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Bending rigidity, sound propagation and ripples in flat graphene.pdf (538.0Kb)
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Izenburua
Bending rigidity, sound propagation and ripples in flat graphene
Egilea
Aseginolaza, UnaiORCID
Egilea (beste erakunde batekoa)
Diego, Josu
Cea, Tommaso
Bianco, Raffaello
Monacelli, Lorenzo
Libbi, Francesco
Calandra, Matteo
Bergara, Aitor
Mauri, Francesco
Errea, Ion
Ikerketa taldea
Análisis de datos y ciberseguridad
Beste erakundeak
https://ror.org/000xsnr85
https://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
Bertsioa
Postprinta
Dokumentu-mota
Artikulua
Bahituraren amaiera data
2024-11-30
Hizkuntza
Ingelesa
Eskubideak
© 2024 Springer Nature
Sarbidea
Sarbide bahitua
URI
https://hdl.handle.net/20.500.11984/6518
Argitaratzailearen bertsioa
https://doi.org/10.1038/s41567-024-02441-z
Non argitaratua
Nature Physics 
Argitaratzailea
Springer Nature
Laburpena
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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