Solid State Physics |
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Page 6
... solid state physics covered . The purpose of this course is to acquaint the student with the fundamental physics of solids . This emphasis is on under- standing the behavior of electrons in metals and semiconduc- tors . In the first 3 ...
... solid state physics covered . The purpose of this course is to acquaint the student with the fundamental physics of solids . This emphasis is on under- standing the behavior of electrons in metals and semiconduc- tors . In the first 3 ...
Page 68
... solid line ) near k = 0 . = Sound propagates through crystals as such a lattice wave . Since 2π / k by definition , very small values of k ( k « a ̄1 ) correspond to very long wavelengths ( λ ≫ a ) . A typical sound wave in a solid has ...
... solid line ) near k = 0 . = Sound propagates through crystals as such a lattice wave . Since 2π / k by definition , very small values of k ( k « a ̄1 ) correspond to very long wavelengths ( λ ≫ a ) . A typical sound wave in a solid has ...
Page 308
... Solid State Physics ( Addison - Wesley , Reading , Mass . , 1975 ) . I have used this book for an upper- division course for physics majors . Gerald Burns , Solid State Physics ( Academic Press , New York , 1985 ) . An excellent book ...
... Solid State Physics ( Addison - Wesley , Reading , Mass . , 1975 ) . I have used this book for an upper- division course for physics majors . Gerald Burns , Solid State Physics ( Academic Press , New York , 1985 ) . An excellent book ...
Common terms and phrases
Answer atoms average bond Bragg angle Bragg's Law Bravais lattice Brillouin zone called Chapter classical model collisions conduction electrons Consider constructively interfere Cooper pairs copper depletion layer direction dispersion curve displacement distance doped effective mass elec electric current electric field electrons and holes energy band equal example fcc lattice Fermi energy Fermi level Fermi surface force free electron free particle frequency given by Eq inside ions k-space laser lattice parameter lattice points lattice vector lattice wave magnetic field n-type semiconductor Na+-Cl NaCl negative neutrons number of electrons obtain occupied one-dimensional oscillate p-n junction p-side n-side photon planes positively charged potential energy primitive unit cell Problem rays reciprocal lattice reverse biased scattered Schroedinger's equation shown in Fig sodium metal superconductor temperature thermal energy tion transistor trons unit cell unoccupied values velocity voltage wave function wave number wave vector wavelength wire x-ray diffraction zero