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98  3 Structural Chemistry of Manganese Dioxide and Related Compounds

                        Subsequently, the difference  d (110) (in angstrom) is calculated from the
                        theoretical value and the measured d value of the (1 1 0) reflection. Using
                        the empirical calibration curve (a second-order polynomial, Equation 3.5), the
                        pyrolusite concentration can be calculated or it may be taken from a diagram,
                        as shown in Figure 3.5.
                    2) The model of De Wolff disorder gives no explanation for the line broadening
                        of reflections which are not affected by this type of lattice disorder. Chabre
                        and Pannetier ascribed this effect to a micro twinning of the ramsdellite/rutile
                        lattice on the planes [0 2 1] and [0 6 1]. These faces are believed to be growth
                        planes of EMD [45, 46]
                        It is well known that in rutile-like structures the planes [0 1 1] and [0 3 1] are
                        twinning planes. Hence, Chabre and Pannetier concluded that twinning faults
                        in the planes [0 2 1] and [0 6 1] (the equivalent planes in the ramsdellite doubled
                        unit cell) are the explanation for some features in the diffraction patterns of
                        γ -MnO 2 : for example, the lineshift of the (1 1 0) reflection toward lower angles
                        or the merging of the reflection groups (h 2l)/(h 4 0) and (h 6l)/(h 02).
                      In Figure 3.6 the arrangement of the manganese atoms is shown in a projection
                    along the a-axis. The unit cells are marked by the shaded regions. It can easily be
                    seen, that no lattice distortion is necessary to form the [0 2 1] and [0 6 1] twins. The
                    very low activation energy for the twinning usually results in a very high number
                    of micro twin boundaries in the crystal structure. The exact number of micro twin
                    domains is difficult to estimate from the diffraction patterns and according to
                    Chabre and Pannetier it is difficult to distinguish between the effects of the two


                       50
                              De wolff disorder
                      Pyrolusite concentration Pr [%]  30
                       40





                       20


                       10



                             0,05  0,10  0,15  0,20  0,25  0,30
                                      ∆d(110) / Å
                    Figure 3.5  Calibration curve for the determination or
                    the pyrolusite concentration of orthorhombically indexed
                    γ -MnO 2 samples by comparison of the calculated with
                    the observed d (110) value.
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