Building up a face centered cubic lattice: Difference between revisions

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{{Jmol_general|Face_centered_cubic_lattice.xyz|A face centered cubic lattice}}
* Consider:
* Consider:
# a cubic simulation box whose sides are of length <math>\left. L  \right. </math>
# a cubic simulation box whose sides are of length <math>\left. L  \right. </math>
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*<math> \alpha = \beta = \gamma = 90^0 </math>
*<math> \alpha = \beta = \gamma = 90^0 </math>
[[category: computer simulation techniques]]
[[category: computer simulation techniques]]
[[category: Contains Jmol]]

Revision as of 14:37, 22 July 2009


<jmol>

 <jmolApplet>
 <script>set spin X 10; spin on</script>
 <size>200</size>
 <color>lightgrey</color>
   <wikiPageContents>Face_centered_cubic_lattice.xyz</wikiPageContents>
</jmolApplet>
</jmol>
A face centered cubic lattice
  • Consider:
  1. a cubic simulation box whose sides are of length L
  2. a number of lattice positions, M given by M=4m3,

with m being a positive integer

  • The M positions are those given by:
{xa=ia×(δl)ya=ja×(δl)za=ka×(δl)}

where the indices of a given valid site are integer numbers that must fulfill the following criteria

  • 0≤ia<2m
  • 0≤ja<2m
  • 0≤ka<2m,
  • the sum of ia+ja+ka must be, for instance, an even number.

with δl=L/(2m)

Atomic position(s) on a cubic cell

  • Number of atoms per cell: 4
  • Coordinates:

Atom 1: (x1,y1,z1)=(0,0,0)

Atom 2: (x2,y2,z2)=(0,l2,l2)

Atom 3: (x3,y3,z2)=(l2,0,l2)

Atom 4: (x4,y4,z2)=(l2,l2,0)

Cell dimensions:

  • a=b=c=l
  • α=β=γ=900