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66                                                       Chapter 2


             effects  of surface roughness, by  replacing the flat plate with the mean
             stochastic roughness amplitude A, to obtain,

                                ª     § A  ·  2  º
                               z
               F  r  () = Fz  0  ()« + 61  ¨  ¸
                 Cas       Cas              » ,                                                     (60)
                                «     © z  ¹  »
                                ¬
                                            ¼
             where A  is  derived from direct measurements via an Atomic  Force
             Microscope (AFM).


             2.4  Quantum Information Theory, Computing and Communications

               The  advent  of nanoscale fabrication techniques  has brought within our
             reach  the  possibility  of producing systems whose predominant behavior is
             described by quantum mechanics (QM). While the engineering of systems
             based  on exploting this new  physics/technological paradigm  is still in  its
             infancy, this new paradigm is ultimately expected  to manifest itself in  the
             ushering  of a  ‘new electronics’ technology era. Obviously,  this  ‘new
             electronics’ is expected to change the way in which systems are implemented
             to effect the  functions of  information processing,  computing  and
             communications  [100-111].  These functions,  in turn, will  exploit the
             properties  of quantum mechanical wave  functions.  In this  section we
             introduce key aspects of the fundamental physics on which these functions
             are predicated, in particular, we focus on the concepts underpinning quantum
             information processing,  namely, quantum  bits  (qubits), quantum
             entanglement, the Einstein-Podolsky-Rosen (EPR) State, quantum gates, and
             quantum teleportation.
                Quantum  information  is  represented by quantum bits or  qubits [103].
             Qubits are fundamental physical entities, such as a two-level atom,  which
             may adopt two possible quantum (stationary) states (see Appendix A), say
             the mutually orthogonal  states  0  and  1 . Due  to its quantum  nature,
             however, the most general state is expressed as,

                ψ  =  a  0 +  b  1 ,                                                                                  (61)


             i.e., as a superposition of both states. Thus, a measurement of the qubit will
                                                                          2
             cause its wavefunction to collapse into the state  0  with probability  a , or
                                               2
             into the  state  1  with  probability  b .  This  means that during  its  time
             evolution a qubit may be partly in both the  0  and  1  state at the same
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