Every solid vibrates. In crystals, those vibrations are well understood. Glasses, however, hide an unexpected excess of low-energy vibrations that has puzzled scientists for more than half a century. This excess of low-energy vibrations, known as the boson peak, is one of the longest-standing mysteries in the physics of disordered materials. Despite decades of research, scientists still disagree about its microscopic origin.
Found in almost every type of glass—from ordinary window glass to polymers, metallic glasses and even granular materials—the boson peak influences how these materials store and transport energy. As such, understanding its origin has become one of the central challenges in the physics of disordered materials. Over the years, numerous—and often contrasting—theories have been proposed, yet no single explanation has gained universal acceptance.
A new study brings together evidence from published experiments, the scientific literature and new large-scale computer simulations to argue that the strongest evidence yet points to a common picture: the boson peak is consistently associated with a flat, weakly dispersive vibrational band.
Unlike ordinary sound waves, whose frequency changes with wavelength, this band remains at nearly the same frequency over a broad range of length scales. Instead of propagating like a conventional sound wave, the vibrational spectral weight associated with the boson peak accumulates within a narrow frequency window.

Conceptual illustration of the proposed flat-band perspective. Evidence from experiments and simulations suggests that the boson peak is consistently associated with the accumulation of vibrational spectral weight into a flat, weakly dispersive band.
The researchers reached this conclusion by revisiting experimental observations reported across many different materials and combining them with new simulations of two- and three-dimensional model glasses, as well as new analyses of experimental data from two-dimensional granular packings. Across these remarkably diverse systems, the same vibrational signature emerged again and again.
These findings also provide a powerful new way to evaluate the many competing theories proposed over the past five decades. Some explanations interpret the boson peak primarily as a consequence of ordinary sound waves that become modified, scattered or strongly damped by structural disorder. Others propose that glasses support additional collective vibrational excitations beyond conventional acoustic phonons.
The observed flat, weakly dispersive band is difficult to reconcile naturally the with explanations based solely on modified acoustic phonons, whereas theories that include additional vibrational excitations remain, in principle, compatible with the full set of observations. More broadly, the study establishes a clear benchmark against which future theories can be tested. A successful microscopic description should explain why this weakly dispersive band emerges, why it coincides with the excess vibrational states that define the boson peak, and why its intensity follows the underlying structure of the material. No existing theoretical framework currently explains all of these observations in its present form.
The study also finds that the flat-band signal is predominantly associated with transverse, or sideways, vibrations, although important exceptions such as silica remain to be understood. This raises new questions about the microscopic origin of the band and whether it represents a universal feature of disordered solids.
By significantly narrowing the range of viable theoretical explanations, the work provides a clearer roadmap for future research. After decades of competing ideas, the study provides clearer picture of the key observations that any successful theory of the boson peak must ultimately explain.
The paper is published in Proc. Natl. Acad. Sci. U.S.A. 123 (34) e2534361123, https://doi.org/10.1073/pnas.2534361123 (2026).









