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PN JUNCTION DIODE
PN Junction Formation
Depletion Region Formation
At the instant of junction formation
Energy Diagram of PN Junction
At Equilibrium
Energy Diagram of PN Junction
Width of the depletion layer of an open circuited PN junction
Barrier Potential of an open circuited PN junction
Type of the semiconductor material
Intrinsic concentration of Si or Ge before doping
Amount of Doping (on P & N sides)
Temperature
Factors deciding the Barrier Potential Value
Depletion Width Penetration as a function of Doping Concentration
Depletion Width Penetration as a function of Doping Concentration
Depletion Width Penetration as a function of Doping Concentration
PN Junction Diode
Diode under Forward Bias
Diode under Forward Bias
Diode under Reverse Bias
Diode under Reverse Bias
Reverse Current
It occurs for high reverse bias voltage
Impact IonizationAvalanche EffectReverse Breakdown Voltage
Reverse Breakdown
VI Characteristics Curve of a Diode
Resistance Levels
DC or Static Resistance AC or Dynamic
Resistance
VI Characteristics of Si & Ge diodes
Effect of Temperature on VI characteristics of a Diode
Diode Equation
The derivative of a function at a point is equal to the slope of the tangent line drawn at that point
Dynamic Resistance
Dynamic Resistance
It is defined as the flow of electric current due to the motion of the charge carriers under the influence of an external electric field
Drift Current
Equation for Drift Current Density
It is defined as the movement of charge carriers taking place from higher concentration region to lower concentration region of the same type of charge carriers under the presence of concentration gradient
Diffusion Current
Diffusion Current
Equation for Diffusion Current Density
It is the sum of drift current & diffusion current
Total Current in a Semiconductor
Einstein Relationship for Semiconductor
Depletion width (d) will increase with increased Reverse-bias potential, the resulting transition capacitance CTwill decrease
Transition or Depletion Region or Space charge Capacitance (CT)
CD exists in the forward bias region
CD is defined as rate of change of injected charge with applied voltage
Diffusion or Storage Capacitance(CD)
Transition & Diffusion Capacitance
Ideal Diode Model
Practical Diode Model
Complete Diode Model
The concentration of NA & ND are constant throughout the p and n sides
The doping density changes abruptly from p-type to n-type
Step Graded Junction
Step Graded Junction
Current Components in PN Junction Diode
Current Components in PN Junction Diode (fig 1)
Two diffusion currents as a function of distance x from the junction can be defined as
1. Inp(x) = Diffusion current due to electrons on the P-side as a function of x.
2. Ipn(x) = Diffusion current due to holes on the N-side as a function of x.
Inp(x) & Ipn(x) are two minority currents
Current Components in PN Junction Diode
A. Currents at the junction (x=0)I = Inp(0) + Ipn(0)
Diffusion currents due to electrons & holes at the junction (for x=o) will be in the same direction
I = the current at the junction, that is, the total current.
Current Components in PN Junction Diode
B. But, the total current should remain constant
These diffusion currents Inp(x) & Ipn(x) decrease exponentially with increase in x
This means that on both sides, there must be some other components of current present which can actually maintain the current I constant
Current Components in PN Junction Diode
C. On P-sideInp(x) + Ipp(x) = I
Ipp(x) = majority carrier current due to holes
Current Components in PN Junction Diode
D. On N-sideIpn(x) + Inn(x) = I
Inn(x) = majority carrier current due to electrons
Current Components in PN Junction Diode
The figure 1 is drawn for an unsymmetrically doped diode so that
Ipn ≠ Inp
Current Components in PN Junction Diode
Rectifier CircuitsClipping circuitsClamping circuitsDemodulation circuitsSwitch in digital logic circuits used in computers
Application of PN Junction Diode
Electronic devices by Floyd Electronic devices & circuits by
Salivahanan Electronic devices & circuits by Millman
& Halkias
Reference