Title: Density%20of%20States%20and%20Fermi%20Energy%20Concepts
1Density of StatesandFermi Energy Concepts
2How do Electrons and Holes Populate the Bands?
- Density of States Concept
The number of conduction band states/cm3 lying in
the energy range between E and E dE (if E ?
Ec).
The number of valence band states/cm3 lying in
the energy range between E and E dE (if E ?
Ev).
General energy dependence of gc (E) and gv (E)
near the band edges.
3How do Electrons and Holes Populate the Bands?
- Density of States Concept
Quantum Mechanics tells us that the number of
available states in a cm3 per unit of energy, the
density of states, is given by
Density of States in Conduction Band
Density of States in Valence Band
4How do electrons and holes populate the bands?
- Probability of Occupation (Fermi Function) Concept
- Now that we know the number of available states
at each energy, then how do the electrons
occupy these states? - We need to know how the electrons are
distributed in energy. - Again, Quantum Mechanics tells us that the
electrons follow the Fermi-distribution
function.
Ef Fermi energy (average energy in the
crystal) k Boltzmann constant
(k8.617?10-5eV/K) T Temperature in Kelvin (K)
- f(E) is the probability that a state at energy
E is occupied. - 1-f(E) is the probability that a state at energy
E is unoccupied.
- Fermi function applies only under equilibrium
conditions, however, is universal in the sense
that it applies with all materials-insulators,
semiconductors, and metals.
5How do electrons and holes populate the bands?
Ef
6How do electrons and holes populate the bands?
- Probability of Occupation (Fermi function) Concept
kT 0.0259eV _at_300K
- At T0K, occupancy is digital No occupation
of states above Ef and complete occupation of
states below Ef . - At Tgt0K, occupation probability is reduced with
increasing energy. - f(EEf ) 1/2 regardless of temperature.
7How do electrons and holes populate the bands?
- Probability of Occupation (Fermi function) Concept
kT 0.0259eV _at_300K
- At T0K, occupancy is digital No occupation
of states above Ef and complete occupation of
states below Ef . - At Tgt0K, occupation probability is reduced with
increasing energy. - f(EEf ) 1/2 regardless of temperature.
- At higher temperatures, higher energy states can
be occupied, leaving more lower energy states
unoccupied 1 - f(Ef ).
8How do electrons and holes populate the bands?
- Probability of Occupation (Fermi function) Concept
- If E ? Ef 3kT ?
- Consequently, above Ef 3kT the Fermi function or
filled-state probability decays exponentially to
zero with increasing energy.
9How do electrons and holes populate the bands?
Example 2.2
The probability that a state is filled at the
conduction band edge (Ec) is precisely equal to
the probability that a state is empty at the
valence band edge (Ev). Where is the Fermi energy
locate?
Solution
The Fermi function, f(E), specifies the
probability of electron occupying states at a
given energy E. The probability that a state is
empty (not filled) at a given energy E is equal
to 1- f(E).
10How do electrons and holes populate the bands?
- Probability of Occupation Concept
The density of electrons (or holes) occupying the
states in energy between E and E dE is
Electrons/cm3 in the conduction band between E
and E dE (if E ? Ec).
Holes/cm3 in the conduction band between E and E
dE (if E ? Ev).
0 Otherwise
11How do electrons and holes populate the bands?
- Fermi function and Carrier Concentration
12How do electrons and holes populate the bands?
- Probability of Occupation Concept
13How do electrons and holes populate the bands?
Fermi-Dirac distribution function describing the
probability that an allowed state at energy E is
occupied by an electron.
The density of allowed states for a semiconductor
as a function of energy note that g(E) is zero
in the forbidden gap between Ev and Ec.
The product of the distribution function and the
density-of-states function
14How do electrons and holes populate the bands?
- Typical band structures of Semiconductor
number of electrons per unit energy per unit
volume The area under nE(E) vs. E is the electron
concentration.
number of states per unit energy per unit volume
probability of occupancy of a state
g(E) X f(E) Energy density of electrons in the CB
Energy band diagram
Density of states
Fermi-Dirac probability function
15Metals vs. Semiconductors
Ef
Ef
Metal
Semiconductor
- Allowed electronic-energy-state systems for metal
and semiconductors. - States marked with an X are filled those
unmarked are empty.
16Metals vs. Semiconductors
- Allowed electronic-energy states g(E)
The Fermi level Ef is at an intermediate energy
between that of the conduction band edge and that
of the valence band edge.
Fermi level Ef immersed in the continuum of
allowed states.
Ef
Ef
Metal
Semiconductor
17How do electrons and holes populate the bands?
- Fermi function and Carrier Concentration
- Note that although the Fermi function has a
finite value in the gap, there is no electron
population at those energies. (that's what
you mean by a gap) - The population depends upon the product of the
Fermi function and the electron density of
states. So in the gap there are no electrons
because the density of states is zero. - In the conduction band at 0K, there are no
electrons even though there are plenty of
available states, but the Fermi function is zero. - At high temperatures, both the density of states
and the Fermi function have finite values in the
conduction band, so there is a finite conducting
population.
18How do electrons and holes populate the bands?
19How do electrons and holes populate the bands?
- Intrinsic Energy (or Intrinsic Level)
Ef is said to equal Ei (intrinsic energy) when
equal number of electrons and holes.
20How do electrons and holes populate the bands?
Intrinsic Equal number of electrons and
holes n-type More electrons than
Holes p-type More holes than electrons
21How do electrons and holes populate the bands?
- Pure-crystal energy-band diagram
22How do electrons and holes populate the bands?
23How do electrons and holes populate the bands?
24Intrinsic, n-Type, p-Type Semiconductors
C
B
E
E
E
c
c
c
E
f
n
E
f
i
E
f
p
E
E
E
v
v
v
V
B
(
c
) p-type
(
a
) intrinsic
(
b
) n-type
np ni2
Note that donor and acceptor energy levels are
not shown.
25How do electrons and holes populate the bands?
- Heavily Doped Dopant States
E
C
B
E
C
B
n
F
Impurities forming bands
E
E
c
c
g
(
E
)
E
E
v
v
E
F
p
V
B
Degenerated n-type semiconductor Large number of
donors form a band that overlaps the CB
Degenerated p-type semiconductor