| 1. | .. . is a reciprocal lattice vector of the reciprocal lattice.
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| 2. | Another helpful ingredient in the proof is the " reciprocal lattice vectors ".
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| 3. | These reciprocal lattice vectors of the FCC represent the basis vectors of a BCC real lattice.
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| 4. | E are energies, k and q are wave vectors and G denotes a reciprocal lattice vector.
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| 5. | An arbitrary vector, G, defines the reciprocal lattice vector between the ends of any two k vectors.
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| 6. | Consider what happens when the lattice vectors are varied, resulting in a change in the reciprocal lattice vectors.
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| 7. | The dispersion relations show conics of the free-electron energy dispersion parabolas for all possible reciprocal lattice vectors.
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| 8. | Physically, the reciprocal lattice vectors act as additional chunks of momentum which the lattice can impart to the phonon.
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| 9. | Measuring the momentum of one electronic state gives a distribution of momenta which are all separated by reciprocal lattice vectors.
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| 10. | In accordance with Bragg's law, each ring corresponds to a particular reciprocal lattice vector G in the sample crystal.
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