B<sub>3</sub>O<sub>7</sub>)<sup>5–</sup> trimer. Adjacent layers are connected by oxygen and disordered Cu/Ti sites. In contrast, both ZrO<sub>2</sub> and HfO<sub>2</sub> grew single crystals of the previously reported material CuB<sub>2</sub>O<sub>4</sub> containing solely tetrahedrally coordinated boron in a 3D framework.

Ex situ X-ray μCT imaging of the ZrO<sub>2</sub> reaction shows CuB<sub>2</sub>O<sub>4</sub> crystals growing at the interface of ZrO<sub>2</sub> and the flux, suggesting that ZrO<sub>2</sub> (and by extension, HfO<sub>2</sub>) acts as a heterogeneous nucleation substrate that stabilizes the four-coordinate boron tetrahedra. Magnetization of Cu<sub>7–<i>x</i>+<i>y</i></sub>Ti<sub><i>x</i></sub>B<sub>6</sub>O<sub>16</sub> is reported, showing an antiferromagnetic transition at <i>T</i><sub><i>N</i></sub> = 12.8 K. We then differentiate refractory additives into two distinct classes, flux-resistant and flux-susceptible, with ZrO<sub>2</sub> and HfO<sub>2</sub> as B<sub>2</sub>O<sub>3</sub>-flux-resistant refractory additives and TiO<sub>2</sub> as a B<sub>2</sub>O<sub>3</sub>-flux-susceptible refractory additive.

These results demonstrate that refractory additives can provide a useful handle for directing phase formation and accessing new materials in flux synthesis, and provide challenge cases to benchmark emerging AI models in unconventional materials stabilization and crystal growth methods.

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