Phy5670/Phonon in Graphene: Difference between revisions
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Then the reciprocal lattice parameters can by generated by using <math>\vec{b_i}\cdot \vec{a_j}=2\pi\delta_{ij}, (i,j=1,2)</math> | Then the reciprocal lattice parameters can by generated by using <math>\vec{b_i}\cdot \vec{a_j}=2\pi\delta_{ij}, (i,j=1,2)</math> | ||
<math>\vec{b_1}=\frac{2\pi}{a}(\frac{\sqrt{3}}{3}\hat{x}+\ | <math>\vec{b_1}=\frac{2\pi}{a}(\frac{\sqrt{3}}{3}\hat{x}+\frac{1}{3}\hat{y})</math> | ||
<math>\vec{b_2}=\frac{2\pi}{a}(-\frac{\sqrt{3}}{2}a\hat{x}+\ | <math>\vec{b_2}=\frac{2\pi}{a}(-\frac{\sqrt{3}}{2}a\hat{x}+\frac{3}{2}a\hat{y})</math> |
Revision as of 17:13, 3 December 2010
Introduction
Structure of Graphene
Carbon atoms in graphene are constructed on a honeycomb lattice, which is shown in Fig. 1. The circle and solid point together combine into a two-point basis in the Bravais lattice. The carbon-carbon distance is . The primitive vectors are
Then the reciprocal lattice parameters can by generated by using