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Difference between revisions of "Atomic modulation function"

From Online Dictionary of Crystallography

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in the basic structure are given by
 
in the basic structure are given by
  
<math>{\bf r}({\bf n},j)~=~{\bf n}+{\bf r}_j+{\bf u}_j({\bf n}+{\bf r}_j).</math>
+
<math>r(n,j) = n~+~r_j+u_j((n+r_j).</math>
  
The occupation probability to find an atom of species ''A'' at the position <math>{\bf n}+{\bf r}_j</math>
+
The occupation probability to find an atom of species ''A'' at the position <math>n+r_j</math>
is <math>p_A({\bf n},j)</math>, where the sum over the species of the functions <math>p_A</math>
+
is <math>p_A(n,j)</math>, where the sum over the species of the functions <math>p_A</math>
 
is one. Instead of a different species, one may have a vacancy. The functions
 
is one. Instead of a different species, one may have a vacancy. The functions
<math>{\bf u}({\bf n},j)</math> and <math>p_A({\bf n},j)</math> are the  ''atomic modulation functions''.
+
<math>u(n,j)</math> and <math>p_A(n,j)</math> are the  ''atomic modulation functions''.
 
For a crystal they should have Fourier modules of finite rank,  ''i.e''. the
 
For a crystal they should have Fourier modules of finite rank,  ''i.e''. the
 
functions have Fourier transforms with delta peaks on wave vectors  '''k''' of the form
 
functions have Fourier transforms with delta peaks on wave vectors  '''k''' of the form
  
   <math>{\bf k}~=~\sum_{i=1}^n h_i {\bf a}_i^*,~~(h_i~~{\rm integers},~n~{\rm finite}.)</math>
+
   <math>k~=~\sum_{i=1}^n h_i a_i^*,~~(h_i~~{\rm integers},~n~{\rm finite}.)</math>
  
 
Modulation functions may be continuous or discontinuous.
 
Modulation functions may be continuous or discontinuous.

Revision as of 17:05, 18 May 2009

Atomic Modulation Function


Fonction de modulation atomique (Fr.)

Definition

A modulated structure is a structure that may be obtained from a crystalline system with space group symmetry, and therefore with lattice periodicity, by a regular displacement of atoms (displacive modulation) and/or change in the occupation probability of a site in the basic structure. The deviation from the positions in the basic structure are given by

[math]r(n,j) = n~+~r_j+u_j((n+r_j).[/math]

The occupation probability to find an atom of species A at the position [math]n+r_j[/math] is [math]p_A(n,j)[/math], where the sum over the species of the functions [math]p_A[/math] is one. Instead of a different species, one may have a vacancy. The functions [math]u(n,j)[/math] and [math]p_A(n,j)[/math] are the atomic modulation functions. For a crystal they should have Fourier modules of finite rank, i.e. the functions have Fourier transforms with delta peaks on wave vectors k of the form

 [math]k~=~\sum_{i=1}^n h_i a_i^*,~~(h_i~~{\rm integers},~n~{\rm finite}.)[/math]

Modulation functions may be continuous or discontinuous.