Point Defects in Semiconductors II: Experimental Aspects

Point Defects in Semiconductors II: Experimental Aspects

J. Bourgoin / Jul 24, 2019

Point Defects in Semiconductors II Experimental Aspects In introductory solid state physics texts we are introduced to the concept of a perfect crystalline solid with every atom in its proper place This is a convenient first step in developing the concept

  • Title: Point Defects in Semiconductors II: Experimental Aspects
  • Author: J. Bourgoin
  • ISBN: 9783540115151
  • Page: 145
  • Format: Hardcover
  • In introductory solid state physics texts we are introduced to the concept of a perfect crystalline solid with every atom in its proper place This is a convenient first step in developing the concept of electronic band struc ture, and from it deducing the general electronic and optical properties of crystalline solids However, for the student who does not proceed furtherIn introductory solid state physics texts we are introduced to the concept of a perfect crystalline solid with every atom in its proper place This is a convenient first step in developing the concept of electronic band struc ture, and from it deducing the general electronic and optical properties of crystalline solids However, for the student who does not proceed further, such an idealization can be grossly misleading A perfect crystal does not exist There are always defects It was recognized very early in the study of solids that these defects often have a profound effect on the real physical properties of a solid As a result, a major part of scientific research in solid state physics has, from the early studies of color centers in alkali halides to the present vigorous investigations of deep levels in semiconductors, been devoted to the study of defects We now know that in actual fact, most of the interest ing and important properties of solids electrical, optical, mechanical are determined not so much by the properties of the perfect crystal as by its im perfections.

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      Published :2019-04-21T02:49:42+00:00

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