Solid State Physics |
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Page 111
... trons with moderate energy have a de Broglie wavelength equal to that of x rays . If de Broglie's postulate is correct , elec- trons should exhibit wave behavior like we usually observe for x rays . For example , electrons should be ...
... trons with moderate energy have a de Broglie wavelength equal to that of x rays . If de Broglie's postulate is correct , elec- trons should exhibit wave behavior like we usually observe for x rays . For example , electrons should be ...
Page 209
... trons , ( b ) the holes , and ( c ) the electrons and holes together . Answer : 21.6 / n - m , 7.3 × 10-10 / N.m , 21.6 / .m . Problem 10-15 . Calculate the mobility of conduction elec- trons in sodium metal ( Na ) . Answer : 5.90 × 10 ...
... trons , ( b ) the holes , and ( c ) the electrons and holes together . Answer : 21.6 / n - m , 7.3 × 10-10 / N.m , 21.6 / .m . Problem 10-15 . Calculate the mobility of conduction elec- trons in sodium metal ( Na ) . Answer : 5.90 × 10 ...
Page 268
... trons in states of energy E2 than in states of energy E1 . Elec- trons in states of energy E1 can absorb photons . If there are more electrons in these states than in states of energy E2 , then a photon would more likely be absorbed ...
... trons in states of energy E2 than in states of energy E1 . Elec- trons in states of energy E1 can absorb photons . If there are more electrons in these states than in states of energy E2 , then a photon would more likely be absorbed ...
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