What Is the Shortest Reciprocal Vector for a BCC Lattice?

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SUMMARY

The shortest reciprocal vector G for a Body-Centered Cubic (BCC) lattice is derived from the equation G = (2π/a)((v2 + v3) x + (v1 + v3) y + (v1 + v2) z). The length of this vector is calculated using l(v1, v2, v3) = √((v2 + v3)² + (v1 + v3)² + (v1 + v2)²). The attempt to minimize this length leads to a linear equation system that only yields trivial solutions, indicating a need for non-zero integer values for v1, v2, and v3. The correct approach involves recognizing the general reciprocal lattice vector for BCC and constructing the first Brillouin zone.

PREREQUISITES
  • Understanding of reciprocal lattice vectors
  • Familiarity with Body-Centered Cubic (BCC) lattice structures
  • Knowledge of Brillouin zones in solid-state physics
  • Basic calculus for optimization techniques
NEXT STEPS
  • Study the derivation of reciprocal lattice vectors for different crystal structures
  • Learn about the construction of Brillouin zones in BCC lattices
  • Explore optimization techniques in multivariable calculus
  • Investigate the implications of reciprocal lattice vectors in electronic band structure
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Students and researchers in solid-state physics, materials science, and crystallography who are working with BCC lattices and reciprocal space analysis.

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Homework Statement



Find the shortest reciprocal vector G, given below, v_1,...,v_3 are integers.

[tex]\vec{G} = \frac{2 \pi}{a}\left( (v_2 + v_3 )\vec{x} + (v_1 + v_3 )\vec{y} + (v_1 + v_2 )\vec{z} \right)[/tex]

Homework Equations



x,y,z are ortonogal, length 1

[tex]l = l(v_1, v_2, v_3) = \vert \vec{G} \vert = \sqrt{\vec{G}\cdot \vec{G}}[/tex]

[tex]l = \sqrt{ (v_2 + v_3 )^{2} + (v_1 + v_3 )^2 +(v_1 + v_2 )^2 }[/tex]

The Attempt at a Solution



I want to minimize l(v_1, v_2, v_3)

[tex]\dfrac{\partial l}{\partial v_1} = \dfrac{2 \pi \left( (v_1 + v_3 ) + (v_1 + v_2 ) \right) }{\sqrt{ (v_2 + v_3 )^{2} + (v_1 + v_3 )^2 +(v_1 + v_2 )^2 }} = 0[/tex]

etc. Gives me following linear equation system, it has only trivial solutions

[tex] \left( \begin{array}{ccc|c} 2 & 1 & 1 & 0 \\ 1 & 2 & 1 & 0 \\ 1 & 1 &2 & 0 \end{array}\right)[/tex]

v_1 = v_2 = v_3 = 0

And that is not true, they should be something like

[tex]\frac{2 \pi}{a} \left( \pm \vec{x} \pm \vec{y} \right)[/tex]

etc.


Now what have I do wrong

by the way, this is the general reciprocal lattice vetctor for bcc lattice. I want to construct the first Brillouion zone.
 
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