Solid State Physics |
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Page 181
... temperature dependent . The ions vibrate with larger amplitude at high temperatures and thus scatter the conduction electrons more often . In general , the resistivity ρ = 1 / σ of a metal due to lattice vibrations is linear in the ...
... temperature dependent . The ions vibrate with larger amplitude at high temperatures and thus scatter the conduction electrons more often . In general , the resistivity ρ = 1 / σ of a metal due to lattice vibrations is linear in the ...
Page 206
... Temperature Dependence of n Consider the effect of temperature on n and p for an n - type semiconductor . If Nd > n ; at room temperature , then raising the temperature a bit does not affect n very much . A few more electrons are ...
... Temperature Dependence of n Consider the effect of temperature on n and p for an n - type semiconductor . If Nd > n ; at room temperature , then raising the temperature a bit does not affect n very much . A few more electrons are ...
Page 311
... temperature dependence of 181 , 209 Constructive interference 39 Contact ohmic 254 rectifying 258 Contact potential 218 , 221 Cooper , L. N. 281 Cooper pairs 281 Copper band structure of 167 Bragg reflections in 57 , 58 dispersion curve ...
... temperature dependence of 181 , 209 Constructive interference 39 Contact ohmic 254 rectifying 258 Contact potential 218 , 221 Cooper , L. N. 281 Cooper pairs 281 Copper band structure of 167 Bragg reflections in 57 , 58 dispersion curve ...
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