Getting started
The objective of this tutorial is to give a basic idea of how Octopus works.
Generating the input file
With a text editor, create a text file called inp containing the following text:
CalculationMode = gs
%Coordinates
'H' | 0 | 0 | 0
%
Spacing = 0.25 * angstrom
Radius = 4.0 * angstrom
This is the simplest example of an Octopus input file:
-
CalculationMode = gs
: This variable defines the run mode – please consult the manual for the full list of the possible run modes. In this case we set it togs
, which instructs the code to start a ground-state calculation. -
%Coordinates
: The entry is not just the definition of a variable, but rather of a full set of them – a “block” of variables. The beginning of a block is marked by the%identifier
line, and ended by a%
line. In this case the identifier is%Coordinates
, where we list the atoms or species in our calculation and its coordinates, one per line. In this case, we put a single hydrogen atom in the center of our simulation box.
The reason this input file can be so simple is that Octopus comes with default values for the simulation parameters, and a set of default pseudopotentials for several elements (for properly converged calculations you might need to adjust these parameters, though).
To get a general idea of the format of the Octopus input file, go and read the page about the Input file in the manual.
The documentation for each input variable can be found in the variable reference online, and can also be accessed via the oct-help utility.
Running Octopus
Once you have written your input file, run the octopus command (using mpirun and perhaps a job script if you are using the parallel version). If everything goes correctly, you should see several lines of output in the terminal (if you don’t, there must be a problem with your installation). As this is probably the first time you run Octopus, we will examine the most important parts of the output.
Be aware that the precise values you find in the output might differ from the ones in the tutorial text. This can be due to updates in the code, or also changes in the compilation and run configuration.
- First there is an octopus drawn in ASCII art, the copyright notice and some information about the octopus version you are using and the system where you are running:
<><><><><><><><><><><><><><><><><><><><><><><><><><><><><><><>
___
.-' `'.
/ \
| ;
| | ___.--,
_.._ |0) ~ (0) | _.---'`__.-( (_.
__.--'`_.. '.__.\ '--. \_.-' ,.--'` `""`
( ,.--'` ',__ /./; ;, '.__.'` __
_`) ) .---.__.' / | |\ \__..--"" """--.,_
`---' .'.''-._.-'`_./ /\ '. \ _.-~~~````~~~-._`-.__.'
| | .' _.-' | | \ \ '. `~---`
\ \/ .' \ \ '. '-._)
\/ / \ \ `=.__`~-.
jgs / /\ `) ) / / `"".`\
, _.-'.'\ \ / / ( ( / /
`--~` ) ) .-'.' '.'. | (
(/` ( (` ) ) '-;
` '-; (-'
This program is free software; you can redistribute it and/or modify
it under the terms of the GNU General Public License as published by
the Free Software Foundation; either version 2, or (at your option)
any later version.
This program is distributed in the hope that it will be useful,
but WITHOUT ANY WARRANTY; without even the implied warranty of
MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
GNU General Public License for more details.
You should have received a copy of the GNU General Public License
along with this program; if not, write to the Free Software
Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, MA
<><><><><><><><><><><><><><><><><><><><><><><><><><><><><><><>
Running octopus
Version : mercatoris
Commit : afbc1c5f59003f4d895e759f8da004e124cf89bd
Configuration time : Thu Feb 1 14:29:48 CET 2024
Configuration options : mpi sse2 avx libxc5 libxc_fxc libxc_kxc
Optional libraries : berkeleygw cgal ELPA etsf_io psolver libvdwxc metis netcdf nfft parmetis scalapack sparskit nlopt
Architecture : x86_64
C compiler : mpicc (gcc)
C compiler flags : -g -Wall -O2 -march=native -Wextra -pedantic -ftest-coverage -fprofile-arcs
C++ compiler : mpicxx (g++)
C++ compiler flags : -g -Wall -O2 -march=native -Wextra -pedantic -ftest-coverage -fprofile-arcs
Fortran compiler : mpifort (gfortran) (GCC version 11.3.0)
Fortran compiler flags : -g -fno-var-tracking-assignments -Wall -Wno-maybe-uninitialized -Wno-surprising -O2 -march=native -fbacktrace -fcheck=all -fbounds-check -finit-real=snan -ffpe-trap=zero,invalid -ftest-coverage -fprofile-arcs
The octopus is swimming in poppyseed (Linux)
Calculation started on 2024/02/02 at 12:37:02
Note that it also gives you the revision number, the compiler, and the compiler flags used. You should always include this information when submitting a bug report!
-
The type of calculation it was asked to perform:
-
The species and pseudopotentials it is using:
****************************** Species ******************************* Species 'H' type : pseudopotential file : '/home/luedersm/Octopus_foss_2022a_mpi_debug/share/octopus/pseudopotentials/PSF/H.psf' file format : PSF valence charge : 1.0 atomic number : 1 form on file : semilocal orbital origin : calculated lmax : 0 llocal : 0 projectors per l : 1 total projectors : 0 application form : local orbitals : 16 bound orbitals : 1 **********************************************************************
-
After some other output, Octopus prints information about the grid: as we didn’t say anything in the input file, Octopus used the parameters recommended for this pseupopotential:
******************************** Grid ******************************** Simulation Box: Type = minimum Radius [b] = 7.559 Main mesh: Spacing [b] = ( 0.472, 0.472, 0.472) volume/point [b^3] = 0.10544 # inner mesh = 17077 # total mesh = 30461 Grid Cutoff [H] = 22.110166 Grid Cutoff [Ry] = 44.220331 **********************************************************************
-
The level of theory and, in the case of (TD)DFT, the approximation to the exchange-correlation term:
**************************** Theory Level **************************** Input: [TheoryLevel = kohn_sham] Exchange-correlation: Exchange Slater exchange (LDA) [1] P. A. M. Dirac, Math. Proc. Cambridge Philos. Soc. 26, 376 (1930) [2] F. Bloch, Z. Phys. 57, 545 (1929) Correlation Perdew & Zunger (Modified) (LDA) [1] J. P. Perdew and A. Zunger, Phys. Rev. B 23, 5048 (1981), modified to improve the matching between the low- and high-rs parts **********************************************************************
-
At this point, Octopus tries to read the wave-functions from a previous calculation. As there are none, it will give a warning.
** Warning: ** Could not find 'restart/gs' directory for restart. ** No restart information will be read. ** Warning: ** Unable to read wavefunctions. ** Starting from scratch!
-
Now Octopus commences the calculation. To get a reasonable starting point for the DFT calculation, the initial wavefunctions are calculated as a Linear Combination of Atomic Orbitals (LCAO).
Info: Performing initial LCAO calculation with 1 orbitals. Info: Getting Hamiltonian matrix elements. ETA: .......1......2.......3......4......5.......6......7.......8......9......0 Eigenvalues [H] #st Spin Eigenvalue Occupation 1 -- -0.233536 1.000000 Info: Ground-state restart information will be written to 'restart/gs'.
-
After the LCAO, the real DFT calculation starts. For each self-consistency step some information is printed. When SCF converges, the calculation is done.
…*********************** SCF CYCLE ITER # 1 ************************ etot = -4.47195440E-01 abs_ev = 1.12E-03 rel_ev = 4.78E-03 ediff = 4.47E-01 abs_dens = 5.49E-03 rel_dens = 5.49E-03 Matrix vector products: 4 Converged eigenvectors: 0 # State Eigenvalue [H] Occupation Error 1 -0.234657 1.000000 ( 1.0E-02) Elapsed time for SCF step 1: 0.01 **********************************************************************
*********************** SCF CYCLE ITER # 12 ************************ etot = -4.46666631E-01 abs_ev = 1.78E-08 rel_ev = 7.65E-08 ediff = 5.24E-09 abs_dens = 7.04E-08 rel_dens = 7.04E-08 Matrix vector products: 11 Converged eigenvectors: 1 # State Eigenvalue [H] Occupation Error 1 -0.233152 1.000000 ( 4.5E-08) Elapsed time for SCF step 12: 0.01 ********************************************************************** Info: Writing states. 2024/02/02 at 12:37:03 Info: Finished writing states. 2024/02/02 at 12:37:03 Info: SCF converged in 12 iterations Info: Number of matrix-vector products: 88 Info: Finished writing information to 'restart/gs'. Calculation ended on 2024/02/02 at 12:37:03 Walltime: 00.745s Octopus emitted 1 warning.
Just running the command octopus will write the output directly to the terminal. To have a saved copy of the output, it is generally advisable to redirect the output into a file, and to capture the standard error stream as well, which can be done like this: octopus &> log . That would create a file called log containing all output including warnings and errors in their context.
Analyzing the results
After finishing the calculation you will find a series of files in the directory you ran:
% ls
exec inp restart static
For the moment we will ignore the ‘‘‘exec’’’ and ‘‘‘restart’’’ directories and focus on the static/info file, which contains the detailed results of the ground-state calculation. If you open that file, first you will see some parameters of the calculations (that we already got from the output) and then the calculated energies and eigenvalues in Hartrees:
Eigenvalues [H]
#st Spin Eigenvalue Occupation
1 -- -0.233013 1.000000
Energy [H]:
Total = -0.44637705
Free = -0.44637705
-----------
Ion-ion = 0.00000000
Eigenvalues = -0.23301327
Hartree = 0.28415332
Int[n*v_xc] = -0.30429841
Exchange = -0.19375604
Correlation = -0.03975282
vanderWaals = 0.00000000
Delta XC = 0.00000000
Entropy = 1.38629436
-TS = -0.00000000
Kinetic = 0.41780616
External = -0.91483022
Non-local = 0.00000000
Since by default Octopus does a spin-unpolarized density-functional-theory calculation with the local-density approximation, our results differ from the exact total energy of 0.5 H. Our exchange-correlation functional can be set by the variable XCFunctional, using the set provided by the libxc library.
Extra
If you want to improve the LDA results, you can try to repeat the calculation with spin-polarization:
SpinComponents = spin_polarized
And if you want to obtain the exact Schödinger equation result (something possible only for very simple systems like this one) you have to remove the self-interaction error (a problem of the LDA). Since we only have one electron the simplest way to do it for this case is to use independent electrons:
TheoryLevel = independent_particles
A more general way would be to include self-interaction correction.