View
226
Download
0
Embed Size (px)
Citation preview
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 1/15
Agenda
• Horario de Clase: Lunes 6:30pm – 9:30pm
• Cursos pasados (Background)
• El Programa y las Reglas de Juego.
• La Importancia del Inglés en este curso y en la
vida misma
05/03/2012 Basic Electronics 1
A Lumped Element
-Quantum Mechanics-Statistical Mechanics
-Solid State
-
-…
01/03/2012 Fundamentals of Electronics - Lecture 1 2
The behavior at the terminals is more important than the details of the behavior
Internal to the black box
Introduction to SemiconductorPh sics
05/03/2012 3Basic Electronics
Introduction
• Materials can be described according to their
properties.
• We are interested in the electrical properties.
• T ere are t ree in s o materia s
– Conductor
– Semiconductor
– Insulator
05/03/2012 4Basic Electronics
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 2/15
Material
Conductor Insulator Semiconductor
A conductor is a material
that easily conducts
electrical current.
Single-element materials:
-copper, silver, gold, and
aluminum
It does not conduct
electrical current under
normal conditions.
Most good insulators are
compounds rather than
-
A semiconductor in its
pure (intrinsic) state is
neither a good conductornor a good insulator.
The most common
-
05/03/2012 Basic Electronics 5
Atoms with only one
valence electron very
loosely bound to the atom
Therefore, a conductive
material has many free
electrons that when moving in
the same direction, make up
the current.
-rubber, plastics, glass,
mica, and quartzsemiconductors:
-silicon, germanium, and
carbon.
We can also find
compounds
Valence electrons are
tightly bound to the
atoms;
there are very few free
electrons in an insulator.
05/03/2012 Basic Electronics 6
Resistivity Values
05/03/2012 Basic Electronics 7
Material
Conductor Insulator Semiconductor
A conductor is a material
that easily conducts
electrical current.
Single-element materials:-copper, silver, gold, and
aluminum
It does not conduct
electrical current under
normal conditions.
Most good insulators are
compounds rather than
sin le-element materials.
A semiconductor in its
pure (intrinsic) state is
neither a good conductor
nor a good insulator.
The most common
-
05/03/2012 Basic Electronics 8
Atoms with only one
valence electron very
loosely bound to the atom
Therefore, a conductive material
has many free electrons that.
when moving in the same
direction, make up the current.
.
semiconductors are
silicon, germanium, and
carbon.
We can also find
compounds.
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 3/15
Morphology
05/03/2012 9Basic Electronics
Solar Cells … $$$$$$
Unit Cells
05/03/2012 10Basic Electronics
Unit Cell: Si, Ge
05/03/2012 11Basic Electronics
Important Semiconducting Materials
05/03/2012 12Basic Electronics
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 4/15
Quantum Phenomena
05/03/2012 13Basic Electronics
Quantum Phenomena I
Photons
Wave-particle duality
05/03/2012 Basic Electronics 14
Discretization – Car Speed?
Mathematics changes
Quantum Phenomena II:
Wave-particle duality
05/03/2012 Basic Electronics 15
Quantum Phenomena III:
Uncertainly Principle
• It is impossible to determine simultaneously both the position
and velocity of an electron with any degree of accuracy or
certainty (Heisenberg).• The result of this principle produces a concept of the atom
,
of where electrons in an atom are most likely to be located.
Bohr Model.
05/03/2012 Basic Electronics 16
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 5/15
Atoms – Generalities
Electronic Distribution and Shells
05/03/2012 17Basic Electronics
Shell 1
Shell 2
05/03/2012 18Shell 3
Atoms – Example: Si
Shell 3
05/03/2012 Basic Electronics 19
Let’s consider carefully this picture!
Shell 1
Take care! Bohr Model
05/03/2012 Basic Electronics 20
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 6/15
Bohr Model VS Quantum Model
05/03/2012 Basic Electronics 21
-The atomic number = the number
of protons in the nucleus (it is the
same as the number of electrons).
-The positive charges cancel the
negative charges, and the atom has
a net charge
-Electrons that are in orbits farther from the nucleus have higher
energy and are less tightly bound to the atom than those closer
05/03/2012 Basic Electronics 22
to the nucleus.
-Electrons with the highest energy -> outermost shell of an atom
and are relatively loosely bound to the atom.
-This outermost shell is known as the valence shell and electrons
in this shell are called valence electrons.
-Valence electrons: contribute to chemical reactions and bonding
within the structure of a material and determine its electrical
properties.
• Each discrete distance (orbit) from the nucleuscorresponds to a certain energy level.
• In an atom, the orbits are grouped into energybands known as shells.
• A given atom has a fixed number of shells. Eachshell has a fixed maximum number of electronsat permissible energy levels (orbits).
• The differences in energy levels within a shell aremuch smaller than the difference in energybetween shells.
• The shells are designated 1, 2, 3 and so on, with1 being closest to the nucleus. Some references
designate shells by the letters K, L M and so on.
05/03/2012 Basic Electronics 23
• The maximum number of electrons (Ne) that can exist in each shell of an
atom is a fact of nature and can be calculated by the formula,
05/03/2012 Basic Electronics 24
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 7/15
Ionization
05/03/2012 25Basic Electronics
Ionization
• Ionization:
– When an atom absorbs energy (from a heat source or fromlight) the energies of the electrons are raised.
– The valence electrons can easily jump to higher orbitswithin the valence shell when external ener is absorbed.
– The departure of a valence electron leaves a previouslyneutral atom with an excess of positive charge (moreprotons than electrons).
– The process of losing a valence electron is known as
ionization, and the resulting positively charged atom iscalled a positive ion.
05/03/2012 Basic Electronics 26
Atoms – Example: Si
Shell 3
05/03/2012 Basic Electronics 27
Let’s consider carefully this picture!
Shell 1
Ionization
• Ionization:
– When an atom absorbs energy (from a heat source or from
light) the energies of the electrons are raised. – The valence electrons can easily jump to higher orbits
within the valence shell when external ener is absorbed.
– The departure of a valence electron leaves a previouslyneutral atom with an excess of positive charge (moreprotons than electrons).
– The process of losing a valence electron is known asionization, and the resulting positively charged atom is
called a positive ion.
05/03/2012 Basic Electronics 28
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 8/15
05/03/2012 Basic Electronics 29 05/03/2012 Basic Electronics 30
05/03/2012 Basic Electronics 31 05/03/2012 Basic Electronics 32
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 9/15
From Atoms to Solids (Crystals)
05/03/2012 33Basic Electronics
More on Atoms: Si Vs Cu
05/03/2012 Basic Electronics 34
The valence electron in copper has more energy than the valence electron in silicon.
This means that it is easier for valence electrons in copper to acquire enough additional
energy to escape from their atoms and become free electrons in the conduction band
than it is in silicon.
More on Atoms: Si Vs GeThe valence electrons in germanium are in the fourth shell while
those in silicon are in the third shell
05/03/2012 Basic Electronics 35
This means that the germanium valence electrons are at higher energy levels than those in
silicon and, therefore, require a smaller amount of additional energy to escape from the
atom.
This property makes germanium more unstable at high temperatures, and this is a basic
reason why silicon is the most widely used semiconductive material.
Covalent Bonds I
-An intrinsic crystal is one that has no
impurities.
-Covalent bonding for germanium is
similar because it also has four valence
electrons.
05/03/2012 Basic Electronics 36
An intrinsic crystal is one that has no impurities.
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 10/15
Covalent Bonds II
05/03/2012 Basic Electronics 37
In a Si crystal, there are billions of Si atoms, each with eight valence electrons.
These valence electrons are covalent bonds that hold the crystal together – that give it solidity.
It produces chemical stability.
Si is almost an insulator @ Troom – That’s why we have to dope☺ !!!
Important Definition: eV
(Let me introduce this concept now)
05/03/2012 Basic Electronics 38
Electronvolt [EV]
• One volt is the potential difference between two points in an
electric circuit when the energy required to move 1 coulomb
of charge (electrons) from one point to the other is 1 joule.
W
Energy [J]
• Applying to an individual electron:
05/03/2012 Basic Electronics 39
Q=ec r ca o en a
Charge [C]
C
W V
1910602.1
1−
×
=
( ( ) eV J V C W 110602.1110602.11919
=×=×=−−
Bands
05/03/2012 40Basic Electronics
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 11/15
-Each shell around the nucleus corresponds
to a certain energy band.
-Each shell is separated from adjacent shells
by energy gaps, in which no electrons can
exist.
At a temperature of absolute 0 Kelvin.
An intrinsic (pure) silicon crystal at room
05/03/2012 Basic Electronics 41
temperature has sufficient heat (thermal
energy) for some valence electrons to
jump the gap from the valence band into
the conduction band, becoming free
electrons. Free electrons are also called
conduction electrons.
☺ Bands come from put toghether
millions of atoms (solid)
05/03/2012 Basic Electronics 42
05/03/2012 Basic Electronics 43 05/03/2012 Basic Electronics 44
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 12/15
05/03/2012 Basic Electronics 45
Conduction in Semiconductors
Electrons and Holes
05/03/2012 46Basic Electronics
Holes
• @ Troom, the heat energy in air causes the atoms in a Si crystal vibrate.
• Temperature: Vibration of atoms!!!
• These vibrations can disloge an electron from the valence orbit.
• Electron gains energy from vibrations and it behaves as a free-electron.
• The departure of the electron creates a vacancy called hole.
• ☺ Holes makes the difference (compared to conductors).
• Generation of holes and free electrons is low because of temperature
(dope it!! )
05/03/2012 Basic Electronics 47
Recombination and Lifetime
05/03/2012 Basic Electronics 48
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 13/15
Processes in a Crystal
05/03/2012 Basic Electronics 49 05/03/2012 Basic Electronics 50
conduction band by external energy, there
is one hole left in the valence band,
creating what is called an electron-hole
pair.
Recombination occurs when a conduction-
band electron loses energy and falls back
into a hole in the valence band.
-This movement of free electrons is one
type of current in a semiconductive material
and is called electron current.
-Electrons remainin in the valence band
-Another type of current occurs in the
valence band, where the holes created by
the free electrons exist.
05/03/2012 Basic Electronics 51
are still attached to their atoms and are not
free to move randomly in the crystal
structure as are the free electrons.
However, a valence electron can move into
a nearby hole with little change in its energy
level, thus leaving another hole where it
came from.
Transport
• @ Troom silicon is an insulator because it has
only few electrons and holes produced by
thermal energy.
05/03/2012 Basic Electronics 52
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 14/15
Transport
05/03/2012 Basic Electronics 53 05/03/2012 Basic Electronics 54
05/03/2012 Basic Electronics 55 05/03/2012 Basic Electronics 56
8/2/2019 Lecture1 BE Semiconducting Materials
http://slidepdf.com/reader/full/lecture1-be-semiconducting-materials 15/15
05/03/2012 Basic Electronics 57