Solid State Physics |
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Page 25
Harold T. Stokes. 1-10 Cesium Chloride Structure Another rather common structure is that of CsCl ( cesium chloride ... STRUCTURE 25 Cesium Chloride Structure.
Harold T. Stokes. 1-10 Cesium Chloride Structure Another rather common structure is that of CsCl ( cesium chloride ... STRUCTURE 25 Cesium Chloride Structure.
Page 26
... structure . The large and small spheres represent two different types of atoms . Problem 1-16 . Using data in Appendix 3 , find the volume of a primitive unit cell in a crystal of cesium chloride ( CsCl ) ... STRUCTURE Zincblende Structure.
... structure . The large and small spheres represent two different types of atoms . Problem 1-16 . Using data in Appendix 3 , find the volume of a primitive unit cell in a crystal of cesium chloride ( CsCl ) ... STRUCTURE Zincblende Structure.
Page 28
... structure are the same type , we can still tell the a Fig . 1-27 . The conventional unit cell of the diamond structure . All atoms are identical . ( a ) ( b ) Fig . 1-28 . 28 CHAPTER 1 CRYSTAL STRUCTURE Diamond Structure.
... structure are the same type , we can still tell the a Fig . 1-27 . The conventional unit cell of the diamond structure . All atoms are identical . ( a ) ( b ) Fig . 1-28 . 28 CHAPTER 1 CRYSTAL STRUCTURE Diamond Structure.
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