Surface Vibrational Modes and Reflection Time of Phonons in a Finite-Size Superlattice

Seiji MIZUNO

doi:10.1380/jsssj.20.272

超格子における表面振動モードとフォノンの反射時間

基板側からの表面フォノンの検出・励起

水野誠司

著者情報

ジャーナルフリー

1999 年 20 巻 4 号 p. 272-278

DOI https://doi.org/10.1380/jsssj.20.272

詳細

発行日: 1999/04/10 受付日: 1998/07/02 J-STAGE公開日: 2009/08/07 受理日: 1998/07/02 早期公開日: - 改訂日: -
訂正情報
訂正日: 2009/08/07 訂正理由: - 訂正箇所: 所属機関情報訂正内容: 訂正前 :
1) 北海道大学大学院工学研究科
2) Institut für Theoretische Physik, Technische Universität Dresden

訂正後 :
1) 北海道大学大学院工学研究科
2) Institut für Theoretische Physik, Technische Universität Dresden

訂正日: 2009/08/07 訂正理由: - 訂正箇所: 引用文献情報訂正内容: Wrong : 1) V. Narayanamurti, H.L. Stormer, M.A. Chin, A.C. Gossard and W. Wiegmann: Phys. Rev. Lett. 43, 2012 (1979).
2) O. Koblinger, J. Mebert, E. Dittrich, S. Dottinger, W. Eisenmenger, P.V. Santos and L. Ley: Phys. Rev. B 35, 9372 (1987).
3) D.C. Hurley, S. Tamura, J.P. Wolfe and H. Morkoc: Phys. Rev. Lett. 58, 2446 (1987).
4) D.C. Hurley, S. Tamura, J.P. Wolfe, K. Ploog and J. Nagle: Phys. Rev. B 37, 8829 (1988).
5) S. Tamura: Proc. 3rd Int. Conf. Phonon Physics and 6th Int. Conf. Phonon Scattering in Condensed Matter, Heidelberg, 1989 (World Scientific, Singapore, 1990) p. 703.
6) S. Tamura: Phys. Rev. B 38, 1427 (1988).
7) S. Tamura: Phys. Rev. B 39, 1261 (1989).
8) R.E. Camley, B. Djafari-Rouhani, L. Dobrzynski and A. A. Maradudin: Phys. Rev. B 27, 1427 (1983).
9) B. Djafari-Rouhani, L. Dobrzynski, O. Hardouin Duparc, R.E. Camley and A.A. Maradudin: Phys. Rev. B 28, 1711 (1983).
10) S. Mizuno and S. Tamura: Phys. Rev. B 45, 734 (1992).
11) S. Mizuno and S. Tamura: Phys. Rev. B 45, 13423 (1992).
12) S. Mizuno, M. Ito and S. Tamura: Jpn. J. Appl. Phys. 33, 2880 (1994).
13) S. Mizuno and S. Tamura: Phys. Rev. B 50, 7708 (1994).
14) V. Narayanamurti: Science 213, 717 (1981).
15) E.P. Wigner: Phys. Rev. 98, 145 (1955).
16) E.H. Hauge, J.P. Falck and T.A. Fjeldly: Phys. Rev. B 36, 4203 (1987).
17) E.H. Hauge and J.A. Stφvneng: Rev. Mod. Phys. 61, 917 (1989).
18) A.M. Steinberg, P.G. Kwiat and R.Y. Chiao: Phys. Rev. Lett. 71, 708 (1993).
19) See, for example, H.J. Mans, C. Thomsen and J. Tauc: “Phonon Scattering in Condensed Matter”;, ed. by A.C. Anderson and J.P. Wolfe (Springer, Berlin, 1986) p. 374.
20) S.Mizuno and S. Tamura: Phys. Rev. B 53, 4549 (1996).

Right : 1) V. Narayanamurti, H.L. Stormer, M.A. Chin, A.C. Gossard and W. Wiegmann: Phys. Rev. Lett. 43, 2012 (1979).
2) O. Koblinger, J. Mebert, E. Dittrich, S. Dottinger, W. Eisenmenger, P.V. Santos and L. Ley: Phys. Rev. B 35, 9372 (1987).
3) D.C. Hurley, S. Tamura, J.P. Wolfe and H. Morkoc: Phys. Rev. Lett. 58, 2446 (1987).
4) D.C. Hurley, S. Tamura, J.P. Wolfe, K. Ploog and J. Nagle: Phys. Rev. B 37, 8829 (1988).
5) S. Tamura: Proc. 3rd Int. Conf. Phonon Physics and 6th Int. Conf. Phonon Scattering in Condensed Matter, Heidelberg, 1989 (World Scientific, Singapore, 1990) p. 703.
6) S. Tamura: Phys. Rev. B 38, 1427 (1988).
7) S. Tamura: Phys. Rev. B 39, 1261 (1989).
8) R.E. Camley, B. Djafari-Rouhani, L. Dobrzynski and A. A. Maradudin: Phys. Rev. B 27, 1427 (1983).
9) B. Djafari-Rouhani, L. Dobrzynski, O. Hardouin Duparc, R.E. Camley and A.A. Maradudin: Phys. Rev. B 28, 1711 (1983).
10) S. Mizuno and S. Tamura: Phys. Rev. B 45, 734 (1992).
11) S. Mizuno and S. Tamura: Phys. Rev. B 45, 13423 (1992).
12) S. Mizuno, M. Ito and S. Tamura: Jpn. J. Appl. Phys. 33, 2880 (1994).
13) S. Mizuno and S. Tamura: Phys. Rev. B 50, 7708 (1994).
14) V. Narayanamurti: Science 213, 717 (1981).
15) E.P. Wigner: Phys. Rev. 98, 145 (1955).
16) E.H. Hauge, J.P. Falck and T.A. Fjeldly: Phys. Rev. B 36, 4203 (1987).
17) E.H. Hauge and J.A. Støvneng: Rev. Mod. Phys. 61, 917 (1989).
18) A.M. Steinberg, P.G. Kwiat and R.Y. Chiao: Phys. Rev. Lett. 71, 708 (1993).
19) See, for example, H.J. Mans, C. Thomsen and J. Tauc: “Phonon Scattering in Condensed Matter”;, ed. by A.C. Anderson and J.P. Wolfe (Springer, Berlin, 1986) p. 374.
20) S.Mizuno and S. Tamura: Phys. Rev. B 53, 4549 (1996).

抄録

We discuss the interaction of bulk phonons with surface vibrational modes in a finite-size superlattice. The incident phonons injected normally on the superlattice from a substrate are perfectly reflected, i.e., the reflection ratee is unity irrespective of frequency. However, these phonons come back to the substrate with a large time delay when the frequency coincides with an eigenfrequency of the surface mode. This is due to the resonant interaction of the incident phonons with a surface vibrational mode. The results suggest that the surface vibrational modes are detectable from the other side of the surface by a time-resolved phonon reflection experiment.

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