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4. NANOMEMS APPLICATIONS: CIRCUITS AND SYSTEMS                161


             The concept consists in exploiting the inherent  entanglement  of
             superconducting Cooper pair together with electron-electron interactions in
             one dimension to enable the sequential injection of entangled pairs from a
             superconductor into two nanotubes located next to each other at a distance
             well below the Cooper pair coherence length.  The key to the Cooper pair
             injection  and separation into entangled  electrons relies on the  Lüttinger
             liquid behavior exhibited by CNTs characterized by an interaction factor g
             and  subband spacing ε . In particular  [189], the  tunneling  rate,
                                    0
                                1
                                  1 −
             Γ   ~  (eV  h )(kT  İ  )g , at  which  Cooper pairs tunnel  from the
              AA              0
             superconductor into the end of a CNT, being proportional to  eVρ , turns
                                                                       2 e
                                                                         1  § 1  · ¸
             out to be much smaller than the tunneling rate  Γ  ~  (eV  h )(kT  İ  ) © g2 ¨ −1 ¸ ¹ ,
                                                                          ¨
                                                       AB              0
             at which split entangled pairs are injected into both CNTs. This difference, is
             rooted in the fact that Lüttinger liquid behavior, manifested as the coherent
             arrangement of all electrons in the  CNT  bulk,  causes  the  single-electron
                                                     1 § 1  · ¸
                                    ρ
             tunneling density of states,  () ~E  ε −1 ( εE  ) © g4  ¨ −1 ¸ ¹  to dominate the Cooper
                                                     ¨
                                      e      0     0
                                                           1
             pair tunneling density of  states,  ρ  () ~E  ε − 1 (E ε  )g . With  Γ  <<  Γ  ,
                                           2 e     0     0          AA     AB
             virtually all the charge tunneling that occurs involves split entangled pairs.
               Once split, the entangled electrons may propagate for long distances due
             to the ballistic property that characterizes  transport  in  CNTs  of  Fermi
             velocity  v  and length L at low temperatures  T <  T =  v =  k  L  at which
                      F                                   φ     F  B
             loss of coherence due to thermal effects are nonexistent.



             4.3.1  Quantum Computing Paradigms

               As indicated in  Chapter 2,  the fundamental  building  block  on  which
             quantum information processing systems are based is the qubit, a two-state
             quantum system. Qubits may take on many physical forms, however, to be
             useful in realizing real, practical, systems, they must be endowed with three
             key properties [190]: 1) They must be decoupled from the environment to
             avoid disturbances which may deviate their time evolution from unitarity; 2)
             They must be able to respond, in a controlled  fashion,  to  purposeful
             manipulation, in order to enable the formation of quantum logic gates and
             entangled states, which rely on such interactions; 3) They must withstand the
             momentary, but strong, coupling to  the  environment  introduced  by  a
             measuring device. In this section, we present the principles of various qubit
             implementations, in particular, ion-trap-, nuclear-magnetic resonance-, solid-
             state-, and superconducting-based qubits.
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