1. Basic Crystallography 26 January 2015 Three general types of solids 1. Amorphous ― with order only within a few atomic and molecular dimensions (Fig. (a)) 2. Polycrystalline ― with multiple sing-crystal regions (called grains) separated by grain boundary (Fig.(b)) 3. Single crystal ― with geometric periodicity throughout the entire material (Fig. (c)) (a) (b) (c) 1

2. DIMENSIONS AND UNITS  1 micrometer (1  m) = 10 -6 m = 10 -4 cm è1 Å = 10 -10 m = 10 -8 cm (Å =Angstrom)  10,000 Å = 1  m = 1000 nm è1 nanometer (1 nm) = 10 -9 m = 10 Å  Wavelength of visible light 0.4  m(violet) to 0.7  m(red) {400 nm to 700 nm, 4,000 Å to 7,000 Å }  1 mil = 0.001 inch = 25.4  m èSheet of notebook paper about 4 mils  1 human hair = 75  m to 100  m = 75,000-100,000 nm èAtomic spacing in a crystal ~ 3 to 5 Å  Fingernail growth rate about 1-3  m/hour ( Not personally verified ) èAggressive production minimum feature sizes, tens of nm, 20 nm used in the iPhone 6 A8 microprocessor.

3. Geometric Description of Single-Crystal — Space Lattices lattice: the periodic arrangement of atoms in the crystal Lattice: unit cell: a small volume that can be used to repeat and form the entire crystal. Unit cells are not necessary unique. Unit cell: 3

4. Space lattices 4 A general 3D unit cell is defined by three vectors Every equivalent lattice point in the 3D crystal can be found by a b c General case a b c Special case

5. Basic Crystal Structures 5 Three common types: a) Simple cubic b) Body-centered cubic (bcc) c) Face-centered cubic (fcc) (a) (c) (b) and

6. 6 Why Are Crystal Planes Important? real crystals are eventually terminate at a surface Semiconductor devices are fabricated at or near a surface many of a single crystal's structural and electronic properties are highly anisotropic

7. 1.Find the intercept on the x, y, and z 2.Reduce to an integer. i.e. lowest common denominator 3.Take the reciprocal and reduce to the smallest set of integers (h, k, l) These are called the Miller Indices 7

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9. 9 (100) Plane with normal direction [100] (110) Plane with normal direction [110] (111) Plane with normal direction [111] Examples of Lattice Planes in Cubic Lattices (100) Plane with normal direction [100] (110) Plane with normal direction [110] (111) Plane with normal direction [111]

10. 10 Set of Planes (001) (010) Due to the high degree of symmetry in simple cubic, bcc and fcc, the axis can be rotated or parallel shift in each of three dimensions, and a set of plane can be entirely equivalent. {100} set of planes: (100), (010), (001) Similarly, {110} set of planes: (110), (101), (011)

11. 11 Set of Planes (001) (010) Due to the high degree of symmetry in simple cubic, bcc and fcc, the axis can be rotated or parallel shift in each of three dimensions, and a set of plane can be entirely equivalent. {100} set of planes: (100), (010), (001) Similarly, {110} set of planes: (110), (101), (011)

12. 12 The Diamond Structure Materials possess diamond structure: Si, Ge 8 atoms per unit cell Any atom within the diamond structure will have 4 nearest neighboring atoms

13. Refer To Crystal WEB Link 12

14. Volume Density of Atoms 14 Volume density Number of atoms per unit volume = Total number of atoms / volume occupied by these atoms = number of atoms per unit cell/volume of the unit cell Unit: m -3 or (cm) -3 Example For Silicon a= 5.43 Å = 5.43 x 10 -8 cm Volume density =

15. 15 Procedure of Silicon Wafer Production Raw material ― Polysilicon nuggets purified from sand Crystal pulling Si crystal ingot Slicing into Si wafers using a diamond saw Final wafer product after polishing, cleaning and inspection A silicon wafer fabricated with microelectronic circuits

16. 16 Identification of Wafer Surface Crystallization Flats can be used to denote doping and surface crystallization