-
1
-
-
16444387140
-
-
C. Thomsen, H T. Grahn, H J. Maris, and J. Tauc, Phys. Rev. B34, 4129 (1986).
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(1986)
Phys. Rev. B
, vol.34
, pp. 4129
-
-
Thomsen, C.1
Grahn, H.T.2
Maris, H.J.3
Tauc, J.4
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5
-
-
84966503230
-
-
M. Abramowitz, I.A. Stegun, National Bureau of Standards, Washington, edited by, and
-
Handbook of Mathematical Functions, edited by M. Abramowitz and I.A. Stegun (National Bureau of Standards, Washington, 1964).
-
(1964)
Handbook of Mathematical Functions
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-
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6
-
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84912037889
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-
For example, at room temperature the attenuation length for 56 GHz longitudinal sound in GaAs is about (formula presented). See, and
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For example, at room temperature the attenuation length for 56 GHz longitudinal sound in GaAs is about (formula presented). See W. Chen, Z R. Wasilewski, S. Tamura, and H J. Maris, Philos. Mag. B70, 687 (1994).
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(1994)
Philos. Mag. B
, vol.70
, pp. 687
-
-
Chen, W.1
Wasilewski, Z.R.2
Tamura, S.3
Maris, H.J.4
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8
-
-
0004427807
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-
G. Tas, J J. Loomis, H J. Maris, A A. Bailes, and L E. Seiberling, Appl. Phys. Lett.72, 2235 (1998).
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(1998)
Appl. Phys. Lett.
, vol.72
, pp. 2235
-
-
Tas, G.1
Loomis, J.J.2
Maris, H.J.3
Bailes, A.A.4
Seiberling, L.E.5
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13
-
-
0001526218
-
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H.-N. Lin, R J. Stoner, H J. Maris, and J. Tauc, J. Appl. Phys.69, 3816 (1991).
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(1991)
J. Appl. Phys.
, vol.69
, pp. 3816
-
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N, H.1
Stoner, R.J.2
Maris, H.J.3
Tauc, J.4
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14
-
-
0004451329
-
-
This is the refractive index of Ge at 800 nm and 120 K as measured by
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This is the refractive index of Ge at 800 nm and 120 K as measured by R F. Potter, Phys. Rev.150, 562 (1966).
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(1966)
Phys. Rev.
, vol.150
, pp. 562
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Potter, R.F.1
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22
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0004432896
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H. Schober, D. Strauch, K. Nützel, and B. Dorner, J. Phys.: Condens. Matter5, 6155 (1993).
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(1993)
J. Phys.: Condens. Matter
, vol.5
, pp. 6155
-
-
Schober, H.1
Strauch, D.2
Nützel, K.3
Dorner, B.4
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27
-
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85013560343
-
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W.P. Mason, R.N. Thurston, Academic, New York, in, edited by, and, p
-
H J. Maris, in Physical Acoustics, edited by W.P. Mason and R.N. Thurston (Academic, New York, 1971), Vol. VIII, p. 279.
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(1971)
Physical Acoustics
, vol.8
, pp. 279
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-
Maris, H.J.1
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29
-
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85038292682
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-
It follows from Eqs. (111) and (226) of Ref., that for (formula presented) the leading term in the temperature dependence of the sound velocity should be proportional to (formula presented)
-
It follows from Eqs. (111) and (226) of Ref. 25 that for (formula presented) the leading term in the temperature dependence of the sound velocity should be proportional to (formula presented).
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-
-
-
32
-
-
85038339714
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Note that we are discussing here just the temperature-dependent part of the attenuation
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Note that we are discussing here just the temperature-dependent part of the attenuation.
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-
-
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33
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36149007591
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A variety of processes involving four or more phonons are also possible
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C. Herring, Phys. Rev.95, 954 (1954). A variety of processes involving four or more phonons are also possible.
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(1954)
Phys. Rev.
, vol.95
, pp. 954
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Herring, C.1
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34
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85038304179
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This estimate was made along the same lines as in Ref
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This estimate was made along the same lines as in Ref. 6.
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