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3. NANOMEMS PHYSICS: Quantum Wave Phenomena                   143


             lens, Fig. 3.30, it causes light originally diverging from a point source S to
             be reversed and to converge back to a point S 1 in the medium.








                                S S                      S S
                                               S S 1 1    2 2

                                     n=1     n=-1    n=1
                                             n=-1
                                                     n=1
                                     n=1
             Figure 3-30. Parallel-sided  medium with negative refractive index refocuses  light.  (After
             [170].)

             The special feature contributed by a negative refraction lens was elucidated
             by Pendry [170]. It consists in that, by  being capable  of  amplifying
             evanescent waves,  all wave components emanating  from  the  source  are
             present at the converging focus; this enables the perfect reconstruction of the
             source  image. This property was proven by Pendry [170] by assuming an
             incident wave with electric field given by,


               E    =  y ˆ  exp (ik  z +  ik  x − iω  ) t ,                                                       (192)
                 0 S+        z     x
             where, since k + k >  ω 2  c , the wave vector,
                              2
                         2
                                      2
                         x    y
                                 ω 2
               k =   i +  k + k −   ,                                                                     (193)
                              2
                         2
                 z       x    y   2
                                 c
             implies an exponentially decaying (evanescent) wave, a reflected wave given
             by,

               E    =  y ˆ r  exp ( ik−  z +  ik  x − iω  ) t ,                                                  (194)
                 0 S−           z     x
             and transmitted wave given by,

               E    =  y ˆ t  exp ( 'ik  z +  ik  x − iω  ) t ,                                                     (195)
                 1 S+         z      x

             where,
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