Lecture 7 amp 8 Hierarchy of Semiconductor Models Introduction Nowadays semiconductor materials are contained in almost all electronic devices Some examples of semiconductor devices and their use are described in ID: 728402
Download Presentation The PPT/PDF document "Modelling & Simulation of Semiconduc..." is the property of its rightful owner. Permission is granted to download and print the materials on this web site for personal, non-commercial use only, and to display it on your personal computer provided you do not modify the materials and that you retain all copyright notices contained in the materials. By downloading content from our website, you accept the terms of this agreement.
Slide1
Modelling & Simulation of Semiconductor Devices
Lecture 7 & 8
Hierarchy of Semiconductor ModelsSlide2
Introduction
Nowadays, semiconductor materials are contained in almost all electronic
de-vices
.
Some
examples of semiconductor devices and their use are described in
the following.
Some examples of semiconductor devices and their use are described in
the following.
Photonic devices
capture light (photons) and convert it into an
electronic signal
. They are used in camcorders, solar cells, and light-wave
communication
systems as optical
fibers
.Slide3
Introduction
Optoelectronic
emitters
convert an electronic signal into light.
Examples are
light-emitting diodes (LED) used in displays and indication lambs
and semiconductor
lasers used in compact disk systems, laser printers, and
eye surgery.
Flat-panel
displays
create an image by controlling light that either
passes through
the device or is
reflected off
of it. They are made, for instance,
of liquid
crystals (liquid-crystal displays, LCD) or of thin semiconductor
films (
electroluminescent displays
).
In
field-effect
devices
the conductivity is modulated by applying an
electric field
to a gate contact on the surface of the device. The most
important field-effect
device is the MOSFET (metal-oxide semiconductor
field-effect transistor
), used as a switch or an
amplifier
. Integrated
circuits
are
mainly made
of MOSFETs.Slide4
Introduction
Quantum devices
are based on quantum mechanical phenomena, like
tunneling
of electrons through potential barriers which are impenetrable
classically
. Examples are resonant tunneling diodes,
super lattices
(
multi-quantum-well
structures), quantum wires in which the motion of carriers is
restricted
to one space dimension and
confined
quantum mechanically in
the other
two directions, and quantum dots
.
Clearly, there are many other semiconductor devices which are not
mentioned (
for instance, bipolar transistors, Schottky barrier
diodes
, thyristors).
Other new developments
are, for instance, nanostructure devices (
hetero-structures
) and
solar cells
made of amorphous silicon or organic semiconductor
materials.Slide5
Introduction
Usually, a semiconductor device can be considered as a device which needs
an input
(an electronic signal or light) and produces an output (light or an
electronic signal
).
The
device is connected to the outside world by contacts at which
a voltage
(potential
difference
) is applied
.
We are mainly interested in
devices which
produce an electronic signal, for instance the macroscopically
measurable electric
current (electron
flow
), generated by the applied bias
.
In this situation
, the
input parameter is the applied voltage and the output parameter is the
electric current
through one contact.Slide6
Introduction
The relation between these two physical quantities
is called
current-voltage characteristic. It is a curve in the two-dimensional
current-voltage
space.
The
current-voltage characteristic does not need to be a
monotone function
and it does not need to be a function (but a relation
).
The main objective of this
subject
is to derive mathematical models which
describe
the electron
flow
through a semiconductor device due to the application
of a
voltage.Slide7
Introduction
Depending on the device structure, the main transport phenomena
of the
electrons may be very
different
, for instance, due to drift,
diffusion
,
convection
, or quantum mechanical
effects
.
For
this reason, we have to devise
different mathematical
models which are able to describe the main physical
phenomena for
a particular situation or for a particular device
.
This leads to a hierarchy of semiconductor models.Slide8
Hierarchy of Semiconductor Models
Roughly speaking, we
can divide
semiconductor models in three classes
:
Quantum models
Kinetic
models
Fluid dynamical
(macroscopic)
models
In order to give some flavor of these models
and the methods used to derive them, we explain these three view-points
: quantum
, kinetic and
fluid dynamic
in a
simplified
situation.Slide9
Quantum Models
Consider a single electron of mass
m
and
elementary charge
q
moving in a vacuum under the action of an electric
field
E = E(x; t
)
.
The motion of the electron in space
and
time
t > 0
is governed by
the single-particle
Schrodinger equationWith some initial condition
Slide10
Quantum ModelsSlide11
Quantum ModelsSlide12
Fluid Dynamic Model
In order to derive fluid dynamical
models,
for instance
, for the evolution of the particle density
n
and the current density
J
;
we assume
that the wave function can be decomposed in its amplitude
and
phase
.
Slide13
Fluid Dynamic Model
The current density is now calculated asSlide14
Semiconductor Crystal
A solid is made of an
infinite three-dimensional
array of atoms arranged
according
to a latticeSlide15
Semiconductor Crystal
The state of an electron moving in this periodic potential is described
Schrodinger
equation:Slide16
Home Work
Apply Madelung Transform on above equation to obtain Fluid dynamical model of
electron moving in
periodic
potential
in semiconductor crystal. Slide17
End of Lectures 7-8
To download this lecture visit
http://imtiazhussainkalwar.weebly.com/
17