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2. NANOMEMS PHYSICS: Quantum Wave-Particle Phenomena            67


             time, i.e., to the degree that a and b may adopt an infinity of values, the qubit
             has the potential to be in any of these. A quantum system possessing n qubits
                             n
             is said  to have  2     accessible  mutually orthogonal quantum states. For
             example, a system containing two noninteracting qubits will have the four
             states: 00 , 01 , 10 , 11 . States  such as these, which  represent  the
             juxtaposition of  independent or  noninteracting systems (qubits), are called
             tensor product states.


             2.4.1  Quantum Entanglement


               In general, a tensor product provides the mathematical description of the
             state of  a  system that is constituted  by  bringing together  noninteracting
             quantum  systems,  assuming  that they remain without  interacting [60].
             Comprehending  this concept is useful to get a clear  understanding  of  the
             definition of an entangled state [107-111].
               In  particular,  if associated with two quantum systems there  are vector
             spaces  V  of dimension  N , in which  resides a vector  φ ,   and  V  of
                    1                1                                    2
             dimension  N , in which resides a vector  χ , and where  N  and  N  may
                        2                                        1       2
             be finite or infinite, then the tensor product of V  and V  is denoted by the
                                                      1
                                                             2
             vector space V  [60],
             V = V ⊗ V ,                                                                                              (62)
                  1
                       2
             of dimension  N  N , where the vector,
                          1  2

                φ ⊗  χ =  φ  χ ,                                                                               (63)


             associated with the overall space V , is called the tensor product of  φ  and
              χ .

               If the vectors  φ  and  χ  can be expressed in terms of the respective
                   u
                             v
             bases { } and { }, so that,
                    i         i
                φ  =  ¦  a i  u ,                                                                                     (64)
                           i
                     i

             and
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