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NEOCLASSICAL THEORY OF INTERACTION                                       75

            Here the constant  =  /  is the metal conductivity and   () = 1. In case of copper
                                 2
                                                                 ′
                                     
                                                                
            the ratio   / ≅ 3.8 ⋅ 10  −17   (see above) and   = 1.602 ⋅ 10  −19 . Therefore,   = 6.75 ⋅
                      
            10 −22 . If so, we can roughly estimate that the average number of conductivity electrons in
            bulk copper  with   = 5.85 ⋅ 10 [S/m] is equal to   = 8.66 ⋅ 10   [m ] (!) or almost  90
                                                                       -3
                                      7
                                                                  28
            octillions. Meanwhile, an octillion is a billion billion billions!! For contrast, our sun mass is
            around 2 octillion tons only. All the oceans on Earth contain much less or about 3.25 ⋅ 10
                                                                                      25
            drops of water, plus or minus several billions (assuming 25 drops per 1 cm ).
                                                                        3
            Figure 2.5.2 illustrates the behavior of  () for copper over the wide frequency range (see
                                             
            (2.79)). The absolute value of this parameter is as minimum the six order of magnitude higher
            than for ordinary dielectrics. This tells us that the total electrical fields inside bulk metals are
            extremely weak at all frequencies up to 50 THz. There is nothing mystical that the value  ()
                                                                                    ′
                                                                                   
            is negative because the net electrical field in a metal is equal to (see Chapter 1)  =   ()⁄    .
                                                                                0
            It means that  the drifting in metal electrons induce their own electric field that is opposite and
            exceeds the applied external field  .
                                        0
            Conclusively notice that any electron takes part in instantaneous interactions with many ions,
            not a single one. Therefore, we can expect many different resonances depending on interaction
            strength. Assuming M types of spring oscillators, the corresponding relative dielectric function

















                      Figure 2.5.2 Complex dielectric constant vs. frequency for copper (Cu)
            of metals can be given as

                                                            2
                                  () = 1 + ∑   � ,   �                  (2.81)
                                                       2
                                             =1
                                 
                                                � 0,   � −(  ) 2 + 
            Here  , ,  0, , and   may be viewed as the plasma frequency, resonance frequency and the
                              
            relaxation time of the   oscillator, respectively. Then the metal complex conductivity can be
                               th
            derived as
                                          () =  ( () − 1) [S/m]     (2.82)
                                                 0
                                                    
            Typically, all the coefficients in (2.81) are estimated from experiment matching the measured
            data and (2.81) through some proper numerical algorithm.
            2.5.3   Ionospheric Plasma with Negative Dielectric Constant
            Encyclopedia Britannica defines plasma as “… an electrically conducting medium in which
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