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5.3 Experimental Analysis  185
                            [5.20]. Accordingto the theoretical analysis, surface refractive index distrib-
                            ution mappingwith a high contrast is predicted to be possible [5.7]. A metal
                            particle probe is considered to have the advantages of high experimental re-
                            producibility, not requiringgap control, and not only the ability to obtain the
                            surface image, but also to obtain the spectroscopic data of the sample. The
                            scattering efficiency of a silver particle is higher than that of a gold particle,
                            but the latter is more chemically stable. Therefore a gold particle is frequently
                            used as an SNOM probe.
                               Sugiura et al. [5.8] observed a dip on a cover glass and a gold colloidal
                            particle adhering to the cover glass. However, these images were thought to
                            have been an artifact problem due to the vertical displacement of the gold
                            probe [5.12]. On the other hand, the followingare observed for a refractive
                            index grating on a flat surface, which was made on a planar light waveguide
                            circuit (PLC) [5.24], by scanningan optically trapped 100-nm-diameter gold
                                                  +
                            particle. The scattered Ar laser light from the gold particle has a high inten-
                            sity due to the high refractive index of the grating with periods of 1.06 and
                            0.53 µm, both by s- and p-polarized illuminations.
                               Moreover, the surface profile of an optical disk trackinggroove is also
                            observed with and without the gold particle and the results compared to
                            discuss the artificial effect due to the vertical displacement of the particle
                            caused by the surface topology.


                            Experimental Setup

                            Figure 5.21 shows an experimental setup to trap a gold particle with an
                            upward-directed Nd:YAG laser beam (λ =1.06 µm) andtoscanitonthe
                            sample surface two-dimensionally usingan XY stage. The upward-directed


                                                                       Sample chamber
                                                 Ar+laser
                                                            XYZ Stage
                                                 l=488 nm
                                                                           Objective
                                                                           (NA=1.3)
                                                     BS2
                                             CCD
                                                              BS1
                                                          Lens
                                                        (f=180 mm)
                                                       PMT  Pinhole        Optical box
                                            PC
                                              Nd:YAG laser
                                               l=1064 nm
                            Fig. 5.21. Experimental setup of SNOM using an optically trapped gold particle.
                                                                   +
                            An Nd:YAG laser is used for trapping, and an Ar laser is used for illuminating the
                            gold particle. All the optical elements except mirrors to guide the lasers are installed
                            inside the small optical box (white box in Fig. 5.22a)for easy operation
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