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80       DIFFRACTION AND INTERFERENCE IN IMAGE FORMATION



                                                                                          Appearance at
                                                                                          back focal
                                                                                          plane of
                                                                                          objective


                                                                                          Back focal
                                                                                          plane of
                                                                                          objective


                                                                                          Objective


                                                                                          Specimen plane
                                       a              b               c           d
                                Figure 5-15
                                Generation of an image by interference requires collection of two adjacent orders of
                                diffracted light by the objective lens. If diffraction at the specimen does not occur (a), or
                                diffracted rays are not collected by the objective (b), no image is formed. In (c), a minimum of
                                two adjacent diffraction orders (0th and 1st) are collected, and an image is formed. In (d),
                                multiple diffracted orders are collected, leading to a high degree of definition in the image.


                                 • A periodic specimen with an interperiod spacing d gives rise to a periodic pattern
                                    with spacing D in the diffraction plane, where D   1/d. Therefore, the smaller the
                                    spacings in the object, the farther apart the spots are in the diffraction plane, and
                                    vice versa. The relationship is

                                                             d   fλ/D cos

                                    where f is the focal length of the lens, λ is the wavelength, and   is the acute angle at
                                    the principal plane in the objective lens from which the focal length is measured and
                                    which forms a right triangle together with the 0th- and 1st-order diffraction spots.

                                    Abbe’s theory of image formation explains the following important points: If a
                                specimen does not diffract light or if the objective does not capture the diffracted light
                                from an object, no image is formed in the image plane. If portions of two adjacent orders
                                are captured, an image is formed, but the image may be barely resolved and indistinct.
                                If multiple orders of diffracted light are captured, a sharply defined image is formed.
                                The theory is also the basis for determining the spatial resolution of the light micro-
                                scope, which is the subject of the next chapter.


                                DIFFRACTION PATTERN FORMATION IN THE BACK APERTURE
                                OF THE OBJECTIVE LENS

                                Let us now consider the diffraction pattern in the microscope’s diffraction plane in the
                                back aperture (back focal plane) of the objective lens. Under conditions of Koehler illu-
                                mination, a diffraction image of a specimen is formed just behind the objective in the
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