Title: Semiconductors and Diodes
1Semiconductors and Diodes
2Semiconductor
- Semiconductors are materials, which are neither
good conductors (like copper, gold, silver) nor
good insulators (like rubber and glass). - The most common semiconductors are silicon and
germanium. - Silicon is directly under Carbon on the periodic
table, Germanium is under Silicon.
3The Importance of Being Semiconducting
- Much of a computers circuitry is made of
semiconductors. - Before semiconductor (solid-state) transistors,
there were vacuum tubes which were huge by
comparison. - The ENIAC was made from tubes.
- In addition to the obvious benefit of taking up
less space, smaller devices tend to be faster and
require less energy.
4ENIAC
By today's standards for electronic computers the
ENIAC was a grotesque monster. Its thirty
separate units, plus power supply and forced-air
cooling, weighed over thirty tons. Its 19,000
vacuum tubes, 1,500 relays, and hundreds of
thousands of resistors, capacitors, and inductors
consumed almost 200 kilowatts of electrical
power.
5Why are they useful?
- Semiconductors can be made to conduct better
under the right circumstances it is this control
over the conductivity that makes them useful. - A semiconductor devices ability to carry current
can depend on the current or voltage applied. - They are NOT Ohmic (i.e they do not obey Ohms
law VIR). - Their properties may also depend on the whether
or not light is shining on them, how much light,
what color light, etc.
6Doping
- One way to change a semiconductors properties is
to dope it. - Doping is adding another substance to a pure
semiconductor. - Typically one dopes with an element that lies
either to the right or left of the pure element
on the Periodic Table.
7Periodic Table
B Boron C Carbon N Nitrogen O Oxygen
Al Aluminum Si Silicon P Phosphorus S Sulfur
Ga Gallium Ge Germanium As Arsenic Se Selenium
In Indium Sn Tin Sb Antimony Te Tellurium
8n and p doping
- Doping with elements on the right increases the
number of free (valence) electrons and is called
n doping. - Doping with elements on the left decreases the
number of free (valence) electrons and is called
p doping. - The material added is called a dopant.
- Both kinds of doping tend to increase the
conductivity.
9Energy levels
- The electrons in atoms do not have arbitrary
amounts of energy. - There are very precise energy levels that the
electrons are allowed to have. - (You might recall 1s, 2s, 2p, 3s, 3p, 3d, etc.
from chemistry.) - The energy is said to be quantized.
10Bands
- When many atoms come together to form a solid,
there are still quantized energy levels, just
many, many more of them. - For some energy levels, the next highest or
lowest energy level is so close, its almost
continuous (sometimes called quasi-continuous). - The closely packed energy levels are said to form
a band.
11Gap
- There are still some energies that the electrons
are not allowed to have. - Thus there are jumps in energy between the
highest energy in one band and the lowest energy
in the next band. - This jump in energy is called the band gap or
just the gap.
12Pauli Exclusion Principle
- Electrons have a property called spin which can
only have two values up and down. - The Pauli Exclusion Principle says that two
electrons with the same spin cannot occupy the
same level. - Thus there can only be two electrons per level
one with spin up, one with spin down.
13Filling in the bands (not the gaps)
- Imagine the energy levels are all empty, and we
begin putting in the electrons. - The first two electrons go into the lowest level.
- The next two go into the next lowest level, etc.
14Where does it all end?
- A materials conductivity depends on whether the
last filled energy level is in the middle of a
band (a metal) or at the top of a band just
before a gap (semiconductors and insulators). - The size of the gap determines whether the
material is a semiconductor (small gap) or
insulator (large gap). - (This is over-simplified.)
15Introducing a current
- To have current, one must move electrons around.
- To move electrons around, one must give them more
energy. - With more energy they go to higher energy levels.
- The energy level an electron goes into cannot
already be occupied.
16Band versus Gap
- If the highest energy level (the Fermi level)
falls within a band, then one only needs to add a
little energy to cause a current (a conductor). - If the Fermi level falls in a gap, then one has
to add a lot of energy to cause a current (a
semiconductor or insulator).
17Valence and Conduction Bands
- If the Fermi level falls in the gap, the highest
filled band is called the valence band and the
lowest unoccupied band is called the conduction
band. - In such a case, electrons must be promoted to the
conduction band in order to move around.
18An Analogy
- Assume a university offers 100-, 200-, 300- and
400- level courses. - That all 100-level courses are of a similar
difficulty, but that 200-level courses are
significantly harder. - The university offers 10 classes at each level
and each class has a strict cap of 20 students.
19Analogy continued
- Each level has an occupancy of 200 (10 classes
? 20 students). - The course levels (100, 200, etc.) correspond to
the bands. - The change in difficulty between 100 and 200
corresponds to a gap.
20The Semiconductor University
- The students at this university must all take
four courses. - This is analogous to Silicons having four
valence electrons. - Say there are 100 students at the university,
they must take 400 courses all together (100
students ? 4 courses each).
21The lazy students
- The students all register for the easiest courses
first, but they fill up. - The students end up only taking 100- and 200-
level courses.
22An afternoon job
- A student wants to take an afternoon job, but has
a schedule conflict. - In order to have some flexibility in his/her
schedule, such a student would have to take a
substantially harder course (the only open
courses are in the 300 and 400 level). - The schedule flexibility is like conductivity
(the ease of motion or lack thereof).
23The exchange program
- Now say a percentage of the 100 students belong
to an exchange program and that they only take
three courses. - In such a case, not all of the 200-level courses
would be filled. - And the student wanting the afternoon job would
not have to take a significantly harder course
(assuming he/she was already taking one of the
harder 200-level courses). - So there is more flexibility (higher
conductivity). - This is analogous to p-doping.
24The three-year program
- A different possibility is that a percentage of
the 100 students belong to an 3-year program and
take five courses. - In such a case, some of the 300-level courses
would be filled. - If the student wanting the afternoon job already
had a 300-level course, he/she would not have to
take a significantly harder course. - So there is more flexibility (higher
conductivity). - This is analogous to n-doping.
25At this juncture (or is that junction?)
- We can change the conductivity, so what?
- The interesting phenomena occurs when a p-doped
semiconductor meets an n-doped semiconductor. - This is called a p-n junction.
26Two nearby universities
- To pursue the analogy, imagine two universities
in the same city. The p-doped University has an
exchange program, n-doped University has a 3-year
program. - Some students taking 300-level courses at N.U.
notice there are open slots in the 200-level
courses at P.U. - There are unoccupied low-energy levels in the
p-doped material.
27The penalty
- For 300-level-taking N.U. students who live in
between the universities, there is a benefit to
taking 200-level classes at P.U., but for others
there is a penalty (a longer commute). - In the materials the penalty is charge
separation. - Recall with batteries and capacitors it required
energy to separate charges.
28Violating Neutrality
- Although one might think of n-doped materials as
having excess electrons, they are neutral. - Similarly p-doped materials may be thought of as
deficient in electrons, but they too are
neutral. - But when electrons from n-doped go over to the
p-doped side, the n-doped side is left with a
positive charge and the p-doped side gets a
negative charge.
29Like a little capacitor
- There is an energy cost involved in separating
charges. - The p-n junction is like a little capacitor
n-doped
n-doped
30A loss in flexibility
- With some N.U. students now taking P.U. classes,
there is a loss in schedule flexibility
(conductivity) especially among students who live
between the universities (at the p-n junction). - There is a loss in conductivity at the p-n
junction.
31Applying a voltage
- Connecting a p-n junction to a battery as shown
below adds positive charges on the n-doped side
making the region of poor conductivity larger. - This is called reverse bias.
n-doped
?
32Applying a voltage II
- Connecting a p-n junction to a battery as shown
below adds positive charges on the p-doped side
making the region of poor conductivity smaller
(oversimplified). - This is called forward bias.
n-doped
?
33Diode
- Thus current at p-n junction flows readily in one
direction and poorly if at all in the other
direction. - Devices with this property are called diodes.
- Its like a valve in the heart that only allows
blood to flow in one direction.
34LED
- Some diodes are configured such that when
electrons cross the junction they must give off a
photon (light). - Thus they glow when they are conducting.
- They are known as light emitting diodes or LEDs.
35Photoconductors
- An electron below the gap can be given the boost
it needs to jump the gap by absorbing the energy
from a photon (light). - Once in the conduction band, the excited electron
is free to move around. - If the boost is provided by visible light, the
material is called a photoconductor.
36Night and day
- A photoconductor is a poor conductor in the dark
but a reasonable conductor in the light. - Photoconductors are the key technology in
photocopiers, laser printers, scanners and
digital cameras.