Amorphous calcium carbonate (ACC) is a precursor to the crystalline phases of CaCO 3 , commonly found in the earliest stages of biomineral development and as one of the metastable states formed during the inorganic precipitation of calcium carbonate crystalline polymorphs. [1] Its isotropic and hydrous moldable character allows many organisms to form very complex conformations of their shells or skeletons by taking advantage of these unique properties. [2] At least two different phases of biogenic ACC have been described to date: a highly hydrated phase with one water molecule per CaCO 3 unit, and an anhydrous phase that forms as a transient phase prior to crystallization to vaterite or calcite. [3,4] Recently, the existence of polyamorphism (the existence of a substance in different amorphous modifications, akin to polymorphism in crystalline materials) in synthetic hydrated ACC has been suggested based mainly on X-ray absorption spectroscopy (XAS) and nuclear magnetic resonance (NMR) data that show different local structures of ACC precipitated from solutions at different pH values: calcite-like ACC is obtained at pH % 8.75 and vaterite-like ACC precipitates from solutions of pH % 9.8 and higher. [5,6] In addition to these two amorphous polymorphs, other studies have shown hints of aragonite local order in ACC from shells of freshwater snails, based on XAS data that show Ca-O coordination numbers of approximately 9, the theoretical value of aragonite. [7,8] These results were reproduced in synthetic samples of ACC doped with Mg 2+ , suggesting a role of this cation in the selection of the ACC amorphous polymorph. [9] Herein we show the existence of pressure-induced polyamorphism in hydrated ACC, and the formation of "aragonitic" ACC upon a decrease of the molar volume. This result suggests a possible mechanism by which Mg 2+ -a cation with smaller ionic radius than Ca 2+ -modifies the local order of ACC to an aragonite-like order by contributing to decrease the molar volume of the amorphous phase. In addition, we report the first values of the bulk modulus and the density of ACC.Experimental structure factors obtained from high-pressure X-ray diffraction experiments and fits to the experimental data using Reverse-Monte Carlo (RMC) modeling are shown in Figure 1 a. The structure factors show the typical broad oscillations of an amorphous solid, with no apparent sign of crystallization within the range of pressures studied. Pressure-induced structural changes can be identified in the diffraction data by looking at the salient feature of the S(Q) function at 11.9 GPa (see small arrow in Figure 1 a), and by plotting the position of the main diffraction peak at Q % 3.3 À1 as a function of pressure (Figure 1 b). A step-like transition is observed that can be fitted with a sigmoidal function centered at P c = 9.8 AE 0.8 GPa. Similar behavior is observed in high-pressure Raman data ( Figure 2; see raw data in Figure S7 and S8). At ambient pressure four peaks are observed: a single peak at 1081 cm À1 corresponding to th...