Page 53 - Microsensors, MEMS and Smart Devices - Gardner Varadhan and Awadelkarim
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3



      MeMS Materials and their

     Preparation









     3.1  OVERVIEW

     Microelectromechanical  system (MEMS) materials may be classified into five main types:
     metals,  semiconductors,  ceramics, polymers, and composites. This  chapter  first  introduces
     the  basic  nature of  each  type of  material  and  then discusses  the  different  ways in which
     they  can be  prepared.  It  also  provides  the  reader  with a brief  overview of the underlying
                                                                         1
     physical structure of these materials  and how they relate to their material properties .  More
     advanced  readers  may  wish to  omit  parts  of  this  chapter  as  the  details  given  here  on  the
     preparation  of  electronic-grade  silicon  (EGS)  are  also  presented  in  Chapter 4,  Standard
     Microelectronic  Technologies, that discusses  the  central role  of  silicon  processing within
     the  fields  of  microsensors  and  smart devices.



     3.1.1  Atomic  Structure  and  the  Periodic  Table

     To  understand the  classification of  materials,  it  is  necessary  to  understand the quantum
     mechanical  structure  of  an  atom  and  relate  it  to  the  nature  of  the  macroscopic  bulk
     material.  Every  atom  in  an  element  is  made  up  of  a  small,  positively  charged  nucleus,
     which is balanced  in charge by the negatively charged  electrons  surrounding the nucleus.
     The  positive  charge  in  the  nucleus  arises  from  nuclear  particles  called  protons.  Each
     proton  possesses  a  positive  charge  that  is  equal  in  magnitude  to  the  negative  charge
     of  an  electron  e,  and  in  a  neutral  atom  the  number of  protons  in  the  nucleus is  equal
     to  the  number  of  electrons  outside  the  nucleus. The  number  of  electrons  around  the
     nucleus,  or  the number of protons  in the nucleus, of  a neutral atom is equal to its  atomic
     number  Z.
        If  we consider a one-electron  atomic model, such as that for hydrogen, then the energy
        of its  single electron  can only have values given by  the following equation (Tuck and
     E n
     Christopoulos  (1986)):
                                           2
                                         Z m ee 4  1


     1
       See Moseley  and Crocker  (1996) for  a review  of  sensor  materials.
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