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

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Calculating the [[:Category:Band structure |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.
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 requires solving the Hamiltonian to get eigenvalues and eigenvectors, which can then be plotted to obtain the band structure. In DFT, you need at least the density (charge and magnetization) and possibly higher derivatives depending on the [[:Category:Exchange-correlation functionals|XC]] functional.  
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]].}}
The unified 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. In contrast, [[METAGGA|meta-GGAs]] need the kinetic energy density and follow a [[Band-structure calculation using meta-GGA functionals|different approach]]. A different approach is also required when using [[Band-structure calculation using hybrid functionals|hybrid functionals]].


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


For DFT, the Hamiltonian can be expressed in terms of the electronic charge and magnetization density. Both are written to the {{FILE|CHGCAR}} file during an initial self-consistent-field (SCF) run. A converged {{FILE|CHGCAR}} file is a prerequisite for computing the band structure. With it, we can obtain the eigenvalues at the desired high-symmetry path from a subsequent NSCF (= fixed density) run.
{{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]].}}


If you want to compute a DFT ([[GGA#Available functionals|LDA]]/[[GGA|GGA]]/deorbitalized meta-GGA) band structure, please adhere to the following steps:
=== Option A: Single run ===
{{Available|6.3.0}}


=== 1. High-symmetry path ===
==== Step 1: Prepare SCF settings ====


[[: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. Which '''k''' points are high-symmetry points depends on the space group of your structure.
: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.


Some external tools{{cite|seekpath}}{{cite|bilbao:kvec}} can be employed to find the space group and plot the Brillouin zone to pick a '''k''' path. Extract the coordinates corresponding to the desired '''k''' path to a new {{FILE| KPOINTS_OPT}} file, which follows the format of a regular {{FILE| KPOINTS}} file.
==== Step 2: High-symmetry path ====


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. Also, keep in mind that the primitive and the conventional unit cell have different reciprocal coordinate systems.
:[[#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.


An example for what such a {{FILE| KPOINTS_OPT}} file might look like (example for face-centered-cubic silicon):
==== Step 3: Run the calculation ====
  k points for band structure
  10  ! intersections
  line
  Fractional
    0.50000  0.50000  0.50000  L
    0.00000  0.00000  0.00000  G
   
    0.00000  0.00000  0.00000  G
    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  G


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. In the example above, we would get 10 points from ''L'' to ''G'', 10 points from ''G'' to ''X'', 10 from ''X'' to ''U'', and 10 from ''K'' to ''G'', including endpoints.
: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]].
For further instructions on how to set up this file and what else to consider, please consult the [[KPOINTS#Band-structure_calculations| KPOINTS]] documentation.


=== 2. Calculation ===
==== Step 4: Plot the band structure ====


To compute the band structure, you have two options. '''Option A''' (single run) is only available as of VASP 6.3.0, while '''Option B''' (split run) is available for all VASP versions. Note that there is no difference between the two methods in terms of computational speed or accuracy.
:{{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.|:}}


==== Option A: Single run ====
=== Option B: Split run ===


As of VASP 6.3.0, you may write '''k''' points of high-symmetry paths to a {{FILE|KPOINTS_OPT}} file. This allows you to calculate the band structure in a single VASP run. Be aware that the SCF run is typically the expensive task and splitting the run might be beneficial (see '''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 {{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.


Following step '''1''', you should already have a {{FILE| KPOINTS_OPT}} file holding your chosen high-symmetry path. To proceed, you will also need:
==== Step 1: Set up and perform a full SCF calculation ====


* {{FILE|POSCAR}} containing structure information,
: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.|:}}


* {{FILE|INCAR}} containing any required tags ({{TAG|NSW}}=0 & {{TAG|IBRION}}=-1 or {{TAG| ISTART}}=0 & {{TAG| ICHARG}}=2, plus other tags as needed - i.e., {{TAG| EDIFF}}, {{TAG| LORBIT}}=11, etc.),
==== Step 2 (optionally): Create a backup ====


* {{FILE|KPOINTS}} containing a regular '''k''' mesh, using e.g. [[KPOINTS#Regular_k-point_mesh|Γ-centered mesh or Monkhorst-Pack mesh]],  
: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.


* {{FILE|POTCAR}} containing the required pseudopotentials.
{{CB|mkdir -f bands
cp INCAR POSCAR POTCAR CHGCAR bands/.|:}}


Note that {{FILE| KPOINTS}} and {{FILE| KPOINTS_OPT}} both co-exist in this method: {{FILE| KPOINTS}} holds the regular ''k''' mesh for the initial SCF computation, while {{FILE| KPOINTS_OPT}} holds the high-symmetry path along which the band structure will be computed at fixed density afterwards.
: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.


==== Option B: Split run ====
==== Step 3: High-symmetry path ====


Independent of VASP version, it is possible to split the band-structure calculation into two separate steps and VASP runs. In this approach, we first obtain a converged {{FILE| CHGCAR}} which holds density (charge & magnetization) information in a self-consistent (SCF) run, then fix the density and start another run by reading in the {{FILE| CHGCAR}} file (NSCF run).
:[[#Choosing a high-symmetry path|Choose a high-symmetry path]] and set it in the {{FILE|KPOINTS}} file.


===== Step B1: SCF Run =====
==== Step 4: Prepare a restart with fixed density ====


If you already have a converged {{FILE|CHGCAR}} file of a self-consistent-field (SCF) calculation, you can skip this step.
: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}}:


Otherwise, in order to obtain a converged {{FILE|CHGCAR}}, perform a static self-consistent-field (SCF) calculation for DFT. Following step '''1''', you should already have a {{FILE| KPOINTS_OPT}} file holding your chosen high-symmetry path. To proceed, you will also need:
<syntaxhighlight lang="python">from py4vasp import Calculation
Calculation.from_path("dir/with/SCF/vaspout.h5").dos.read()["fermi_energy"]
</syntaxhighlight>
|:}}


* {{FILE|POSCAR}} containing structure information,
==== Step 5: Run the NSCF calculation ====


* {{FILE|INCAR}} containing any required tags ({{TAG|NSW}}=0 & {{TAG|IBRION}}=-1 or {{TAG| ISTART}}=0 & {{TAG| ICHARG}}=2, {{TAG| LKPOINTS_OPT}}=<code>.FALSE.</code> plus other tags as needed, i.e., {{TAG| EDIFF}}),
: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}}.|:}}


* {{FILE|KPOINTS}} containing a regular '''k''' mesh, using e.g. [[KPOINTS#Regular_k-point_mesh|Γ-centered mesh or Monkhorst-Pack mesh]],
==== Step 6: Plot the band structure ====


* {{FILE|POTCAR}} containing the required pseudopotentials.
:{{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(".")
calc.band.plot()
</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>|:}}


Once everything has been set up, start VASP and wait for the calculation to converge.
== Choosing a high-symmetry path ==
{{NB|warning| As of VASP 6.3.0, when a {{FILE|KPOINTS_OPT}} file exists, it is automatically read in. If you want to split the run in two, you need to disable reading it by setting {{TAG| LKPOINTS_OPT}} to <code>.FALSE.</code> in the {{FILE|INCAR}} file.}}
{{NB|warning| For the initial SCF run to obtain the converged {{FILE|CHGCAR}} file, '''do not''' specify the {{TAG|ICHARG}} tag. You may find mentions of the {{TAG|ICHARG}} tag related to DFT band-structure calculations: This is specific to ''the next step''.}}


===== Step B2: NSCF Run =====
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.


Please follow the next steps exactly:
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.}}


* You may wish to copy your {{FILE|INCAR}}, {{FILE|POSCAR}}, {{FILE|POTCAR}}, {{FILE|KPOINTS}} and {{FILE|CHGCAR}} from step '''2B-1''' to a new folder before proceeding.
Example high-symmetry path for face-centered-cubic silicon:
   
  k points for band structure
* Override the contents of your {{FILE|KPOINTS}} file with your {{FILE| KPOINTS_OPT}} file.
  10  ! intersections
 
  line
* In your {{FILE|INCAR}} file:
  Fractional
** Remove any of the following tags, if present: {{TAG| NSW}}, {{TAG| IBRION}} & {{TAG| ISTART}}.
    0.50000  0.50000  0.50000  L
** Add the {{TAG|ICHARG}}=11 tag. Setting {{TAG|ICHARG}}=11 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.
    0.00000  0.00000 0.00000  Γ
** Add additional relevant tags as needed, i.e., {{TAG| LORBIT}}=11.
   
 
    0.00000  0.00000  0.00000  Γ
* Then, start another VASP run. This will restart the DFT calculation from the {{FILE|CHGCAR}} file. This run is non-self-consistent (NSCF), and the densities will remain fixed.
    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


=== 3. Visualization (optional) ===
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.
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 (or a different directory - see input to <code>py4vasp.Calculation.from_path</code>), you can run the following code:
 
<syntaxhighlight lang="python">
import py4vasp
calc = p4vasp.Calculation.from_path(".")
calc.band.plot()
</syntaxhighlight>
{{NB|mind| As of VASP 6.3.0, you may use {{FILE|KPOINTS_OPT}} for the high-symmetry path. In that case, you need to pass "kpoints_opt" as an argument to <code>calc.band.plot</code>: <syntaxhighlight lang="python">calc.band.plot("kpoints_opt")</syntaxhighlight>}}


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


In case a {{FILE|KPOINTS_OPT}} file is present (only for VASP 6.3.0+), VASP computes the band energies for the '''k''' points of the {{FILE|KPOINTS_OPT}} file after SCF is reached within the same submitted job. Therefore, there is no computational advantage to splitting the run into two steps (one for SCF, and one for computing the band structure at fixed density). However, reaching convergence for the SCF run and obtaining the converged {{FILE|CHGCAR}} file is typically more expensive, and storing these results might be beneficial for subsequent calculations.
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.


Note that 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]].
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.


A number of post-processing options for the Kohn-Sham (KS) orbitals exist. These directly affect the computation of the band structure. Usually, these options are set directly in the {{FILE|INCAR}} file: See, for example, {{TAG|LORBIT}}=11 and [[Constructing_Wannier_orbitals | Constructing Wannier orbitals]].
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]].


== Practical examples ==
== Practical examples ==
Line 127: Line 132:
== Related tags and articles ==
== Related tags and articles ==


{{FILE| KPOINTS}}, {{FILE| KPOINTS_OPT}}, {{FILE| KPOINTS_WAN}}, {{TAG|ICHARG}}, [[GGA#Available functionals|LDA]], [[GGA|GGA]]
{{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