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An optically controllable terahertz filter
1.D. Grischkowsky, S. Keiding, M. van Exter, and Ch. Fattinger, J. Opt. Soc. Am. B 7, 2006 (1990).
2.M. M. Sigalas, C. T. Chan, K. M. Ho, and C. M. Soukoulis, Phys. Rev. B 52, 11744 (1995);
2.J. S. McCalmont, M. M. Sigalas, G. Tuttle, K. M. Ho, and C. M. Soukolis, Appl. Phys. Lett. 68, 2759 (1996).
3.F. Keilmann, Int. J. Infrared Millim. Waves 2, 259 (1981);
3.K. Sakai and T. Yoshida, Infrared Phys. 18, 137 (1978).
4.C. Winnewisser, F. Lewen, and H. Helm, Appl. Phys. A: Mater. Sci. Process. 66, 593 (1998).
5.J. N. Heyman, R. Kersting, and K. Unterrainer, Appl. Phys. Lett. 72, 644 (1998).
6.J. Feldmann, R. Sattmann, E. O. Göbel, J. Kühl, J. Hebling, K. Ploog, R. Muralidharan, P. Dawson, and C. T. Foxon, Phys. Rev. Lett. 62, 1892 (1989).
7.J. Feldmann, M. Preis, E. O. Göbel, P. Dawson, C. T. Foxon, and I. Galbraith, Solid State Commun. 83, 245 (1992).
8.P. Dawson (private communication).
9.I. Galbraith, P. Dawson, and C. T. Fox, Phys. Rev. B 45, 13499 (1992).
10.A. M. Malik, M. J. Godfrey, and P. Dawson, Phys. Rev. B 59, 2861 (1999).
11.M. C. Nuss and J. Orenstein, Millimeter Wave Spectroscopy of Solids, edited by G. Grüner (Springer, Berlin, 1997).
12.E. T. Yu, M. K. Jackson, and T. C. McGill, Appl. Phys. Lett. 55, 744 (1989).
13.We have neglected the contribution to the absorption by the heavy holes located in the narrow well, since their mass is much heavier than that of the electrons.
14.Max Born and Emil Wolf, Principles of Optics, 6th ed. (Pergamon, Oxford, 1980).
15.M. Schall and P. U. Jepsen, Opt. Lett. 25, 13 (2000).
16.There has recently been alot of discussion on the superluminal behavior of the shifting of the THz wave forms in highly absorbing medium (see Ref. 17). While it appears at first glance that the peak velocity passes through the sample with speeds greater than that of light, the shifting is actually a consequence of a phase shift of the THz wave as it enters a highly conducting medium. This phase shift is small and therefore generally not observable, but it does dramatically effect the behavior of the THz pulses when they are measured in the time domain.
17.K. Wynne and D. A. Jaroszynski, Opt. Lett. 24, 25 (1999).
18.S. Baumgärtner, I. H. Libon, P. Jepsen, M. Schall, P. Dawson, N. E. Hecker, and J. Feldmann (unpublished).
19.See a discussion of the Drude model in N. Katzenellenbogen and D. Grischkowsky, Appl. Phys. Lett. 61, 840 (1992).
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