Physics of Semiconductor Devices - PowerPoint PPT Presentation

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Physics of Semiconductor Devices

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Physics of Semiconductor Devices Formation of PN - Junction When a P-type Semiconductor is joined together with an N-type Semiconductor a PN junction is formed. – PowerPoint PPT presentation

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Title: Physics of Semiconductor Devices


1
Physics of Semiconductor Devices
2
  • Formation of PN - Junction
  • When a P-type Semiconductor is joined together
    with an N-type Semiconductor a PN junction is
    formed. And it is also known as a Semiconductor
    Diode.
  • Semiconductor diodes are widely used in
    Rectifiers which converts input AC signal into
    DC output signal.

3
Formation of a PN-junction
P
N
Space charge region
(OR)
Depletion region
Potential barrier height(V0)
Potential barrier width (W)
4
  • Depletion Region Space Charge
  • The diffusing majority carriers from the two
    regions recombine near the junction and
    disappear.
  • The uncompensated Acceptor and Donor ions set up
    an Electric field which halts majority carrier
    Diffusion and causes minority carrier Drift.
  • The two kinds of majority carriers diffusing
    across the junction meet each other near the
    junction and undergo recombination's, leaving
    negative ions on the P-side and positive ions on
    the N-side of the junction.
  • This distribution of Positive and Negative
    Charges is called Space charge.

5
Diode Symbol
N
P
Cathode
Anode
6
Energy level diagram
7
  • V - I Characteristics of PN Junction
  • The diode can be operated in two different ways,
    as Forward and Reverse bias.
  • When positive terminal of the battery is
    connected to the P-type negative terminal is to
    the N-type of the PN-junction diode, known the
    diode is kept in forward bias.
  • When negative terminal of the battery is
    connected to the P-type positive terminal is to
    the N-type of the PN-junction diode, known the
    diode is kept in reverse bias.

8
Open circuit PN -junction
P
N
Space charge region
P
N
Forward bias
VF
9
Open circuit PN -junction
P
N
Space charge region
P
N
Reverse bias
VR
10
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11
From the graph the following points are noted.
  • The region between knee voltage breakdown
  • voltage is known as non-ohmic region.
  • Above the knee breakdown voltage the current
  • increases.
  • Breakdown voltage is due to thermally broken
  • covalent bonds.
  • Diode is conducting in forward bias
  • non-conducting in reverse bias.

12
  • Rectifiers
  • A Rectifier is a device which converts
    alternating current to direct or unidirectional
    current.
  • Rectifiers are mainly three types
  • 1.Half wave Rectifiers
  • 2.Full wave Rectifiers
  • 3.Bridge Rectifiers

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14
Full Wave Rectifier
15
Efficiency of a Rectifier The efficiency of a
Rectifier is defined as the ratio of D.C. out
put power to the A.C. input power supplied to
the Rectifier.
16
  • Light emitting diodes
  • LED s are the most visible type of diode, that
    emits a fairly visible colored light, invisible
    infra-red or laser type light when a forward
    current is passed through them.
  • Principle
  • Basically LED are made from a very thin layer
    of fairly heavily doped semiconductor material.
  • When the diode is forward biased, electrons
    from conduction band combine with holes from in
    valence band, releasing sufficient energy to
    produce photons of light.

17
Semiconductor material Wave length Color Vf _at_ 20mA
GaAs 850-940nm Infra-Red 1.2V
GaAsP 630-660nm Red 1.8v
GaAsP 605-620nm Amber 2.0v
GaAsPN 585-595nm yellow 2.2v
GaP 550-570nm Green 3.5v
SiC 430-505nm Blue 3.6v
GAInN 450nm white 4.0v
18
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19
Current I(MA)
V
20
  • Photo diode
  • A photodiode is a diode optimized to produce an
    electron current flow in response to irradiation
    by ultraviolet, visible, or infrared light.
  • Silicon, Ge gallium arsenide is most often
    used to fabricate photodiodes.
  • Few electron-hole pairs in the N and Pregions,
    and most in the depletion region contribute to
    photo current.

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