Various expressions for transit times in frustrated total internal reflection are analysed. The incompatibility of evanescent-wave propagation with Einstein causality is established.
Waveguides: Basic Equations...............................................................................................312 13.3 Coherent Destruction of Optical Tunneling ..........................................................................314 13.4 Optical Analog of Field-Induced Barrier Transparency........................................................316 13.5 Coherent Photonic Tunneling by Adiabatic Passage.............................................................319 13.6 Photonic Tunneling in Optical Lattices: Optical Analog of the Quantum Zeno Effect ....................................................................................325 13.7 Photonic Landau-Zener Tunneling .......................................................................................331 13.8 Conclusions ...........................................................................................................................333 References......................................................................................................................................334 Tunneling is a universal phenomenon to wave physics which arises when an evanescent field transfers energy through a barrier to a region where a propagating wave is allowed. Tunneling phenomena have been predicted and observed in countless quantum and classical physical systems. In particular, optical (or photonic) tunneling usually refers to light propagation across forbidden photonic barriers, such as in photonic band gap structures or undersized waveguides, as well as to evanescent field coupling among waveguides or resonators or to light passage via evanescent coupling in frustrated total internal reflection (FTIR). The first observation of FTIR and of photonic tunneling date back to three centuries ago, when Newton reported on light transmission through a gap between prisms. Nowadays, FTIR at plane interfaces is generally viewed as an optical analog of quantum mechanical tunneling across a one-dimensional potential barrier [1]. Optical tunneling across photonic barriers, realized by for example, FTIR or photonic band gaps, has attracted a great deal of attention in the past two decades as an experimentally accessible system with which to measure tunneling times [2-7]. FTIR has been also exploited to study wave packet reshaping [8] and to provide an optical realization of curious quantum-mechanical effects such as quantum evaporation [9]. Similarly, photonic tunneling in spherical dielectric media has been proposed as an optical analog of nuclear decay arising form particle escape from a three-dimensional potential well [10]. In deformed dielectric microcavities, chaos-assisted tunneling phenomena have been investigated as well [11-14]. A different optical system that provides an experimentally accessible laboratory tool to visualize and control photonic tunneling, which is at the focus of this chapter, is represented
There have been many recent theoretical and experimental reports on the propagation of light pulses at speeds exceeding the speed of light in vacuum c within media with anomalous dispersion, either opaque or with gain. Superluminal propagation has also been reported within vacuum, in the case of inhomogeneous pulses. In this paper we show that the observations of superluminal and non-causal propagation of evanescent pulses under the conditions of frustrated internal reflection are only apparent, and that they can be simply explained employing an explicitly (sub)luminal causal theory. However, the usual one-dimensional approach to the analysis of pulse propagation has to be abandoned and the spatial extent of the incoming pulse along the directions normal to the propagation direction has to be accounted for to correctly interpret the propagation speed of these evanescent waves. We illustrate our theory with animations of the time development of a pulse built upon the Huygen's construction.
The group delay in frustrated total internal reflection (FTIR) is shown to equal the dwell time plus a self-interference delay. The self-interference delay originates from the energy stored in the overlap between incident and reflected waves above the interface. The group delay in FTIR for finite beams is thus shown to be the lifetime of stored energy in the gap between the prisms and in the partial standing wave above the gap. As in other manifestations of tunneling the saturation of group delay with barrier length (Hartman effect) is explained by the saturation of stored energy in the region defined. No superluminal propagation is implied.