MindMap Gallery Semiconductor Physics and Devices
Semiconductor physics is a discipline that studies the atomic and electronic states of semiconductors and the internal electronic processes of various semiconductor devices. Is a branch of solid state physics. The study of atomic states in semiconductors is based on crystal structure and lattice dynamics. It mainly studies the crystal structure and crystal growth of semiconductors, as well as impurities and various types of defects in crystals.
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This is a mind map about plant asexual reproduction, and its main contents include: concept, spore reproduction, vegetative reproduction, tissue culture, and buds. The summary is comprehensive and meticulous, suitable as review materials.
This is a mind map about the reproductive development of animals, and its main contents include: insects, frogs, birds, sexual reproduction, and asexual reproduction. The summary is comprehensive and meticulous, suitable as review materials.
Semiconductor Physics and Devices
Necessary knowledge for self-study
Quantum mechanics
advanced mathematics
partial differential
Derivative
Some knowledge of college physics
Notes on formulas
1. Pay attention to boundary conditions and scene constraints
2. Expression
(1), the meaning expressed by the formula
(2) The meaning of the letters
(3) Different books have different expressions, but the meaning may be the same.
The state of electron motion in a crystal
solid lattice structure
Semiconductor material
Classification
Element Semiconductor
compound semiconductor
Substance classification
Conductivity: conductors, semiconductors, insulators
Form: solid, liquid, gas
solid lattice
Grid points: Pay attention to the lattice
Lattice: the entire lattice structure
grid vector, grid vector
Unit cell: A small number of lattice points correspond to a small number of crystals Unit cell: The smallest unit cell used to replicate the entire crystal
Note: The possibility of selecting an orthogonal edge unit cell is smaller than the possibility of selecting an orthogonal unit cell.
basic lattice structure
Simple cube
body centered cube
face-centered cube
Crystal plane, Miller index (describes the plane)
Crystallographic orientation: the orientation of parallel lines
Impurities and Defects
Point defects, line defects, surface defects
Substitutional impurities, interstitial impurities
Quantum mechanics
Three basic principles
energy quantization
Wave-particle duality: λ=h/p (λ reflects the wave nature, p reflects the particle nature)
uncertainty principle
Schrödinger equation
Wave function (note: probability wave)
Free electrons and bound electrons
Free electrons: not subject to any external force
Bound electrons: Electrons in a one-dimensional infinitely deep potential well, their movement space is limited within the one-dimensional infinitely deep potential well.
Single electron: represents: H atom
Quantum number n
Angular quantum number ι=n-1
Magnetic quantum number|m|=n-1
Polyelectrons: their quantum states are discrete
Electronic motion state
energy band formation
electronic communization
Allowed
forbidden band
hybridization
sp hybrid orbital
One-dimensional infinite crystal energy band
Kronik-Panner model
Schrödinger equation
Boundary conditions, non-zero solution conditions
k-space energy band diagram
carrier
electronic
hole
Balance carrier concentration in semiconductors
Density of state function and Fermi release function
state density function
Fermi-Dirac distribution function
equilibrium carrier concentration
formula
Intrinsic semiconductor: A pure semiconductor that has no other impurities and no lattice defects.
Product of carrier concentration
Intrinsic Fermi level position
1. When the effective electron mass of the electron and the effective electron mass of the hole are equal, the intrinsic Fermi level is strictly in the center of the forbidden band.
2. When the two are out of phase, the state density function of the conduction band electrons and the state density function of the valence band holes are asymmetric. Therefore, in order to make the intrinsic electron concentration and the intrinsic hole concentration equal, the intrinsic Fermi level is also Accordingly, the occurrence and hyperactivity should occur near the center of the forbidden zone.
3. In practice, the effective mass of electrons in the conduction band and the effective mass of holes in the valence band of semiconductor materials are not equal. Strictly speaking, the position of the intrinsic Fermi level deviates from the center of the forbidden band at this time, but the deviation is very small due to various reasons. , in future calculations and applications, this deviation is ignored, and the intrinsic Fermi level is approximately considered to be in the center of the forbidden band.
Impurity semiconductor carrier concentration with only one impurity
Donor impurities: generated due to the introduction of impurities, are called donor electrons, corresponding to the doping of donor impurities.
Acceptor impurity: After doping with other elements, it accepts electrons in the valence band for ionization and generates holes in the valence band.
Electricity Neutrality Condition: All positively charged charge densities present inside a uniformly doped thermally balanced semiconductor are equal to all negatively charged charge densities.
Extrinsic Semiconductor: Doped Semiconductor
Compensation semiconductor
Definition: A semiconductor containing both donor and acceptor impurities.
Classification
P-type compensation semiconductor: Na>Nd
N-type compensation semiconductor: Na<Nd
Fully compensated semiconductor: Na=Nd
Fermi level position
1. The Fermi level moves to both sides of the forbidden band as the doping concentration increases.
2. The Fermi level also changes with temperature. As the temperature increases, the Fermi level of both N-type and P-type semiconductors moves closer to the center of the forbidden band. This result is consistent with the behavior of semiconductors in the intrinsic excitation region with the highest temperature, because It satisfies 10=po, so the Fermi level also approaches the intrinsic Fermi level, which is the center of the forbidden band.
3. When the Fermi level is located in the center of the forbidden band, it is an intrinsic semiconductor.
Degenerate Semiconductor
carrier concentration
Classification: When the doped impurity concentration is small (compared to Nc, Nv), it is called a non-degenerate semiconductor. When the doped impurity degree is large (larger than Nc, Nv), it is called a degenerate semiconductor. Given that the one between the two is called a weakly degenerate semiconductor.
Bandgap narrowing effect: the lower position of the conduction band is lowered and the bandgap width is narrowed.
carrier transport
Drift motion: Because the carrier is charged, it moves under the action of the electric field.
Carrier scattering and mobility
scattering
Ionized impurity scattering
Lattice vibrational scattering
Mobility versus temperature and doping concentration
Resistivity: ρ=1/σ=1/e (Nμn Pμp)
Saturation velocity and strong field mobility
diffusion movement
Diffusion: The process by which carriers move from a high concentration area to a low concentration area under the influence of concentration gradient.
Einstein relationship
Mobility: A quantity that describes the ease with which carriers move under the influence of an external electric field.
Diffusion coefficient: A quantity that describes the ease with which carriers move under the influence of concentration gradients
Einstein's relationship is the relationship between Miao's carrier mobility and diffusion coefficient
excess carriers
Generation and recombination of carriers
definition
Generation: generation of carriers
Recombination: disappearance of carriers
production rate and recombination rate
Generation rate: how quickly carriers are generated
Recombination rate: how quickly carriers disappear
Source: temperature, light, etc.
Factors affecting carrier recombination: electrons, holes, etc.
Generation and recombination of carriers under thermal equilibrium
Carrier recombination under non-equilibrium
nature
continuity equation
diffusion equation
Bipolar transport and its equations
Definition: Excess electrons and excess holes will be closely connected to drift or diffuse together with a single mobility or diffusion coefficient.
bipolar transport equation
Bipolar transport equation under small injection
For P-type semiconductors, assuming P0>>n0, small injection conditions: excess carrier concentration is much smaller than the thermal equilibrium majority carrier hole concentration, that is, p0>>δn=δp. The opposite is true for N-type semiconductors.
application
Quasi-Fermi level
EF
EF
EFn-EFp=qV
PN junction
According to the impurity distribution on both sides of the metallurgical junction
Mutation knot (when the concentration on one side is much greater than the other side - one-sided mutation knot)
linear grade junction
equilibrium carrier
Many children
P area: hole pp0=NA
N area: electron nn0=ND
Young son
P area: electron np0
N area: hole pn0
Space charge region (N points to P)
Positive and negative ionized impurities have equal charges
Under equilibrium state, the net hole and electron current density is 0 -> Derivation of Vbi
General PN junction built-in potential
Abrupt junction built-in potential
At room temperature, Si Vbi 0.8V
Ge Vbi 0.35V
Depletion approximation (carriers completely diffused away) depletion region
The electric field distribution in the space charge region can be derived from the depletion approximation
Derivation of depletion region width
Use Vbi to represent the width of the depletion region
Depletion zone width of single-sided mutation junction
neutral approximation neutral zone
The above-derived formulas for balanced PN junctions can be extended to the case where there is an external voltage. If it is assumed that the external voltage all falls on the depletion region, then Vbi in the formula only needs to be replaced by Vbi-V Note: 1. The reference direction of the applied voltage is opposite to Vbi, and V<=Vbi 2. When V approaches Vbi, a large current situation will occur, and the voltage drop in the quasi-neutral region cannot be ignored.
Balanced PN junction energy band diagram and carrier distribution in space charge region
Energy band diagram
barrier area
Carrier distribution in space charge region
equilibrium carrier concentration
n0(x)
p0(x)
Movement of carriers in PN junction with external bias voltage
At equilibrium
Diffusion equals drift
Forward bias V>0
The barrier height becomes q(Vbi-V)
Diffusion is greater than drift
The potential barrier decreases linearly with the applied voltage, but the minority carrier distribution changes exponentially with the energy level position (Boltzmann distribution)
Since the source of forward current is N-region electrons and P-region holes, both of which are multipliers, the forward current is large.
forward current density
hole current density
electron current density
Reverse bias V<0
The barrier height becomes q(Vbi-V)
Drift is greater than diffusion
Since there are limited minority carriers near the interface, the reverse current will saturate.
Since the source of the reverse current is the minority carrier, the reverse current is very small and saturated.
The reason why the reverse current is very small and saturated
reverse current density
hole current density
electron current density
Ideal PN junction DC current and voltage characteristics
Solution ideas
Without considering the potential barrier area, Jn and Jp are constants.
Jn(xn)=Jn(-xp)
Jp(xn)=Jp(-xp)
Minority birth distribution
Minority carrier distribution under external bias voltage, knot law
Diffusion current
Factors affecting reverse saturation current
Material type
Doping concentration
temperature
Effect of current recombination in barrier region on IV characteristics of PN junction
Barrier region generates recombination current
forward
J=Jdp Jdn Jr
reverse
J=Jdp Jdn Jg
Calculation of composite current
large injection effect
small injection conditions
Large injection conditions
Large injection current concentration
Self-constructed electric field under large injection
Metal-Semiconductor Contacts and Heterojunctions
metal semiconductor contact
Work functions of metals and semiconductors
Ideal metal-to-semiconductor contact
Note: barrier layer Anti-barrier layer
Ideal semiconductor contact properties
The conductor performance of the structure formed by metal and semiconductor has nothing to do with the external bias voltage and is always low impedance.
Metal semiconductors mostly use polyons, and those that use polyons are thermionic emission theory; Homogeneous pn junction uses minority carriers and uses the storage effect of pn junction.
Current-Voltage Relationship
Ohmic contact: When the semiconductor is connected to the positive electrode of the power supply, the amount of energy band bending is reduced, and electrons can easily pass through the potential barrier and flow from the metal to the semiconductor.
Heterojunction
Classification
inversion heterojunction
homojunction
Its energy band diagram
Abrupt inversion heterojunction built-in electric field and space charge region width
mutant homojunction
Current-Voltage Characteristics of Heterojunctions
Current transport model in mutant inversion heterojunction
heterojunction barrier
Negative peak barrier mutation pn junction current-voltage characteristics: The value of electron current is smaller than the value of hole current.
Positive peak barrier: When at the heterojunction interface, the barrier peak position of the N-type semiconductor with a large bandgap is higher than the conduction band bottom of the P-type semiconductor with a large bandgap outside the barrier area.
Current transport model in mutant homoheterojunctions