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Lecture 14 OUTLINE pn Junction Diodes (cont d) Transient response: turn-on Summary of important concepts Diode applications Varactor diodes Tunnel diodes – PowerPoint PPT presentation

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Title: OUTLINE


1
Lecture 14
  • OUTLINE
  • pn Junction Diodes (contd)
  • Transient response turn-on
  • Summary of important concepts
  • Diode applications
  • Varactor diodes
  • Tunnel diodes
  • Optoelectronic diodes
  • Reading Pierret 9 Hu 4.12-4.15

2
Turn-On Transient
  • Consider a pn diode (Qp gtgt Qn)

i(t)
Dpn(x)
t
vA(t)
x
xn
t
For t gt 0
Lecture 14, Slide 2
EE130/230A Fall 2013
3
  • By separation of variables and integration, we
    have
  • If we assume that the build-up of stored charge
    occurs quasi-statically so that
  • then

Lecture 14, Slide 3
EE130/230A Fall 2013
4
  • If tp is large, then the time required to turn on
    the diode is approximately DQ/IF

Lecture 14, Slide 4
EE130/230A Fall 2013
5
Summary of Important Concepts
  • Under forward bias, minority carriers are
    injected into the quasi-neutral regions of the
    diode.
  • The current flowing across the junction is
    comprised of hole and electron components.
  • If the junction is asymmetrically doped (i.e. it
    is one-sided) then one of these components will
    be dominant.
  • In a long-base diode, the injected minority
    carriers recombine with majority carriers within
    the quasi-neutral regions.

Lecture 14, Slide 5
EE130/230A Fall 2013
6
  • The ideal diode equation stipulates the
    relationship between JN(-xp) and JP(xn)
  • For example, if holes are forced to flow across a
    forward-biased junction, then electrons must also
    be injected across the junction.

Lecture 14, Slide 6
EE130/230A Fall 2013
7
  • Under reverse bias, minority carriers are
    collected into the quasi-neutral regions of the
    diode.
  • Minority carriers generated within a diffusion
    length of the depletion region diffuse into the
    depletion region and then are swept across the
    junction by the electric field.
  • The negative current flowing in a reverse-biased
    diode depends on the rate at which minority
    carriers are supplied from the quasi-neutral
    regions.
  • Electron-hole pair generation within the
    depletion region also contributes negative diode
    current.

Lecture 14, Slide 7
EE130/230A Fall 2013
8
pn Junction as a Temperature Sensor
C. C. Hu, Modern Semiconductor Devices for ICs,
Figure 4-21
Lecture 14, Slide 8
EE130/230A Fall 2013
9
Varactor Diode
  • Voltage-controlled capacitance
  • Used in oscillators and detectors
  • (e.g. FM demodulation circuits in your radios)
  • Response changes by tailoring doping profile

Lecture 14, Slide 9
EE130/230A Fall 2013
10
Optoelectronic Diodes
Lecture 14, Slide 10
EE130/230A Fall 2013
R.F. Pierret, Semiconductor Fundamentals, Figure
9.2
11
Open Circuit Voltage, VOC
Lecture 14, Slide 11
EE130/230A Fall 2013
C. C. Hu, Modern Semiconductor Devices for ICs,
Figure 4-25(b)
12
Solar Cell StructureCyferz at en.wikipedia
Lecture 14, Slide 12
EE130/230A Fall 2013
13
Textured Si surface for reduced reflectance
  • Achieved by anisotropic wet etching (e.g. in KOH)

M. A. Green et al., IEEE Trans. Electron Devices,
Vol. 37, pp. 331-336, 1990
P. Papet et al., Solar Energy Materials and Solar
Cells, Vol. 90, p. 2319, 2006
EE130/230A Fall 2013
Lecture 14, Slide 13
14
p-i-n Photodiodes
  • W ? Wi-region, so most carriers are generated in
    the depletion region
  • ? faster response time (10 GHz operation)
  • Operate near avalanche to amplify signal

R.F. Pierret, Semiconductor Fundamentals, Figure
9.5
Lecture 14, Slide 14
EE130/230A Fall 2013
15
Light Emitting Diodes (LEDs)
  • LEDs are made with compound semiconductors
    (direct bandgap)

R.F. Pierret, Semiconductor Fundamentals, Figure
9.13
R.F. Pierret, Semiconductor Fundamentals, Figure
9.15
Lecture 14, Slide 15
EE130/230A Fall 2013
16
  • Question 1 (re Slide 12) Why are the contacts
    to the back (non-illuminated) side of a solar
    cell made only at certain points (rather than
    across the entire back surface)?
  • Answer To increase energy conversion efficiency
  • The absorption depth (average distance a photon
    travels before transferring its energy to an
    electron) for long-wavelength photons is greater
    than the Si thickness.
  • ? The bottom surface oxide and metal layer
    effectively form a mirror that reflects light
    back into the silicon.
  • There is more recombination in heavily doped
    contacts than at a good Si/SiO2 interface most
    of the back surface should be covered by SiO2 so
    that generated carriers have a high probability
    of diffusing to the depletion region before they
    recombine.

EE130/230A Fall 2013
Lecture 14, Slide 16
17
  • Question 2 (re Slide 15) What limits the
    lifetime of an LED?
  • Answer
  • LED lifetime is defined to be the duration of
    operation after which the light output falls to
    only 70 of original.
  • (Even afterwards, the LED will continue to
    function.)
  • The power density of an LED can be high (up to 10
    W/cm2, comparable to an electric stove top),
    causing significant heating which can degrade the
    light output through various mechanisms
  • Degradation of epoxy package causing partial
    absorption of light
  • Mechanical stress weakening the wire bond
    (electrical connection)
  • Formation/growth of crystalline defects, or
    diffusion of metal into the semiconductor,
    resulting in increased recombination via mid-gap
    states

EE130/230A Fall 2013
Lecture 14, Slide 17
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