Bravais basis lattice vectors b,, b2, b3 are defined with the real space basis vectors a1, a2, az in the following: 2π(a, x α,) ,b2 [а, (аz х аз)1" 2n (az x a,) 2π(α x ,) b1 and b3 [а, (аz х аз)] [a1 · (a2 x a3)] 27(b2xb3) [b1•(b2×b3)] Prove its inversion vector relation a, = etc by vector identities like A × (B × C) = В (A- С) — С(А В) and A - (В x С) B· (C × A) = C ·(A × B). %|
Bravais basis lattice vectors b,, b2, b3 are defined with the real space basis vectors a1, a2, az in the following: 2π(a, x α,) ,b2 [а, (аz х аз)1" 2n (az x a,) 2π(α x ,) b1 and b3 [а, (аz х аз)] [a1 · (a2 x a3)] 27(b2xb3) [b1•(b2×b3)] Prove its inversion vector relation a, = etc by vector identities like A × (B × C) = В (A- С) — С(А В) and A - (В x С) B· (C × A) = C ·(A × B). %|
Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
Problem 1RQ
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