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Semi-classical Bulk Transport: EM
field and Transport Equations
• In the previous lecture, we have discussed the balance
equations. We showed that the Boltzmann's Transport
Equation is equivalent to infinite series of balance equation
then we said however we truncate the balance equations
after the energy balance equation namely that is we take only
the 3 balance equation and they are sufficient to model most
of the device phenomena such as velocity saturation, velocity
overshoot and so on
• Now the truncation is achieved by assuming a
phenomenological relation for the energy flux FW. Now we
did not give a relation for FW because the kind of phenomena
that we modeled we really did not have to use FW and so we
just left it at that. Then for these 3 balance equations namely
the carrier balance equations, the momentum balance
equation and the energy balance equation we showed how in
practice in many situations we do not have to use all the
terms of the equation.
we say that spatial non-uniformity of Tn is small that is this term in the gradient of the kinetic
energy is neglected which depends on the temperature gradient. In other words, dou Tn/dou X is
much < Tn/N into dou N/dou X.
The kinetic energy flux and the carrier temperature, electron temperature
and finally the thermal kinetic energy is much greater than the drift kinetic
energy
• So we recall that had said that while for modeling the
effects of electromagnetic field there are standards
equations namely the Maxwell equations and the Lorentz
force equation whereas for modeling the carrier
transport in a semiconductor there are hierarchy and
various levels of equations and various forms of
equations.
• This is because we said that the movement of an
electron in a semiconductor is fairly complex. The
electron undergoes random thermal motion. It collides
with so many particles which are present, so many
entities which are present in a semiconductor and then
there is a directed motion, super imposed over this
random motion and millions of electrons and holes are
all colliding with each other and moving and causing the
flow of current. So because the situation is complex there
are many ways of approaching the modeling of this
problem
THANKYOU

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Semi classical bulk transport

  • 1. Semi-classical Bulk Transport: EM field and Transport Equations
  • 2. • In the previous lecture, we have discussed the balance equations. We showed that the Boltzmann's Transport Equation is equivalent to infinite series of balance equation then we said however we truncate the balance equations after the energy balance equation namely that is we take only the 3 balance equation and they are sufficient to model most of the device phenomena such as velocity saturation, velocity overshoot and so on • Now the truncation is achieved by assuming a phenomenological relation for the energy flux FW. Now we did not give a relation for FW because the kind of phenomena that we modeled we really did not have to use FW and so we just left it at that. Then for these 3 balance equations namely the carrier balance equations, the momentum balance equation and the energy balance equation we showed how in practice in many situations we do not have to use all the terms of the equation.
  • 3.
  • 4.
  • 5. we say that spatial non-uniformity of Tn is small that is this term in the gradient of the kinetic energy is neglected which depends on the temperature gradient. In other words, dou Tn/dou X is much < Tn/N into dou N/dou X.
  • 6. The kinetic energy flux and the carrier temperature, electron temperature and finally the thermal kinetic energy is much greater than the drift kinetic energy
  • 7. • So we recall that had said that while for modeling the effects of electromagnetic field there are standards equations namely the Maxwell equations and the Lorentz force equation whereas for modeling the carrier transport in a semiconductor there are hierarchy and various levels of equations and various forms of equations. • This is because we said that the movement of an electron in a semiconductor is fairly complex. The electron undergoes random thermal motion. It collides with so many particles which are present, so many entities which are present in a semiconductor and then there is a directed motion, super imposed over this random motion and millions of electrons and holes are all colliding with each other and moving and causing the flow of current. So because the situation is complex there are many ways of approaching the modeling of this problem
  • 8.
  • 9.
  • 10.
  • 11.