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exercises:2016_uzh_cmest:defects_in_graphene [2016/11/13 17:13] – created tmuellerexercises:2016_uzh_cmest:defects_in_graphene [2020/08/21 10:15] (current) – external edit 127.0.0.1
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 ======= Analyzing defects in graphene ======= ======= Analyzing defects in graphene =======
 +
 +In this exercise we follow-up on what was started previously with [[defects_in_silicon|defects in silicon]], but this time you will have to figure out the setup as well.
 +
 +<note tip>When comparing scaled coordinates between papers and code input scripts, always make sure that they use the same coordinate systems and definitions for a unit cell (both real and reciprocal space). For example while many sources (like the [[http://www.sciencedirect.com/science/article/pii/S0927025610002697|paper of Curtarolo, Setyawan]]) assume a 120° degree angle between $a$ and $b$ for a hexagonal cell, you can also define it to be a 60° angle (like the default in CP2K).</note>
 +
 +
 +<note important>Once you have verified that your calculation setup works, use ''nohup mpirun -np 8 cp2k.popt ... &'' to run the calculations in parallel and in the background since they may take longer to complete than before.</note>
 +
 +====== Vacancy in graphene ======
 +
 +===== Comparing energies =====
 +
 +Use the template and initial geometry provided when [[calculating_pdos|calculating the projected density of states for graphene]] to setup a single point energy calculation for a 6x6x1 supercell of graphene.
 +
 +Create a vacancy by removing one carbon atom from this supercell and perform the energy calculation again.
 +
 +Quick question: Does it matter which carbon atom you remove? (hint: what kind of boundary conditions do we impose?)
 +
 +Calculate the energy of the vacancy formation, that is $E_v = E_2 - \frac{N-1}{N} \cdot E_1$ where $E_1$ is the energy of the complete system, $E_2$ that of the system with a vacancy and $N$ the number of atoms.
 +
 +===== Analyze the PDOS =====
 +
 +Would you expect the vacancy to haven any influence on the projected density of states? Check whether your assumption was right by visualizing the PDOS.
 +
 +===== Replacement with oxygen =====
 +
 +Now, instead of removing one carbon atom from the 6x6x1 supercell, simply replace it with an oxygen atom. Perform first a single point calculation and second a geometry optimization and compare the energy of adsorption for both cases.
 +
 +====== Oxygen atom adsorbed on graphene ======
 +
 +Now we are going to investigate the effect an adsorbent has on graphene.
 +
 +===== Change in energy =====
 +
 +
 +In order to adsorb an oxygen atom on top of a graphene layer, modify the coordinate section by adding one oxygen atom which has them same coordinates as a carbon (except the z-component of course). Check whether the addition of an oxygen atom has an effect on the structure of graphene by optimizing its geometry and calculate the adsorption energy.
 +
 +Use $E_\text{ad} = E_3 – (E_1 + \frac{1}{2}E_2)$, with:
 +
 +  ; $E_\text{ad}$ : energy of adsorption
 +  ; $E_1$ : energy of graphene
 +  ; $E_2$ : energy of molecular oxygen (-31.929714235694995 a.u.)
 +  ; $E_3$ : energy of oxygen adsorbed on graphene
 +
 +
 +<note tip>The formation of oxygen is more difficult to obtain, here we use $\frac{1}{2}$ of the total energy of molecular oxygen. This approximation introduces a large uncertainty to our calculations because the calculation of dioxygen is difficult using KS-DFT.
 +
 +Try to explain based on the lecture what might be the problem.</note>
 +===== Displacements =====
 +
 +We are furthermore interested in the change of structure this adsorbent causes. Try to visualize which atoms have to assume a new position in order to minimize the total energy. That is: plot $\sqrt{(x^i-x^i_0)^2 + (y^i-y^i_0)^2 + (z^i-z^i_0)^2}$ in a sensible manner (one which also retains the geometry of graphene).
 +
 +
 +======= Analyzing defects in hexagonal Boron-Nitride =======
 +
 +Repeat the calculations of the vacancy formation, defect formation and adsorption for the h-BN-layer structure, taking into account that now both the N and the B can be replaced.
 +
 +Compare the energies for the two cases, where is a vacancy more likely to be and on top of which atom does an oxygen atom preferably adsorb.
 +
 +<note tip>Use the total energy of a B or N atom when calculating the vacancy formation energy.</note>
 +
 +Since N and B are radicals, you have to include the following keywords/options in the right places (use the CP2K manual):
 +
 +  * ''UKS = .TRUE.''
 +  * ''MULITPLCITY = ...''
  
exercises/2016_uzh_cmest/defects_in_graphene.1479057188.txt.gz · Last modified: 2020/08/21 10:15 (external edit)