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1.6 Young's double-slit experiment               23

                        The time Ät for a wave packet to pass a given point equals the uncertainty in
                        its position x divided by the group velocity v g
                                                      Äx    Äx    m
                                                 Ät ˆ    ˆ     ˆ    Äx                    (1:47)
                                                      v g   v     p
                        Combining equations (1.46) and (1.47), we see that ÄEÄt ˆ ÄxÄp. Thus, the
                        relation (1.45) follows from (1.44). The Heisenberg uncertainty relation (1.45)
                        is treated more thoroughly in Section 3.10.



                                           1.6 Young's double-slit experiment
                        The essential features of the particle±wave duality are clearly illustrated by
                        Young's double-slit experiment. In order to explain all of the observations of
                        this experiment, light must be regarded as having both wave-like and particle-
                        like properties. Similar experiments on electrons indicate that they too possess
                        both particle-like and wave-like characteristics. The consideration of the
                                                                                       È
                        experimental results leads directly to a physical interpretation of Schrodinger's
                        wave function, which is presented in Section 1.8.
                          The experimental apparatus is illustrated schematically in Figure 1.8. Mono-
                        chromatic light emitted from the point source S is focused by a lens L onto a
                        detection or observation screen D. Between L and D is an opaque screen with
                        two closely spaced slits A and B, each of which may be independently opened
                        or closed.
                          A monochromatic light beam from S passing through the opaque screen with
                        slit A open and slit B closed gives a diffraction pattern on D with an intensity
                        distribution I A as shown in Figure 1.9(a). In that ®gure the points A and B are
                        directly in line with slits A and B, respectively. If slit A is closed and slit B
                        open, the intensity distribution of the diffraction pattern is given by the curve
                        labeled I B in Figure 1.9(a). For an experiment in which slit A is open and slit
                        B is closed half of the time, while slit A is closed and slit B is open the other
                        half of the time, the resulting intensity distribution is the sum of I A and I B ,as
                        shown in Figure 1.9(b). However, when both slits are open throughout an


                                                                         D
                                                         L  A

                                       S
                                                            B


                                     Figure 1.8 Diagram of Young's double-slit experiment.
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