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According to the Landauer formalism [51], the electric current
can be calculated using the electronic transmission function
:
|
(2.27) |
Here,
are the Fermi distribution functions of the source and drain contacts, respectively. In the linear response regime, the electrical current is proportional to the applied voltage:
|
(2.28) |
where the electrical conductance
is defined as:
|
(2.29) |
The derivative of the Fermi function:
|
(2.30) |
is known as the thermal broadening function, where
is the Fermi-level of the system. It has a width of a few
around
, indicating that electrons around the Fermi energy have a major contribution to the electrical current.
Other than the applied voltage, a temperature difference can also result in a flow of charge carriers, as explained in Chapter 1. In the linear response regime, the electrical and heat currents are proportional to the applied voltage, when the temperature difference is zero. They are also proportional to the temperature difference, if there is no applied voltage. These currents are expressed as:
|
(2.31) |
|
(2.32) |
where
and
are the electric and the heat current, respectively. Here,
is the electronic contribution to the thermal conductivity for zero electric field, defined as [52]:
|
(2.33) |
As we show later, the proportionality factor of the temperature difference
in Eq. 2.31 is equal to the product
, where
is the Seebeck coefficient and
is the electrical conductance. We represent this factor by
. Similarly, the proportionality factor of
in Eq. 2.32 is represented by
. Eqs. 2.31 and 2.32 can be rewritten as [30,52]:
|
(2.34) |
|
(2.35) |
where
is the Peltier coefficient and
|
(2.36) |
The Seebeck coefficient can be evaluated by
as [52]:
|
(2.37) |
Next: 2.3.2 Transmission Function
Up: 2.3 Electron Transport
Previous: 2.3 Electron Transport
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H. Karamitaheri: Thermal and Thermoelectric Properties of Nanostructures