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50                                                                UEC Int’l Mini-Conference No.53

                    The University of Electro-Communications                                SAITO LABORATORY
                        Ground State of Spin-1 and Spin-2 Bose-Einstein Condensates

                                             Uyen Ha Phuong MAI and Hiroki SAITO
                             Department of Engineering Science, The University of Electro-Communications
                                                   Tokyo 182-8585, Japan

              Abstract                                         Ground State
              Spinor Bose-Einstein condensate (BEC) was first realized
                                                                 Table: Scattering lengths coefficient of  Na,  Rb
                                                                                                23
                                                                                                     87
              in 1988 and has inspired many new researches on BEC
                                                                              spin-1 and spin-2
              atomic gases, especially the ground-state properties of
                                                                         23 Na   c = 1.87a               [1]
              spinor BEC systems. Monte Carlo is an efficient method              1     B
                                                               Spin-1
              for finding the minimal value in many physics problems.    87 Rb   c = 1  −  0.47a B         [1]
              In this work, Monte Carlo is used to find the energy of    23 Na   c =  2.67a B    , c = − 2.89a B      [1]
                                                                                            2
                                                                                  1
              spin-1  and  spin-2  BEC  systems'  ground  states,   Spin-2
                                                                                        a
                                                                         87 Rb   c = 0.99 , c = − 0.53a      [2,3]
              respectively.  Their  spin  states  are  demonstrated  by           1      B    2    B
              spherical-harmonic representation.                   (a)                (b)
              Spin-1 and Spin-2 BEC
              Spinor order parameters of spin-1 and spin-2 BEC:
                         ( ) 1   (  1 ( ) 1 , 0 ( ) 1  , − ( ) 1 1  ) ;

                         ( ) 2   (  2 ( ) 2  , 1 ( ) 2  , 0 ( ) 2  , −  ( ) 2 1  , −  ( ) 2 2  )
                                                                   (c)
              The  spherical-harmonic  representation:  visualizing  the
                                                                                                     phase
              symmetry of spin states.                                                                 2
                              ) 
                         S ( ,   =  f   m ( ) f  Y f m ( ,   )
                                 m= −  f
              The energy of uniform spin-1 and spin-2 BEC:
                                                                                                        0
                       c   2              c   2  c    2
                   E ( ) 1  =  1  F  ;  E ( ) 2  =  1  F  +  2  A
                        2                  2     2  00
                                                               Figure:  Spherical  harmonic  representations  of  the
                                                                                                       23
              Monte Carlo method                               spin-1 and spin-2 states. (a) Polar state of spin-1  Na
                                                                                              87
                                                               and (b) ferromagnetic state of spin-1  Rb of spin-1;
                                                                                                 87
                                                                                          23
                    Create random complex wave functions       (c) biaxial nematic state of spin-2  Na and  Rb.
                                                                                                       23
                                                               For spin-1, the ground state is polar when c > 0 ( Na)
                                                                                                  1
                                                                                        87
                                                               or ferromagnetic when c < 0  ( Rb). For spin-2, when
                                                                                   1
                       Compute the energy of the system
                                                               c > 0 and c < 0, the ground state is biaxial nematic for
                                                                1       2
                                                                   23
                                                                          87
                                                               both  Na and  Rb.
                     Larger than         Smaller than          References
                   the initial energy   the initial energy
                                                             [1] Y. Kawaguchi and M. Ueda. “Spinor Bose-Einstein
                                                                 Condensates.” Physics Reports, 2012.
                                                             [2]  A. Widera et. al., Precision measurement of spin-dependent
                                        Minimal energy           interaction strengths for spin-1 and spin-2  Rb atoms, New
                                                                                              87
                                      (new initial energy)       J. Phys. 8, 152 (2006).
                                                             [3] M. Egorov, et. al., Measurement of s-wave scattering
                                                                 lengths in a two-component Bose-Einstein condensate,
                                                                 Phys. Rev. A 87, 053614 (2013).
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