PN Junction
Engineering Physics • 1st Semester
Introduction to PN Junction
• • A PN junction is formed by joining P-type
and N-type semiconductors.
• • It is the fundamental unit of diodes,
transistors, LEDs, and solar cells.
• • Controls how current flows in electronic
devices.
• • Key concepts: diffusion, depletion region,
biasing, energy bands.
P-type Semiconductor
• • Doped with trivalent impurities (Boron,
Gallium).
• • Creates 'holes' which act as positive charge
carriers.
• • Majority carriers: Holes
• • Minority carriers: Electrons
• • Used to form one side of the PN junction.
N-type Semiconductor
• • Doped with pentavalent impurities
(Phosphorus, Arsenic).
• • Provides extra electrons for conduction.
• • Majority carriers: Electrons
• • Minority carriers: Holes
• • Forms the other half of the PN junction.
Formation of PN Junction
• • When P and N materials are joined,
electrons diffuse to P-side and holes diffuse to
N-side.
• • This creates a region with no free carriers
called the depletion region.
• • Immobile ions remain, forming an internal
electric field.
• • This electric field opposes further carrier
movement.
Depletion Region
• • Also called the space-charge region.
• • Contains immobile positive and negative
ions.
• • Acts like an insulating barrier.
• • Wider depletion region → harder for current
to pass.
• • Narrow depletion region → easier current
flow.
Energy Band Explanation
• • PN junction energy bands bend due to built-
in electric field.
• • P-side has higher energy holes; N-side has
higher energy electrons.
• • At equilibrium, Fermi level becomes
constant.
• • Band bending creates the potential barrier
preventing current flow.
Forward Biasing the PN Junction
• • Positive terminal is connected to P-side,
negative to N-side.
• • External voltage reduces the depletion
barrier.
• • Majority carriers cross the junction, allowing
current to flow.
• • Depletion region becomes narrow.
Reverse Biasing the PN Junction
• • Positive terminal connected to N-side,
negative to P-side.
• • Increases the barrier potential.
• • Depletion region widens.
• • Only a tiny leakage current flows.
• • No conduction of majority carriers.
I–V Characteristics of PN Junction
• Forward Bias:
• • Current increases exponentially after
threshold voltage (≈ 0.7V for Si).
• Reverse Bias:
• • Very small leakage current.
• • Breakdown occurs at high reverse voltage
(Zener or Avalanche breakdown).
Applications of PN Junction
• • Rectifiers (AC to DC Conversion)
• • LEDs and Laser Diodes
• • Photodiodes and Solar Cells
• • Transistors (BJT, MOSFET)
• • Voltage Regulators (Zener)
• • Signal Clipping and Clamping Circuits

PN_Junction_FullContent_Professional.pptx

  • 1.
  • 2.
    Introduction to PNJunction • • A PN junction is formed by joining P-type and N-type semiconductors. • • It is the fundamental unit of diodes, transistors, LEDs, and solar cells. • • Controls how current flows in electronic devices. • • Key concepts: diffusion, depletion region, biasing, energy bands.
  • 3.
    P-type Semiconductor • •Doped with trivalent impurities (Boron, Gallium). • • Creates 'holes' which act as positive charge carriers. • • Majority carriers: Holes • • Minority carriers: Electrons • • Used to form one side of the PN junction.
  • 4.
    N-type Semiconductor • •Doped with pentavalent impurities (Phosphorus, Arsenic). • • Provides extra electrons for conduction. • • Majority carriers: Electrons • • Minority carriers: Holes • • Forms the other half of the PN junction.
  • 5.
    Formation of PNJunction • • When P and N materials are joined, electrons diffuse to P-side and holes diffuse to N-side. • • This creates a region with no free carriers called the depletion region. • • Immobile ions remain, forming an internal electric field. • • This electric field opposes further carrier movement.
  • 6.
    Depletion Region • •Also called the space-charge region. • • Contains immobile positive and negative ions. • • Acts like an insulating barrier. • • Wider depletion region → harder for current to pass. • • Narrow depletion region → easier current flow.
  • 7.
    Energy Band Explanation •• PN junction energy bands bend due to built- in electric field. • • P-side has higher energy holes; N-side has higher energy electrons. • • At equilibrium, Fermi level becomes constant. • • Band bending creates the potential barrier preventing current flow.
  • 8.
    Forward Biasing thePN Junction • • Positive terminal is connected to P-side, negative to N-side. • • External voltage reduces the depletion barrier. • • Majority carriers cross the junction, allowing current to flow. • • Depletion region becomes narrow.
  • 9.
    Reverse Biasing thePN Junction • • Positive terminal connected to N-side, negative to P-side. • • Increases the barrier potential. • • Depletion region widens. • • Only a tiny leakage current flows. • • No conduction of majority carriers.
  • 10.
    I–V Characteristics ofPN Junction • Forward Bias: • • Current increases exponentially after threshold voltage (≈ 0.7V for Si). • Reverse Bias: • • Very small leakage current. • • Breakdown occurs at high reverse voltage (Zener or Avalanche breakdown).
  • 11.
    Applications of PNJunction • • Rectifiers (AC to DC Conversion) • • LEDs and Laser Diodes • • Photodiodes and Solar Cells • • Transistors (BJT, MOSFET) • • Voltage Regulators (Zener) • • Signal Clipping and Clamping Circuits