Page 35 - PRINCIPLES OF QUANTUM MECHANICS as Applied to Chemistry and Chemical Physics
P. 35

26                           The wave function

                             and with the photons passing through the slit one at a time, wave behavior is
                             observed.
                               Analogous experiments using electrons instead of photons have been carried
                             out with the same results. Electrons passing through a system with double slits
                             produce an interference pattern. If a detector determines through which slit
                             each electron passes, then the interference pattern is not observed. As with the
                             photon, the electron exhibits both wave-like and particle-like behavior and its
                             location on a detection screen is randomly determined by a probability
                             distribution.




                                                  1.7 Stern±Gerlach experiment
                             Another experiment that relates to the physical interpretation of the wave
                             function was performed by O. Stern and W. Gerlach (1922). Their experiment
                             is a dramatic illustration of a quantum-mechanical effect which is in direct
                             con¯ict with the concepts of classical theory. It was the ®rst experiment of a
                             non-optical nature to show quantum behavior directly.
                               In the Stern±Gerlach experiment, a beam of silver atoms is produced by
                             evaporating silver in a high-temperature oven and allowing the atoms to escape
                             through a small hole. The beam is further collimated by passage through a
                             series of slits. As shown in Figure 1.10, the beam of silver atoms then passes
                             through a highly inhomogeneous magnetic ®eld and condenses on a detection
                             plate. The cross-section of the magnet is shown in Figure 1.11. One pole has a
                             very sharp edge in order to produce a large gradient in the magnetic ®eld. The
                             atomic beam is directed along this edge (the z-axis) so that the silver atoms
                             experience a gradient in magnetic ®eld in the vertical or x-direction, but not in
                             the horizontal or y-direction.
                               Silver atoms, being paramagnetic, have a magnetic moment M.Ina
                             magnetic ®eld B, the potential energy Vof each atom is
                                                                    .
                                                           V ˆÿM B
                             Between the poles of the magnet, the magnetic ®eld B varies rapidly in the x-

                                                                                x


                                                                                      z
                                            Oven  Collimating                 y
                                                     slits
                                                             Magnet        Detection
                                                                           plate
                                          Figure 1.10 Diagram of the Stern±Gerlach experiment.
   30   31   32   33   34   35   36   37   38   39   40