Solid State Physics |
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Page 6
... consider only crystalline solids . A crystal is a solid in which all the atoms are arranged in a periodic manner . As a simple example , consider the cubic ar- rangement of atoms shown in Fig . 1-1 . We show only a portion of the ...
... consider only crystalline solids . A crystal is a solid in which all the atoms are arranged in a periodic manner . As a simple example , consider the cubic ar- rangement of atoms shown in Fig . 1-1 . We show only a portion of the ...
Page 63
... Consider the one - dimensional lattice shown in Fig . 3-2 . The atoms each have mass m and are connected to nearest neighbors by springs , each with spring constant a . When at rest in their positions of equilibrium , the atoms are ...
... Consider the one - dimensional lattice shown in Fig . 3-2 . The atoms each have mass m and are connected to nearest neighbors by springs , each with spring constant a . When at rest in their positions of equilibrium , the atoms are ...
Page 238
... Consider the junction in Problem 11-4 . If we reverse - bias this junction with 10.0 V , find the width of the depletion layer ( e , -12 in Si ) . Answer : 5.30 μm . 11-9 Capacitance of Junction A p - n junction has capacitance . As we ...
... Consider the junction in Problem 11-4 . If we reverse - bias this junction with 10.0 V , find the width of the depletion layer ( e , -12 in Si ) . Answer : 5.30 μm . 11-9 Capacitance of Junction A p - n junction has capacitance . As we ...
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