Solid State Physics |
From inside the book
Results 1-3 of 7
Page 246
... emitter and collector are each made of n-type semiconductor. As can be seen in Fig. 12-5, the free charge carriers consist of mainly holes in the base, and electrons in the emitter and collector. Let us apply a voltage across the base- ...
... emitter and collector are each made of n-type semiconductor. As can be seen in Fig. 12-5, the free charge carriers consist of mainly holes in the base, and electrons in the emitter and collector. Let us apply a voltage across the base- ...
Page 246
... emitter and collector are each made of n - type semiconductor . As can be seen in Fig . 12-5 , the free charge carriers consist of mainly holes in the base , and electrons in the emitter and collector . Let us apply a voltage across the ...
... emitter and collector are each made of n - type semiconductor . As can be seen in Fig . 12-5 , the free charge carriers consist of mainly holes in the base , and electrons in the emitter and collector . Let us apply a voltage across the ...
Page 249
... emitter . This results in a much smaller density of holes in the base than the density of electrons in the emitter . Consequently , when the base - emitter junction is for- ward biased , the hole current across the junction is much less ...
... emitter . This results in a much smaller density of holes in the base than the density of electrons in the emitter . Consequently , when the base - emitter junction is for- ward biased , the hole current across the junction is much less ...
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