Condensed Matter Physics, 2010, vol. 13, No. 2, p. 23606:1-6
DOI:10.5488/CMP.13.23606
Title: Sound attenuation and anharmonic damping in solids
with correlated disorder Author(s):
 
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W. Schirmacher
(Physik-Department E13, Technische Universität München,
James-Franck-Strasse 1, D-85747 Garching, Germany; Fachbereich Physik, Universität Mainz, Germany)
,
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C. Tomaras
(Arnold Sommerfeld Center for Theoretical Physics,
Ludwig-Maximilians-Universität München, Theresienstr. 37, D-80333
München, Germany)
,
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B. Schmid
(Fachbereich Physik, Universität Mainz, Germany)
,
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G. Baldi
(ESRF Grenoble)
,
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G. Viliani
(Dipt. di Fisica, Universit\'a di Trento, Italy)
,
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G. Ruocco
(Dipt. di Fisica, Universit Ža di Roma, Italy; IPCF-CNR, Sezione di Roma, c/o Sapienza Universita' di Roma, Italy)
,
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T. Scopigno
(Dipt. di Fisica, Universit Ža di Roma, Italy; IPCF-CNR, Sezione di Roma, c/o Sapienza Universita' di Roma, Italy) |
We study via self-consistent Born approximation a
model for sound waves in a disordered environment, in which the
local fluctuations of the shear modulus G are spatially
correlated with a certain correlation length ξ. The theory
predicts an enhancement of the density of states over Debye's
ω2 law (boson peak) whose intensity increases for
increasing correlation length, and whose frequency position is
shifted downwards as 1/ξ. Moreover, the predicted
disorder-induced sound attenuation coefficient Γ(k) obeys
a universal scaling law ξ Γ(k) = f(kξ) for a given
variance of G. Finally, the inclusion of the lowest-order
contribution to the anharmonic sound damping into the theory allows
us to reconcile apparently contradictory recent experimental data in
amorphous SiO2.
Key words: sound attenuation, vibrational properties of
disordered solids, boson peak, anharmonic interactions
PACS: 63.50.-x, 43.20.+g, 65.60.+a
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