Band-structure calculation using density-functional theory: Difference between revisions

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[[:Category:Band structure |Calculating the band structure]] for [[GGA|density-functional theory]] (DFT) requires multiple steps. On this page, you will find step-by-step instructions, as well as references to some practical examples to explore. Additionally, we provide some advice to reduce computational and human effort.
The step-by-step instructions below cover calculating the [[:Category:Band structure|band structure]] within density-functional theory (DFT), including references to practical examples.
 
Obtaining the band structure involves first solving the Hamiltonian to get eigenvalues and eigenvectors, then plotting them as electronic energy levels versus [[crystal momentum]]. The Kohn-Sham (KS) Hamiltonian requires at least the density (charge and possibly magnetization) and may contain higher derivatives depending on the [[:Category:Exchange-correlation functionals|exchange-correlation (XC) functional]].  
{{NB|mind| The approach presented on this page applies to [[GGA#Available functionals|LDA]] (needs density), [[GGA|GGA]] (needs density and gradient), and deorbitalized meta-GGA (needs density, gradient, and Laplacian) functionals. Additionally, it can be used for [[METAGGA|meta-GGAs]] that need the kinetic energy density as of VASP 6.6.0. In contrast, another approach is required [[Band-structure calculation using hybrid functionals|for computing the band structure for hybrid functionals]] and [[Band-structure calculation using hybrid functionals|for computing the band structure for MGGAs before VASP 6.6.0]].}}


== Step-by-step instructions ==
== Step-by-step instructions ==


For [[GGA|density-functional theory]] (DFT), the Hamiltonian can be expressed in terms of the electronic charge density. Therefore, the electronic charge density written to the {{FILE|CHGCAR}} file from a previous self-consistent-field (SCF) run suffices to restart a DFT calculation. Generally, computing the band-structure consists of the following steps:
{{NB|tip|[[#Option A: Single run|Option A: Single run]] is convenient, because it does not require restarting the calculation. On the other hand, there is less control, e.g., over the used algorithm ({{TAG|ALGO}}), and depending on the number of '''k''' points on the regular mesh and the [[parallelization]], it can be less performant than [[#Option B: Split run|Option B: Split run]].}}
 
=== Option A: Single run ===
{{Available|6.3.0}}
 
==== Step 1: Prepare SCF settings ====
 
:Follow [[Setting_up_an_electronic_minimization#Create_the_input_files|the steps to create input files]] on the instructions for [[setting up an electronic minimization]]. Typically, this involves defining the input settings using the {{FILE|INCAR}}, {{FILE|POSCAR}}, {{FILE|KPOINTS}}, and {{FILE|POTCAR}} files.
 
==== Step 2: High-symmetry path ====


=== 1. Perform a self-consistent field calculation ===
:[[#Choosing a high-symmetry path|Choose a high-symmetry path]] and set it in the {{FILE|KPOINTS_OPT}} file. Both {{FILE|KPOINTS}} and {{FILE|KPOINTS_OPT}} define crystal momenta: The {{FILE|KPOINTS}} file holds the regular '''k''' mesh for the initial SCF computation, while the {{FILE|KPOINTS_OPT}} file holds the high-symmetry path usually in line mode along which the band structure will be evaluated.


In order to obtain a converged {{FILE|CHGCAR}}, perform a static ({{TAG|NSW}}=0, {{TAG|IBRION}}=-1) self-consistent-field (SCF) calculation for DFT. To achieve this, you will need:
==== Step 3: Run the calculation ====


* {{FILE|POSCAR}} containing structure information,
:Start the VASP run, which will internally perform an SCF run to obtain the converged KS orbitals and densities, and then perform the NSCF run at fixed density to evaluate the eigenvalues along the high-symmetry path. The progress is written to '''stdout'''. For more detailed suggestions on [[Setting_up_an_electronic_minimization#Optimize_your_settings|optimizing your settings]] and [[Setting_up_an_electronic_minimization#Run_the_calculation|running the calculation]] check the article on [[setting up an electronic minimization]].


* {{FILE|INCAR}} containing any required tags ({{TAG|NSW}}=0, {{TAG|IBRION}}=-1, plus other tags as needed),
==== Step 4: Plot the band structure ====


* {{FILE|KPOINTS}} containing a regular '''k''' mesh, using e.g. [[KPOINTS#Regular_k-point_mesh|Γ-centered mesh or Monkhorst-Pack mesh]],
:{{py4vasp|url=calculation/band/#py4vasp.calculation._band.Band.to_graph}} provides utilities for plotting the band structure. Run the following in a Python notebook in the directory of the calculation:
<syntaxhighlight lang="python">
import py4vasp
calc = py4vasp.Calculation.from_path(".")
ef = calc.dos.read()["fermi_energy"]
calc.band.plot("kpoints_opt", fermi_energy=ef)
</syntaxhighlight>
{{NB|tip|Set the {{TAG|EFERMI}} tag or pass the Fermi energy explicitly, because {{py4vasp}} reads the Fermi energy from the {{FILE|KPOINTS_OPT}} density of states (<code>results/electron_dos_kpoints_opt/efermi</code>), which is computed from the line-mode '''k''' points and is therefore unreliable.|:}}


* {{FILE|POTCAR}} containing the desired potentials ([[GGA|GGA]]).
=== Option B: Split run ===


Make sure you copy the converged {{FILE|CHGCAR}} alongside the other files if you want to run the band structure calculation in a separate folder.
In a nutshell, the KS Hamiltonian within DFT can be expressed in terms of the electronic charge and possibly the magnetization density. Both are written to the {{FILE|CHGCAR}} file during an initial self-consistent-field (SCF) run. From this converged {{FILE|CHGCAR}} file, we can obtain the eigenvalues at the desired [[#Choosing a high-symmetry path|high-symmetry path]] via a subsequent non-self-consistent-field (NSCF) run at fixed density.


=== 2. Determine the high-symmetry path ===
==== Step 1: Set up and perform a full SCF calculation ====


[[:Category:Band structure |Band-structure calculations]] generally compute the Kohn-Sham orbitals and eigenenergies along a path in reciprocal space which usually connects high-symmetry points in the first Brillouin zone. Some external tools{{cite|bilbao:kvec}}{{cite|seekpath}} help to identify the high-symmetry points and '''k''' points along a high-symmetry path for materials of any symmetry.  
:Follow the steps described in [[setting up an electronic minimization]].
{{NB|important|Set {{TAG|LMAXMIX|4}} for d-electron systems and {{TAG|LMAXMIX|6}} for f-electron systems to adjust the maximum l-quantum number up to which the one-center PAW charge densities are written to the {{FILE|CHGCAR}} file. If you are unsure about the appropriate value for {{TAG|LMAXMIX}}, restart with fixed density using the regular '''k''' mesh and check that the total energy is identical to the SCF run.|:}}


In any event, we need to determine the high-symmetry path along which VASP should compute the band structure. Once that path is known, we proceed to set it in  step '''3'''.
==== Step 2 (optionally): Create a backup ====


=== 3. Supply a regular '''k''' mesh and '''k''' points along the high-symmetry path ===
:The simplest procedure is to create a new directory for the band-structure calculation and copy the input files of the SCF calculation (usually the {{FILE|INCAR}} file, {{FILE|POSCAR}} file, and the {{FILE|POTCAR}} file) as well as the {{FILE|CHGCAR}} file to the new directory.


There are two options to simultaneously supply a regular '''k''' mesh ''and'' '''k''' points along a high-symmetry path to VASP.
{{CB|mkdir -f bands
:;1. Provide an [[KPOINTS#Explicit_k-point_mesh|explicit list of '''k''' points]] with zero-weighted '''k''' points.
cp INCAR POSCAR POTCAR CHGCAR bands/.|:}}
::Here, the explicit list of the irreducible '''k''' points of the regular '''k''' mesh can be copied from the {{FILE|IBZKPT}} file of a previous run to the {{FILE|KPOINTS}} file. For instance, use the {{FILE|IBZKPT}} file of '''Step 1'''. These irreducible '''k''' points must be weighted by their multiplicity according to the system's symmetry. Additionally, the '''k''' points along a high-symmetry path must be added to the {{FILE|KPOINTS}} file with the value of all weights set to zero.


:;2. Provide an additional {{FILE|KPOINTS_OPT}} file that can specify the [[KPOINTS#Band-structure_calculations|high-symmetry path in line mode]].
:Alternatively, backup the {{FILE|OUTCAR}} file, {{FILE|KPOINTS}} file and possibly the {{FILE|OSZICAR}} file and {{FILE|vaspout.h5}} to be able to reconstruct the SCF calculation, if needed.
::Generally, the {{FILE|KPOINTS}} file and the {{FILE|KPOINTS_OPT}} file accept the same format. But again, the regular '''k''' mesh needs to be supplied in the {{FILE|KPOINTS}} file and the high-symmetry path in the {{FILE|KPOINTS_OPT}} file. We therefore recommend using the [[KPOINTS#Regular_k-point_mesh|Γ-centered mesh or Monkhorst-Pack mesh]], and [[KPOINTS#Band-structure_calculations|line mode]], respectively.


The {{FILE|KPOINTS_OPT}} method is more convenient because it allows using the automatic generation modes for the '''k''' points. The computational cost and memory requirement can vary for the two methods due to the scaling behaviour with the number of '''k''' points.
==== Step 3: High-symmetry path ====


=== 4. Edit {{FILE|INCAR}} ===
:[[#Choosing a high-symmetry path|Choose a high-symmetry path]] and set it in the {{FILE|KPOINTS}} file.


Setting {{TAG|ICHARG}} = 11 in the {{FILE|INCAR}} file allows the DFT calculation to pick up from the {{FILE|CHGCAR}} at the same densities. Notice that the computed Fermi energy for this case will no longer be correct once a '''k'''-path has been declared and the '''k''' mesh is no longer regular.
==== Step 4: Prepare a restart with fixed density ====


=== 5. Restart the calculation ===
:Adjust the {{FILE|INCAR}} file:
::* Remove any of the following tags, if present: {{TAG|NSW}}, {{TAG|IBRION}} and {{TAG|ISTART}}.
::* Add {{TAG|ICHARG|11}}. This restarts from the converged charge density read from the {{FILE|CHGCAR}} file and continues with the density held fixed.
::* Add additional relevant tags as needed, i.e., {{TAG|LORBIT}}=11.
{{NB|tip|Set the {{TAG|EFERMI}} tag to the Fermi energy obtained during the SCF calculation. Infact, the Fermi energy cannot be computed based on '''k''' points along a path, and the Fermi energy given by the NSCF calculation will therefore be unreliable. The Fermi energy of the SCF calculation is written to the {{FILE|OUTCAR}} file or can be extracted using {{py4vasp}}:


Lastly, we restart the DFT calculation from the {{FILE|CHGCAR}} file using the new setup defined in steps '''2-4'''.
<syntaxhighlight lang="python">from py4vasp import Calculation
Calculation.from_path("dir/with/SCF/vaspout.h5").dos.read()["fermi_energy"]
</syntaxhighlight>
|:}}


=== 6. Visualization using py4vasp (optional) ===
==== Step 5: Run the NSCF calculation ====


Plot the band structure, e.g., using {{py4vasp|url=calculation/band/#py4vasp.calculation._band.Band.to_graph}}. In a python notebook in the directory of the calculation, you can run the following code:
:Perform the NSCF calculation with the prepared files. This will read the {{FILE|CHGCAR}} file and keep the density fixed.
{{NB|mind| Any existing {{FILE|KPOINTS_OPT}} file triggers '''[[#Option A: Single run|Option A]]''' unless you disable this by setting {{TAG|LKPOINTS_OPT|F}}.|:}}


==== Step 6: Plot the band structure ====
:{{py4vasp|url=calculation/band/#py4vasp.calculation._band.Band.to_graph}} provides utilities for plotting the band structure. Run the following in a Python notebook in the directory of the calculation:
<syntaxhighlight lang="python">
<syntaxhighlight lang="python">
import py4vasp as pv
import py4vasp
calc = pv.Calculation.from_path(".")
calc = py4vasp.Calculation.from_path(".")
calc.band.plot()
calc.band.plot()
# calc.band.plot("kpoints_opt") # if the high-symmetry path is in KPOINTS_OPT
</syntaxhighlight>
</syntaxhighlight>
{{NB|tip|If you did not set {{TAG|EFERMI}} in Step 4, pass the Fermi energy from the SCF run at the plotting stage:
<syntaxhighlight lang="python">calc.band.plot(fermi_energy=...)  # plug in the Fermi energy from the SCF run</syntaxhighlight>|:}}
== Choosing a high-symmetry path ==
Band-structure calculations generally compute the '''Kohn-Sham orbitals''' and eigenenergies along a path in reciprocal space which usually connects high-symmetry points in the first '''Brillouin zone'''. Which '''k''' points are high-symmetry points depends on the '''space group''' of the structure.
Use external tools{{cite|seekpath}}{{cite|bilbao:kvec}} to find the space group, plot the Brillouin zone, and pick a high-symmetry '''k''' path. Extract the corresponding coordinates and provide them in {{FILE|KPOINTS}}-file format, either as a list of [[KPOINTS#Explicit_k-point_mesh|explicit coordinates]] or (more commonly) using [[KPOINTS#Band-structure_calculations|line mode]].
{{NB|tip|The tools provide the coordinates and the labels for a given structure. Because these paths depend on the symmetry, take special care that the analysis is not tainted by finite precision or rounding (see {{TAG|SYMPREC}}). Also, keep in mind that the primitive and the conventional unit cell have different reciprocal coordinate systems.}}
Example high-symmetry path for face-centered-cubic silicon:
  k points for band structure
  10  ! intersections
  line
  Fractional
    0.50000  0.50000  0.50000  L
    0.00000  0.00000  0.00000  Γ
   
    0.00000  0.00000  0.00000  Γ
    0.00000  0.50000  0.50000  X
   
    0.00000  0.50000  0.50000  X
    0.25000  0.62500  0.62500  U
   
    0.37500  0.7500  0.37500  K
    0.00000  0.00000  0.00000  Γ
The empty lines and labels are optional and meant for readability. The labels will be used by {{py4vasp}}. VASP produces equidistant '''k''' points for each segment. The example above would yield 10 points from ''L'' to ''Γ'', 10 points from ''Γ'' to ''X'', 10 from ''X'' to ''U'', and 10 from ''K'' to ''Γ'', including endpoints.
For further details and instructions, please consult the section on [[KPOINTS#Band-structure_calculations|band-structure calculations in the KPOINTS]] documentation.


== Recommendations and advice ==
== Recommendations and advice ==


In case a {{FILE|KPOINTS_OPT}} file is present, VASP computes the band energies for the '''k''' points of the {{FILE|KPOINTS_OPT}} file after SCF is reached within the same submitted job. Their convergence is checked independently by requiring the sum over occupied band energies not to change in two successive iterations. Hence, for the computational time, there is no advantage to restart from a converged hybrid calculation, but in principle it is possible.
In case a {{FILE|KPOINTS_OPT}} file is present ([[#Option A: Single run |Option A]]), VASP computes the band energies for the '''k''' points of the {{FILE|KPOINTS_OPT}} file after SCF convergence is reached within the same submitted job. There may, however, be a '''computational advantage''' to splitting the run  ([[#Option B: Split run |Option B]]) because of different optimal batching options for the '''k''' mesh.


In contrast, the method using an explicit list including zero-weighted '''k''' points computes the band energies for all '''k''' points at each SCF step. The convergence criterion considers the total energy and, thus, does not account for convergence of KS orbitals at zero-weighted '''k''' points. Taking the KS orbitals of the zero-weighted '''k''' points along the entire SCF run makes their convergence highly likely. However, restarting from a converged hybrid calculation can result in premature stopping. This can be counteracted by setting the {{TAG|NELMIN}} tag to a higher value. Especially if the hybrid calculation needs many SCF steps to reach convergence and each SCF step is very expensive when including zero-weighted '''k''' points, one may consider to restart from a converged hybrid calculation with {{TAG|NELMIN}} set to a large number. We recommend carefully checking the convergence of the band structure in this case.
There are additional advantages to using the {{FILE|KPOINTS_OPT}} file for computing the band structure [[Band-structure calculation using hybrid functionals|using hybrid functionals]] or [[Band-structure calculation using meta-GGA functionals|using meta-GGA functionals]]. Refer to these references for details.
{{NB|tip|For a band-structure calculation with an explicit list including zero-weighted '''k''' points, avoid restarting from a converged hybrid {{FILE|WAVECAR}} file.}}


It is possible to achieve very fine sampling along the '''k''' path with both methods, but there are some aspects to take into account. As mentioned, the computational cost and memory requirement can vary for the two methods due to the scaling with the number of '''k''' points. For the {{FILE|KPOINTS_OPT}} method, the number of '''k''' points treated simultaneously can be controlled by means of the {{TAG|KPOINTS_OPT_NKBATCH}} tag. For the explicit list including zero-weighted '''k''' points, VASP may exceed the available memory if the number of zero-weighted '''k''' points is large. In that case, split the hybrid band-structure calculation into multiple calculations. For each calculation, add part of the zero-weighted '''k''' points.
A number of '''post-processing options''' for the Kohn-Sham (KS) orbitals can affect the computation of the band structure. Usually, these options are set directly in the {{FILE|INCAR}} file: See, for example, {{TAG|LORBIT}}=11 or [[constructing Wannier orbitals]].
{{NB|tip|Make fine sampling computationally feasible using the {{TAG|KPOINTS_OPT_NKBATCH}} tag or splitting the calculation with part of the zero-weighted '''k''' points.}}


Let us stress a significant difference between hybrid band-structure calculations and DFT band-structure calculations. The electronic charge density suffices for density functionals to define the Hamiltonian, and no regular '''k''' mesh is required during DFT band-structure calculations. However, if no regular '''k''' mesh is provided, the electronic charge density must be fixed during the DFT band-structure calculation by setting {{TAG|ICHARG}}=11 in the {{FILE|INCAR}} file.
== Practical examples ==
{{NB|warning| The electronic charge density must not be fixed for any hybrid calculation, i.e., never set {{TAG|ICHARG}}{{=}}11!}}
{{NB|tip|To understand how the two methods work in practice, try using them with a DFT calculation as if it were a hybrid calculation.}}
If you forgot setting {{TAG|HFRCUT}} you may be able to mitigate the band structure. Semi-core states can be assumed to be dispersionless but you will see the same discontinuities featured on the semi core states. By subtracting the faulty dispersion of the semi-core state from all bands, you can recover the true dispersion of the conduction bands.


== Practical examples ==
We offer additional tutorials for calculating and visualizing DFT band structures:


We offer additional tutorials for calculating and visualizing the DFT band-structure of bulk systems:
* [https://www.vasp.at/tutorials/latest/bulk/part1/#bulk-e03 Bulk systems, Part 1]: band structure of face-centered-cubic silicon.


* [[fcc Si bandstructure |fcc Si]]: band structure of face-centered Si, and
* [https://www.vasp.at/tutorials/latest/bulk/part2/#Step-3.) Bulk systems, Part 2]: band structure of cubic-diamond silicon.


* [[cd Si |cd Si]]: band structure of cubic-diamond Si.
* [https://www.vasp.at/tutorials/latest/bulk/part3/#Step-3.) Bulk systems, Part 3]: band structure of face-centered-cubic nickel.


== Related tags and articles ==
== Related tags and articles ==


{{FILE| KPOINTS}}, {{FILE| KPOINTS_OPT}}, [[Band-structure calculation using hybrid functionals]], [[Band-structure calculation using meta-GGA functionals]]
{{FILE|KPOINTS}}, {{FILE|KPOINTS_OPT}},
 
{{TAG|ICHARG}}, {{TAG|LMAXMIX}}
 
[[XC functionals]], [[Setting up an electronic minimization]]
 
[[Band-structure calculation using meta-GGA functionals]], [[Band-structure calculation using hybrid functionals]]


== References ==
== References ==


<!--[[Category:Band structure |Band structure]][[Category:Howto|Howto]]-->
<references/>
 
[[Category:Band structure]]
[[Category:Howto]]
[[Category:Crystal momentum]]

Latest revision as of 16:08, 20 March 2026

The step-by-step instructions below cover calculating the band structure within density-functional theory (DFT), including references to practical examples.

Obtaining the band structure involves first solving the Hamiltonian to get eigenvalues and eigenvectors, then plotting them as electronic energy levels versus crystal momentum. The Kohn-Sham (KS) Hamiltonian requires at least the density (charge and possibly magnetization) and may contain higher derivatives depending on the exchange-correlation (XC) functional.

Mind: The approach presented on this page applies to LDA (needs density), GGA (needs density and gradient), and deorbitalized meta-GGA (needs density, gradient, and Laplacian) functionals. Additionally, it can be used for meta-GGAs that need the kinetic energy density as of VASP 6.6.0. In contrast, another approach is required for computing the band structure for hybrid functionals and for computing the band structure for MGGAs before VASP 6.6.0.

Step-by-step instructions

Tip: Option A: Single run is convenient, because it does not require restarting the calculation. On the other hand, there is less control, e.g., over the used algorithm (ALGO), and depending on the number of k points on the regular mesh and the parallelization, it can be less performant than Option B: Split run.

Option A: Single run

Mind: Available as of VASP 6.3.0

Step 1: Prepare SCF settings

Follow the steps to create input files on the instructions for setting up an electronic minimization. Typically, this involves defining the input settings using the INCAR, POSCAR, KPOINTS, and POTCAR files.

Step 2: High-symmetry path

Choose a high-symmetry path and set it in the KPOINTS_OPT file. Both KPOINTS and KPOINTS_OPT define crystal momenta: The KPOINTS file holds the regular k mesh for the initial SCF computation, while the KPOINTS_OPT file holds the high-symmetry path usually in line mode along which the band structure will be evaluated.

Step 3: Run the calculation

Start the VASP run, which will internally perform an SCF run to obtain the converged KS orbitals and densities, and then perform the NSCF run at fixed density to evaluate the eigenvalues along the high-symmetry path. The progress is written to stdout. For more detailed suggestions on optimizing your settings and running the calculation check the article on setting up an electronic minimization.

Step 4: Plot the band structure

py4vasp provides utilities for plotting the band structure. Run the following in a Python notebook in the directory of the calculation:
import py4vasp
calc = py4vasp.Calculation.from_path(".")
ef = calc.dos.read()["fermi_energy"]
calc.band.plot("kpoints_opt", fermi_energy=ef)
Tip: Set the EFERMI tag or pass the Fermi energy explicitly, because py4vasp reads the Fermi energy from the KPOINTS_OPT density of states (results/electron_dos_kpoints_opt/efermi), which is computed from the line-mode k points and is therefore unreliable.

Option B: Split run

In a nutshell, the KS Hamiltonian within DFT can be expressed in terms of the electronic charge and possibly the magnetization density. Both are written to the CHGCAR file during an initial self-consistent-field (SCF) run. From this converged CHGCAR file, we can obtain the eigenvalues at the desired high-symmetry path via a subsequent non-self-consistent-field (NSCF) run at fixed density.

Step 1: Set up and perform a full SCF calculation

Follow the steps described in setting up an electronic minimization.
Important: Set LMAXMIX = 4 for d-electron systems and LMAXMIX = 6 for f-electron systems to adjust the maximum l-quantum number up to which the one-center PAW charge densities are written to the CHGCAR file. If you are unsure about the appropriate value for LMAXMIX, restart with fixed density using the regular k mesh and check that the total energy is identical to the SCF run.

Step 2 (optionally): Create a backup

The simplest procedure is to create a new directory for the band-structure calculation and copy the input files of the SCF calculation (usually the INCAR file, POSCAR file, and the POTCAR file) as well as the CHGCAR file to the new directory.
mkdir -f bands
cp INCAR POSCAR POTCAR CHGCAR bands/.
Alternatively, backup the OUTCAR file, KPOINTS file and possibly the OSZICAR file and vaspout.h5 to be able to reconstruct the SCF calculation, if needed.

Step 3: High-symmetry path

Choose a high-symmetry path and set it in the KPOINTS file.

Step 4: Prepare a restart with fixed density

Adjust the INCAR file:
  • Remove any of the following tags, if present: NSW, IBRION and ISTART.
  • Add ICHARG = 11. This restarts from the converged charge density read from the CHGCAR file and continues with the density held fixed.
  • Add additional relevant tags as needed, i.e., LORBIT=11.
Tip: Set the EFERMI tag to the Fermi energy obtained during the SCF calculation. Infact, the Fermi energy cannot be computed based on k points along a path, and the Fermi energy given by the NSCF calculation will therefore be unreliable. The Fermi energy of the SCF calculation is written to the OUTCAR file or can be extracted using py4vasp:
from py4vasp import Calculation
Calculation.from_path("dir/with/SCF/vaspout.h5").dos.read()["fermi_energy"]

Step 5: Run the NSCF calculation

Perform the NSCF calculation with the prepared files. This will read the CHGCAR file and keep the density fixed.
Mind: Any existing KPOINTS_OPT file triggers Option A unless you disable this by setting LKPOINTS_OPT = F.

Step 6: Plot the band structure

py4vasp provides utilities for plotting the band structure. Run the following in a Python notebook in the directory of the calculation:
import py4vasp
calc = py4vasp.Calculation.from_path(".")
calc.band.plot()
Tip: If you did not set EFERMI in Step 4, pass the Fermi energy from the SCF run at the plotting stage:
calc.band.plot(fermi_energy=...)  # plug in the Fermi energy from the SCF run

Choosing a high-symmetry path

Band-structure calculations generally compute the Kohn-Sham orbitals and eigenenergies along a path in reciprocal space which usually connects high-symmetry points in the first Brillouin zone. Which k points are high-symmetry points depends on the space group of the structure.

Use external tools[1][2] to find the space group, plot the Brillouin zone, and pick a high-symmetry k path. Extract the corresponding coordinates and provide them in KPOINTS-file format, either as a list of explicit coordinates or (more commonly) using line mode.

Tip: The tools provide the coordinates and the labels for a given structure. Because these paths depend on the symmetry, take special care that the analysis is not tainted by finite precision or rounding (see SYMPREC). Also, keep in mind that the primitive and the conventional unit cell have different reciprocal coordinate systems.

Example high-symmetry path for face-centered-cubic silicon:

 k points for band structure
 10  ! intersections 
 line
 Fractional
   0.50000  0.50000  0.50000   L
   0.00000  0.00000  0.00000   Γ
   
   0.00000  0.00000  0.00000   Γ
   0.00000  0.50000  0.50000   X
   
   0.00000  0.50000  0.50000   X
   0.25000  0.62500  0.62500   U
   
   0.37500  0.7500   0.37500   K
   0.00000  0.00000  0.00000   Γ

The empty lines and labels are optional and meant for readability. The labels will be used by py4vasp. VASP produces equidistant k points for each segment. The example above would yield 10 points from L to Γ, 10 points from Γ to X, 10 from X to U, and 10 from K to Γ, including endpoints. For further details and instructions, please consult the section on band-structure calculations in the KPOINTS documentation.

Recommendations and advice

In case a KPOINTS_OPT file is present (Option A), VASP computes the band energies for the k points of the KPOINTS_OPT file after SCF convergence is reached within the same submitted job. There may, however, be a computational advantage to splitting the run (Option B) because of different optimal batching options for the k mesh.

There are additional advantages to using the KPOINTS_OPT file for computing the band structure using hybrid functionals or using meta-GGA functionals. Refer to these references for details.

A number of post-processing options for the Kohn-Sham (KS) orbitals can affect the computation of the band structure. Usually, these options are set directly in the INCAR file: See, for example, LORBIT=11 or constructing Wannier orbitals.

Practical examples

We offer additional tutorials for calculating and visualizing DFT band structures:

Related tags and articles

KPOINTS, KPOINTS_OPT,

ICHARG, LMAXMIX

XC functionals, Setting up an electronic minimization

Band-structure calculation using meta-GGA functionals, Band-structure calculation using hybrid functionals

References