Title
Bending rigidity, sound propagation and ripples in flat grapheneAuthor
Author (from another institution)
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https://ror.org/000xsnr85https://ror.org/01j9p1r26
https://ror.org/02skytd81
https://ror.org/02be6w209
https://ror.org/042t93s57
https://ror.org/02mw21745
https://ror.org/02d4c4y02
https://ror.org/0042e5975
https://ror.org/02s376052
https://ror.org/05trd4x28
https://ror.org/03t2f0a12
https://ror.org/02e24yw40
Version
http://purl.org/coar/version/c_ab4af688f83e57aa
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© 2024 Springer NatureAccess
http://purl.org/coar/access_right/c_f1cfPublisher’s version
https://doi.org/10.1038/s41567-024-02441-zPublished at
Nature Physics Publisher
Springer NatureAbstract
Many of the applications of graphene rely on its uneven stiffness and high thermal conductivity, but the mechanical properties of graphene—and, in general, of all two-dimensional materials—are still n ... [+]
Many of the applications of graphene rely on its uneven stiffness and high thermal conductivity, but the mechanical properties of graphene—and, in general, of all two-dimensional materials—are still not fully understood. Harmonic theory predicts a quadratic dispersion for the out-of-plane flexural acoustic vibrational mode, which leads to the unphysical result that long-wavelength in-plane acoustic modes decay before vibrating for one period, preventing the propagation of sound. The robustness of quadratic dispersion has been questioned by arguing that the anharmonic phonon–phonon interaction linearizes it. However, this implies a divergent bending rigidity in the long-wavelength regime. Here we show that rotational invariance protects the quadratic flexural dispersion against phonon–phonon interactions, and consequently, the bending stiffness is non-divergent irrespective of the temperature. By including non-perturbative anharmonic effects in our calculations, we find that sound propagation coexists with a quadratic dispersion. We also show that the temperature dependence of the height fluctuations of the membrane, known as ripples, is fully determined by thermal or quantum fluctuations, but without the anharmonic suppression of their amplitude previously assumed. These conclusions should hold for all two-dimensional materials. [-]
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