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CARRIER TRANSPORT - Coggle Diagram
CARRIER TRANSPORT
Transport Mechanism
Diffusion (Paramees)
Current
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q= electric charge,D = Diffusion constant, dn/dx =change in carriers with distance.
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Diffusion of carriers due to the existence of carrier gradient.
The carrier gradient is due to temperature and dopant ion concentration.
The charge carriers will move from high density region to low density region of carriers.This movement of carriers is called the diffusion current
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Drift (Uziel)
Carrier mobility
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The mobility of a carrier is defined as the ratio of carrier's speed and the applied E-field strength, which is proportional to the relaxation time and inversely proportional to the effective mass of the carrier
Current
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The moving charge carrier will produce a net current in the material. The current density depends on the charge density and the velocity.
For low E-field the v-E relation is linear, however for high E-field the speed will reach the saturation velocity.
When an E-field is applied, charge carriers' will move parallel to the field's direction. Their speed is assumed to be constant due to collision and scattering.
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Characteristics
Excitation (Sarah)
- Excitation of electron into higher energy level by
light/photon or Electric field.
- Example of electron excitation process is Auger recombination.
Carrier Excitation
Scattering
Without E field (Atiqah)
Thermal Velocity
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In the absence of an electric field, electrons in a semiconductor move randomly because of thermal motion.
The thermal velocity is the average speed at which electrons (or holes) move between two successive collisions.
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The carrier moves randomly in the absence of an applied electric field, moves quickly through the semiconductor, and frequently changes directions as a result of scattering.
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With E field (Anis)
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Average Carrier Velocity
By combining Newton's law and scattering force, we get:
:smiley: When an electric field is applied, the random motion still occurs and it has average net motion along the direction of the field.
:smiley: Charge carrier do not follow straight lines instead they bounce and change direction and v.
Recombination (Sarah)
processes by which a conduction band electron loses energy and re-occupies the energy state of an electron hole in the valence band.
Carrier Recombination.There are three type of recombination - Band to Band - Trap-assisted - Auger recombination
Band to Band: emitted photon has an energy similar to the band gap and only weakly absorbed
Trap-assisted: electron is likely to be re-emitted to the conduction band edge
Auger recombination : energy is given to a third carrier, an electron in the conduction band