Calculating Band Structure
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1 Calculating Band Structure Nearly free electron Assume plane wave solution for electrons Weak potential V(x) Brillouin zone edge Tight binding method Electrons in local atomic states (bound states) Interatomic interactions >> lower potential Unbound states for electrons Energy Gap difference between bound / unbound states Crystal Field Splitting Group theory to determine crystalline symmetry Crystalline symmetry establishes relevant energy levels Field splitting of energy levels However all approaches assume a crystal structures. Bands and energy gaps still exist without the need for crystalline structure. For these systems, Molecular Orbital theory is used.
2 Free Electron Model Energy bands consist of a large number of closely spaced energy levels. Free electron model assumes electrons are free to move within the metal but are confined to the metal by potential barriers. This model is OK for metals, but does not work for semiconductors since the effects of periodic potential have been ignored.
3 Kronig-Penny Model This model takes into account the effect of periodic arrangement of electron energy levels as a function of lattice constant a As the lattice constant is reduced, there is an overlap of electron wavefunctions that leads to splitting of energy levels consistent with Pauli exclusion principle. A further lowering of the lattice constant causes the energy bands to split again Energy bands for diamond versus lattice constant.
4 Formation of Bands Periodic potential Band gap Inter-atom interactions Many more states
5 Conduction / valence bands Free electron model Conduction band states Valence band states Bound states
6 Conduction / valence bands Conduction band states Lowest Unoccupied Molecular Level (LUMO) Valence band states Highest Occupied Molecular Orbital (HOMO)
7 Electrons fill from bottom up Semiconductor filled valence band
8 Example band structures Ge Si GaAs Find: Valence bands? Conduction bands? Energy Gap? Highest Occupied Molecular Level (HOMO)? Lowest Unoccupied Molecular Level (LUMO)?
9 Simple Energy Diagram A simplified energy band diagram used to describe semiconductors. Shown are the valence and conduction band as indicated by the valence band edge, E v, and the conduction band edge, E c. The vacuum level, E vacuum, and the electron affinity,, are also indicated on the figure.
10 Metals, Insulators and Semiconductors Possible energy band diagrams of a crystal. Shown are: a) a half filled band, b) two overlapping bands, c) an almost full band separated by a small bandgap from an almost empty band and d) a full band and an empty band separated by a large bandgap.
11 Semiconductors Filled valence band (valence 4, 3+5, 2+6) Insulator at zero temperature Metals Free electrons Valence not 4 Binary system III-V: GaAs, InP, GaN, GaP Binary II-VI: CdTe, ZnS, Semiconductors Si, Ge Filled p shells 4 valence electrons
12 E g Temperature Dependence
13 E g Doping Dependence Doping, N, introduces impurity bands that lower the bandgap.
14 Energy bands in Electric Field Electrons travel down. Holes travel up. Energy band diagram in the presence of a uniform electric field. Shown are the upper almost-empty band and the lower almost-filled band. The tilt of the bands is caused by an externally applied electric field.
15 The effective mass The presence of the periodic potential, due to the atoms in the crystal without the valence electrons, changes the properties of the electrons. Therefore, the mass of the electron differs from the free electron mass, m 0. Because of the anisotropy of the effective mass and the presence of multiple equivalent band minima, we define two types of effective mass: 1) the effective mass for density of states calculations and 2) the effective mass for conductivity calculations.
16 Motion of Electrons and Holes in Bands Electron excited out of valence band Temperature Light Defect Electron in conduction band state Empty state in valence band (Hole empty state)
17 Electrons - holes Electron in conduction band NOT localized Hole in valence band Usually less Mobile (higher effective mass), but not always Electron hole pairs in different bands large separation
18 Region Near Gap In the region near the gap, e(k) Local maximum / minimum de/dk 0 Conduction band effective mass m* h 2 /(d 2 E/dk 2 ) Electrons Minimum energy Bottom of conduction band Holes Opposite E(k) derivative Opposite effective charge Top of valence band k x Valence band
19 General Carrier Concentration Probability of hopping into state n 0 (number of states / energy) * energy distribution Conduction band Gap g c (E) density of states f (E) energy distribution Valence band
20 Density of states The density of states in a semiconductor equals the density per unit volume and energy of the number of solutions to Schrödinger's equation. Calculation of the number of states with wavenumber less than k
21 Fermi-surface (3-D) K-space Set of allowed k vectors Fermi surface Electrons occupy all k f2 states less than Ef*2m/h k F ~ wavelength of electron wavefunction k y Allowed state for k-vector k x 2p/L Area of sphere / k states in spheres 3 4pk F 1 3 kf 3 L 3 2 6p 3 (2p / L) N Volume in lattice
22 Density of states Number of states: N k 3 F 6p 2 2 L 3 Density in energy: Kinetic energy of electron: Density of states / energy: In conduction band, Nc: Different m* in conduction and valence band
23 Density of States in 1, 2 and 3D
24 Probability density functions The distribution or probability density functions describe the probability that particles occupy the available energy levels in a given system. Of particular interest is the probability density function of electrons, called the Fermi function. The Fermi-Dirac distribution function, also called Fermi function, provides the probability of occupancy of energy levels by Fermions. Fermions are halfinteger spin particles, which obey the Pauli exclusion principle.
25 Fermi-Dirac vs other distributions Maxwell-Boltzmann: Noninteracting particles Bose-Einstein: Bosons Intrinsic: Ec Ef ½ Eg High temperature: Fermi ~ Boltzmann
26 Carrier Densities The density of occupied states per unit volume and energy, n(e), ), is simply the product of the density of states in the conduction band, gc(e) and the Fermi-Dirac probability function, f(e). Since holes correspond to empty states in the valence band, the probability of having a hole equals the probability that a particular state is not filled, so that the hole density per unit energy, p(e), equals:
27 Carrier Densities Product of density of states and distribution -- defines accessible bands -- within kt of Ef
28 Carrier Densities Electrons Holes
29 Limiting Cases 0 K: Non-degenerate semiconductors: semiconductors for which the Fermi energy is at least 3kT away from either band edge.
30 Intrinsic Semiconductor Intrinsic semiconductors are usually non-degenerate
31 Mass Action Law The product of the electron and hole density equals the square of the intrinsic carrier density for any non-degenerate semiconductor. The mass action law is a powerful relation which enables to quickly find the hole density if the electron density is known or vice versa
32 Doped Semiconductor Add alternative element for electron/holes Si valence 4 P valence 5 B valence3 Si Si Si Si Si Si Si Si Si Si Si Si Hole Si Si Si Si Si Si P Si Si Si -- B Si Si Si Si Si Si Si Si Si e- Si Si Si Si Si Si Si Si Si Si Si Si Si Si Si Si Pure Si All electron paired Insulator at T0 Phosphorous n-doped Electron added to conduction band Boron p-doped Positive hole added to conduction band
33 Dopant Energy levels P 0.046eV As 0.054eV Easily ionized easily donate electrons Energy required to donate electron Si Eg1.2eV Cu 0.53eV Cu 0.40eV Au 0.54eV Au 0. 35eV Large energy bad. Add scattering Donate no carriers Cu 0.24eV Au 0. 29eV B 0.044eV Energy required to donate hole
34 Carrier concentration in thermal equilibrium Carrier concentration vs. inverse temperature Thermally activated Intrinsic carriers Region of Functional device n e N(carriers) N(dopants) Activation of dopants 1/T(K)
35 Dopants and Fermi Level Free electron metal: n e 3 k F 2 3p, e F 2 kf 2m 2 Intrinsic semiconductor n(electrons) n(holes) Fermi energy middle n-doped material n(electrons) >> n(holes) Fermi level near conduction band Ec Ef Ev Ec Ef Ev p-doped materials n(electrons) >> n(holes) Fermi level near conduction band Fermi Energy is not material specific but depends on doping level and type Ec Ef Ev
36 Mobility and Dopants Dopants destroy periodicity Scattering, lower mobility e Mobility (cm 2 /V-s) e e h 1E14 1E15 1E16 1E17 1E18 Dopant Concentration (cm -3 ) GaAs Si
37 Doping / Implantation Implants: (1)NBL (isolation) (2) Deep n (Collector) (3) Base well (p) (4) Emitter (n) (5) Base contact Simple bipolar transistor 5 implants Complicated CMOS circuit >12
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