cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.93879.v1/t6
title: "Figure 2f" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_3$ as a function of $p_T$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t7
title: "Figure 3a" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_2$ as a function of $p_T$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t8
title: "Figure 3b" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_2$ as a function of $p_T$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t9
title: "Figure 3c" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_2$ as a function of $p_T$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t11
title: "Figure 3e" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_3$ as a function of $p_T$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t12
title: "Figure 3f" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_3$ as a function of $p_T$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t13
title: "Figure 4a" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_2$ as a function of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t14
title: "Figure 4b" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_2$ as a function of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t15
title: "Figure 4c" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_3$ as a function of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t16
title: "Figure 4d" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_3$ as a function of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t17
title: "Figure 4e" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_2$ as a function of rapidity in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t18
title: "Figure 4f" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $v_3$ as a function of rapidity in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.17182/hepdata.93879.v1/t19
title: "Figure 5" of "Search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV using azimuthal anisotropy of prompt $\mathrm{D}^0$ and $\overline{\mathrm{D}}^0$ mesons"

description: Prompt $D^0$ meson $\Delta v_2$ as a function of rapidity in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$.
description: The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapidity-dependent difference ($\Delta v_2$) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, $v_2$) between $D^0$ ($\overline{u}c$) and $\overline{D}^0$ ($u\overline{c}$) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of $\Delta v_2$. The rapidity-averaged value is found to be $&lt;\Delta v_2&gt;=0.001\pm0.001(stat)\pm0.003(syst)$ in PbPb collisions at $\sqrt{s_{NN}}=5.02~TeV$. In addition, the influence of the collision geometry is explored by measuring the $D^0$ and $\overline{D}^0$ mesons $v_2$ and triangular flow coefficient ($v_3$) as functions of rapidity, transverse momentum ($p_T$), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt $D^0$ meson $v_2$ values is observed, while the $v_3$ is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry.
DOI: 10.15468/dl.fqdp2h
title: Occurrence Download

description: A dataset containing 2426 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Loddigesia mirabilis"
 ]
}

 The dataset includes 2426 records from 24 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015782-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.93013.v1/t1
title: "Prompt D0 without vertexing analysis, Figure 6 " of "Measurement of prompt D$^0$, D$^+$, D$^{*+}$, and D$^+_s$ production in p$-$Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$"

description: $p_{\rm{T}}$ differential cross section of prompt D0 mesons obtained from the analysis without vertexing reconstruction in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.
description: No data abstract available.
DOI: 10.17182/hepdata.93013.v1/t7
title: "D* pp reference, Figure 7 " of "Measurement of prompt D$^0$, D$^+$, D$^{*+}$, and D$^+_s$ production in p$-$Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$"

description: $p_{\rm{T}}$ differential cross section of prompt D* mesons in pp collisions at $\mathbf{\sqrt{{\textit s}}~=~5.02~TeV}$ multiplied by A=208.
description: No data abstract available.
DOI: 10.17182/hepdata.93013.v1/t6
title: "D* pPb cross section, Figure 7 " of "Measurement of prompt D$^0$, D$^+$, D$^{*+}$, and D$^+_s$ production in p$-$Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$"

description: $p_{\rm{T}}$ differential cross section of prompt D* mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.
description: No data abstract available.
DOI: 10.15468/dl.xefn5u
title: Occurrence Download

description: A dataset containing 3471 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Country is Brazil",
 "StateProvince is one of (Alagoas State, Alagoas state, alagoas, Alagoas, Maceio, Alagoas)",
 "TaxonKey is Polypodiopsida"
 ]
}

 The dataset includes 3471 records from 60 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015780-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.5281/zenodo.16545118
title: Benchmark dataset for production planning and detailed scheduling in process industries

description: This dataset is intended for research on production planning (PP) and detailed scheduling (DS) in process industries. It is derived from the Westenberger-Kallrath (WK) problem, a prominent case from the chemical process industry, and it is enhanced with additional data regarding customer due dates, sales prices, and costs factors for production, storage and raw material purchase. The size of the problem instances is determined by the customer order count.

The folder "generated-dataset" contains all generated problem instances. Each file name contains the number of customer orders and a reference if a low-margin or a high-margin price profile was applied. All text files are mapped to optimization tasks in the Excel file "overview-instance-files". An explanation on the different optimization tasks is provided in the Excel file "overview-optimization-tasks".

The folder "source-data" contains all primary data from other scientific resources, which were used in data generation process.

The folder "task1-no-prices" contains two special problem instances with 40 customer orders, following the pattern of "kallrath2002-instance-task1.txt". For one instance, the divergent material flow is de-activated, hence, it contains only linear and convergent material flows.
DOI: 10.5281/zenodo.17493292
title: Benchmark dataset for production planning and detailed scheduling in process industries

description: This dataset is intended for research on production planning (PP) and detailed scheduling (DS) in process industries. It is derived from the Westenberger-Kallrath (WK) problem, a prominent case from the chemical process industry, and it is enhanced with additional data regarding customer due dates, sales prices, and costs factors for production, storage and raw material purchase. The size of the problem instances is determined by the customer order count.

The folder "generated-dataset" contains all generated problem instances. Each file name contains the number of customer orders and a reference if a low-margin or a high-margin price profile was applied. All text files are mapped to optimization tasks in the Excel file "overview-instance-files". An explanation on the different optimization tasks is provided in the Excel file "overview-optimization-tasks".

The folder "source-data" contains all primary data from other scientific resources, which were used in data generation process.

The folder "task1-no-prices" contains two special problem instances with 40 customer orders, following the pattern of "kallrath2002-instance-task1.txt". For one instance, the divergent material flow is de-activated, hence, it contains only linear and convergent material flows.