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ECE 371 – Chapter 1 Crystal Structure of solids
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Classifying materials on the basis of their ability to conduct current. Conductor – allows for flow of current ex: copper Insulator – prevents flow of current ex: rubber Semiconductor - A semiconductor is a substance, usually a solid chemical element or compound, that can conduct electricity under some conditions but not others, making it a good medium for the control of electrical current. ECE 317 Chapter 1 Crystal structure of solids 2
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Classification of semiconductors On the basis of the periodic chart ECE 317 Chapter 1 Crystal structure of solids 3 Group IVIII-VII-VI ElementalCompound
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Group IV semiconductors Consists of Carbon, Silicon and Germanium. Silicon is the dominant semiconductor material. Germanium has certain niche uses in high speed electronics, optoelectronics and photovoltaics. Carbon semiconductor research is currently being conducted with very promising results with carbon nanotube, diamond and graphene based semiconductors. ECE 317 Chapter 1 Crystal structure of solids 4
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III-V compound semiconductors Consists of group III and group V elements. This class of material is considered as alloys. III-N also referred to as nitrides are the basis of most visible light emitting diodes and lasers in the blue to green range. Ex: Blue-ray DVD players III-P alloys are called phosphides – mainly used for red lasers and solar cells. III-As are referred to as arsenides used for a variety of near-IR opto-electronic and electronic technologies. III-Sb alloys are called antimonides these are used for high speed electronics and mid-IR technologies like countermeasures lasers and thermal cameras. ECE 317 Chapter 1 Crystal structure of solids 5 Group III Group V
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CD Vs DVD Vs Blue-ray ECE 317 Chapter 1 Crystal structure of solids 6 AlGaAs laser InGaP laser InGaN laser
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II-VI semiconductors Mainly used in detectors made of HgCdTe. These detectors are very useful for MWIR and LWIR applications such as thermal sensing and night vision. ECE 317 Chapter 1 Crystal structure of solids 7 Group II Group VI
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classification for compound semiconductors based on number of constituent elements Binary: One group III and one group V. Simplistic model consists of one layer of group III and one layer of group V. Group III and V atomic site are mutually exclusive to their respective elements. Ex: GaAs, InP. Ternary: Three elements in all. Could be two group IIIs and one group V or vice-versa. Again group III sites and group V sites are exclusive thus in ternary with two group III species the group III atoms divide the spots up amongst themselves. Ex1: Al 0.7 Ga 0.3 As. Here 70% of the group III sites are occupied by Al and the rest by Ga and 100% of the group V sites are taken by As. Ex2: GaAs 0.6 P 0.4. Here 100% of the group III sites are occupied by Ga and 60% of the group V sites are occupied by As and the rest and 40% of the group V sites are taken by P. ECE 317 Chapter 1 Crystal structure of solids 8
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Binaries and ternaries (cont.) ECE 317 Chapter 1 Crystal structure of solids 9 Group III Group V Ga Ga Ga Ga Ga As As As As As Ga Ga Ga Ga Ga As As As As As Group III Group V GaAs – Binary alloy Group III Group V Al Ga Al Al Ga Al Al Ga Al Al As As As As As Al 0.7 Ga 0.3 As – Ternary alloy Ga Ga Ga Ga Ga As P As As P As As P As P Group III Group V GaAs 0.6 P 0.4 – Ternary alloy
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Quaternary alloys Three group IIIs one group V Ex: Al 0.3 Ga 0.3 In 0.4 As Two group IIIs and two group Vs Ex: Al 0.4 Ga 0.6 As 0.2 Sb 0.8 One group III and three group Vs. Ex: GaAs 0.8 Sb 0.1 P 0.1 Verify this yourself – in the above examples all the group III constituents add to give a 100% and all the group V constituents add to give 100%. Can you think of a quintinary (5 element) alloy? Is Al 0.1 Ga 0.9 In 0.1 As 0.7 Sb 0.2 a valid composition? (hint: its not ). Feel free to change the compositions of this alloy to make it correct. ECE 317 Chapter 1 Crystal structure of solids 10
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Types of solids Amorphous – no order in the atoms. Poly-crystalline – short range order. Single crystal – Long range order. See fig. 1.1 in neamen. ECE 317 Chapter 1 Crystal structure of solids 11
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Lattice and basis The lattice is a periodic arrangement of points in space. Each point on the lattice is called a Lattice point. (duh!) The basis consists of the simplest arrangement of atoms which is repeated at every point in the lattice to build up the crystal structure. Translation to produce the lattice: Each lattice point can be translated by a 1 in one direction and b 1 in another non-colinear direction. This results in a 2-D lattice. A third translation along another non-colinear direction results in a 3-D lattice. ECE 317 Chapter 1 Crystal structure of solids 12 See fig. 1.2
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Unit Cell Mathematical Definition (from P.K. Bhattacharya): A unit cell is the region of a crystal defined by vectors a, b and c and the angles α, β and γ such which when translated by integral multiples of those vectors reproduce a similar region of the crystal. OR A unit cell is a small volume of the crystal that can be used to reproduce the entire crystal. See fig. 1.3 Translation property: r = ha + kb + lc a,b,c are basis vectors. r is the translational vector. a, b and c could be inter-atomic distances in which case they are called lattice-constants. Primitive Cell: A primitive cell is the smallest unit cell in volume that can be defined for a specific lattice. See fig. 1.4 ECE 317 Chapter 1 Crystal structure of solids 13
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Bravais Lattices The number of ways in which lattice points can be specified in space while maintaining translational symmetry, is limited. Auguste Bravais demonstrated 14 types of such point lattices in 1848. Nobody has come up with new ones since. ECE 317 Chapter 1 Crystal structure of solids 14 Auguste Bravais
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The 14 bravais lattices ECE 317 Chapter 1 Crystal structure of solids 15
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Cubic lattices Simple cubic (SC) Body-centered cubic (BCC) Face centered cubic (FCC) See fig 1.5 in the text. ECE 317 Chapter 1 Crystal structure of solids 16
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Class problem #1 Calculate the packing fraction of a BCC cell assuming spherical atoms. If the interatomic distance is 5 Å what is the density of atoms in the crystal. Do the same for SC FCC ECE 317 Chapter 1 Crystal structure of solids 17
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Defining planes (hkl) See Fig. 1.6 for an example of a plane. Miller indices are an effective nomenclature for naming planes. Miller indices refer to the integers (hkl). Ex: (110), (111), (100) See fig. 1.7 All parallel planes have the same indices and are equivalent to each other. So avoid planes through the origin. ECE 317 Chapter 1 Crystal structure of solids 18
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Class problems Example 1.3, see fig. 1.8 Problem #2: TYU E 1.3 Determine the distance between the nearest (110) planes in a SC lattice with a lattice constant of a o = 4.83 Å. Problem #3: TYU E 1.4 The lattice constant of a FCC structure is 4.75 Å. Calculate the surface density of atoms for (a) a (100) plane and (b) a (110) plane. ECE 317 Chapter 1 Crystal structure of solids 19
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Expressing directions Fig. 1.9 So (hkl) is the plane, [hkl] is the direction. ECE 317 Chapter 1 Crystal structure of solids 20
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Diamond structure ECE 317 Chapter 1 Crystal structure of solids 21
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GaAs - ZincBlende ECE 317 Chapter 1 Crystal structure of solids 22
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Atomic bonding Ionic bond: Na + Cl - Covalent bond – sharing e - to complete an octet H need only one atom to complete the octet and therefore we only have H 2. Silicon needs 4 e - and so can bond to four other Si atoms, forming a crystal. Metallic bond Van der Waals ECE 317 Chapter 1 Crystal structure of solids 23
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Imperfections in solids Lattice vibrations Point defect Vacancy Interstitial Frenkel defect (vacancy-interstitial) Line dislocation ECE 317 Chapter 1 Crystal structure of solids 24
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ECE 317 Chapter 1 Crystal structure of solids 25
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Point defect ECE 317 Chapter 1 Crystal structure of solids 26
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Impurities in solids Substitution Interstitial Doping ECE 317 Chapter 1 Crystal structure of solids 27
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Semiconductor growth ECE 317 Chapter 1 Crystal structure of solids 28
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From a melt ECE 317 Chapter 1 Crystal structure of solids 29
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Epitaxy - MOCVD ECE 317 Chapter 1 Crystal structure of solids 30
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Epitaxy -MBE ECE 317 Chapter 1 Crystal structure of solids 31
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