Page 228 - Fundamentals of Light Microscopy and Electronic Imaging
P. 228

THE OPTICAL PRINCIPLE OF CONFOCAL IMAGING      211




                                               Galvanometer
                                                  mirror




                                                              Laser beam













                                                                 Specimen
                                               Scanning

                       Figure 12-5
                       The scan-control mechanism in a CLSM. The sketch shows the delivery of the excitatory
                       laser beam to the specimen by one of two galvanometer-driven mirrors that vibrate in
                       mutually perpendicular axes within the confocal scan head. One mirror controls scanning
                       along the x-axis, the other along the y-axis; both motions are coordinated to generate a
                       pattern of a raster on the specimen. The speed and angular extent of deflection of the
                       mirrors can be controlled to regulate the scanning rate and the extent of the scan.



                          a computer monitor. Thus, a confocal image of an object is reconstructed from pho-
                          ton signals and is displayed by a computer; the confocal image never exists as a real
                          image that can be seen by the eye in the microscope.
                        • A microscope system of this design is called a confocal laser scanning microscope
                          (CLSM).



                                 Demonstration: Isolation of Focal Plane Signals
                                             with a Confocal Pinhole

                         Warning—Care should be taken not to accidentally reflect the light beam into the
                         eye during this exercise!
                             To become familiar with confocal optics, construct the confocal reflection
                         optical system shown in Figure 12-6 using common optical components mounted
                         on an I-beam optical bench, a 1–5 mW HeNe laser, and a coin as a specimen. The
                         specimen support plate must be rigid enough so that you can slide a coin or other
                         reflective specimen on its surface without moving the plate. Position the objective
                         lens so that reflections from the coin are refocused at the pinhole aperture (a pinhole
   223   224   225   226   227   228   229   230   231   232   233