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168                                                       Chapter 4


             spin orients itself in the direction of the field. If, in addition, an RF field is
             applied  in  a  pulsed  fashion,  the spins are made to tip off-axis, while
             precessing  about the direction of the constant field. The precession
             frequency is the so-called Larmor frequency and is given by  Ȧ =  µB . For
             the hydrogen atom (proton), the magnetic moment is 42.7MHz/T and, at a
             typical  field  of  B=11.7T, its  precession frequency is 500MHz. Sample
             examination is accomplished placing a coil around it, tuned to the precession
             frequency, which picks up the oscillating currents induced as a consequence
             of the magnetic field produced by the precessing protons. The device that
             applies the static magnetic field and the RF control pulses, and then detects
             the magnetic induction is called an NMR spectrometer, see Fig. 4-15.

                      Sa m p le  T u b
                      Sa m p le  T u b e e



                                                         Mix er r
                                                         Mix e
                                           C C
                                                             RF
                                                             RF
                                                                   Co m p u ter r
                                                  D irectio n a l a l
                                                  D irectio n      Co m p u te
                                                  C o uple  Osc illa to
                                                  C o upler r
                                                            Osc illa to r r
                                RF  Co il il
                                RF  Co
                                                  Am p lifier r
                                                  Am p lifie
                                   B B
                                     0 0
                                      Sta tic F ie ld C o
                                      Sta tic F ie ld C o il il
                     Figure 4-15. Sketch of experimental NMR spectrometer. (After [195].)
               NMR  phenomena,  which were first observed in 1946 [196], [197],
             became the basis for a multitude  of  analytical  studies of  materials,  in
             particular, the determination of  molecular structures [198],  and  magnetic
             resonance imaging [199].  In these contexts,  the technology  of  NMR
             spectroscopy is rather mature.
               The  application  of  NMR to QC was advanced Cory, Fahmy and Havel
             [200], and Gershenfeld and Chuang  [201] in 1997. To overcome  the
             difficulty  in detecting the spin of individual, adoption was made of qubits
             implemented in the liquid state, where additive effects could be exploited to
             yield a reasonably large signal amplitude. Also  adopted were methods  to
             discern the fraction of nuclear spins pointing in the external field direction,
             despite the effects of temperature-induced random spin orientation. The two-
             state quantum system was realized by choosing molecules possessing spin-
             1/2 nuclei, which in the presence of the external magnetic field adopts two
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