(2,0,0) plane for simple cubic lattice

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SUMMARY

The (2,0,0) plane exists in a simple cubic lattice, although it may not contain any atoms. In a simple cubic structure, such as cesium chloride, the (200) plane can contribute to diffraction patterns due to the presence of atoms at specific lattice points. For single-atom basis structures like Polonium, the (200) reflection exists but is related to the (100) reflection's intensity by a geometric factor of 1/2, indicating that only half of the (200) planes are occupied. This high degree of symmetry in simple cubic lattices allows for all reflections to be theoretically possible.

PREREQUISITES
  • Understanding of Miller indices in crystallography
  • Familiarity with simple cubic lattice structures
  • Knowledge of X-ray diffraction techniques
  • Basic concepts of atomic basis in crystal structures
NEXT STEPS
  • Research the role of Miller indices in crystal diffraction patterns
  • Explore the properties of cesium chloride as a simple cubic lattice with a two-atom basis
  • Study the diffraction patterns of single-atom basis structures like Polonium
  • Learn about the geometric factors affecting intensity in X-ray diffraction
USEFUL FOR

Crystal physicists, materials scientists, and anyone studying the properties and behaviors of simple cubic lattices and their diffraction characteristics.

feiyangflash
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Hi All,

Does the plane of miller index (2,0,0) exist in simple cubic lattice?

It is easy to understand that (1,0,0) plane exist. But for (2,0,0) plane, I feel confused.

If (2,0,0) plane exists, the plane intersect with the x-axis at 1/2*a, if a is the lattice constant; and the plane is parallel with y-axis and z-axis. However, there is no atoms deployed in this plane! Is there any physical meaning for this plane, since no atom is there? When the X-ray diffraction is done, does this plane ever play a role?

Thank you!

Fei
 
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Hi Fei,

A simple cubic lattice can have a multiple-atom basis. For example, cesium chloride is simple cubic with a two atom basis. The atom at the center of the cell would create a diffraction at the (200) plane. In fact, for simple cubic, all reflections are possible due to the very high degree of symmetry.
 
Hi UBY,

Thank you! Your explanation makes sense.

The alpha form of Polonium (Po) has a simple cubic crystal structure in a single atom basis. Does the plane (2,0,0) have a physical meaning for Polonium?


uby said:
Hi Fei,

A simple cubic lattice can have a multiple-atom basis. For example, cesium chloride is simple cubic with a two atom basis. The atom at the center of the cell would create a diffraction at the (200) plane. In fact, for simple cubic, all reflections are possible due to the very high degree of symmetry.
 
For a single-atom basis, a (200) reflection will still exist, but only as a family member of the (100) reflection. In other words, its intensity would be related to the intensity of the (100) reflection by a geometric factor indicating the fraction of planes present (1/2).

In 2D, draw a series of parallel lines and pretend they are the (100) planes. Now draw a series of dashed lines in between these. The dashed lines AND the parallel lines represent all the equivalent (200) reflections, but only half are actually present in the crystal (the dashed lines are unoccupied).
 

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