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Problems are listed in approximate order of difficulty. A single dot (•) indicates straigh...

Problems are listed in approximate order of difficulty. A single dot (•) indicates straightforward problems involving just one main concept and sometimes requiring no more than substitution of numbers in the appropriate formula. Two dots (••) identify problems that are slightly more challenging and usually involve more than one concept. Three dots (•••) indicate problems that are distinctly more challenging, either because they are intrinsically difficult or involve lengthy calculations. Needless to say, these distinctions are hard to draw and are only approximate.

•• The donor state wave functions in silicon have small binding energies (Ebinding ≈ 0.05 eV) and large Bohr radii (ad ≈ 3 nm) for two reasons: (1) Because of the interaction between the lattice and the “nearly free” electrons in the conduction band, the electrons behave as if their mass was smaller than the free-electron mass. The “effective mass” in silicon is m* ≈ 0.2 me. (2) The polarization of the silicon lattice partially shields the +1e charge of the impurity site. In general, the force of electrostatic attraction between two charges in a polarizable medium is given by F = kq1 q2/(Kr2), where K is a dimensionless number called the dielectric constant. In silicon, K = 11.7. (a) Derive expressions for the Bohr radius and the ionization energy of the ground state of a donor wave function with effective mass m* and in a medium with dielectric constant K. (b) Compute the values of the ionization energy and Bohr radius of a donor state in silicon. (Compare your values with the known values for phosphorus in silicon of (Ebinding = 45 meV and adonor = 3.0 nm.)

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