Bethe-Salpeter: Difference between revisions
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* understand the content of the outputs | * understand the content of the outputs | ||
[[File:HBN-2D.png|thumb|Atomic structure of two-dimensional hBN]] | [[File:HBN-2D.png|thumb|Atomic structure of two-dimensional hBN]] | ||
'''Material properties''': | '''Material properties''': | ||
* exagonal lattice | * exagonal lattice | ||
* 2 atoms per cell, B and N ( | * 2 atoms per cell, B and N (8 electrons, ) | ||
* Lattice constants: ''a'' = 4.716 [a.u.] | * Lattice constants: ''a'' = 4.716 [a.u.] | ||
* Plane wave cutoff 40 Ry | * Plane wave cutoff 40 Ry | ||
'''You will need''': | '''You will need''': | ||
* PWSCF input files and pseudopotentials for hBN-2D | * PWSCF input files and pseudopotentials for hBN-2D | ||
* <code>pw.x</code> executable, version 5.0 or later | * <code>pw.x</code> executable, version 5.0 or later | ||
* <code>p2y</code> executable | * <code>p2y</code> executable |
Revision as of 10:43, 15 March 2017
UNDER CONSTRUCTION (MP)
In this tutorial you will learn how to:
- generate input files to run a BSE calculation for a two-dimensional material
- run the code and control inputs and outputs
- understand the content of the outputs
Material properties:
- exagonal lattice
- 2 atoms per cell, B and N (8 electrons, )
- Lattice constants: a = 4.716 [a.u.]
- Plane wave cutoff 40 Ry
You will need:
- PWSCF input files and pseudopotentials for hBN-2D
pw.x
executable, version 5.0 or laterp2y
executable
Unpack the TARFILE:
$ tar -xcvf hBN-2D.tar $ cd hBN-2D/PWSCF $ ls hbn-2D_bands.in hbn-2D_nscf.in hbn-2D_scf.in hbn-2D_scf_b.in REFERENCES
Prerequisites
- Complete the Generating the Yambo databases tutorial for 2D-hBN
SAVE
folder for hBN-2D.yambo
executable
Initialization
Every Yambo run must start with this step. Go to the folder containing the hBN-2D SAVE
directory:
$ cd TUTORIALS/hBN-2D/YAMBO $ ls SAVE
and simply launch the code
yambo
This will run the initialization (setup) runlevel.
TIP: do not run yambo from inside the SAVE
folder! It will complain that "databases not found".
BSE Tutorials at present:
- SiH_4
- Fantastic dimension
- LiF
- you Hydrogen
- GaSb (SOC)
- hexagonal BN (on slides only)
The material
The h-BN is a layered material similar to graphite. It is an indirect wide band-gap material. Its optical spectrum is characterized by large excitonic effects. 5.95 eV is the minimum electronic indirect gap. 6.47 eV is the minimum direct gap. See the literature [1]
Bulk hexagonal BN
|
[[File:|Band Structure]] |
Calculate the screening
A key ingredient to construct the BS kernel in the Screeened EXchange approximation (sex) is the screened electron-electron dielectric matrix W which is normally evaluated in the static approximation.
You have two main options to generate the input :
1) yambo -b -F yambo_Ws.in
This will create the input to calculate W (database ndb.em1s)
2) yambo -p p -F yambo_Wp.in
This will create the input to calculate (or read) W in the PPA approximation (database ndb.pp) This second option is useful if you want to read the static part of W from a previous database ndb.pp generated in a GW-PPA run
Calculate the BS kernel in the SEX (Screened Exchange approximation) in the transitions space
Here we learn how to create the BS kernel in the screened exchange (SEX) approximation which includes both exchange (V) and correlation (-W) terms Runlevel to be used yambo -o b -k sex
Solve the BSE by haydock solver and and calculate spectrum
Generate the input file for solving the BSE using the Haydock solver:
yambo -o-y h
Solve the BSE by diagonalizing the excitonic matrix and calculate spectrum
Runlevel to be used yambo -y d
Steps:
-Calculate screening
-Calculate the BS Kernel
-Diagonalize the BS Matrix and calculate spectrum
-Visualize/Analyze excitons (with ypp)
-How to Converge
-How to work with SOC