Solid State Physics |
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Page 8
... integers inside a set of square brackets . The direction R = n1aî + n2aĵ + nзak in a cubic crystal , for example , is written as [ n1 , n2 , ng ] . The integers are usually chosen to be as small as possible . Three common directions in ...
... integers inside a set of square brackets . The direction R = n1aî + n2aĵ + nзak in a cubic crystal , for example , is written as [ n1 , n2 , ng ] . The integers are usually chosen to be as small as possible . Three common directions in ...
Page 11
... integers inside a set of parentheses . In cubic crystals , a plane denoted by ( n1 , n2 , n3 ) is perpendicular to the direction [ n1 , n2 , n3 ] . These three integers n1 , n2 , n3 , when referring to crystal planes , are called Miller ...
... integers inside a set of parentheses . In cubic crystals , a plane denoted by ( n1 , n2 , n3 ) is perpendicular to the direction [ n1 , n2 , n3 ] . These three integers n1 , n2 , n3 , when referring to crystal planes , are called Miller ...
Page 72
... integers ( 2n , 2n + 2 , etc. ) and atoms of mass m2 with odd integers ( 2n − 1 , 2n + 1 , 2n + 3 , etc. ) . The equations of motion for the two kinds of atoms are given by - d2u2n ― -a ( 2u2n − U2n + 1 − U2n− - u2n - 1 ) = m1 ( 3 ...
... integers ( 2n , 2n + 2 , etc. ) and atoms of mass m2 with odd integers ( 2n − 1 , 2n + 1 , 2n + 3 , etc. ) . The equations of motion for the two kinds of atoms are given by - d2u2n ― -a ( 2u2n − U2n + 1 − U2n− - u2n - 1 ) = m1 ( 3 ...
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