Results
[
{
"executables": [
"runner",
"test_template/template_"
],
"domain": "openkim.org",
"publication-year": "2014",
"created_on": "2018-05-08 15:31:13.187898",
"properties": [
"tag:staff@noreply.openkim.org,2014-04-15:property/cohesive-energy-relation-cubic-crystal"
],
"contributor-id": "4d62befd-21c4-42b8-a472-86132e6591f3",
"makeable": true,
"author": "Daniel Karls",
"kimid-version": "002",
"kimcode": "LammpsExample2__TD_887699523131_002",
"short-id": "TD_887699523131_002",
"version": 2,
"pipeline-api-version": "1.0",
"inserted_on": "2018-05-08 22:57:28.184532",
"kimnum": "887699523131",
"shortcode": "TD_887699523131",
"description": "This example Test Driver illustrates the use of LAMMPS in the openkim-pipeline\nto compute an energy-volume curve (more specifically, a cohesive energy-lattice\nconstant curve) for a given cubic lattice (fcc, bcc, sc, diamond) of a single given\nspecies. The curve is computed for lattice constants ranging from a_min to a_max,\nwith most samples being about a_0 (a_min, a_max, and a_0 are specified via stdin.\na_0 is typically approximately equal to the equilibrium lattice constant.). The precise\nscaling of sample points going from a_min to a_0 and from a_0 to a_max is specified\nby two separate parameters passed from stdin. Please see README.txt for further\ndetails.",
"kimid-version-as-integer": 2,
"extended-id": "LammpsExample2__TD_887699523131_002",
"driver": true,
"simulator-name": "LAMMPS",
"path": "td/LammpsExample2__TD_887699523131_002",
"kim-api-version": "1.9.0",
"approved": true,
"kimid-typecode": "td",
"name": "LammpsExample2",
"kimid-prefix": "LammpsExample2",
"type": "td",
"title": "LammpsExample2: energy-volume curve for monoatomic cubic lattice",
"maintainer-id": "4d62befd-21c4-42b8-a472-86132e6591f3",
"kimid-number": "887699523131",
"latest": true
},
{
"domain": "openkim.org",
"publication-year": "2016",
"created_on": "2018-05-08 15:31:13.203897",
"properties": [
"tag:staff@noreply.openkim.org,2015-05-26:property/cohesive-energy-lattice-invariant-shear-path-cubic-crystal"
],
"contributor-id": "e2ada8d8-70b2-4ffc-843e-a69df752ed91",
"makeable": true,
"author": "Jiadi Fan",
"kimid-version": "001",
"kimcode": "LatticeInvariantShearPathCubicCrystalCBKIM__TD_083627594945_001",
"short-id": "TD_083627594945_001",
"version": 1,
"pipeline-api-version": "1.0",
"inserted_on": "2018-05-08 22:58:28.001841",
"kimnum": "083627594945",
"shortcode": "TD_083627594945",
"description": "This test driver is used to test lattice invariance shear in a cubic crystal based on cb-kim code. Initial guess of lattice parameter, shear direction vector, shear plane normal vector, relaxation optional key need to be set as input. The output will be first PK stress, stiffness matrix, cohesive energy, and displacement of shuffle (if relaxation optional key is true)",
"kimid-version-as-integer": 1,
"extended-id": "LatticeInvariantShearPathCubicCrystalCBKIM__TD_083627594945_001",
"driver": true,
"simulator-name": "none",
"path": "td/LatticeInvariantShearPathCubicCrystalCBKIM__TD_083627594945_001",
"kim-api-version": "1.6",
"approved": true,
"kimid-typecode": "td",
"name": "LatticeInvariantShearPathCubicCrystalCBKIM",
"kimid-prefix": "LatticeInvariantShearPathCubicCrystalCBKIM",
"type": "td",
"title": "Cohesive energy versus shear parameter relation for a cubic crystal",
"maintainer-id": "e2ada8d8-70b2-4ffc-843e-a69df752ed91",
"kimid-number": "083627594945",
"latest": true
},
{
"executables": [
"runner"
],
"domain": "openkim.org",
"publication-year": "2018",
"created_on": "2018-05-08 15:31:13.223897",
"properties": [
"tag:staff@noreply.openkim.org,2014-04-15:property/bulk-modulus-isothermal-cubic-crystal-npt",
"tag:staff@noreply.openkim.org,2014-05-21:property/elastic-constants-isothermal-cubic-crystal-npt",
"tag:staff@noreply.openkim.org,2014-04-15:property/structure-cubic-crystal-npt"
],
"contributor-id": "e2ada8d8-70b2-4ffc-843e-a69df752ed91",
"makeable": true,
"author": "Jiadi Fan",
"kimid-version": "000",
"kimcode": "binary_alloy_elastic_constant__TD_601231739727_000",
"short-id": "TD_601231739727_000",
"version": 0,
"inserted_on": "2018-05-08 22:58:59.403416",
"kimnum": "601231739727",
"shortcode": "TD_601231739727",
"description": "Computes the elastic constant for binary alloy system.",
"kimid-version-as-integer": 0,
"extended-id": "binary_alloy_elastic_constant__TD_601231739727_000",
"driver": true,
"path": "td/binary_alloy_elastic_constant__TD_601231739727_000",
"kim-api-version": "1.9.0",
"approved": true,
"kimid-typecode": "td",
"name": "binary_alloy_elastic_constant",
"kimid-prefix": "binary_alloy_elastic_constant",
"type": "td",
"title": "Elastic constants of cubic binary alloys",
"maintainer-id": "e2ada8d8-70b2-4ffc-843e-a69df752ed91",
"kimid-number": "601231739727",
"latest": true
},
{
"executables": [
"runner"
],
"domain": "openkim.org",
"publication-year": "2018",
"created_on": "2018-07-12 22:49:25.400736",
"properties": [
"tag:staff@noreply.openkim.org,2014-04-15:property/cohesive-potential-energy-cubic-crystal"
],
"contributor-id": "4d62befd-21c4-42b8-a472-86132e6591f3",
"makeable": true,
"author": "Daniel Karls",
"kimid-version": "004",
"kimcode": "LammpsExample__TD_567444853524_004",
"short-id": "TD_567444853524_004",
"version": 4,
"inserted_on": "2018-07-13 03:49:25.671370",
"kimnum": "567444853524",
"shortcode": "TD_567444853524",
"description": "This example Test Driver illustrates the use of LAMMPS to compute the equilibrium lattice spacing and cohesive energy of fcc argon using Polak-Ribiere conjugate gradient minimization in LAMMPS and an initial guess at the equilibrium lattice spacing supplied by the user through pipeline.stdin.tpl.",
"kimid-version-as-integer": 4,
"extended-id": "LammpsExample__TD_567444853524_004",
"driver": true,
"simulator-name": "LAMMPS",
"path": "td/LammpsExample__TD_567444853524_004",
"kim-api-version": "1.9.0",
"approved": true,
"kimid-typecode": "td",
"name": "LammpsExample",
"kimid-prefix": "LammpsExample",
"type": "td",
"title": "LammpsExample: cohesive energy and equilibrium lattice constant of fcc argon",
"maintainer-id": "4d62befd-21c4-42b8-a472-86132e6591f3",
"kimid-number": "567444853524",
"latest": true
},
{
"extended-id": "LatticeConstantCubicEnergy__TD_475411767977_007",
"short-id": "TD_475411767977_007",
"kimid-prefix": "LatticeConstantCubicEnergy",
"kimid-typecode": "td",
"kimid-number": "475411767977",
"kimid-version": "007",
"kimid-version-as-integer": 7,
"name": "LatticeConstantCubicEnergy",
"type": "td",
"kimnum": "475411767977",
"version": 7,
"shortcode": "TD_475411767977",
"kimcode": "LatticeConstantCubicEnergy__TD_475411767977_007",
"path": "td/LatticeConstantCubicEnergy__TD_475411767977_007",
"approved": true,
"inserted_on": "2019-07-10 20:23:29.773758",
"latest": true,
"makeable": true,
"driver": true,
"contributor-id": "4d62befd-21c4-42b8-a472-86132e6591f3",
"description": "Equilibrium lattice constant and cohesive energy of a cubic lattice at zero temperature and pressure.",
"doi": "10.25950/2765e3bf",
"domain": "openkim.org",
"executables": [
"runner",
"test_template/runner"
],
"kim-api-version": "2.0",
"maintainer-id": "4d62befd-21c4-42b8-a472-86132e6591f3",
"properties": [
"tag:staff@noreply.openkim.org,2014-04-15:property/cohesive-potential-energy-cubic-crystal",
"tag:staff@noreply.openkim.org,2014-04-15:property/structure-cubic-crystal-npt"
],
"publication-year": "2019",
"simulator-name": "ase",
"title": "Equilibrium lattice constant and cohesive energy of a cubic lattice at zero temperature and pressure v007",
"created_on": "2019-07-10 15:23:29.384734",
"developer": [
"4d62befd-21c4-42b8-a472-86132e6591f3",
"c429164b-1b03-4ce3-a3a8-2568dd2bc449"
]
},
{
"extended-id": "ElasticConstantsCubic__TD_011862047401_006",
"short-id": "TD_011862047401_006",
"kimid-prefix": "ElasticConstantsCubic",
"kimid-typecode": "td",
"kimid-number": "011862047401",
"kimid-version": "006",
"kimid-version-as-integer": 6,
"name": "ElasticConstantsCubic",
"type": "td",
"kimnum": "011862047401",
"version": 6,
"shortcode": "TD_011862047401",
"kimcode": "ElasticConstantsCubic__TD_011862047401_006",
"path": "td/ElasticConstantsCubic__TD_011862047401_006",
"approved": true,
"inserted_on": "2019-07-11 20:50:03.335764",
"latest": true,
"makeable": true,
"driver": true,
"contributor-id": "360c0aed-48ce-45f6-ba13-337f12a531e8",
"description": "Computes the cubic elastic constants for some common crystal types (fcc, bcc, sc, diamond) by calculating the hessian of the energy density with respect to strain. An estimate of the error associated with the numerical differentiation performed is reported.",
"doi": "10.25950/5853fb8f",
"domain": "openkim.org",
"executables": [
"runner",
"test_template/runner"
],
"kim-api-version": "2.0",
"maintainer-id": "360c0aed-48ce-45f6-ba13-337f12a531e8",
"properties": [
"tag:staff@noreply.openkim.org,2014-04-15:property/bulk-modulus-isothermal-cubic-crystal-npt",
"tag:staff@noreply.openkim.org,2014-05-21:property/elastic-constants-isothermal-cubic-crystal-npt"
],
"publication-year": "2019",
"simulator-name": "ase",
"source-citations": [
{
"address": "New York",
"author": "H.B. Huntington",
"doi": "10.1016/S0081-1947(08)60553-6",
"journal": "Solid State Physics",
"pages": "213--351",
"publisher": "Academic Press",
"recordkey": "TD_011862047401_006a",
"recordtype": "article",
"title": "The Elastic Constants of Crystals",
"volume": "7",
"year": "1958"
}
],
"title": "Elastic constants for cubic crystals at zero temperature and pressure v006",
"created_on": "2019-07-11 15:50:02.944366",
"developer": [
"360c0aed-48ce-45f6-ba13-337f12a531e8",
"c429164b-1b03-4ce3-a3a8-2568dd2bc449"
]
},
{
"extended-id": "CohesiveEnergyVsLatticeConstant__TD_554653289799_003",
"short-id": "TD_554653289799_003",
"kimid-prefix": "CohesiveEnergyVsLatticeConstant",
"kimid-typecode": "td",
"kimid-number": "554653289799",
"kimid-version": "003",
"kimid-version-as-integer": 3,
"name": "CohesiveEnergyVsLatticeConstant",
"type": "td",
"kimnum": "554653289799",
"version": 3,
"shortcode": "TD_554653289799",
"kimcode": "CohesiveEnergyVsLatticeConstant__TD_554653289799_003",
"path": "td/CohesiveEnergyVsLatticeConstant__TD_554653289799_003",
"approved": true,
"inserted_on": "2019-07-12 02:18:36.315233",
"latest": true,
"makeable": true,
"driver": true,
"author": "Daniel S. Karls",
"contributor-id": "4d62befd-21c4-42b8-a472-86132e6591f3",
"description": "This Test Driver uses LAMMPS to compute the cohesive energy of a given monoatomic cubic lattice (fcc, bcc, sc, or diamond) at a variety of lattice spacings. The lattice spacings range from a_min (=a_min_frac*a_0) to a_max (=a_max_frac*a_0) where a_0, a_min_frac, and a_max_frac are read from stdin (a_0 is typically approximately equal to the equilibrium lattice constant). The precise scaling and number of lattice spacings sampled between a_min and a_0 (a_0 and a_max) is specified by two additional parameters passed from stdin: N_lower and samplespacing_lower (N_upper and samplespacing_upper). Please see README.txt for further details.",
"doi": "10.25950/64cb38c5",
"domain": "openkim.org",
"executables": [
"runner",
"test_template/template_"
],
"kim-api-version": "2.0",
"maintainer-id": "4d62befd-21c4-42b8-a472-86132e6591f3",
"properties": [
"tag:staff@noreply.openkim.org,2014-04-15:property/cohesive-energy-relation-cubic-crystal"
],
"publication-year": "2019",
"simulator-name": "LAMMPS",
"title": "Cohesive energy versus lattice constant curve for monoatomic cubic lattices v003",
"created_on": "2019-07-11 21:18:34.667473",
"developer": [
"4d62befd-21c4-42b8-a472-86132e6591f3"
],
"implementer": []
},
{
"extended-id": "PhononDispersionCurve__TD_530195868545_004",
"short-id": "TD_530195868545_004",
"kimid-prefix": "PhononDispersionCurve",
"kimid-typecode": "td",
"kimid-number": "530195868545",
"kimid-version": "004",
"kimid-version-as-integer": 4,
"name": "PhononDispersionCurve",
"type": "td",
"kimnum": "530195868545",
"version": 4,
"shortcode": "TD_530195868545",
"kimcode": "PhononDispersionCurve__TD_530195868545_004",
"path": "td/PhononDispersionCurve__TD_530195868545_004",
"approved": true,
"inserted_on": "2019-07-12 06:51:21.433810",
"latest": true,
"makeable": true,
"driver": true,
"contributor-id": "8f8225b4-8b9c-439d-879d-45ee35db5757",
"description": "Calculates the phonon dispersion relations for fcc lattices and records the results as curves.",
"doi": "10.25950/64f4999b",
"domain": "openkim.org",
"executables": [
"runner",
"test_template/runner"
],
"kim-api-version": "2.0",
"maintainer-id": "8f8225b4-8b9c-439d-879d-45ee35db5757",
"properties": [
"tag:staff@noreply.openkim.org,2014-05-21:property/phonon-dispersion-dos-cubic-crystal-npt",
"tag:staff@noreply.openkim.org,2014-05-21:property/phonon-dispersion-relation-cubic-crystal-npt"
],
"publication-year": "2019",
"simulator-name": "ase",
"title": "Phonon dispersion relations for an fcc lattice v004",
"created_on": "2019-07-12 01:51:21.037358",
"developer": [
"8f8225b4-8b9c-439d-879d-45ee35db5757"
]
},
{
"extended-id": "SurfaceEnergyCubicCrystalBrokenBondFit__TD_955413365818_004",
"short-id": "TD_955413365818_004",
"kimid-prefix": "SurfaceEnergyCubicCrystalBrokenBondFit",
"kimid-typecode": "td",
"kimid-number": "955413365818",
"kimid-version": "004",
"kimid-version-as-integer": 4,
"name": "SurfaceEnergyCubicCrystalBrokenBondFit",
"type": "td",
"kimnum": "955413365818",
"version": 4,
"shortcode": "TD_955413365818",
"kimcode": "SurfaceEnergyCubicCrystalBrokenBondFit__TD_955413365818_004",
"path": "td/SurfaceEnergyCubicCrystalBrokenBondFit__TD_955413365818_004",
"approved": true,
"inserted_on": "2019-07-12 16:37:22.287242",
"latest": true,
"makeable": true,
"driver": true,
"contributor-id": "8f8225b4-8b9c-439d-879d-45ee35db5757",
"description": "Calculates the surface energy of several high symmetry surfaces and produces a broken-bond model fit. In latex form, the fit equations are given by:\n\nE_{FCC} (\\vec{n}) = p_1 (4 \\left( |x+y| + |x-y| + |x+z| + |x-z| + |z+y| +|z-y|\\right)) + p_2 (8 \\left( |x| + |y| + |z|\\right)) + p_3 (2 ( |x+ 2y + z| + |x+2y-z| + |x-2y + z| + |x-2y-z| + |2x+y+z| + |2x+y-z| +|2x-y+z| +|2x-y-z| +|x+y+2z| +|x+y-2z| +|x-y+2z| +|x-y-2z| ) + c\n\nE_{BCC} (\\vec{n}) = p_1 (6 \\left( | x+y+z| + |x+y-z| + |-x+y-z| + |x-y+z| \\right)) + p_2 (8 \\left( |x| + |y| + |z|\\right)) + p_3 (4 \\left( |x+y| + |x-y| + |x+z| + |x-z| + |z+y| +|z-y|\\right)) +c.\n\nIn Python, these two fits take the following form:\n\ndef BrokenBondFCC(params, index):\n\n import numpy\n x, y, z = index\n x = x / numpy.sqrt(x**2.+y**2.+z**2.)\n y = y / numpy.sqrt(x**2.+y**2.+z**2.)\n z = z / numpy.sqrt(x**2.+y**2.+z**2.)\n\n return params[0]*4* (abs(x+y) + abs(x-y) + abs(x+z) + abs(x-z) + abs(z+y) + abs(z-y)) + params[1]*8*(abs(x) + abs(y) + abs(z)) + params[2]*(abs(x+2*y+z) + abs(x+2*y-z) +abs(x-2*y+z) +abs(x-2*y-z) + abs(2*x+y+z) +abs(2*x+y-z) +abs(2*x-y+z) +abs(2*x-y-z) + abs(x+y+2*z) +abs(x+y-2*z) +abs(x-y+2*z) +abs(x-y-2*z))+params[3]\n\ndef BrokenBondBCC(params, x, y, z):\n\n\n import numpy\n x, y, z = index\n x = x / numpy.sqrt(x**2.+y**2.+z**2.)\n y = y / numpy.sqrt(x**2.+y**2.+z**2.)\n z = z / numpy.sqrt(x**2.+y**2.+z**2.)\n\n return params[0]*6*(abs(x+y+z) + abs(x-y-z) + abs(x-y+z) + abs(x+y-z)) + params[1]*8*(abs(x) + abs(y) + abs(z)) + params[2]*4* (abs(x+y) + abs(x-y) + abs(x+z) + abs(x-z) + abs(z+y) + abs(z-y)) + params[3]",
"doi": "10.25950/6c43a4e6",
"domain": "openkim.org",
"executables": [
"runner",
"test_template/runner"
],
"kim-api-version": "2.0",
"maintainer-id": "8f8225b4-8b9c-439d-879d-45ee35db5757",
"properties": [
"tag:staff@noreply.openkim.org,2014-05-21:property/surface-energy-broken-bond-fit-cubic-bravais-crystal-npt",
"tag:staff@noreply.openkim.org,2014-05-21:property/surface-energy-cubic-crystal-npt",
"tag:staff@noreply.openkim.org,2014-05-21:property/surface-energy-ideal-cubic-crystal"
],
"publication-year": "2019",
"simulator-name": "ase",
"title": "High-symmetry surface energies in cubic lattices and broken bond model v004",
"created_on": "2019-07-12 11:37:21.870746",
"developer": [
"8f8225b4-8b9c-439d-879d-45ee35db5757"
]
},
{
"extended-id": "StackingFaultFccCrystal__TD_228501831190_002",
"short-id": "TD_228501831190_002",
"kimid-prefix": "StackingFaultFccCrystal",
"kimid-typecode": "td",
"kimid-number": "228501831190",
"kimid-version": "002",
"kimid-version-as-integer": 2,
"name": "StackingFaultFccCrystal",
"type": "td",
"kimnum": "228501831190",
"version": 2,
"shortcode": "TD_228501831190",
"kimcode": "StackingFaultFccCrystal__TD_228501831190_002",
"path": "td/StackingFaultFccCrystal__TD_228501831190_002",
"approved": true,
"inserted_on": "2019-07-12 21:06:32.556604",
"latest": true,
"makeable": true,
"driver": true,
"author": "Subrahmanyam Pattamatta",
"contributor-id": "8d139a3f-870c-4328-9090-4904209bc1e9",
"description": "Intrinsic and extrinsic stacking fault energies, unstable stacking fault energy, unstable twinning energy, stacking fault energy as a function of fractional displacement, and gamma surface for a monoatomic FCC lattice at zero temperature and pressure.",
"disclaimer": "Computes all properties at zero temperature.",
"doi": "10.25950/b4cfaf9a",
"domain": "openkim.org",
"executables": [
"runner",
"test_template/runner"
],
"kim-api-version": "2.0",
"maintainer-id": "8d139a3f-870c-4328-9090-4904209bc1e9",
"properties": [
"tag:staff@noreply.openkim.org,2015-05-26:property/unstable-stacking-fault-relaxed-energy-fcc-crystal-npt",
"tag:staff@noreply.openkim.org,2015-05-26:property/intrinsic-stacking-fault-relaxed-energy-fcc-crystal-npt",
"tag:staff@noreply.openkim.org,2015-05-26:property/unstable-twinning-fault-relaxed-energy-fcc-crystal-npt",
"tag:staff@noreply.openkim.org,2015-05-26:property/extrinsic-stacking-fault-relaxed-energy-fcc-crystal-npt",
"tag:staff@noreply.openkim.org,2015-05-26:property/stacking-fault-relaxed-energy-curve-fcc-crystal-npt",
"tag:staff@noreply.openkim.org,2015-05-26:property/gamma-surface-relaxed-fcc-crystal-npt"
],
"publication-year": "2019",
"simulator-name": "LAMMPS",
"source-citations": [
{
"author": "Bernstein, N. and Tadmor, E. B.",
"doi": "10.1103/PhysRevB.69.094116",
"issue": "9",
"journal": "Physical Review B",
"month": "Mar",
"numpages": "10",
"pages": "094116",
"publisher": "American Physical Society",
"recordkey": "TD_228501831190_002a",
"recordtype": "article",
"title": "Tight-binding calculations of stacking energies and twinnability in fcc metals",
"volume": "69"
}
],
"title": "Stacking and twinning fault energies of an fcc lattice at zero temperature and pressure v002",
"created_on": "2019-07-12 16:06:32.134989"
},
{
"extended-id": "LatticeConstant2DHexagonalEnergy__TD_034540307932_002",
"short-id": "TD_034540307932_002",
"kimid-prefix": "LatticeConstant2DHexagonalEnergy",
"kimid-typecode": "td",
"kimid-number": "034540307932",
"kimid-version": "002",
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"abstract": "Empirical databases of crystal structures and thermodynamic properties are fundamental tools for materials research. Recent rapid proliferation of computational data on materials properties presents the possibility to complement and extend the databases where the experimental data is lacking or difficult to obtain. Enhanced repositories that integrate both computational and empirical approaches open novel opportunities for structure discovery and optimization, including uncovering of unsuspected compounds, metastable structures and correlations between various characteristics. The practical realization of these opportunities depends on a systematic compilation and classification of the generated data in addition to an accessible interface for the materials science community. In this paper we present an extensive repository, aflowlib.org, comprising phase-diagrams, electronic structure and magnetic properties, generated by the high-throughput framework AFLOW. This continuously updated compilation currently contains over 150,000 thermodynamic entries for alloys, covering the entire composition range of more than 650 binary systems, 13,000 electronic structure analyses of inorganic compounds, and 50,000 entries for novel potential magnetic and spintronics systems. The repository is available for the scientific community on the website of the materials research consortium, aflowlib.org.",
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"abstract": "The realization of novel technological opportunities given by computational and autonomous materials design requires efficient and effective frameworks. For more than two decades, aflow++ (Automatic-Flow Framework for Materials Discovery) has provided an interconnected collection of algorithms and workflows to address this challenge. This article contains an overview of the software and some of its most heavily-used functionalities, including algorithmic details, standards, and examples. Key thrusts are highlighted: the calculation of structural, electronic, thermodynamic, and thermomechanical properties in addition to the modeling of complex materials, such as high-entropy ceramics and bulk metallic glasses. The aflow++ software prioritizes interoperability, minimizing the number of independent parameters and tolerances. It ensures consistency of results across property sets \u2014 facilitating machine learning studies. The software also features various validation schemes, offering real-time quality assurance for data generated in a high-throughput fashion. Altogether, these considerations contribute to the development of large and reliable materials databases that can ultimately deliver future materials systems.",
"author": "Oses, Corey and Esters, Marco and Hicks, David and Divilov, Simon and Eckert, Hagen and Friedrich, Rico and Mehl, Michael J. and Smolyanyuk, Andriy and Campilongo, Xiomara and {van de Walle}, Axel and Schroers, Jan and Kusne, A. Gilad and Takeuchi, Ichiro and Zurek, Eva and Nardelli, Marco Buongiorno and Fornari, Marco and Lederer, Yoav and Levy, Ohad and Toher, Cormac and Curtarolo, Stefano",
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"url": "https://www.sciencedirect.com/science/article/pii/S0927025622006000",
"volume": "217",
"year": "2023"
}
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