|
Glossary
for Semiconductors
|
Absolute Zero
The lowest possible temperature and energy of a thermodynamic system. It
is equal to 0 Kelvin,
-273.15° Celsius, or -459.67° F. Click
here
to see a primer on the three temperature scales.
Acceptor
An element that "accepts" an electron
from a semiconductor
atom. Acceptors will have one fewer valence
band
than the semiconductor they accept from. For example,
Gallium (Z=31, 3 valence electrons) could be an acceptor
for a semiconductor like silicon (Z=14) or germanium (Z=32),
both of which have 4 valence electrons. Acceptors facilitate conduction
when used to dope
semiconductors, since they provide an extra hole.
Semiconductors that are doped with acceptor atoms are called p-type
Semiconductor. Since semiconductors tend to fall into group
IVA of the periodic
table, acceptors will be found in group IIIA.
Angular Momentum
Generally denoted by L, the angular momentum about a given
point equals the cross product
of
distance r from that point and linear
momentum
p:
L = r x p.
The figure on the left shows Rensselaer president Dr. Shirley Ann Jackson
using a modified bicycle wheel to demonstrate how angular momentum is always
conserved (never changes).
It is assumed that the user of these materials has some familiarity
with angular momentum. If not, see this
link (click "Visit Site") for a ThinkQuest page explaining
angular momentum.
Atomic Number (Z)
The number identifying an element in the periodic
table, the atomic number of an element equals the number
of protons
(which also equals the number of electrons)
in the nucleus
of a neutral atom.
Atomic Spectra
The collection of wavelengths (or their corresponding colors) of
light that can be emitted or absorbed by an element. Light
is emitted (or absorbed) by an atom when electrons change from one energy
state to another as the atom loses (or gains) energy.
(Disclaimer)
Since each element has its own characteristic set of allowed energy states,
the set of allowed transitions between energy states is unique to a particular
element. Thus the atomic spectrum of an element can be used to identify
it. For an overview of atomic spectra, see
this this
page of the University of Colorado's Physics
2000 project. Or, go to this
page in the project to see an explanation of how spectra are formed.
(Energy) Band
The continuous range of allowed energies for electrons
in a solid. Individual atoms can have only certain quantized
energies. As atoms bond to form solids, each energy
level "spreads" to accommodate the shifted levels of adjacent atoms.
Atoms in the solid can occupy any energy in one of the newly-formed "bands".
This
page of this module provides more detail and animations depicting
the formation of energy bands.
Band Gap
Bohr, Niels
The "father of the atom", Niels Bohr explained several experimental results
with his solar-system-like atomic model. He applied the idea of quantized
energies to atoms, proposing that electrons
in atoms can only take certain discrete, or "quantized", values of energy.
(Disclaimer)
They don't spiral into the nucleus
because they can only emit certain values of energy (values equal to a
difference between allowed energy levels) and are thus "stuck" in their
orbits. (See
this
word of caution about visualizing electron orbits.)
Bohr's quantization of energy in the atom also explained why elements only
emit certain colors (and certain energies) of light. These spectra
are characteristic of an element and determined by the energy levels in
atoms of that element. Click here
for more information on Niels Bohr.
Boltzmann Constant (kB)
A constant of nature, converting the temperature of a gas (in degrees Kelvin)
to the kinetic
energy (in Joules
or electonVolts)
associated with the thermal motion of the particles comprising the gas.
It has the numeric value of
kB = 1.38 x 10-23 J/K = 8.62 x 10-5
eV/K
Bound (States)
An
electron
is in a bound state of an atom (or of a solid) when it does not have enough
energy to leave the vicinity of the atom (or solid). (Disclaimer)
The lower the energy of the electron, the more "tightly" bound it is and
the less likely it is to take part in interactions with electrons of other
atoms or to stray from the atom to which it is bound. In this author's
convention, tightly-bound electrons in a solid are represented in an energy
diagram (such as the one to the right) by blue circles.
The green circles represent more loosely-bound conduction
electrons, which can move freely through a solid.
Charge Carrier
A particle having electric charge that can move freely through the material.
In conductors,
electrons are free to move, so they are the charge carriers. Holes
are the charge carriers in p-type semiconductors. Positive
or negative ions can be charge carriers in some liquids.
Charge Carrier Number Density (n)
The number
density (number per volume) of charge
carriers in a material. In conductors,
electrons are free to move, so
n for a conductor equals the number
density of conduction
electrons in the material. Most conductors have one conduction
electron per atom, but some have as many as four conduction electrons per
atom. One can use this property, along with the density of the solid
and the atomic mass of the material, to calculate the number density of
charge carriers per volume. Charge is carried by both electrons and
holes
in intrinsic
semiconductors, and some plasmas and solutions contain both positive
and negative charge carriers as well. One must add the density of
holes (or other positive charge carriers) to the density of conduction
electrons (or other negative charge carriers) to obtain the total charge
carrier number density n. Take note: this usage of the
symbol n should not be confused with the principle
quantum number, which also uses the symbol n.
Conduction Band
The unfilled top Energy
band in a solid. Since this band is not filled, electrons
with energies in this band can move easily through the solid, creating
an electric
current. (Disclaimer)
The image to the right follows this author's convention of representing
electrons in the conduction band by green circles. The blue
circles represent electrons in filled (or mostly filled) bands, such as
the valence
band in the energy
diagram to the right. |
 |
Conduction Electrons
| Electrons
that are free to move within a solid. The motion of these electrons
can give rise to the conduction of electricity by creating an electric
current through the solid . The energy
diagram of an intrinsic
semiconductor found to the right follows this author's convention
of representing conduction electrons by green circles. The
blue circles represent tightly bound
electrons that do not significantly contribute to conduction through a
solid. |
 |
Conductor
A material with low resistivity
used for contacts and interconnects
in semiconductor
processing. Conductors have a partially filled
valence
band, through which electrons
can move freely, as shown in the energy
diagram to the left. Thus, in a conductor, the conduction
band is the same as the valence band, and the charge
carriers are primarily electrons. In keeping with this author's
convention, the electrons in this partially-filled conduction band are
represented by green circles.
Conductivity (s)
A measure of how freely current
can flow through a material. Copper, with its high conductivity of
5.95 x 107 W-1m-1,
conducts electric current more freely than does aluminum, with its slightly
lower conductivity of 3.77 x 107 W-1m-1.
Conductivity is the inverse of resistivityr:
s = 1/r.
Contact Potential
A potential
difference that arises at the junction of two different conducting
materials. For example, aluminum has a higher Fermi
energy than does copper, so it is easier to remove an electron
from aluminum than from copper. When copper and aluminum are placed
in contact, the discontinuity in Fermi energy at the boundary is quickly
smoothed out - some of the conduction
electrons from the aluminum flow into the copper, until the Fermi
energy is the same on either side of the boundary. This produces
a net negative charge on the copper and a net positive charge on the aluminum.
The separation of charge sets up a potential difference, or voltage,
across the boundary. The size of this "contact potential" difference
is dependent upon the difference in Fermi energies between the materials.
Continuous
Smoothly varying; taking any value. An electron
moving through empty space can have any value of energy, so we say the
allowed energies for this free electron are continuous. An
electron in an atom, however, can only have certain discrete, or quantized,
energies, according to the quantum atomic theory first suggested by Niels
Bohr. (Disclaimer)
(Atomic) Core
| The nucleus
along with the electrons in completely-filled energy
shells. These tightly-bound
electrons stay near the nucleus and do not contribute to conduction or
interactions with other atoms. They are of less interest than the
valence
electrons of partially-filled shells. In the
cartoon to the right, the pink sphere surrounds the core of Silicon; only
the four valence electrons are outside this core. (Disclaimer) |
Note: Figure not to scale or,
for that matter, an accurate rep-
resentation of electron behavior. For
details, see our word
of caution.
|
Coulomb (C)
The SI unit of electric charge. One coulomb is a fairly large amount
of charge, equaling the charge of 6.25 x 1018 protons.
Covalent Bond
An interaction between atoms by which they "share" valence
electrons in the outermost energy
shell, thereby filling the outer shell of both atoms involved in
the interaction. The electrons orbit both
nuclei,
binding the atoms together. For example, each hydrogen atom in a
hydrogen gas molecule has a single electron. The valence energy level
of a hydrogen atom is filled by two electrons; sharing their electrons
allows each hydrogen atom to fill its energy shell. A
nice pictorial explanation of ionic and covalent bonding is found
on
this
page by Access Excellence @ the national health museum.
Cross-Sectional Area (A)
 |
The (2-dimensional) area formed when one "slices" through a (3-dimensional)
solid. When discussing electric
current, we typically take a cross section that is perpendicular
to the direction of current flow, like the two cross sections of the pipe
shown to the left. Link
here
for a more technical definition from Wolfram's MathWorld. |
Crystalline Structure
| Regularly repeating array of atoms forming a solid. The image
to the right shows how carbon atoms are arranged in 3-D to make diamond.
The red atoms are closest to you, and the violet atoms are the furthest
away. The pattern of carbon atoms is exactly duplicated many times.
Such a repeating arrangement of atoms is called a "crystal"; the crystalline
structure is the pattern that is repeated. |
 |
(Electric) Current (I)
The rate at which electric charge flows past a given point. The convention
in physics is to discuss the flow of positive charges, even though
we now know that the motion of (negatively-charged) electrons
is what creates a current in conductors.
According to this convention, if a beam of electrons traveled from right
to left across your screen, we would say the current flows from left to
right. The SI unit is the Ampere, or Amp; one Amp is equal to one
Coulomb
of charge per second of time. For example, if particles carrying
5 Coulombs of net electric charge flowed into a light bulb each second,
we would say that the current through the bulb was 5 Amps. For
a good introduction to current and other circuit properties, try this
page of the All
About Circuits site.
Degrees Kelvin (K)
One degree Kelvin represents the same change in temperature as one degree
centigrade, or Celsius, but the Kelvin scale "starts" at a different temperature.
Zero degrees Kelvin is absolute
zero, the lowest temperature anything could ever take.
In contrast, zero degrees Celsius is the temperature at which water freezes.
When measuring changes in temperature, the Kelvin and Celsius scales
give the same result. But when you need the absolute temperature,
such as when calculating how much thermal energy an object has, Kelvin
is the preferred unit. One can convert temperature (T) between
degrees Celsius (°C) or degrees Ferenheit (°F) and degrees Kelvin
(K) using the following relationships:
T(K) = T(°C) + 273.15, and
T(K) = T(°F) * 5/9 +241.15
Click here
to see a primer on the three temperature scales.
Diffuse
To spread out, particularly when substance was originally concentrated.
Consider a drop of red food coloring placed in a glass of water.
Initially, the dye is concentrated in the single drop. As time elapses,
however, the dye will diffuse, spreading out through the entire
glass of water.
Diffusion Current
The current occurring at a p-n
junction due to diffusion
of charge
carriers. The n-side of the junction contains conduction
electrons, while the p-side contains holes.
These electrons and holes will move across the junction as they diffuse,
causing a net (positive) electric
current from the p-side to the
n-side.
Diode
A semiconductor device which allows current
to flow in only one direction. A is composed of a single p-n
junction, and the words can often be used interchangeably.
When a forward
bias is applied (positive terminal of a battery connected
to the p-side of the junction and negative terminal to the n-side),
current flows freely through the device. But when the battery terminals
are reversed and this reverse
bias applied, no significant amount of current will flow. Operation
of diodes is discussed on this
page of this module.
Donor
An element that "donates" an electron
to a semiconductor
atom. Donors will have one more valence
electron than the semiconductor they accept from. For
example, Phosphorus (Z=15, 5 valence electrons) could be
a donor for a semiconductor like silicon (Z=14) or germanium (Z=32),
both of which have 4 valence electrons. Donors facilitate conduction
when used to dope
semiconductors, since they provide an extra conduction
electron. Semiconductors that are doped with donor atoms
are called n-type
Semiconductors. Since semiconductors tend to fall into group
IVA of the periodic
table, acceptors will be found in group VA.
Doping
The process of introducing impurities
into a substance to enhance or control its properties. For example,
silicon is often doped with gallium or with phosphorus. Both increase
the conductivity
of silicon; gallium increases the concentration of holes
in the silicon, and phosphorus increases the concentration of conduction
electrons. Doping not only increases the conductivity but
it can be used to produce
diodes,
transistors,
and many other devices. The discussion of doping
starts on
this page of this module.
Drift Velocity
The average velocity of charge
carriers in a material. This is not the same as the average
speed.
In general, charge carriers move very quickly, but mostly randomly, colliding
with each other and with the atomic cores
around them. When a voltage
is applied, the random motion continues, but with an overall net "drift"
in the direction of the force due to the applied voltage. The average
speed of a charge carrier may be on the order of 106 m/s, while
the magnitude of the drift velocity is about 10-5 m/s.
Effective Mass
The value of mass one must use to model electronbehavior
in solids as the motion of independent particles. A conduction
electron in a solid interacts with the atomic
cores of nearby atoms, as well as with other conduction electrons
in the solid. The motion of all the electrons is very interconnected
and complicated, yet we can successfully describe observed effects by treating
each conduction electron as an independent particle with an "effective
mass" determined by experiment and characteristic of a material.
Typically the effective mass is less than the mass of an electron in free
space ( 9.11 x 10-31 kg). See
this
page of the Wikpedia
for more information on, and some representative values of, effective mass.
Electron
A fundamental particle with negative charge found in atoms. It has
a mass of 9.11 x 10-31 kilograms and a charge of - 1.6 x 10-19Coulombs.
Conduction occurs primarily from the movement of
electrons
through materials. Click this
link to go to the Particle
Adventure webpage for more information on
electrons.
ElectronVolt (eV)
A unit of energy,
equal to the energy gained by an electron
that passes through a potential
difference of 1 Volt. An electronVolt is related to the SI
energy unit Joule
by the charge of the electron
e as follows:
1 eV = 1.6 x 10-19 J.
Energy
Energy comes in many different forms, such as "kinetic energy" (energy
of motion), heat, and even mass. Energy can never be created or destroyed;
it can merely change from one form to another. These materials assume
the reader has some prior knowledge of energy as it is defined in science.
If
you are not confident in your prior knowledge, you can access Glenbrook
High's Physics Classroom pages on energy, by clicking
here.
If you only want an overview, try this
nice site by the Danish
Wind Industry Association.
Energy Diagram
A
plot showing energies on the vertical axis, typically used to illustrate
the specific quantized
energies allowable for electrons (Disclaimer)
in atoms and solids. The energy diagram for a silicon atom shown
on the left indicates the fourteen electrons in their lowest states.
(The Pauli
exclusion principle determines how many electrons can "fit" into
each value of energy.) The band diagram on the right, shown for a
pure semiconductor
such as silicon,
shows
electrons populating the energy bands
of a solid. Energy is again the vertical axis; the horizontal axis
represents location in one dimension. Both diagrams follow this author's
color convention: blue electrons are tightly bound in filled states
or bands and not likely to move or interact; green electrons are more loosely
bound and participate in bonding (between atoms) or conduction (within
a solid).
Energy Level
Essentially synonymous with energy
shell, an energy level is a collection of energy
states with the same energy
(in the absence of electromagnetic fields) for electrons
in atoms (Disclaimer).
According to the Pauli
Exclusion Principle, electrons can never occupy identical states.
Electrons in different states within an energy level are distinguished
by other characteristics, such as their
angular
momentum and spin.
In an atom, the lowest energy level (having
principle
quantum number n=1) has two distinct states, the second
energy level (n=2) contains eight different states, and so on.
You may see a pattern emerging - the number of energy states within an
energy level determines the shape of the periodic
table.
(Energy) State
A complete set of variable values that a particle can exhibit. For
example, an electron
in a hydrogen atom can be described by its location, its energy
(Disclaimer),
and its angular
momentum. The collection of these properties constitutes
the "state" of the electron. According to quantum theory, an electron
in an atom can take only certain, quantized,
values of energy and angular momentum, so the number of states in an atom
is limited.
Excited State
Any energy
state of an atom, or of a solid, above its ground
state. For our purposes, we are primarily interested in the
energy
levels of electrons in atoms and solids (Disclaimer),
so when we refer to "excited state" we mean at least one of the electrons
having an energy higher than its ground-state energy. Excited states
are not indefinitely stable, so the atom will eventually return to its
ground state.
(Pauli) Exclusion Principle
First proposed by Wolfgang Pauli to explain the arrangement of electrons
in atoms, the Exclusion Principle asserts that no two electrons can be
in the same state.
In other words, two electrons in the same atom cannot have the same energy(Disclaimer),
angular
momentum and spin.
We now know that the Exclusion Principle applies not just to electrons,
but to an entire class of particles called "fermions", which includes protons
and neutrons.
Click
here to go to the Particle
Adventure's website, or click
here to go to the Physics
2000 page explaining the Exclusion Principle.
Faraday's Law
Michael Faraday (and Joseph Henry, working independently in America) performed
a series of experiments proving that changing the magnetic field through
a loop of wire will produce a current through the loop. The direction
of the current "induced" by the changing magnetic field depends upon the
direction of change of the field. Try this
site for more information about Faraday's Law (Note: this
site employs calculus; non-calculus-savvy users may try this
site or they might look up Faraday's Law a conceptual-based introductory
physics text, such as the one by Hewitt).
Features
The individual pieces making up a circuit element. For example, a
transistor
such as the one shown here has several features,
including
the region(s) of n-type
semiconductor (green), the region(s) of p-type
semiconductor (blue), the gate(red),
and the (yellow) region of insulating
material that separates the gate from the semiconductor regions.
Of these four features, the insulation between the gate and the semiconductors
is generally the narrowest, limited by the manufacturing process.
(Note: the colors in this picture are fictitious, used only to aid
the reader in identifying features. True transistors are not multicolored
but are pretty much gray all over.)
To learn more
about the manufacturing process, try
this
page of howstuffworks.
Fermi Energy
The energy of the highest occupied state in a solid in its ground
state. The Fermi Energy represents the kinetic
energy of electrons
responsible for conduction. For more on the Fermi energy, try this
Wikipedia page.
Forward Bias
A voltage
applied to a diode
(a p-n
junction) in a direction that does produce electric
current. When a p-n junction is forward biased,
the positive terminal of a battery is connected to the p-side of
the diode, and the negative terminal to the n-side. Biasing
of a diode is discussed on this
page of this module.
Gate (on Transistor)
The
part of the transistor
that controls the flow of electric
current through the device. Applying a voltage
to the (red) gate terminal in the transistor shown to the left allows conduction
electrons to flow from one (green) n-type
semiconductor region, through the (blue) p-type
semiconductor region, to the other n-type region. For
more on how transistors work, see
this
page (and the following) of this module.
Ground State
The energy
state of an atom, or of a solid, when its total energy equals the
minimum possible energy for that atom or solid. For solids, this
only occurs at a temperature of absolute
zero. Individual atoms may be in their ground state at non-zero
temperatures, but they will not stay there indefinitely. Instead,
they can occasionally absorb thermal energy and move to an excited
state for a while before they decay back to the ground state.
For our purposes, we are primarily interested in the energy
levels of electrons in atoms and solids (Disclaimer),
so when we refer to "ground state" we mean all the electrons having their
lowest possible energy.
Group
A column in the periodic
table. Elements in the same group have the same number of
valence
electrons and so will tend to interact in similar manners.
For example, regular table salt consists of an atom of sodium (group IA)
bound to an atom of chlorine (group VIIA). Potassium is in the same
group as sodium; it bonds with chlorine to make potassium chloride, which
has many of the same properties as table salt.
Hole
Essentially the absence of an electron
in an otherwise filled energy
band, a hole can be treated as a positively-charged particle moving
through the valence
band of a solid. Its effective
mass can be experimentally determined. According to the Wikipedia
entry for effective mass, a hole in solid silicon has an effective
mass of about 81% of the rest mass of the electron, or 7.38 x 10-31
kg. Holes are explained on this
page of this module.
Impurity
| Different type of atom scattered through an otherwise regular crystal.
The image to the right depicts silicon atoms (in red) in a regular array,
with blue lines depicting shared electrons
providing covalent
bonds. The lighter-colored atom could be gallium, an impurity
that leads to p-type
behavior in the solid. |
 |
Insulator
A
material with very high resistivity
(low conductivity)
often
used to prevent contact between conductors.
The poor conductivity is due to the completely full valance band, illustrated
in the energy diagram to the right. An insulator has no charge
carriers at absolute
zero and very few charge carriers at room temperature. The
energy
diagram to the right follows this author's convention of representing
conduction electrons by green circles. The blue circles represent
tightly bound
electrons that do not significantly contribute to conduction through a
solid. The absence of a blue circle is a hole,
which can contribute to conduction, as described
on this page
of this module.
Interconnect
A strip of conductor
on a computer chip that connects circuit elements such as transistors
and resistors
to each other.
Intrinsic (Pure) Semiconductors
A
semiconductor
comprised of a single type of molecule, with no impurities.
Pure semiconductors are typically poor conductors of electricity.
In an intrinsic semiconductor, each conduction
electron in the conduction
band leaves behind a hole
in the valence band that also contributes to conduction, as shown in the
energy
diagram to the right. This diagram follows this author's
convention of representing conduction electrons by green
circles. The blue circles represent tightly bound
electrons that do not significantly contribute to conduction through a
solid. Each white circle represents a hole.
Ionic Bonding
An interaction between atoms in which one atom "donates" valence
electron(s) to the other atom, resulting in filled energy
shells for both atoms involved in the interaction. The electrons
originally from the donor atom move to the vicinity of the other "acceptor"
atom, binding the atoms together. For example, a chlorine atom has
seven electrons, out of the eight needed to fill its valence
band. Sodium, on the other hand has a single electron in
its valence band. When sodium and chlorine bind, sodium donates its
single valence electron to chlorine. The remaining 10 electrons surrounding
sodium comprise filled shells (2 in the lowest energy level, 8 in the next
level), and the donated electron fills the valence shell for chlorine.
A
nice pictorial explanation of ionic and covalent bonding is found
on
this
page by Access Excellence @ the national health museum.
Joule
The SI unit of energy,
one Joule is a Newton-meter, or a kg m2/s2.
Kinetic Energy (KE)
The energy
of motion, determined by the mass n of an object and its speed v,
according to the following relationship:
KE = 1/2 mv2.
Light-Emitting Diode (LED)
 |
A diodethat
has been constructed a) to optimize the emission of light as conduction
electrons and holes
recombine at a
p-n
junction, and b) to maximize the fraction of the produced light
that escapes the device and is seen. LEDs are energy-efficient sources
of light in widespread use as indicator lights and in traffic signals,
among other applications. The photo to the left shows three LEDs
that produce different colors of light. The color of the plastic
surrounding the diode does not filter the light, since LED light is monochromatic
when produced, but merely aids the user in identifying the LED. |
Majority Carrier
The type of charged particle that is primarily responsible for current
flow in a material. In conductors,
current is produced by the motion of electrons
through the material, so electrons are the majority carrier in conductors.
But in some solutions and in p-type
Semiconductors, the current is due to the motion of positive ions
or
holes.
In these cases, the positive ion or the hole would be the majority carrier.
Micron
One millionth of a meter, or one thousandth of a millimeter. (In
good SAT-question-style, a micron is to a millimeter what a millimeter
is to a meter.) At the time of this writing (2004), semiconductor
devices can be manufactured to such precision that features
on a chip can be smaller than a tenth of a micron!
Minority Carrier
The type of charged particle that does NOT contribute significantly to
current flow in a material. In n-type
semiconductors, the number of conduction
electrons is far larger than the number of holes,
so holes are the minority carrier (and electrons are the
majority
carrier). In p-type
Semiconductors, the current is primarily due to the motion of hole,
making conduction electrons the minority carrier.
Minority Current
Electric current
due to the motion of minority
carriers.
(Linear) Momentum
Generally denoted by p, linear momentum is the mass m
of an object times its velocity v:
p = mv.
Since velocity has direction, so does momentum. It is conserved (doesn't
change) in the absence of forces. It is assumed that the user of
these materials has some familiarity with momentum. If
not, see
this
link to the Glenbrook
High's Physics Classroom Webpage for a good introduction to the
topic.
Neutron
A fundamental particle with no electric charge found in the nuclei
of atoms. It has a mass of 1.675 x 10-27 kilograms. Click
this
link to go to the Particle
Adventure webpage for more information on
neutrons.
Nucleus (Nuclei)
| The positively-charged "center" of an atom, comprised of protons and
neutrons. In the cartoon of a silicon atom shown to the right, the
protons are represented by red spheres, and the neutrons by turquoise spheres.
Electrons are blue (when in a completely filled energy
level) or green (when in a partially full energy level).
These colors are purely a convention, unique to this author, and do not
represent optical properties of the particles. |
Note: Figure not to scale or,
for that matter, an accurate rep-
resentation of electron behavior. For
details, see our word
of caution. |
Number Density (n)
The number of a particular type of object found in each unit volume.
For example, if 2500 cattle are fairly uniformly spread across 100 acres
of grassland, the number density of cattle in the region is 25 cattle per
acre. In circuits, we often discuss the number
density of charge carriers n, which denotes the average
number of charge carriers per cubic meter of material. Take note:
this usage of the symbol
n should not be confused with the principle
quantum number, which also uses the symbol n.
n-type Semiconductor
Consists of a semiconductor,
such as silicon, which has been
doped
with atoms of an donor
element, such as phosphorus. The extra
valence
electrons of the donor atoms provide filled energy states in the
band
gap, just below the conduction
band.
Electrons
from these "extra" states can easily move into the conduction band and
become conduction
electrons,
as shown in the energy
diagram to the right. Replacing even one in every million
silicon atoms with a phosphorus atom can increase the conductivity
of the solid by a factor of five million. Because the density
of conduction electrons provided by the donor is much larger than the density
of holes
contributed by the semiconductor atoms, conduction in this material is
primarily due to the motion of (negatively-charged) electrons.
Thus it is called an n-type semiconductor.
Ohmic (Materials)
Materials obeying Ohm's
Law. Ohmic materials have resistances
that do not change over a wide range of voltages and currents. For
an ohmic device, a graph of voltage
across the device vs the
current
through that device will yield a straight line, with constant slope equal
to the resistance of the device.
Ohm's Law
An observation (first made by Georg Simon Ohm) that applies to certain
materials or devices, called ohmic
materials or devices. States that many materials have resistances
that are independent of voltage and current under regular operating conditions.
Ohm's Law is NOT the statement V = IR, as many believe.
That statement is instead the definition of resistance. Ohm's Law
instead says that, for many materials under a wide range of conditions,
the voltage
V and current
I are linearly related, which implies a resistance
R independent
of V and I. To read more about Ohm's Law, try this
page, of the ohmslaw.com
website.
(in) Parallel
Two segments of an electric circuit are "in parallel" if they offer distinct
paths between the same two points.
Because
houses are wired in parallel, turning off one appliance does not keep current
from flowing to other appliances - each is on its own parallel path.
The figure to the right depicts a circuit diagram of two resistors connected
in parallel to a battery. Notice how removing one resistor will not
alter the current flow from the battery through the other resistor. To
read more about circuits, try the links from this
page by Electronics
Lab. Another good source of circuit information is AllAboutCircuits
- try this
link for their treatment of series and parallel circuits.
P-N Junction
An interface between a p-type
semiconductor and an n-type
semiconductor device which can be used for many different applications.
A single p-n junction acts as a diode,
conducting current when a forward
bias is applied (positive terminal of a battery connected
to the p-side of the junction and negative terminal to the n-side)
but not when the terminals are switched to apply a reverse
bias. This
page of this module discusses the structure of p-n
junctions. p-n junctions also figure prominently in
transistors,
as discussed on
this page of this module. For an alternate
look at p-n junctions, see this
page of Georgia State's HyperPhysics
project.
P-type Semiconductor
Consists of a semiconductor,
such as silicon, which has been
doped
with atoms of an acceptor
element, such as gallium.
The
unfilled valence
shells of the acceptor atoms provide empty energy states in the
band
gap, just above the valence band. Valence electrons can move
into these "extra" states, leaving behind holes
in the valence band, as shown in the energy
diagram to the right. Replacing even one in every million
silicon atoms with a gallium atom can increase the conductivity
of the solid by a factor of five million. Because the density
of holes provided by the acceptor is much larger than the density of conduction
electrons contributed by the semiconductor atoms, conduction in
this material is primarily due to the motion of (positively-charged)
holes. Thus it is called a p-type
semiconductor.
Periodic Table
A table of all known elements, sorted into columns by their chemical properties
and into rows by their relative masses within the columns. Mendeleev
was the first to organize elements in such a manner, and he successfully
predicted the existence of elements that had not been previously detected
or expected. Click
here for a nice on-line table coded by Michael Dayah. Another
nice on-line periodic table can be found at this
site by webelements.com.
For a description of how Mendeleev organized the elements, try this
Physics 2000 page.
Potential Energy
Energy
that is stored in an item, potential energy can take many forms, including
chemical, electrical, and gravitational. This module assumes basic
familiarity with the concept of potential energy. If you need a review,
try Glenbrook
High's Physics Classroom treatment
of energy.
(Principle) Quantum Number (n)
An integer that identifies the energy
level of electrons in atoms (Disclaimer).
n=1
corresponds to the lowest energy possible for an electron in an atom.
Be careful not to confuse this use of the symbol n for other meanings,
such as number
density, of this common symbol.
For more
on quantum numbers and how they underlie the periodic table, go
to this
Physics 2000 site.
Proton
A fundamental particle with positive charge found in the nuclei
of atoms. It has a mass of 1.673 x 10-27 kilograms and
a charge of 1.6 x 10-19 Coulombs.
Protons are fairly fixed in solids and so don't contribute to conduction.
Click
this
link to go to the Particle
Adventure webpage for more information on
protons.
Quantized
Having only certain, discrete values. For example, whole numbers
are quantized. They can only take the values 0, 1, 2, 3, etc. and
will never fall between those discrete values. Decimals, on the other
hand, can take any value and thus are continuous
rather than being quantized. (Disclaimer)
Resistance (R)
The ratio between the voltage
applied to a device and the electric
current I that flows through it:
R = V/I.
Certain materials (called ohmic
materials) have resistance that is independent of voltage and current.
Typically, the word "resistor" refers to an ohmic device in a circuit.
For
a good introduction to resistance and other circuit properties, try this
page of the All
About Circuits site.
Resistivity (r)
The "part" of the resistance
of an object independent of the geometry of the object. Resistivity
depends on the type of material used and on the temperature of the object.
For a homogeneous solid, resistivity r is related
to resistance R in the following manner:
r = R A / L,
where A is the cross-sectional
area of the solid, and
L is its length, as shown to the
right. Resistivity is the inverse of conductivitys:
r = 1/s
.
Copper, with its low resistivity of 1.68 x 10-8 Wm
conducts electric current more freely than does aluminum, with its slightly
higher resistivity of
2.65 x 10-8 Wm.
Reverse Bias
A voltage
applied to a diode
(a p-n
junction) in a direction that does NOT produce significant electric
current. When a p-n junction is reverse biased,
the positive terminal of a battery is connected to the n-side of
the diode, and the negative terminal to the p-side. Biasing
of a diode is discussed on this
page of this module.
Semiconductor
A subclass of insulators,
semiconductors are materials with conductivity
that can be controlled through methods such as doping
or changing the temperature. Like all insulators, they have a valence
band that is completely full in the ground
state. A semiconductor has no charge
carriers at absolute
zero; pure
semiconductors have very few charge carriers even at room temperature.
Conductivity can be increased through doping, creating either p-type
semiconductors or n-type
semiconductors.
Shell
Note: Figure not to scale or,
for that matter, an accurate rep-
resentation of electron behavior. For
details, see our word
of caution. |
Essentially synonymous with energy
level, a shell is a collection of energy
states with the same energy
(in the absence of electromagnetic fields) for electrons
in atoms (Disclaimer).
In an atom, the innermost energy shell (having
principle
quantum number n=1) can "hold" two electrons, as shown in the cartoon
to the left. The second shell (n=2) holds 8 electrons, and
so on. |
Spin
A property of elementary particles having the units
of angular
momentum, spin was originally thought to
be the angular momentum associated with an elementary particle's spinning
on its axis. More modern experiments have shown that this physical
interpretation is in error, and spin is now considered an intrinsic property
of a particle, like its mass and electric charge. Click
here
to go to the Physics
2000 page that discusses spin.
Transistor
An electronic switch. Transistors allow a (relatively) large amount
of current
to flow when a (relatively) small voltage is applied, just like a light
switch can provide a large amount of electric energy
to a lamp when a small amount of mechanical energy is expended to flip
the switch. Transistors in modern electronics are made from layered
p-
and n-
type semiconductors. This module's discussion
of transistors starts on this
page.
Valence Band
The outermost energy
band that contains electrons when a solid is in the ground
state. An intrinsic
semiconductor (or insulator)
in its ground state will have a completely filled valence band, while the
conduction
band above the valence band is completely empty.
The
energy
diagram to the right depicts a semiconductor in which some electrons
have gained energy to jump to the conduction band, leaving behind holes
in the valence band. (Disclaimer)
These holes can move through the nearly-full valence band, just as the
electrons can move through the nearly-empty conduction band. The
image follows this author's convention of representing electrons bound
in the valence band by blue circles. The green circles represent
electrons that are free to move, such as the ones in the conduction band
in the image to the right.
Valence Electron
An electron in the valence
shell of an atom, or in the valence
band of a solid. Valence electrons are more active than non-valence
electrons, so valence electrons are responsible for most of an atom's or
solid's electrical and chemical properties.
Valence Shell
| The outermost energy
shell that contains electrons when an atom is in the ground
state. In the cartoon of a silicon atom to the right, the
four "green" electrons occupy the valence shell. The image follows
this author's convention of representing tightly-bound electrons (those
in inner shells) by blue circles; the green circles represent electrons
that are free to interact. |
Note: Figure not to scale or,
for that matter, an accurate rep-
resentation of electron behavior. For
details, see our word
of caution. |
Voltage (V), or Potential Difference
The change in energy per unit of electric charge, measured in the SI unit
of Volt (V). For example, a 1.0 Volt battery increases the energy
of each Coulomb
of charge by one Joule.
For
a good introduction to voltage and other circuit properties, try this
page of the All
About Circuits site.
Copyright
© 2004 Doris Jeanne Wagner and Rensselaer Polytechnic Institute.
All Rights Reserved.