Fundamentals of Carrier Transport, Second Edition

When the carrier density is high, collisions between carriers are an important scattering mechanism. Two types of processes must be distinguished a binary process in which one carrier collides with another and a collective process in which a carrier interacts with the plasma comprised by the carriers.
For the binary process, which is depicted in Fig. 2.17, momentum and energy conservation dictate that
| (2.99a) | |
and
| (2.99b) | |
where p and p ? are the momentum of the carrier before and after the collision, and p 2 and
refer to the carrier it collides with. Although the total momentum and energy of the carrier ensemble cannot change by carrier-carrier scattering, the distribution of momenta can be affected. By altering the distribution, carrier-carrier scattering affects the average relaxation times and, therefore, the value of observables such as the average carrier velocity and energy.
To write the collision term for carrier-carrier scattering, we define a pair transition rate, S (p, p 2; p ?,
) which is the probability per unit time that carrier at p and p 2 collide and scatter to p ? and
. When viewed in the center-of-mass reference frame, the binary carrier-carrier collision looks just like an ionized impurity scattering event. By analogy with eq. (2.36a) for ionized impurity scattering, we write the pair...