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Published byArlene Lambert Modified over 9 years ago
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The review of modern physics has given us a description of nature. Waves are described with a wave equation. Particles are described with particle equations. Experiments indicated that particle phenomena could be explained with a wave theory. Experiments indicated that wave phenomena could be described with particle theory. Schrodinger equation evolved whose solutions yielded a probability density of finding a state. Fermi function determined whether the state was filled.
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Materials could now be described. Materials were understood in terms of an energy band diagram. Conduction band – valence band – Fermi energy. Electrons being promoted from the valence band into the conduction band left a vacancy (“hole”) in the valence band. “n type” semiconductor and “p type” semiconductor.
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Basic model pn Homogeneous doping model
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Homogeneous doping model p n +- Electrons diffuse into the p region and holes diffuse into the n region. This creates an electric field.
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p n
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Forces on electrons and holes p n diffusion force on electrons diffusion force on holes E field force on holes E field force on electrons
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Basic model – thermal equilibrium p n +-
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electrons and holes face a barrier p n +- + -
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Electron density in the conduction band of the n type material p n +-
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Hole density in the p type semiconductor material p n +-
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Barrier potential can now be defined
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Potential distribution in the depletion region p n +-
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V = 0
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Voltage is continuous
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Reverse biased PN junction p n p n
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Reverse biased PN junction energy diagram
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Voltage-dependent capacitor
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Simple three-dimensional unit cell
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