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1
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16444387140
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C. Thomsen, H. T. Grahn, H. J. Maris, and J. Tauc, Phys. Rev. B 34, 4129 (1986).
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(1986)
Phys. Rev. B
, vol.34
, pp. 4129
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Thomsen, C.1
Grahn, H.T.2
Maris, H.J.3
Tauc, J.4
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4
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0003080827
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H.-N. Lin, H. J. Maris, L. B. Freund, K. Y. Lee, H. Luhn, and D. P. Kern, J. Appl. Phys. 73, 37 (1993).
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(1993)
J. Appl. Phys.
, vol.73
, pp. 37
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Lin, H.-N.1
Maris, H.J.2
Freund, L.B.3
Lee, K.Y.4
Luhn, H.5
Kern, D.P.6
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5
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0034431035
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J. M. E. Harper, S. G. Malhotra, C. Cabral, Jr., C. Lavoie, H.-Y. Hao, W. Homsi, and H. J. Maris, Mater. Res. Soc. Symp. Proc. 612, D7.5.1 (2001).
-
(2001)
Mater. Res. Soc. Symp. Proc.
, vol.612
, pp. 751
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Harper, J.M.E.1
Malhotra, S.G.2
Cabral Jr., C.3
Lavoie, C.4
Hao, H.-Y.5
Homsi, W.6
Maris, H.J.7
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6
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0029307028
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-
Rigorous Coupled Wave Analysis [see, for example, M. G. Moharam, E. B. Grann, D. A. Pommet, and T. K. Gaylord, J. Opt. Soc. Am. A 12, 1068 (1995)] can be used to calculate the reflectivity of a patterned structure. To calculate ΔR(t), it would be necessary to calculate the reflectivity R of the structure before excitation and again at time t after the geometry has changed as a result of the propagating strain pulses.
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(1995)
J. Opt. Soc. Am. A
, vol.12
, pp. 1068
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Moharam, M.G.1
Grann, E.B.2
Pommet, D.A.3
Gaylord, T.K.4
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7
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0002387823
-
Digest of Technical Papers
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D. Edelstein, C. Uzoh, C. Cabral, Jr., P. DeHaven, P. Buchwalter, A. Simon, E. Cooney, S. Malhotra, D. Klaus, H. Rathore, B. Agarwala, and D. Nguyen, Digest of Technical Papers, IEEE International Interconnect Technology Conference, 2001, pp. 9-11.
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(2001)
IEEE International Interconnect Technology Conference
, pp. 9-11
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Edelstein, D.1
Uzoh, C.2
Cabral Jr., C.3
Dehaven, P.4
Buchwalter, P.5
Simon, A.6
Cooney, E.7
Malhotra, S.8
Klaus, D.9
Rathore, H.10
Agarwala, B.11
Nguyen, D.12
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9
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0000881998
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W. S. Capinski, H. J. Maris, M. Cardona, D. S. Katzer, K. Ploog, and T. Ruf, Phys. Rev. B 59, 8105 (1999).
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(1999)
Phys. Rev. B
, vol.59
, pp. 8105
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Capinski, W.S.1
Maris, H.J.2
Cardona, M.3
Katzer, D.S.4
Ploog, K.5
Ruf, T.6
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10
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33845394901
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As heat flows into the dielectric films, their optical constants will also change
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As heat flows into the dielectric films, their optical constants will also change.
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12
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84866575717
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x of the wave number parallel to the wafer is zero
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x of the wave number parallel to the wafer is zero.
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16
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0032613383
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J.-H. Zhao, T. Ryan, P. S. Ho, A. J. McKerrow, and W. Y. Shih, J. Appl. Phys. 85, 6421 (1999).
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(1999)
J. Appl. Phys.
, vol.85
, pp. 6421
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Zhao, J.-H.1
Ryan, T.2
Ho, P.S.3
McKerrow, A.J.4
Shih, W.Y.5
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17
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0001526218
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H. N. Lin, R. J. Stoner, T. Tauc, and H. J. Maris, J. Appl. Phys. 69, 3816 (1991).
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(1991)
J. Appl. Phys.
, vol.69
, pp. 3816
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Lin, H.N.1
Stoner, R.J.2
Tauc, T.3
Maris, H.J.4
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19
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0033719568
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T.-Y. Zhang, Y.-J. Su, C.-F. Qian, M.-H. Zhao, and L.-Q. Chen, Acta Mater. 48, 2843 (2000).
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(2000)
Acta Mater.
, vol.48
, pp. 2843
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Zhang, T.-Y.1
Su, Y.-J.2
Qian, C.-F.3
Zhao, M.-H.4
Chen, L.-Q.5
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21
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33845460866
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note
-
The density of bulk TaN may be found in Ref. 13; however, the density of thin film TaN depends on the deposition technique.
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22
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33845399916
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note
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Strictly this orthogonality relation holds only for a closed system, but since the modes radiate at a slow rate we expect it to be a good approximation.
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-
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24
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33845400613
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We have used the sound velocities in the [100] direction
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We have used the sound velocities in the [100] direction.
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-
-
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25
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33845421341
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note
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We are ignoring the fact that mode 6 has a frequency that is slightly above the cutoff for transverse radiation.
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-
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26
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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
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Tas, G.1
Loomis, J.J.2
Maris, H.J.3
Bailes, A.A.4
Seiberling, L.E.5
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27
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33845451354
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note
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-3, 3.5 GPa, and 0.4 which are consistent with values found in
-
-
-
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30
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36449002061
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G. Tas, R. J. Stoner, H. J. Maris, G. W. Rubloff, G. S. Oehrlein, and J. M. Halbout, Appl. Phys. Lett. 61, 1787 (1992).
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(1992)
Appl. Phys. Lett.
, vol.61
, pp. 1787
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Tas, G.1
Stoner, R.J.2
Maris, H.J.3
Rubloff, G.W.4
Oehrlein, G.S.5
Halbout, J.M.6
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31
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0035119701
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M. Georgiadou, D. Veyret, R. L. Sani, and R. C. Alkire, J. Electrochem. Soc. 148, C54 (2001).
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(2001)
J. Electrochem. Soc.
, vol.148
, pp. 54
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Georgiadou, M.1
Veyret, D.2
Sani, R.L.3
Alkire, R.C.4
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36
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33845438221
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note
-
Problems of modes of nearby frequency could be fixed by applying the mode identification technique discussed in Ref. 23.
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