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142                                                      Chapter 3

             permittivity,  ε  <  0 , and an array of interspersed split-ring resonators
                         eff
             which created  a  frequency region with negative permeability,  µ  <  0 .
                                                                        eff
             These  materials  have become known as  metamaterials and, when
             implemented so that  both the permittivity and the permeability are
             simultaneously  negative,  they exhibit a negative refractive index
                               ω
             n () =ω  ε  ()µω  () , which  is real and  gives  rise to the  existence  of
                      eff   eff
             propagating modes with  the remarkable property that  they  follow  a  “left-
                                                   G   G   G
             hand” (LH)  rule. In this  case  the vectors  E , H , k  form a left-handed
             system, i.e., the  direction of  propagation is reversed  with respect  to  the
             direction of energy flow [169]. Left-handed materials have been the subject
             of much attention because they exhibit unusual propagation properties. For
             instance,  they  exactly reverse  the propagation paths of  rays within  them,
             which may be exploited to implement low reflectance surfaces  by  exactly
             canceling  the scattering  properties  of other materials. Another application,
             exploits their potential to produce perfect lenses.



             3.2.2.3.1  Negative Refraction and Perfect Lenses

               The concept of a  perfect lens  was  introduced  by Pendry [170],  upon
             further examining the earlier analysis of Veselago [169] on the consequences
             of negative  refractive index materials.  Veselago [169],  in  particular,  had
             indicated  that  reflection  and  refraction between vacuum and a negative
             refraction material, would follow the situation depicted in Fig. 3-29.




                             1 1                    2 2
                                        φ φ  φ φ
                                               Vacuum
                                               Va  c  u  u  m
                                               R
                                                ef
                                                  ract
                                                        I
                                                     i
                                                     ve
                                               Refractive Index n n
                                                          ex
                                                         d
                                                        n
                                        ψ
                                          ψ
                                        ψ ψ
                                  3 3           4 4
             Figure 3-29. Consequences of negative refractive index on refraction properties. 1—Incident
             beam. 2—Reflected beam. 3—Refracted beam for n<0. 4—Refracted beam for n>0. (After
             [169].)
             Fig. 3-29 shows, that contrary to the usual case of a positive index, when the
             refraction index is  negative the  angle of refraction is also negative  with
             respect to the surface normal. As a result, when such a medium is used as a
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