This material bears the advantages of both the fluoride crystallites and the oxide glass matrix. [3] The crystallites have a low phonon energy environment, while the oxide glass matrix possesses both high optical transparency and excellent chemical and thermal stabilities, which are crucial for protecting the fluoride crystallites from reacting with the moisture from the environment. For the oxyfluoride GCs doped with rare earth (RE) ions, the RE ions, which serve as the up-conversion (UC) luminescence centers, preferentially enter the fluoride crystallites, and hence, reduce the rate of nonradiative relaxation, thereby benefiting the UC luminescence. [4] Thus, oxyfluoride GCs are a promising candidate for optical applications such as optical amplifiers, [5] multicolor displays, [6] UC fibers, [7] lasers, [8] and optical thermometry. [9] However, it is a challenge to achieve the oxyfluoride GCs with both high transparency and superior UC luminescence.Usually, the optical transmittance of the oxyfluoride GCs is lower than that of their corresponding precursor glass since the former has stronger optical absorption and light scattering It is known that the optical transparency of an oxide glass decreases with an increase in the size and fraction of crystals in the glass during heat-treatment. Here, the authors report an opposite scenario, where a translucent Er 3+ −Yb 3+ doped oxyfluoride precursor glass-ceramic (P-GC) becomes transparent with increasing crystal size and crystallinity. Specifically, in the heat-treated P-GC samples, the authors observe that the growth of the existing Ba 2 LaF 7 crystals and particularly the formation of small spherical Ba 2 LaF 7 crystals greatly enhanced the light transmittance. To reveal the origin of this anomalous pheno menon, the authors perform detailed morphology and structure analyses on both P-GC and the heat-treated P-GC samples and molecular dynamics simulations of the precursor glass. The results show that the composition of the residual glass phase is altered (e.g., depletion of La 3+ ) in the way that the differences in refractive index between the glass matrix and the crystals are greatly reduced. As a consequence, the light scattering of the heat-treated P-GC is suppressed, and hence, the derived P-GC becomes transparent. In addition, a proper heat-treatment can also enhance the luminescence of the studied P-GC system.