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Partition function for electrons/holes

  1. May 4, 2009 #1
    1. The problem statement, all variables and given/known data
    By shining and intense laser beam on to a semiconductor, one can create a collection of electrons (charge -e, and effective mass me) and holes (charge +e, and effective mass mh) in the bulk. The oppositely charged particle may pair up (as in a hydrogen atom) to form a gas of excitons, or they may dissociate into an electron hole plasma.

    a) Write down the single particle partition functions Ze(1) and Zh(1) at temperature T in a volume V for electrons and holes respectively. (The thermal wavelength [tex]\lambda[/tex] for a particle is [tex]\lambda[/tex] = [tex]\frac{h}{\sqrt{2 \pi mkT}}[/tex]


    2. Relevant equations


    3. The attempt at a solution
    I know that the partition function is exp[-E/kT] summed over all energies or integrated with a density of states over all energies. But how do I go about it in this case?
     
  2. jcsd
  3. May 4, 2009 #2
    In our notes somewhere (section 11/12/13), you can see that he uses the equation:

    Z(1) = (V/λ^3), where V is the volume.

    I'm not sure where it comes from, but I think we just need to learn it.
     
  4. May 4, 2009 #3
    You can obtain that formula by summing over all the energy states by approximating the summation by an integral using the fact that the number of quantum states within a volume V_p of momentum space is

    V V_p/h^3

    So, if you integrate over all momenta, the energy is E = p^2/(2m) and you can write:

    Z1 = Integral of V d^3p/h^3 exp[-beta p^2/(2m)] =

    V/h^3 Integral from |p| = 0 to infinity of 4 pi p^2
    exp[-beta p^2/(2m)] d|p|

    For electrons you must multiply this by 2 because there are two spin states for each energy eigenstate.
     
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