1.1 Conductors - Insulators - Semiconductors
1 Fundamentals
1.1 Conductors - Insulators - Semiconductors
1.1.1 Conductors
Conductors are generally substances which have the property to pass different types
of energy. In the following, the conductivity of electricity is the value of interest.
Metals:
The conductivity of metals is based on the free electrons (so-called Fermi gas) due to
the metal bonding. Already with low energy electrons become sufﬁciently detached
from the atoms and a conductivity is achieved.
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Free electrons form an electron gas
Fixed aluminum atoms
Fig. 1.1: Metallic bonding: ﬁxed ions and free valence electrons (Fermi gas)
The conductivity depends, inter alia, on the temperature. If the temperature rises, the
metal atoms swing ever stronger, so that the electrons are constrained in their move-
ments. Consequence, the resistance increases. The best conductors, gold and silver, are
used relatively rare because of the high costs (gold e.g. for the contacting of the ﬁn-
ished chips). The alternatives in the semiconductor technology for the wiring of the
individual components of microchips are aluminum and copper.
Page 1. 

Scene 1

1.1 Conductors - Insulators - Semiconductors
1 Fundamentals
1.1 Conductors - Insulators - Semiconductors
1.1.1 Conductors
Conductors are generally substances which have the property to pass different types
of energy. In the following, the conductivity of electricity is the value of interest.
Metals:
The conductivity of metals is based on the free electrons (so-called Fermi gas) due to
the metal bonding. Already with low energy electrons become sufﬁciently detached
from the atoms and a conductivity is achieved.
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Al
3+
Free electrons form an electron gas
Fixed aluminum atoms
Fig. 1.1: Metallic bonding: ﬁxed ions and free valence electrons (Fermi gas)
The conductivity depends, inter alia, on the temperature. If the temperature rises, the
metal atoms swing ever stronger, so that the electrons are constrained in their move-
ments. Consequence, the resistance increases. The best conductors, gold and silver, are
used relatively rare because of the high costs (gold e.g. for the contacting of the ﬁn-
ished chips). The alternatives in the semiconductor technology for the wiring of the
individual components of microchips are aluminum and copper.
Page 1

1.1 Conductors - Insulators - Semiconductors
Salts:
In addition to metals, salts can also conduct electricity. There are no free electrons,
so the conductivity depends on ions which can be solved when a salt is melting or
dissolving, so that the ions are free to move (see chapter chemical bonds for details).
1.1.2 Insulators
Insulators possess no free charge carriers and thus are non-conductive.
The atomic bond:
The atomic bond is based on shared electron pairs of nonmetals. The elements which
behave like nonmetals have the desire to catch electrons, thus there are no free electrons
which might serve as charge carriers.
The ionic bond:
In the solid state, ions are arranged in a grid network. By electrical forces, the parti-
cles are held together. There are no free charge carriers to enable a current ﬂow. Thus
substances composed of ions can be both conductor and insulator.
1.1.3 Semiconductors
Semiconductors are solids whose conductivity lies between the conductivity of con-
ductors and insulators. Due to exchange of electrons - to achieve the noble gas conﬁg-
uration - semiconductors arrange as lattice structure. Unlike metals, the conductivity
increases with increasing temperature.
Increasing temperatures leads to broken bonds and free electrons are generated. At the
location at which the electron was placed, a so-called defect electron (“hole”) remains.
The electron ﬂow is based on the conductivity properties of semiconductors. The elec-
tronic band structure illustrates why semiconductors behave like this.
1.1.4 The band model
The electronic band structure is an energy schema to describe the conductivity of con-
ductors, insulators, and semiconductors. The schema consists of two energy bands (va-
lence and conduction band) and the band gap. The valence electrons - which serve as
Page 2. 

Scene 2

1.1 Conductors - Insulators - Semiconductors
Salts:
In addition to metals, salts can also conduct electricity. There are no free electrons,
so the conductivity depends on ions which can be solved when a salt is melting or
dissolving, so that the ions are free to move (see chapter chemical bonds for details).
1.1.2 Insulators
Insulators possess no free charge carriers and thus are non-conductive.
The atomic bond:
The atomic bond is based on shared electron pairs of nonmetals. The elements which
behave like nonmetals have the desire to catch electrons, thus there are no free electrons
which might serve as charge carriers.
The ionic bond:
In the solid state, ions are arranged in a grid network. By electrical forces, the parti-
cles are held together. There are no free charge carriers to enable a current ﬂow. Thus
substances composed of ions can be both conductor and insulator.
1.1.3 Semiconductors
Semiconductors are solids whose conductivity lies between the conductivity of con-
ductors and insulators. Due to exchange of electrons - to achieve the noble gas conﬁg-
uration - semiconductors arrange as lattice structure. Unlike metals, the conductivity
increases with increasing temperature.
Increasing temperatures leads to broken bonds and free electrons are generated. At the
location at which the electron was placed, a so-called defect electron (“hole”) remains.
The electron ﬂow is based on the conductivity properties of semiconductors. The elec-
tronic band structure illustrates why semiconductors behave like this.
1.1.4 The band model
The electronic band structure is an energy schema to describe the conductivity of con-
ductors, insulators, and semiconductors. The schema consists of two energy bands (va-
lence and conduction band) and the band gap. The valence electrons - which serve as
Page 2

1.1 Conductors - Insulators - Semiconductors
This process repeats everywhere in the lattice. While electrons move to the right, holes move to the left.
Si
Si
Si
Si
Si
Si
Si
Si
Si
+
An electron detaches from an atom, a positive charged hole is generated.
Another electron fills the hole. Thereby a new hole is generated.
+
Si
Si
Si
Si
Si
Si
Si
Si
Si
+
Si
Si
Si
Si
Si
Si
Si
Si
Si
+
+
+
+
+
Fig. 1.2: Cut-out of a silicon lattice
charge carriers - are located in the valence band, in the ground state the conduction
band is occupied with no electrons. Between the two energy bands there is the band
gap, its width affects the conductivity of materials.
The energy bands
If we consider a single atom, there are according to the Bohr model of atoms sharply
distinct energy levels, which may be occupied by electrons. If there are multiple atoms
side by side they are interdependent, the discrete energy levels are fanned out. In a
silicon crystal, there are approximately 1023 atoms per cubic centimeter, so that the
individual energy levels are no longer distinguishable from each other and thus form
broad energy ranges.
The width of the energy bands depends on how strongly the electrons are bound to
the atom. The valence electrons in the highest energy level interact strongly with those
of neighboring atoms and can be solved relatively easily from an atom; with a very
large number of atoms, a single electron can no longer be assigned to one single atom.
As a result, the energy bands of the individual atoms merge to a continuous band, the
valence band.
The band model of conductors
In conductors, the valence band is either not fully occupied with electrons, or the ﬁlled
valence band overlaps with the empty conduction band. In general, both states occure
at the same time, the electrons can therefore move inside the partially ﬁlled valence
band or inside the two overlapping bands. In conductors there is no band gap between
Page 3. 

Scene 3

1.1 Conductors - Insulators - Semiconductors
This process repeats everywhere in 
the lattice. While electrons move to 
the right, holes move to the left.
Si
Si
Si
Si
Si
Si
Si
Si
Si
+
An electron    detaches from 
an atom, a positive charged 
hole     is generated.
Another electron fills the hole. 
Thereby a new hole is generated.
+
Si
Si
Si
Si
Si
Si
Si
Si
Si
+
Si
Si
Si
Si
Si
Si
Si
Si
Si
+
+
+
+
+
Fig. 1.2: Cut-out of a silicon lattice
charge carriers - are located in the valence band, in the ground state the conduction
band is occupied with no electrons. Between the two energy bands there is the band
gap, its width affects the conductivity of materials.
The energy bands
If we consider a single atom, there are according to the Bohr model of atoms sharply
distinct energy levels, which may be occupied by electrons. If there are multiple atoms
side by side they are interdependent, the discrete energy levels are fanned out. In a
silicon crystal, there are approximately 1023 atoms per cubic centimeter, so that the
individual energy levels are no longer distinguishable from each other and thus form
broad energy ranges.
The width of the energy bands depends on how strongly the electrons are bound to
the atom. The valence electrons in the highest energy level interact strongly with those
of neighboring atoms and can be solved relatively easily from an atom; with a very
large number of atoms, a single electron can no longer be assigned to one single atom.
As a result, the energy bands of the individual atoms merge to a continuous band, the
valence band.
The band model of conductors
In conductors, the valence band is either not fully occupied with electrons, or the ﬁlled
valence band overlaps with the empty conduction band. In general, both states occure
at the same time, the electrons can therefore move inside the partially ﬁlled valence
band or inside the two overlapping bands. In conductors there is no band gap between
Page 3

1.1 Conductors - Insulators - Semiconductors
Energy
Atoms
E1
E2
E3
2
1
3
1023
1023 energy levels
Fig. 1.3: Energy levels of atoms which are in interdependency with other atoms
Energy
E1
E2
E3
E4
E5
Valence band
Atom distance
Location in the crystal
Conduction band
Fig. 1.4: Energy bands of atoms which are in interdependency with other atoms
the valence band and conduction band.
The band model of insulators
In insulators the valence band is fully occupied with electrons due to the covalent
bonds. The electrons can not move because they are “locked up” between the atoms.
Page 4. 

Scene 4

1.1 Conductors - Insulators - Semiconductors
Energy
Atoms
E1
E2
E3
2
1
3
1023
1023 energy 
levels
Fig. 1.3: Energy levels of atoms which are in interdependency with other atoms
Energy
E1
E2
E3
E4
E5
Valence band
Atom distance
Location in the 
crystal
Conduction band
Fig. 1.4: Energy bands of atoms which are in interdependency with other atoms
the valence band and conduction band.
The band model of insulators
In insulators the valence band is fully occupied with electrons due to the covalent
bonds. The electrons can not move because they are “locked up” between the atoms.
Page 4

1.1 Conductors - Insulators - Semiconductors
To achieve a conductivity, electrons from the valence band have to move into the con-
duction band. This prevents the band gap, which lies in-between the valence band and
conduction band.
Only with considerable energy expenditure (if at all possible) the band gap can be
overcome; thus leading to a negligible conductivity.
The band model of semiconductors
Even in semiconductors, there is a band gap, but compared to insulators it is so small
that even at room temperature electrons from the valence band can be lifted into the
conduction band. The electrons can move freely and act as charge carriers. In addition,
each electron also leaves a hole in the valence band behind, which can be ﬁlled by
other electrons in the valence band. Thus one gets wandering holes in the valence
band, which can be viewed as positive charge carriers.
There are always pairs of electrons and holes, so that there are as many negative as pos-
itive charges, the semiconductor crystal as a whole is neutral. A pure undoped semi-
conductor is known as intrinsic semiconductor. Per cubic centimeter there are about
1010 free electrons and holes (at room temperature).
Since the electrons always assume the energetically lowest state, they fall back into the
valence band and recombine with the holes if there is no energy supply. At a certain
temperature an equilibrium is arranged between the electrons elevated to the conduc-
tion band and the electrons falling back. With increasing temperature the number of
electrons that can leap the band gap is increased, and thus increasing the conductivity
of semiconductors.
Since the width of the band gap represents a certain energy corresponding to a partic-
ular wavelength, one tries to alter the width selective in order to obtain certain colors
of light emitting diodes (LED). This may be achieved by combining different materials.
Gallium arsenide (GaAs) has a band gap of 1.4 eV (electron volts, at room temperature)
and thus emits red light.
The intrinsic conductivity of silicon is of no interest for the functioning of components,
since it depends, inter alia, on the supplied energy. Which means that it changes with
the temperature; in addition a conductivity comparable to metals is only possible at
very high temperatures (several hundred degrees Celsius). In order to deliberately in-
ﬂuence the conductivity of semiconductors, impurity atoms can be introduced into the
regular silicon lattice to alter the number of free electrons and holes.
Page 5. 

Scene 5

1.1 Conductors - Insulators - Semiconductors
To achieve a conductivity, electrons from the valence band have to move into the con-
duction band. This prevents the band gap, which lies in-between the valence band and
conduction band.
Only with considerable energy expenditure (if at all possible) the band gap can be
overcome; thus leading to a negligible conductivity.
The band model of semiconductors
Even in semiconductors, there is a band gap, but compared to insulators it is so small
that even at room temperature electrons from the valence band can be lifted into the
conduction band. The electrons can move freely and act as charge carriers. In addition,
each electron also leaves a hole in the valence band behind, which can be ﬁlled by
other electrons in the valence band. Thus one gets wandering holes in the valence
band, which can be viewed as positive charge carriers.
There are always pairs of electrons and holes, so that there are as many negative as pos-
itive charges, the semiconductor crystal as a whole is neutral. A pure undoped semi-
conductor is known as intrinsic semiconductor. Per cubic centimeter there are about
1010 free electrons and holes (at room temperature).
Since the electrons always assume the energetically lowest state, they fall back into the
valence band and recombine with the holes if there is no energy supply. At a certain
temperature an equilibrium is arranged between the electrons elevated to the conduc-
tion band and the electrons falling back. With increasing temperature the number of
electrons that can leap the band gap is increased, and thus increasing the conductivity
of semiconductors.
Since the width of the band gap represents a certain energy corresponding to a partic-
ular wavelength, one tries to alter the width selective in order to obtain certain colors
of light emitting diodes (LED). This may be achieved by combining different materials.
Gallium arsenide (GaAs) has a band gap of 1.4 eV (electron volts, at room temperature)
and thus emits red light.
The intrinsic conductivity of silicon is of no interest for the functioning of components,
since it depends, inter alia, on the supplied energy. Which means that it changes with
the temperature; in addition a conductivity comparable to metals is only possible at
very high temperatures (several hundred degrees Celsius). In order to deliberately in-
ﬂuence the conductivity of semiconductors, impurity atoms can be introduced into the
regular silicon lattice to alter the number of free electrons and holes.
Page 5

1.1 Conductors - Insulators - Semiconductors
Conduction band
Valence band
Band gap
Valence band
Band gap
Valence band
Insulator
Semiconductor
Conductor
Electron
Energy
Energy
Energy
Conduction band
Conduction band
Fig. 1.5: The band model
Page 6. 

Scene 6

1.1 Conductors - Insulators - Semiconductors
Conduction band
Valence band
Band gap
Valence band
Band gap
Valence band
Insulator
Semiconductor
Conductor
Electron
Energy
Energy
Energy
Conduction band
Conduction band
Fig. 1.5: The band model
Page 6

Fundamentals - Conductors - Insulators - Semiconductors