From 04b2e961a75b0be9a4df34e73bfcccad03865700 Mon Sep 17 00:00:00 2001 From: Lorenzo <79980269+bastonero@users.noreply.github.com> Date: Tue, 6 Jun 2023 12:03:32 +0200 Subject: [PATCH 1/4] `Parser`: fix typo in the q point regex matching (#46) --- .../parsers/parse_raw/hp.py | 2 +- .../aiida.in | 13 + .../aiida.out | 234 ++++++++++++++++++ tests/parsers/test_hp.py | 34 +++ ...p_initialization_only_mesh_more_points.yml | 4 + 5 files changed, 286 insertions(+), 1 deletion(-) create mode 100644 tests/parsers/fixtures/hp/initialization_only_mesh_more_points/aiida.in create mode 100644 tests/parsers/fixtures/hp/initialization_only_mesh_more_points/aiida.out create mode 100644 tests/parsers/test_hp/test_hp_initialization_only_mesh_more_points.yml diff --git a/src/aiida_quantumespresso_hp/parsers/parse_raw/hp.py b/src/aiida_quantumespresso_hp/parsers/parse_raw/hp.py index 6b4f101..b291af2 100644 --- a/src/aiida_quantumespresso_hp/parsers/parse_raw/hp.py +++ b/src/aiida_quantumespresso_hp/parsers/parse_raw/hp.py @@ -31,7 +31,7 @@ def parse_raw_output(stdout): detect_important_message(logs, line) # A calculation that will only perturb a single atom will only print one line - match = re.search(r'.*The grid of q-points.*\s+([0-9])+\s+q-points.*', line) + match = re.search(r'.*The grid of q-points.*\s+([0-9]+)+\s+q-points.*', line) if match: parsed_data['number_of_qpoints'] = int(match.group(1)) diff --git a/tests/parsers/fixtures/hp/initialization_only_mesh_more_points/aiida.in b/tests/parsers/fixtures/hp/initialization_only_mesh_more_points/aiida.in new file mode 100644 index 0000000..bd64f89 --- /dev/null +++ b/tests/parsers/fixtures/hp/initialization_only_mesh_more_points/aiida.in @@ -0,0 +1,13 @@ +&INPUTHP + conv_thr_chi = 1.0000000000d-06 + determine_q_mesh_only = .true. + find_atpert = 3 + iverbosity = 2 + max_seconds = 3.4200000000d+03 + nq1 = 4 + nq2 = 4 + nq3 = 4 + outdir = 'out' + perturb_only_atom(13) = .true. + prefix = 'aiida' +/ diff --git a/tests/parsers/fixtures/hp/initialization_only_mesh_more_points/aiida.out b/tests/parsers/fixtures/hp/initialization_only_mesh_more_points/aiida.out new file mode 100644 index 0000000..a5b4b02 --- /dev/null +++ b/tests/parsers/fixtures/hp/initialization_only_mesh_more_points/aiida.out @@ -0,0 +1,234 @@ + Program HP v.7.2 starts on 5Jun2023 at 13:54:28 + + This program is part of the open-source Quantum ESPRESSO suite + for quantum simulation of materials; please cite + "P. Giannozzi et al., J. Phys.:Condens. Matter 21 395502 (2009); + "P. Giannozzi et al., J. Phys.:Condens. Matter 29 465901 (2017); + "P. Giannozzi et al., J. Chem. Phys. 152 154105 (2020); + URL http://www.quantum-espresso.org", + in publications or presentations arising from this work. More details at + http://www.quantum-espresso.org/quote + + Parallel version (MPI), running on 48 processors + + MPI processes distributed on 1 nodes + K-points division: npool = 16 + R & G space division: proc/nbgrp/npool/nimage = 3 + 24962 MiB available memory on the printing compute node when the environment starts + + + =---------------------------------------------------------------------------= + + Calculation of Hubbard parameters using the HP code based on DFPT + + Please cite the following papers when using this program: + + - HP code : Comput. Phys. Commun. 279, 108455 (2022). + + - Theory : Phys. Rev. B 98, 085127 (2018) and + + Phys. Rev. B 103, 045141 (2021). + + =-----------------------------------------------------------------------------= + + Reading xml data from directory: + + out/aiida.save/ + + IMPORTANT: XC functional enforced from input : + Exchange-correlation= PBESOL + ( 1 4 10 8 0 0 0) + Any further DFT definition will be discarded + Please, verify this is what you really want + + + Parallelization info + -------------------- + sticks: dense smooth PW G-vecs: dense smooth PW + Min 905 905 271 30463 30463 5034 + Max 906 906 271 30465 30465 5035 + Sum 2717 2717 813 91393 91393 15103 + + Using Slab Decomposition + + + Check: negative core charge= -0.000036 + Reading collected, re-writing distributed wavefunctions + + + bravais-lattice index = 0 + lattice parameter (alat) = 12.3672 (a.u.) + unit-cell volume = 1453.9300 (a.u.)^3 + number of atoms/cell = 16 + number of atomic types = 2 + kinetic-energy cut-off = 60.00 (Ry) + charge density cut-off = 240.00 (Ry) + conv. thresh. for NSCF = 1.0E-11 + conv. thresh. for chi = 1.0E-06 + Input Hubbard parameters (in eV): + V ( 1, 1) = 5.0000 + V ( 1, 229) = 0.0000 + V ( 1, 230) = 0.0000 + V ( 2, 2) = 5.0000 + V ( 2, 6) = 0.0000 + V ( 2, 405) = 0.0000 + V ( 3, 3) = 5.0000 + V ( 4, 4) = 5.0000 + V ( 5, 5) = 0.0000 + V ( 5, 34) = 0.0000 + V ( 5, 209) = 0.0000 + V ( 6, 2) = 0.0000 + V ( 6, 6) = 0.0000 + V ( 6, 209) = 0.0000 + V ( 7, 7) = 0.0000 + V ( 8, 8) = 0.0000 + V ( 9, 9) = 0.0000 + V ( 10, 10) = 0.0000 + V ( 11, 11) = 0.0000 + V ( 12, 12) = 0.0000 + V ( 13, 13) = 0.0000 + V ( 14, 14) = 0.0000 + V ( 15, 15) = 0.0000 + V ( 16, 16) = 0.0000 + + celldm(1) = 12.36723 celldm(2) = 0.00000 celldm(3) = 0.00000 + celldm(4) = 0.00000 celldm(5) = 0.00000 celldm(6) = 0.00000 + + crystal axes: (cart. coord. in units of alat) + a(1) = ( 0.5609 0.5784 0.5924 ) + a(2) = ( 0.5609 -0.5784 -0.5924 ) + a(3) = ( -0.5609 0.5784 -0.5924 ) + + reciprocal axes: (cart. coord. in units 2 pi/alat) + b(1) = ( 0.8915 0.8645 0.0000 ) + b(2) = ( 0.8915 0.0000 -0.8440 ) + b(3) = ( 0.0000 0.8645 -0.8440 ) + + Atoms inside the unit cell (Cartesian axes): + site n. atom mass positions (alat units) + 1 W 183.8400 tau( 1) = ( -0.28043 0.57835 -0.55568 ) + 2 W 183.8400 tau( 2) = ( 0.84128 0.00000 -0.03673 ) + 3 W 183.8400 tau( 3) = ( 0.28043 0.00000 -0.55450 ) + 4 W 183.8400 tau( 4) = ( 0.28043 0.57835 -0.03791 ) + 5 O 15.9994 tau( 5) = ( 0.00000 0.00000 0.00000 ) + 6 O 15.9994 tau( 6) = ( 0.56086 0.00000 0.00000 ) + 7 O 15.9994 tau( 7) = ( 0.56086 0.57835 0.00000 ) + 8 O 15.9994 tau( 8) = ( 0.00000 0.57835 0.00000 ) + 9 O 15.9994 tau( 9) = ( 0.28043 0.28397 0.03317 ) + 10 O 15.9994 tau( 10) = ( 0.28043 0.29438 -0.62558 ) + 11 O 15.9994 tau( 11) = ( -0.28043 0.29438 -0.55923 ) + 12 O 15.9994 tau( 12) = ( 0.84128 0.28397 -0.03317 ) + 13 O 15.9994 tau( 13) = ( 0.28043 0.00000 -0.87440 ) + 14 O 15.9994 tau( 14) = ( 0.28043 0.57835 0.28199 ) + 15 O 15.9994 tau( 15) = ( 0.28043 0.00000 -0.26540 ) + 16 O 15.9994 tau( 16) = ( 0.28043 0.57835 -0.32701 ) + + Atom which will be perturbed: + + 13 O 15.9994 tau(13) = ( 0.28043 0.00000 -0.87440 ) + + Reading xml data from directory: + + out/aiida.save/ + + IMPORTANT: XC functional enforced from input : + Exchange-correlation= PBESOL + ( 1 4 10 8 0 0 0) + Any further DFT definition will be discarded + Please, verify this is what you really want + + + Parallelization info + -------------------- + sticks: dense smooth PW G-vecs: dense smooth PW + Min 905 905 271 30463 30463 5034 + Max 906 906 271 30465 30465 5035 + Sum 2717 2717 813 91393 91393 15103 + + Using Slab Decomposition + + + Check: negative core charge= -0.000036 + Reading collected, re-writing distributed wavefunctions + + ===================================================================== + + PERTURBED ATOM # 13 + + site n. atom mass positions (alat units) + 13 O 15.9994 tau(13) = ( 0.28043 0.00000 -0.87440 ) + + ===================================================================== + + The perturbed atom has a type which is not unique! + Changing the type of the perturbed atom and recomputing the symmetries... + The number of symmetries is reduced : + nsym = 4 nsym_PWscf = 8 + Changing the type of the perturbed atom back to its original type... + + + The grid of q-points ( 4, 4, 4) ( 18 q-points ) : + N xq(1) xq(2) xq(3) wq + 1 0.000000000 0.000000000 0.000000000 0.015625000 + 2 0.000000000 0.216131358 -0.211002628 0.062500000 + 3 0.000000000 -0.432262716 0.422005257 0.031250000 + 4 0.222873502 0.000000000 -0.211002628 0.062500000 + 5 0.222873502 0.216131358 -0.422005257 0.125000000 + 6 0.222873502 -0.432262716 0.211002628 0.125000000 + 7 0.222873502 -0.216131358 0.000000000 0.062500000 + 8 -0.445747005 0.000000000 0.422005257 0.031250000 + 9 -0.445747005 0.216131358 0.211002628 0.125000000 + 10 -0.445747005 -0.432262716 0.844010513 0.031250000 + 11 0.445747005 0.432262716 -0.422005257 0.031250000 + 12 0.445747005 0.000000000 0.000000000 0.031250000 + 13 -0.222873502 -0.216131358 0.844010513 0.062500000 + 14 -0.222873502 0.000000000 0.633007885 0.062500000 + 15 0.000000000 0.432262716 0.000000000 0.031250000 + 16 0.000000000 -0.216131358 0.633007885 0.062500000 + 17 0.000000000 0.000000000 0.422005257 0.031250000 + 18 -0.891494009 -0.864525432 0.844010513 0.015625000 + + PRINTING TIMING FROM PWSCF ROUTINES: + + + Called by init_run: + + Called by electrons: + v_of_rho : 0.17s CPU 0.21s WALL ( 2 calls) + v_h : 0.01s CPU 0.01s WALL ( 2 calls) + v_xc : 0.17s CPU 0.20s WALL ( 2 calls) + + Called by c_bands: + + Called by sum_band: + + Called by *egterg: + + Called by h_psi: + + General routines + fft : 0.09s CPU 0.16s WALL ( 22 calls) + davcio : 0.00s CPU 0.02s WALL ( 6 calls) + + Parallel routines + + Hubbard U routines + alloc_neigh : 0.33s CPU 0.34s WALL ( 2 calls) + + init_vloc : 0.37s CPU 0.37s WALL ( 2 calls) + init_us_1 : 0.02s CPU 0.03s WALL ( 2 calls) + + PRINTING TIMING FROM HP ROUTINES: + + + PRINTING TIMING FROM LR MODULE: + + + HP : 2.09s CPU 3.79s WALL + + + This run was terminated on: 13:54:32 5Jun2023 + +=------------------------------------------------------------------------------= + JOB DONE. +=------------------------------------------------------------------------------= diff --git a/tests/parsers/test_hp.py b/tests/parsers/test_hp.py index 14d174b..bca62b5 100644 --- a/tests/parsers/test_hp.py +++ b/tests/parsers/test_hp.py @@ -204,6 +204,40 @@ def test_hp_initialization_only_mesh( }) +def test_hp_initialization_only_mesh_more_points( + aiida_localhost, generate_calc_job_node, generate_parser, generate_inputs_mesh_only, data_regression, tmpdir +): + """Test an initialization only `hp.x` calculation with intersites with more points.""" + name = 'initialization_only_mesh_more_points' + entry_point_calc_job = 'quantumespresso.hp' + entry_point_parser = 'quantumespresso.hp' + + # QE generates the ``HUBBARD.dat``, but with empty values, thus we make sure the parser + # does not recognize it as a final calculation and it does not crash as a consequence. + attributes = {'retrieve_temporary_list': ['HUBBARD.dat']} + node = generate_calc_job_node( + entry_point_calc_job, + aiida_localhost, + test_name=name, + inputs=generate_inputs_mesh_only, + attributes=attributes, + retrieve_temporary=(tmpdir, ['HUBBARD.dat']) + ) + parser = generate_parser(entry_point_parser) + results, calcfunction = parser.parse_from_node(node, store_provenance=False, retrieved_temporary_folder=tmpdir) + + assert calcfunction.is_finished, calcfunction.exception + assert calcfunction.is_finished_ok, calcfunction.exit_message + assert 'parameters' in results + assert 'hubbard' not in results + assert 'hubbard_chi' not in results + assert 'hubbard_matrices' not in results + assert 'hubbard_structure' not in results + data_regression.check({ + 'parameters': results['parameters'].get_dict(), + }) + + def test_hp_failed_invalid_namelist(aiida_localhost, generate_calc_job_node, generate_parser, generate_inputs_default): """Test an `hp.x` calculation that fails because of an invalid namelist.""" name = 'failed_invalid_namelist' diff --git a/tests/parsers/test_hp/test_hp_initialization_only_mesh_more_points.yml b/tests/parsers/test_hp/test_hp_initialization_only_mesh_more_points.yml new file mode 100644 index 0000000..0194b68 --- /dev/null +++ b/tests/parsers/test_hp/test_hp_initialization_only_mesh_more_points.yml @@ -0,0 +1,4 @@ +parameters: + hubbard_sites: + '13': O + number_of_qpoints: 18 From bd952ac2d2f5a87e19780e3baa9f70171861df12 Mon Sep 17 00:00:00 2001 From: Marnik Bercx Date: Wed, 22 Nov 2023 23:13:18 +0100 Subject: [PATCH 2/4] =?UTF-8?q?=F0=9F=93=9A=20`README.md`=20correct=20supp?= =?UTF-8?q?orted=20Python=20version?= MIME-Version: 1.0 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: 8bit --- README.md | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/README.md b/README.md index 1c6e2f9..8253251 100644 --- a/README.md +++ b/README.md @@ -1,6 +1,6 @@ # aiida-quantumespresso-hp AiiDA plugin for the Hubbard module of Quantum ESPRESSO. -The plugin requires HP v6.5 or above and is not compatible with older versions. +The plugin requires HP v7.2 or above and is not compatible with older versions. # Requirements This package depends directly on `aiida-core>=2.0.0` and the `aiida-quantumespresso>=4.0.0` package. From 64bd32dbcc1a424ffd8178a59a422b00692dc500 Mon Sep 17 00:00:00 2001 From: Marnik Bercx Date: Wed, 22 Nov 2023 23:11:32 +0100 Subject: [PATCH 3/4] =?UTF-8?q?=F0=9F=93=9A=20Update=20documentation=20dep?= =?UTF-8?q?endencies?= MIME-Version: 1.0 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: 8bit There were issues with building the documentation using Python 3.10. Here we update several documentation-related dependencies to newer versions. --- pyproject.toml | 6 +++--- 1 file changed, 3 insertions(+), 3 deletions(-) diff --git a/pyproject.toml b/pyproject.toml index be3d813..47ad3fc 100644 --- a/pyproject.toml +++ b/pyproject.toml @@ -37,15 +37,15 @@ Documentation = 'https://aiida-quantumespresso-hp.readthedocs.io' [project.optional-dependencies] docs = [ - 'myst-nb~=0.17', + 'myst-nb~=1.0', 'jupytext>=1.11.2,<1.15.0', 'sphinx-togglebutton', - 'sphinx~=5.2', + 'sphinx~=6.2', 'sphinx-copybutton~=0.5.2', 'sphinx-book-theme~=1.0.1', 'sphinx-design~=0.4.1', 'sphinxcontrib-details-directive~=0.1.0', - 'sphinx-autoapi~=2.0.1', + 'sphinx-autoapi~=3.0', ] pre-commit = [ 'pre-commit~=2.17', From 71f5a4ad91de07ec17cc307f1758bd03516854cf Mon Sep 17 00:00:00 2001 From: Marnik Bercx Date: Wed, 22 Nov 2023 23:12:05 +0100 Subject: [PATCH 4/4] =?UTF-8?q?=F0=9F=93=9A=20Small=20fixes=20to=20basic?= =?UTF-8?q?=20tutorial?= MIME-Version: 1.0 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: 8bit --- docs/source/1_computing_hubbard.ipynb | 40 ++++++++++++++++++--------- docs/source/index.md | 2 +- 2 files changed, 28 insertions(+), 14 deletions(-) diff --git a/docs/source/1_computing_hubbard.ipynb b/docs/source/1_computing_hubbard.ipynb index cba2ae4..431664f 100644 --- a/docs/source/1_computing_hubbard.ipynb +++ b/docs/source/1_computing_hubbard.ipynb @@ -19,7 +19,7 @@ "* __DFPT calculation__: use the {py:class}`~aiida_quantumespresso_hp.workflow.hp.base.HpBaseWorkChain` to do a self-consistent perturbation calculation to predict the Hubbard parameters.\n", "\n", "In this tutorial we will make use of the silicon structure to give you an overall understanding of the usage of the package.\n", - "If you are interested in more advanced features, please have a look at the [next tutorial](./2_parallel_hubbard.ipynb) or to the [how tos](../howto/index.rst).\n", + "If you are interested in more advanced features, please have a look at the [next tutorial](./2_parallel_hubbard.ipynb) or to the [how tos](howto).\n", "\n", "Let's get started!" ] @@ -141,10 +141,14 @@ "cell_type": "markdown", "metadata": {}, "source": [ - "As you can see, the desired interactions has been initialized correctly. This is important because ``hp.x`` needs to know which atoms need to be perturbed. As you will see later, the ``hp.x`` will take care of adding the remaining interactions with neighbouring atoms.\n", + "As you can see, the desired interactions have been initialized correctly. \n", + "This is important because `hp.x` needs to know which atoms need to be perturbed. \n", + "As you will see later, `hp.x` will take care of adding the remaining interactions with neighbouring atoms.\n", "\n", ":::{important}\n", - "When you will use your own structures, make sure to have your 'Hubbard atoms' first in the list of atoms. This is due to the way the ``hp.x`` routine works internally, requiring those to be first. You can simply do this with the following snippet (IF THE NODE IS YET NOT STORED!):\n", + "When you use your own structures, make sure to have your 'Hubbard atoms' first in the list of atoms.\n", + "This is due to the way the `hp.x` routine works internally, requiring those to be first.\n", + "You can simply do this with the following snippet (IF THE NODE IS YET NOT STORED!):\n", "\n", "```python\n", "from aiida_quantumespresso.utils.hubbard import HubbardUtils\n", @@ -161,7 +165,7 @@ "## Calculating the SCF ground-state\n", "\n", "Now that we have defined the structure, we can calculate its ground-state via an SCF using the `PwBaseWorkChain`.\n", - "We can fill the inputs of the builder of the PwBaseWorkChain through the `get_builder_from_protocol`." + "We can fill the inputs of the builder of the `PwBaseWorkChain` through the `get_builder_from_protocol()` method." ] }, { @@ -197,7 +201,8 @@ "cell_type": "markdown", "metadata": {}, "source": [ - "As you can notice from the results, the workchain (actually, the `PwCalculation`!) has a `remote_folder` output namespace. This is what we need in order to run the `HpBaseWorkChain`. " + "As you can notice from the results, the workchain (actually, the `PwCalculation`!) has a `remote_folder` output.\n", + "This is what we need in order to run the `HpBaseWorkChain`. " ] }, { @@ -208,7 +213,7 @@ "## DFPT calculation of Hubbard parameters\n", "\n", "We can perturb the ground-state previously found to compute the Hubbard parameters.\n", - "Here we will need to use the `HpBaseWorkChain`, and link the `parent folder` previously produced." + "Here we will need to use the `HpBaseWorkChain`, and link the `remote_folder` previously produced via the `parent_scf` input." ] }, { @@ -286,12 +291,15 @@ "source": [ "## Final considerations\n", "\n", - "We managed to compute the Hubbard parameters __fully__ ___ab initio___! :tada:\n", - "Although, as you could have noticed, there were some quite few passages to do by end. Moreover, there are the following considerations:\n", - "\n", - "1. For larger and more complex structures you will need to perturb many more atoms. Moreover, to get converged results you will need more the one q points. Clieck [here](./2_parallel_hubbard.ipynb). to learn how to parallelize over atoms and q points\n", - "2. To do a _full_ self-consistent calculation of these parameters, you should _relax_ your structure with the Hubbard parameters from the ``hp.x`` run, repeat the steps of this tutorial, relax _again_, and do this procedure over and over till convergence. Learn the automated way [here](./3_self_consistent.ipynb)!\n", + "We managed to compute the Hubbard parameters of LiCoO2 __fully__ ___ab initio___! :tada:\n", + "However, we had to execute quite a few steps manually, which can be tedious and error prone.\n", + "Moreover, there are the following considerations:\n", "\n", + "1. For larger and more complex structures you will need to perturb many more atoms.\n", + " Moreover, to get converged results you will need more than one q point.\n", + " Click [here](./2_parallel_hubbard.ipynb) to learn how to parallelize over atoms and q points.\n", + "2. To do a _full_ self-consistent calculation of these parameters, you should _relax_ your structure with the Hubbard parameters from the `hp.x` run, repeat the steps of this tutorial, relax _again_, and do this procedure over and over till convergence.\n", + " Learn the automated way [here](./3_self_consistent.ipynb)!\n", "\n", ":::{admonition} Learn more and in details\n", ":class: hint\n", @@ -302,9 +310,15 @@ ":::\n", "\n", ":::{note}\n", - "We suggest to proceed first with the tutorial for point (1) and then the one for point (2). Nevertheless, tutorial (1) is not strictly necessary for (1).\n", + "We suggest to proceed first with the tutorial for point (1) and then the one for point (2). \n", + "Nevertheless, tutorial (1) is not strictly necessary for (2).\n", ":::" ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [] } ], "metadata": { @@ -323,7 +337,7 @@ "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython3", - "version": "3.8.10" + "version": "3.10.13" }, "orig_nbformat": 4, "vscode": { diff --git a/docs/source/index.md b/docs/source/index.md index a578ca6..8cd20c9 100644 --- a/docs/source/index.md +++ b/docs/source/index.md @@ -155,7 +155,7 @@ To the reference guides If you use this plugin for your research, please cite the following work: -> Lorenzo Bastonero, Cristiano Malica, Marnik Bercx, Eric Macke, Iurii Timrov, Nicola Marzari, and Sebastiaan P. Huber, [*Automated self-consistent prediction of extended Hubbard parameters for Li-ion batteries*](), npj Comp. Mat., **?**, ? (2023) +> Lorenzo Bastonero, Cristiano Malica, Marnik Bercx, Eric Macke, Iurii Timrov, Nicola Marzari, and Sebastiaan P. Huber, [*Automated self-consistent prediction of extended Hubbard parameters for Li-ion batteries*](https://media.giphy.com/media/zyclIRxMwlY40/giphy.gif), npj Comp. Mat., **?**, ? (2023) > Sebastiaan. P. Huber, Spyros Zoupanos, Martin Uhrin, Leopold Talirz, Leonid Kahle, Rico Häuselmann, Dominik Gresch, Tiziano Müller, Aliaksandr V. Yakutovich, Casper W. Andersen, Francisco F. Ramirez, Carl S. Adorf, Fernando Gargiulo, Snehal Kumbhar, Elsa Passaro, Conrad Johnston, Andrius Merkys, Andrea Cepellotti, Nicolas Mounet, Nicola Marzari, Boris Kozinsky, and Giovanni Pizzi, [*AiiDA 1.0, a scalable computational infrastructure for automated reproducible workflows and data provenance*](https://doi.org/10.1038/s41597-020-00638-4), Scientific Data **7**, 300 (2020)