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438  15 Lithiated Carbons

                    for example, carbons with a remarkably high lithium storage capacity (see
                    Sections 15.2.4 and 15.2.5), and tailored carbons, which were prepared by the use
                    of inorganic templates [61, 62]. It has to be emphasized that the assumed suitability
                    of a carbonaceous material for a lithium intercalation host depends strongly on the
                    method of its evaluation, and quite a few carbons may have been rejected as anode
                    materials due to an inadequate evaluation method. As a consequence, sometimes
                    the classification of a carbon as ‘good’ or ‘poor’ anode material can be only prelim-
                    inary. For instance, though in principle electrochemical intercalation in graphite
                    was already observed in the mid-1970s [63, 64], it took about 15 years for an appro-
                    priate electrolyte allowing the highly reversible operation of a graphite anode to be
                    found [65].

                    15.2.1
                    Carbons: Classification, Synthesis, and Structures

                    Because of the variety of available carbons, classification is inevitable. Most car-
                    bonaceous materials which are capable of reversible lithium intercalation can be
                    classified roughly as graphitic and nongraphitic (disordered).
                                                      2
                      Graphitic carbons basically comprise sp -hybridized carbon atoms which are
                    arranged in a planar hexagonal (‘honeycomb-like’) network such that a so-called
                    ‘graphene layer’ is formed. Van der Waals forces provide a weak cohesion of
                    the graphene layers, leading to the well-known layered graphite structure. From a
                    strictly crystallographic point of view the term ‘graphite’ is, however, only applicable
                    for carbons having a layered lattice structure with a perfect stacking order of
                    graphene layers, either the prevalent AB (hexagonal graphite, Figure 15.3) or the


                                                graphene layers
                                                                      arm-chair face
                 A
                prismatic surface  B      layer plane      zig-zag

                                                            face

                                                  2
                 A                         spacing (  C  = 0.3354 nm)

                                 0.246     0.142 nm                         layer A
                    outline of                                              layer B
                     unit cell     nm

                    Figure 15.3  (a) Schematic drawing of the crystal structure
                    of hexagonal graphite showing the AB graphene layer stack-
                    ing sequence and the unit cell. (b)View perpendicular to the
                    basal plane of hexagonal graphite. Prismatic surfaces can be
                    subdivided into armchair and zig-zag faces. Modified and
                    redrawn from Ref. [2].
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