Page 121 -
P. 121

3.3 Experimental Measurement and Comparison  111
                                           16
                                         Minimum trapping power (mW)  10 8 6 4  Glass
                                           14
                                           12










                                            0 2                     Polystyrene
                                             0   10    20   30   40    50   60   70
                                                       Stage velocity (mm/s)

                            Fig. 3.37. Relationship between minimum trapping power obtained using solitary
                            optical fiber and stage velocity for microsheres of 10 micrometer in diameter


                               microspheres. This is because the trappingforce is equivalent to F g − F s
                               for downward illumination, but to F g + F s for upward illumination. The-
                               oretically, the minimum trappingpower ratios between the upward- and
                               downward-directed beams are 1.8 for polystyrene sphere and 1.6 for glass
                               sphere.
                             2. The experimental minimum trapping powers are in fairly good agreement
                               with the theoretical ones for axial trapping, but not in good agreement for
                               transverse trapping. This is because the trapping position for transverse
                               trapping changes due to the large gravitational force, particularly for high-
                               density and/or large particles.
                             3. The minimum axial trappingpower increases as the trappingposition
                               increases from the chamber surface. This is because the spherical aberra-
                               tion due to the refractive index difference between the immersion oil of the
                               objective and the aqueous medium in which a microsphere is suspended.
                             4. Brownian motion is active for microspheres less than about 1 µm in diam-
                               eter, which increases trappingpower.
                             5. Optical fiber trappingis expected to improve both the operation and
                               implementation.
                            Example 3.6. Show that the force due to Brownian motion of a microsphere
                            suspended in water is equivalent to F =2kT/d where k is the Boltzman con-
                            stant, T is the absolute temperature and d is the diameter of a microsphere.

                            Solution. Microspheres smaller than about 1 µm in diameter seem to fall out
                            of the optical trap when laser power is reduced below a certain level. This
                            is due to the thermal energy driving the particle in the weakest direction of
                            the optical trap, i.e., parallel to the beam axis. To express the thermal effect
                                                                                   2
                            in force units we assume that the harmonic trap potential Kz /2(K is the
   116   117   118   119   120   121   122   123   124   125   126