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Introduction to Nanotechnology

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10 INTRODUCTION TO PHYSICS OF THE SOLID STATE<br />

A- B<br />

B- A<br />

A- B<br />

B- A<br />

A- B<br />

B- A<br />

A- B<br />

B- A<br />

Figure 2.2. Sketch of a two-dimensional crystal structure based on a primitive rectangular lattice<br />

containing two dia<strong>to</strong>mic molecules A-B in each unit cell.<br />

A crystal structure is formed by associating with a lattice a regular arrangement of<br />

a<strong>to</strong>ms or molecules. Figure 2.2 presents a two-dimensional crystal structure based on<br />

a primitive rectangular lattice containing two dia<strong>to</strong>mic molecules A-B in each unit<br />

cell. A single unit cell can generate the overall lattice.<br />

In three dimensions there are three lattice constants, a, b, and c, and three angles:<br />

c( between b and c; b between a and c, and y between lattice constants a and b. There<br />

are 14 Bravais lattices, ranging from the lowest-symmetry triclinic type in which all<br />

three lattice constants and all three angles differ from each other (a # b # c and<br />

c( # b # y), <strong>to</strong> the highest-symmetry cubic case in which all the lattice constants are<br />

equal and all the angles are 90" (a = b = c and c( = b = y = 90"). There are<br />

three Bravais lattices in the cubic system, namely, a primitive or simple cubic (SC)<br />

lattice in which the a<strong>to</strong>ms occupy the eight apices of the cubic unit cell, as shown in<br />

Fig. 2.3a, a body-centered cubic (BCC) lattice with lattice points occupied at the<br />

apices and in the center of the unit cell, as indicated in Fig. 2.3b, and a face-centered<br />

cubic (FCC) Bravais lattice with a<strong>to</strong>ms at the apices and in the centers of the faces,<br />

as shown in Fig. 2.3~.<br />

In two dimensions the most efficient way <strong>to</strong> pack identical circles (or spheres) is<br />

the equilateral triangle arrangement shown in Fig. 2.4a, corresponding <strong>to</strong> the<br />

hexagonal Bravais lattice of Fig. 2.ld. A second hexagonal layer of spheres can<br />

be placed on <strong>to</strong>p of the first <strong>to</strong> form the most efficient packing of two layers, as<br />

shown in Fig. 2.4b. For efficient packing, the third layer can be placed either above<br />

Figure 2.3. Unit cells of the three cubic Bravais lattices: (a) simple cubic (SC); (b) body-centered<br />

cubic (BCC); (c) face-centered cubic (FCC).

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