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3.2 Theoretical Analysis  95
                                            0.40
                                                                             Diameter
                                                              Beam waist     40 mm
                                            0.35
                                          Trapping efficiency  0.25  s  Ray optics  10
                                                                             20
                                            0.30
                                                                             4
                                                                             2
                                            0.20
                                            0.15
                                            0.10
                                            0.05
                                              0
                                              0     0.2  0.4   0.6   0.8   1.0
                                         Normarized distance between microsphere center and focus point
                            Fig. 3.16. Transverse trapping efficiency of polystyrene microsphere by two con-
                            verging ray approximations


                                                        n
                                                   w 2   2    R
                                                       r(z)      n  1     w 1




                                                       d 2        d  1

                            Fig. 3.17. Geometry for calculating trapping efficiency for microsphere along prop-
                            agation axis by laser beam emitted from tapered lensed optical fiber

                            lensed optical fiber of curvature R =10 µm, beam waist radius ω 1 =5.0 µm,
                            core refractive index n 1 =1.462, as shown in Fig. 3.17. The focus distance
                            from the tapered lensed fiber end d 2 and the beam radius r(z) with the beam
                            waist ω 2 are given as

                                                                                      2

                                              n 2 R(n 2 − n 1 )                   z

                                   d 2 = −                    ,   r(z)= ω 2  1+        .
                                                              2                  kω 2
                                          (n 2 − n 1 ) + R 2  λ                    2
                                                  2
                                                         πω 2
                                                           1
                            Solution. An equation of a ray going along the z-direction is expressed by
                            the variable parameter t(0 ≤ t ≤ 1) as

                                                                 2
                                                             z             2
                                              y = tω 2  1+       ,  Z 0 = kω ,
                                                                           2
                                                            Z 0
                            where t = r/R m and
                                                              ω 1
                                                                          .
                                                ω 2 =
                                                             2
                                                           2          2
                                                         πω
                                                           1   n 2 −n 1  +1
                                                         λ      n 1 R
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