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Calculate the band gap under the assumption that the variation in the<br />

conductivity is partly caused by the increase in the density of charge<br />

carriers and partly arises from the mobility, µ, of the charge carriers being<br />

temperature dependent because of the thermal vibrations of the atoms.<br />

Assume that µ ∝ T -3/2 in the relevant temperature interval.<br />

3. Determine the maximum concentration (atomic fraction) of donor atoms<br />

that can be allowed in the substances in the table below for intrinsic<br />

conduction to dominate at room temperature. Is it possible to realise this<br />

practically in any of these cases?<br />

Substance Bandgap [eV] Density [kg/m 3 ]<br />

Diamond 5.33 3.51 x 10 3<br />

Silicon 1.14 2.42 x 10 3<br />

Germanium 0.62 5.35 x 10 3<br />

4. A silicon crystal is doped with Sb atoms to a concentration of 10 21 m -3 .<br />

The impurity level lies 0.04 eV from the nearest band edge. Assume that<br />

the band gap at 450 K is Eg = 1.14 eV. Calculate the conductivity at T = 450<br />

K. Approximate the effective masses with the free electron mass and<br />

assume that all impurity centres are ionised at room temperature. The<br />

mobilities are: µe = 0.13 m 2 /Vs and µ h = 0.05 m 2 /Vs.<br />

5. Calculate the concentration of electrons and holes in a p-type<br />

semiconductor if the conductivity σ = 10 (Ωm) -1 , the mobilities are µ h =<br />

0.2 m 2 /Vs and µe = 0.4 m 2 /Vs and the concentration of intrinsic carriers<br />

is ni = 2.2 x 10 19 m -3 .<br />

6. A silicon crystal is doped with 5 x 10 20 As atoms/m 3 . The donor level<br />

lies 0.05 eV from the edge of the conduction band, and the band gap is<br />

5

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