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NEOCLASSICAL THEORY OF INTERACTION                                      105

            From these observations, the real and imaginary part of impedance () must be related as


                                               1  ∞  ()
                                      () = − ∫  
                                                −∞  −                   (2.110)
                                                         �
                                              1  ∞  ()
                                       () = ∫  
                                               −∞  −
            In case of transmission or reflection coefficient, it is convenient first to separate the magnitude
            and phase taking  the  natural  logarithm of  ()  or  ()  and only then to apply the K-K
            relations
                                   ln�()� = ln(|()|) + ()
                                                               ⎫
                                                               ⎪
                                               1  ∞  ln(|()|)
                                      () = − ∫                      (2.111)
                                                −∞  −
                                                               ⎬
                                                  1  ∞  ()
                                      ln(|()|) = ∫    ⎪
                                                   −∞  −  ⎭
            Step 3 is the transform of the integrals in (2.109) making them suitable for numerical evaluation
            by subtracting out the integrand divergence at the point  = . Taking into account that
                                    1  ∞    1    +∞  = 0                  (2.112)
                                      ∫     = (ln| − |)|
                                     −∞  −    −∞
            we can rewrite (2.109) as

                                                        ′
                                                    ′
                                              1  ∞    ()−  ()
                                     ′′
                                     () = − ∫      
                                     
                                               −∞  −  �                  (2.113)
                                                    ′′
                                                        ′′
                                              1
                                    ′
                                    () − 1 = ∫ ∞    ()−  ()  
                                    
                                               −∞  −
            L’Hopital’s rule and the fact that  () and  () are indefinitely differentiable functions give
                                                ′′
                                       ′
                                                
                                       
            us assurance that the ratio in each of integrands does not diverge any more at  = .
            2.10.2  Eliminating Negative Frequencies in the K-K Relations
            The KK relations in (2.113) spin positive and negative frequencies. It follows from (2.106) that
            the real part of  () is an even while its imaginary part is an odd function of frequency
                         
                                                  ′
                                         ′
                                         (−) =  ()
                                                �                           (2.114)
                                         ′′
                                                    ′′
                                         (−) = − ()
                                                    
                                         
            Step 4. Due to (2.114) the equation (2.113) can be transformed into
                                                  ′   ′
                                                   ()−  () 
                                               ∞
                                            2
                                   ′′
                                   () = −  ∫
                                   
                                              0  −  +  �         (2.115)
                                                   ′′
                                                         ′′
                                              2  ∞    ()−  () 
                                    ′
                                    () = 1 + ∫
                                   
                                               0  −  +
            2.10.3  Remote Sensing and K-K Relations
            One of the  most remarkable applications of the K-K relations is the remote sensing aka
            acquisition of information about some object or objects without being in physical contact with
            them. Particularly, the  critical  mission of such sensing is the  identification  of remote
            object/objects. We are doing such identification at a distance every moment of our life using
            our eyes, ears, nose as a smell sensor and quite sophisticated recognition algorithms buried deep
            in our brain cells. If natural human sensors are not worldly-wise the required for identification
            information can be collected by all kind of active and passive radars, microphones and cameras,
            spectrometers and radiometers,  microscopes and telescopes,  multiple devices for  magnetic
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