Understanding the cracking behavior of oxide glasses under sharp contact is challenging due to not only the complicated stress field in the samples, but also the composition dependence of the mechanical behavior of glasses. [1][2][3] Characterized by the cracking pattern and the dominant plastic response under the indentation experiment, glass compositions can be roughly classified as anomalous glasses (e.g., pure silica), normal glasses (e.g., most silicate glass), and intermediate glasses (e.g., N-BasF from SCHOTT). The anomalous glasses exhibit cone cracking under the indentation experiment, where the plastic response is dominated by densification. In contrast, normal glasses feature radial-median cracking and apparent pile-up which results from plastic flow. 1,2 It has been shown that this difference in the mechanical response to indentation can be ascribed, at least in part, to the glass's Poisson ratio: densification is preferred in glasses with relatively low Poisson's ratio while the plastic flow is preferred in glasses with high