Solution LAB3 graphene: Difference between revisions
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==Step 3 == | |||
*Let's consider the path Gamma-->M-->K-->Gamma |
Revision as of 11:57, 1 April 2021
- Back to the previous page: Electronic properties of 2D and 1D systems#Exercise 1: Graphene
Step 1
- Graphene has an honeycomb lattice and we can define the unit cell by considering an hexagonal lattice and two atoms per cell. The CC distance is 0.142nm. An input file can be set using an hexagonal bravais lattice as:
&system ibrav= 4, celldm(1) =4.6542890, celldm(3)=something appropriate, nat= 2, ntyp= 1, [...] / ATOMIC_POSITIONS {crystal} C 0.0000000 0.0000000 0.000000 C 0.3333333 0.6666666 0.000000
- Graphene is a quasi-metal, pay attention to the smearing
- K point sampling on the plane. If multiple of 3 you can include the high symmetry point K in your sampling
- You may want visualise your input using xcrysden and measure the CC distance
Step 2
- When relaxing the system you may want to keep fixed the direction orthogonal to the graphene sheet. This is done by inserting in your input the CELL namelist
&CELL cell_dofree='2Dxy' ... /
Step 3
- Let's consider the path Gamma-->M-->K-->Gamma