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The Quantum Theory of Solids Allowed and forbidden energy bands Pauli Exclusion Principle In any given system, no two electrons can occupy the same state Application Two interacting hydrogen atoms
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The Quantum Theory of Solids Allowed and forbidden energy bands Application to Silicon nlmspin 3s3001/2 or -1/2 3p31-1,0,11/2 or -1/2 n - principal; l - angular (0..n-1); m- magnetic (-l..+l)
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The Quantum Theory of Solids Allowed and forbidden energy bands The k-space diagram where
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The Quantum Theory of Solids Allowed and forbidden energy bands The k-space diagram (cont.)
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The Quantum Theory of Solids Electrical Conduction in Solids Silicon at T = 0K All valence electrons are in the valence band
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The Quantum Theory of Solids Electrical Conduction in Solids Silicon at T > 0K Some electrons have moved into the conduction band
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The Quantum Theory of Solids Effective Mass but, difficult to know Fint, therefore where m* takes into account internal forces Analogy a force acting on ball in air vs. ball in oil Given concept of m*, we can determine acceleration in normal way F= -eE = m*a, therefore a = -eE/m*
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The Quantum Theory of Solids Concept of a Hole Current flow may be thought of as the movement of valence electrons elevated to the conduction band Alternatively, can think of this process as the flow of (positively-charged) holes
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The Quantum Theory of Solids Metals, Insulators, and Semiconductors Insulator Semiconductor Conductor non-overlapping overlapping
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The Quantum Theory of Solids Extension to three dimensions direct bandgap indirect bandgap
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The Quantum Theory of Solids Density of states E c - lowest energy of the conduction band E v - highest energy of the valence band
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The Quantum Theory of Solids Statistical mechanics Number of possibilities for N particles in g states For n energy levels Most probable distribution
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The Quantum Theory of Solids Statistical mechanics(cont.)
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The Quantum Theory of Solids Statistical mechanics(cont.) Boltzmann approximation
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