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Three-dimensional Bernal graphite

Figure 15-33 (a) The FBZ and RFBZ for three-dimensional Bernal graphite, (b) View of the... [Pg.571]

Let us see if we can predict the modifications in energies of COs that should occur at some of the special points in the RFBZ as a result of intersheet interactions. Because three-dimensional Bernal graphite is symmetric for reflection through the plane of a hexagonal sheet, we continue to have a valid distinction between a and n COs. We expect intersheet interactions to be small, so we can take a perturbational approach. The interactions involving jt COs should be largest since p AOs project farthest from the plane, so we will restrict our attention to the n bands. [Pg.572]

Fig. 1 Atomic structures of graphites, a) Bernal structure of perfect three-dimensional graphite, b) Warren structure of two-dimensional turbostatic graphite with no layer registration. (Reproduced by kind permission of Thermo-Hypersil-Keystone.)... Fig. 1 Atomic structures of graphites, a) Bernal structure of perfect three-dimensional graphite, b) Warren structure of two-dimensional turbostatic graphite with no layer registration. (Reproduced by kind permission of Thermo-Hypersil-Keystone.)...

See other pages where Three-dimensional Bernal graphite is mentioned: [Pg.1244]    [Pg.1891]    [Pg.1172]   
See also in sourсe #XX -- [ Pg.57 , Pg.572 ]




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