This letter demonstrates non-universality of vibrational density of states in glasses, suggesting implications for non-phononic excitations.
In a recent paper E. Lerner and E. Bouchbinder, Phys. Rev. E { 111}, L013402 (2025) raised concerns regarding the validity of the theory and the interpretation of the data, presented in our previous study on non-phononic vibrational excitations in glasses, W. Schirmacher { et al.}, Nature Comm. { 15}, 3107 (2024). In that work, we presented evidence suggesting that the commonly observed low-frequency regime of the non-phononic vibrational density of states (DoS) is, in fact, highly dependent on technical aspects of the molecular dynamics simulations employed to compute the DoS. Specifically, we showed that the ω⁴ scaling results from the use of a tapering function applied to ensure continuity of the interaction potential at the cutoff distance. In this letter we report further evidence in favor of our previous findings, namely the non-universality of the ω⁴ DoS scaling, and the existence of an important class of non-phononic excitations in glasses, which we call defect states, and are induced by frozen-in stresses. These modes can be classified as quasi-localized.
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