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4.2 Theoretical Analysis I – Optical Torque  133
                            Effect of Light Beam Profiles

                            The trappingforce and rotation rate are calculated for various beam intensity
                            profiles of the form

                                                                             2
                                                                                2
                                      TEM 00 (Gaussian) mode : I(r)= I 0 exp(−2r /w ),    (4.16)
                                                                                0
                                      uniformly filled aperture mode : I(r)= I 0 ,         (4.17)
                                                                                2
                                                                        2
                                                                                    2
                                      TEM 01 (donut) mode : I(r)= I 0 (r/w 0 ) exp(−2r /w ).  (4.18)
                                                                                    0
                            The fractions of the total beam power that enters the lens aperture are 87%
                            (a), 100% (b), and 59% (c). Below, all the light powers are normalized after
                            the lens aperture.
                            Example 4.1. Analyze the relationship between the rotation rate and the slope
                            angle with illuminated by beams with Gaussian (a), uniformly filled (b), and
                            donut (c) intensity profiles.
                            Solution. Figure 4.15 shows the numerical results for the rotor of d =
                            3 µm,h =10 µm, and n 2 =1.53 in water of µ = 1 mPa s at the laser power of
                            P = 100 mW. Since the torque at an arbitrary point is defined as the product
                            of force F t and distance r from the rotation axis, a high rotation rate (torque
                            efficiency) can be obtained with beam profile (c) which has high intensity at
                            the outer part of the aperture. Optical torque increases in linear proportion
                            to the radius of the rotor, and the dragforce increases as twice the radius,
                            therefore, rotation rate decreases inversely proportional to the radius. Rota-
                            tion rate increases as the slope angle a increases and reaches a maximum at
                            a =75 . As a result, a laser beam with a strongprofile at the outer part and
                                  ◦
                            a rotor with small radius are effective for increasingthe rotation rate.
                            Example 4.2. Analyze the relationship between torque efficiency Q torque and
                            beam waist position z f for the rotor illuminated by converging laser beams of
                            the intensity profiles with (a)–(c).


                                              2,500
                                                                         (c)
                                              2,000  (a) Gaussian        (b)
                                             Rotation rate (rpm)  1,500  (c) Donut  (a)
                                                   (b) Uniform

                                              1,000
                                               500

                                                 0
                                                  0        30       60        90
                                                          Slope angle (Deg)
                            Fig. 4.15. Relationship between rotation rate and slope angle of the rotor of d =
                            3 µm,h =10 µm, and n 2 =1.53 in water at P = 100 mW for the Gaussian (a),
                            uniformly filled (b), and donut (c)beam intensity profiles
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