corner
corner

Phys. Rev. E 63, 036610 (2001) [5 pages]

Group velocity, energy velocity, and superluminal propagation in finite photonic band-gap structures

Download: PDF (118 kB) Buy this article Export: BibTeX or EndNote (RIS)

G. D’Aguanno1,2, M. Centini1,2, M. Scalora2,3, C. Sibilia1, M. J. Bloemer2, C. M. Bowden2, J. W. Haus4, and M. Bertolotti1
1INFM at Dipartimento di Energetica, Università di Roma ”La Sapienza,” Via Scarpa 16, I-00161 Rome, Italy
2Weapons Sciences Directorate, AMSMI-RD-WS, RD&E Center, U.S. Army Aviation & Missile Command, Building 7804, Redstone Arsenal, Alabama 35898-5000
3Time Domain Corporation, Cummings Research Park, 7057 Old Madison Pike, Huntsville, Alabama 35806
4Electro-Optics Program, University of Dayton, Dayton, Ohio 45469-0245

Received 14 June 2000; revised 27 September 2000; published 23 February 2001

We have analyzed the notions of group velocity Vg and energy velocity VE for light pulses propagating inside one-dimensional photonic band gap structures of finite length. We find that the two velocities are related through the transmission coefficient t as VE=|t|2Vg. It follows that VE=Vg only when the transmittance is unity (|t|2=1). This is due to the effective dispersive properties of finite layered structures, and it allows us to better understand a wide range of phenomena, such as superluminal pulse propagation. In fact, placing the requirement that the energy velocity should remain subluminal leads directly to the condition Vg<~c/|t|2. This condition places a large upper limit on the allowed group velocity of the tunneling pulse at frequencies of vanishingly small transmission.

© 2001 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevE.63.036610
DOI:
10.1103/PhysRevE.63.036610
PACS:
42.25.Bs, 42.70.Qs, 73.40.Gk