Electronic properties of 2D and 1D systems: Difference between revisions

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==Exercises:==
==Exercises:==
===Exercise 1: Grapehene===
===Exercise 1: Grapehene===
 
[[File:honeycomb.png|200px|thumb]]
*build a supercell for an ideal graphene structure
*build a supercell for an ideal graphene structure
*relax the supercell
*relax the supercell
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[[Solution_LAB3_graphene | Hints]]
[[Solution_LAB3_graphene | Hints]]
===Exercise 2: Hexagonal Boron Nitrite (hBN)===
===Exercise 2: Hexagonal Boron Nitrite (hBN)===


===Exercise 3: A small CNT===
===Exercise 3: A small CNT===

Revision as of 09:52, 1 April 2021

Prev:LabQSM#Module 3: Low dimensional structures (6h)

Input set-up for a low dimensional system:

Now we want to deal with systems of reduced dimensionality, e.g. periodic in one or two dimension but isolated in the other directions. This is accomplished by:

  • Isolating the system in the non-periodic dimension as seen in Electronic properties of isolated molecules, so inserting an amount of vacuum in the supercell.
  • Sampling the Brillouin zone that now has reduced dimension:

In Quantum ESPRESSO one needs to set the following:

  K_POINTS automatic
  nk nk 1   0 0 0     

this will generate a 2D sampling. In brief: you will need large supercells because of the present of vacuum which reflects in a large number of plane waves and a converged sampling of the BZ. The combination of this two issues makes the calculations of 2D system rather cumbersome.

Exercises:

Exercise 1: Grapehene

  • build a supercell for an ideal graphene structure
  • relax the supercell
  • calculate the graphene band structure
  • calculate the density of states projected on π and σ states

Hints

Exercise 2: Hexagonal Boron Nitrite (hBN)

Exercise 3: A small CNT