Can Mixing Materials Make Electromagnetic Signals Travel Faster?

Suppose that a composite is constructed from two phases and that we propagate an electromagnetic signal through it. The velocity of the signal in the composite depends on the microstructure. What microstructures are associated with the maximum and minimum speeds of the electromagnetic signal? Here we show that the group velocity of a pulse can be higher in the composite than in either of the two phases. We derive sharp bounds for the relative increase and decrease in the group velocity of the electromagnetic signal in the composite and give the associated optimal microstructures. We also find that a pulse in a composite can have substantially smaller dispersion and, at the same time, substantially larger group velocity than pulses traveling in the pure phases.

[1]  William T. Joines,et al.  THEORY AND MODELING OF BANDPASS FILTERS IN WAVEGUIDE USING THIN FERRITE LAYERS , 1998 .

[2]  Michael J. Miksis,et al.  Wave propagation in bubbly liquids at finite volume fraction , 1985, Journal of Fluid Mechanics.

[3]  Henry Schriemer,et al.  Group Velocity in Strongly Scattering Media , 1996, Science.

[4]  Graeme W. Milton,et al.  Bounds on the complex dielectric constant of a composite material , 1980 .

[5]  S. Shtrikman,et al.  A Variational Approach to the Theory of the Effective Magnetic Permeability of Multiphase Materials , 1962 .

[6]  Ruggeri,et al.  Observation of superluminal behaviors in wave propagation , 2000, Physical review letters.

[7]  Jerzy S. Krasinski,et al.  Passive pulse shaping of femtosecond pulses using birefringent dispersive media , 1996 .

[8]  Zvi Hashin,et al.  The Elastic Moduli of Heterogeneous Materials , 1962 .

[9]  Jörgen Axell,et al.  Bounds for field fluctuations in two‐phase materials , 1992 .

[10]  Andrej Cherkaev,et al.  On the effective conductivity of polycrystals and a three‐dimensional phase‐interchange inequality , 1988 .

[11]  Graeme W. Milton,et al.  Bounds on the transport and optical properties of a two‐component composite material , 1981 .

[12]  S. Harris,et al.  Light speed reduction to 17 metres per second in an ultracold atomic gas , 1999, Nature.

[13]  D. A. Dunnett Classical Electrodynamics , 2020, Nature.

[14]  G. Milton The Theory of Composites , 2002 .

[15]  L. J. Wang,et al.  Gain-assisted superluminal light propagation , 2000, Nature.

[16]  S. Prager,et al.  Improved Variational Bounds on Some Bulk Properties of a Two‐Phase Random Medium , 1969 .

[17]  M M Fejer,et al.  Engineerable femtosecond pulse shaping by second-harmonic generation with Fourier synthetic quasi-phase-matching gratings. , 1998, Optics letters.

[18]  David J. Bergman,et al.  Exactly Solvable Microscopic Geometries and Rigorous Bounds for the Complex Dielectric Constant of a Two-Component Composite Material , 1980 .

[19]  Graeme W. Milton,et al.  Bounds on the complex permittivity of a two‐component composite material , 1981 .

[20]  Fadil Santosa,et al.  A dispersive effective medium for wave propagation in periodic composites , 1991 .

[21]  Randall J. LeVeque,et al.  High-resolution finite-volume methods for acoustic waves in periodic and random media , 1999 .