cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.114363.v1/t21
title: "Table 21" of "Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed lower limit on WIMP-nucleon cross section at 90% CL as a function of m(WIMP), assuming Higgs-portal scenario with Scalar WIMP.
description: No data abstract available.
DOI: 10.17182/hepdata.114363.v1/t22
title: "Table 22" of "Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed lower limit on WIMP-nucleon cross section at 90% CL as a function of m(WIMP), assuming Higgs-portal scenario with Majorana WIMP.
description: No data abstract available.
DOI: 10.5281/zenodo.17209571
title: Data for "G6-1.5K-MCB: Marine Cloud Brightening Scenario design for the Geoengineering Model Intercomparison Project (GeoMIP)"

description: Data and analysis code for "G6-1.5K-MCB: Marine Cloud Brightening Scenario design for the Geoengineering Model Intercomparison Project (GeoMIP)", a manuscript under review at Geoscientific Model Development. 

File descriptions:



e3smv2_cases.zip : Case directory with configuration files for E3SMv2 G6-1.5K-MCB simulation and netCDF file storing the SSA emission distribution in the simulation.

cesm2_cases.zip : Case directories with configuration files for CESM2 G6-1.5K-MCB simulations and netCDF files storing the SSA emission distribution in the simulations.

G6-1.5K-MCB Figure notebook.ipynb : Jupyter notebook with code to generate figures used in manuscript

plotting_utils.py ; aprp.py : Python scripts including functions used by Jupyter notebook

mcb_simulation_info.json : JSON file with information on simulation names and MCB emission regions used by Jupyter notebook

grid_info.tar.gz : netCDF files with latitude, longitude, area, and land fraction information for the three ESMs used in this manuscript

ControlLog_{CASENAME}.txt : text files logging emission rates used in each MCB controller simulation

netcdf_files_for_g6mcb.tar.gz : Tarball containing netCDF data outputs from CESM2, UKESM1, and E3SMv2. Included variables are those required to generate files in the Jupyter notebook.


Steps to reproduce CESM2 simulations



Install CESM2 to machine from https://github.com/ESCOMP/CESM using tag release-cesm2.1.5-0-g7a6c5b0

copy cesm2_cases/namelist_definition.xml to CESM2ROOT/components/cam/bld/namelist_files/

Create a new BSSP245 case

Copy case files from cesm2_cases/BSSP245.G6-1.5K-MCB.massbal.001 including:



user_nl_cam

SourceMods/

controller/



Edit mcb_filename in user_nl_cam to point to the MCB SSA emission file

Remove controller/ControlLog*

Build and run simulations


Steps to reproduce E3SMv2 simulations



Install E3SMv2 to machine from https://github.com/ESCOMP/CESM using tag archive/v2-narrm-perf-study-35-gb1987633be

copy e3smv2_cases/namelist_definition.xml to E3SM2ROOT/components/eam/bld/namelist_files/

Create a new WCYCLSSP585 case

Copy case files from e3smv2_cases/WCYCLSSP245.G6-1.5K-MCB.massbal.001 including:



user_nl_eam

SourceMods/

controller/



Edit mcb_filename in user_nl_eam to point to the MCB SSA emission file

Remove controller/ControlLog*

Build and run simulations
DOI: 10.5281/zenodo.17525291
title: Data for "G6-1.5K-MCB: Marine Cloud Brightening Scenario design for the Geoengineering Model Intercomparison Project (GeoMIP)"

description: Data and analysis code for "G6-1.5K-MCB: Marine Cloud Brightening Scenario design for the Geoengineering Model Intercomparison Project (GeoMIP)", a manuscript under review at Geoscientific Model Development. 

File descriptions:



e3smv2_cases.zip : Case directory with configuration files for E3SMv2 G6-1.5K-MCB simulation and netCDF file storing the SSA emission distribution in the simulation.

cesm2_cases.zip : Case directories with configuration files for CESM2 G6-1.5K-MCB simulations and netCDF files storing the SSA emission distribution in the simulations.

G6-1.5K-MCB Figure notebook.ipynb : Jupyter notebook with code to generate figures used in manuscript

plotting_utils.py ; aprp.py : Python scripts including functions used by Jupyter notebook

mcb_simulation_info.json : JSON file with information on simulation names and MCB emission regions used by Jupyter notebook

grid_info.tar.gz : netCDF files with latitude, longitude, area, and land fraction information for the three ESMs used in this manuscript

ControlLog_{CASENAME}.txt : text files logging emission rates used in each MCB controller simulation

netcdf_files_for_g6mcb.tar.gz : Tarball containing netCDF data outputs from CESM2, UKESM1, and E3SMv2. Included variables are those required to generate files in the Jupyter notebook.


Steps to reproduce CESM2 simulations



Install CESM2 to machine from https://github.com/ESCOMP/CESM using tag release-cesm2.1.5-0-g7a6c5b0

copy cesm2_cases/namelist_definition.xml to CESM2ROOT/components/cam/bld/namelist_files/

Create a new BSSP245 case

Copy case files from cesm2_cases/BSSP245.G6-1.5K-MCB.massbal.001 including:



user_nl_cam

SourceMods/

controller/



Edit mcb_filename in user_nl_cam to point to the MCB SSA emission file

Remove controller/ControlLog*

Build and run simulations


Steps to reproduce E3SMv2 simulations



Install E3SMv2 to machine from https://github.com/ESCOMP/CESM using tag archive/v2-narrm-perf-study-35-gb1987633be

copy e3smv2_cases/namelist_definition.xml to E3SM2ROOT/components/eam/bld/namelist_files/

Create a new WCYCLSSP585 case

Copy case files from e3smv2_cases/WCYCLSSP245.G6-1.5K-MCB.massbal.001 including:



user_nl_eam

SourceMods/

controller/



Edit mcb_filename in user_nl_eam to point to the MCB SSA emission file

Remove controller/ControlLog*

Build and run simulations
DOI: 10.17182/hepdata.114363.v1/t10
title: "Table 10" of "Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The observed exclusion contours as a function of (m(H), tan($\beta$)), with sin($\theta$) = 0.35)
description: No data abstract available.
DOI: 10.17182/hepdata.114363.v1/t23
title: "Table 23" of "Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed lower limit on the spin-dependent WIMP–proton scattering cross-section.
description: No data abstract available.
DOI: 10.17182/hepdata.114363.v1/t24
title: "Table 24" of "Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed lower limit on the spin-independent WIMP–nucleon scattering cross-section.
description: No data abstract available.
DOI: 10.17182/hepdata.114363.v1/t26
title: "Table 26" of "Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Cutflow of unweighted and weighted events of $ZH$ signals in the muon channel.
description: No data abstract available.
DOI: 10.17182/hepdata.114363.v1/t27
title: "Table 27" of "Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Cutflow of unweighted and weighted events of DM signals (simplified DM axial-vector with m(med) = 900 GeV and m($\chi$) = 40 GeV, 2HDM+$a$ signal with m(A) = 600 GeV, m(a) = 400 GeV, tan($\beta$) = 1.0 and m($\chi$) = 10 GeV) in the electron channel.
description: No data abstract available.
DOI: 10.17182/hepdata.114363.v1/t28
title: "Table 28" of "Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Cutflow of unweighted and weighted events of DM signals (simplified DM axial-vector with m(med) = 900 GeV and m($\chi$) = 40 GeV, 2HDM+$a$ signal with m(A) = 600 GeV, m(a) = 400 GeV, tan($\beta$) = 1.0 and m($\chi$) = 10 GeV) in the muon channel.
description: No data abstract available.
DOI: 10.17182/hepdata.114363.v1/t25
title: "Table 25" of "Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Cutflow of unweighted and weighted events of $ZH$ signals in the electron channel.
description: No data abstract available.
DOI: 10.17182/hepdata.114364.v1/t1
title: "Table 1" of "Measurements of the associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s}$ = 8 TeV"

description: Signal yields after background subtraction, efficiency*acceptance correction factors, and cross section measurements for the four channels (W decay to muon or electron and charm identification via muon or secondary vertex inside a jet).
description: Measurements of the associated production of a W boson and a charm (c) quark in proton-proton collisions at a centre-of-mass energy of 8 TeV is reported. The analysis uses a data sample corresponding to a total integrated luminosity of 19.7 {\rm fb}$^{-1}$ collected by theCMS detector at the LHC. The W bosons are identified through their leptonic decays to an electron or a muon, and a neutrino. Charm quark jets are selectedusing distinctive signatures of charm hadron decays.The product of the cross section and branching fraction $ \sigma({\rm pp} \rightarrow {\rm W + c + X}) B({\rm W}\rightarrow \ell \nu)$, where $\ell =$ e or $\mu$, and the cross section ratio $ \sigma({\rm pp} \rightarrow {\rm W^+ + \bar{c} + X}) / \sigma( {\rm pp} \rightarrow {\rm W^- + c + X}) $ are measured inclusively and differentially as functions of the absolute pseudorapidity and of the transverse momentum of the lepton from the W boson decay.The results are compared with theoretical predictions.The impact of these measurements on the determination of the strange quark distribution is assessed.
DOI: 10.17182/hepdata.114364.v1/t2
title: "Table 2" of "Measurements of the associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s}$ = 8 TeV"

description: Measured production cross sections $\sigma(W^+ + \overline{c})$, $\sigma(W^- + c)$ and their ratio.
description: Measurements of the associated production of a W boson and a charm (c) quark in proton-proton collisions at a centre-of-mass energy of 8 TeV is reported. The analysis uses a data sample corresponding to a total integrated luminosity of 19.7 {\rm fb}$^{-1}$ collected by theCMS detector at the LHC. The W bosons are identified through their leptonic decays to an electron or a muon, and a neutrino. Charm quark jets are selectedusing distinctive signatures of charm hadron decays.The product of the cross section and branching fraction $ \sigma({\rm pp} \rightarrow {\rm W + c + X}) B({\rm W}\rightarrow \ell \nu)$, where $\ell =$ e or $\mu$, and the cross section ratio $ \sigma({\rm pp} \rightarrow {\rm W^+ + \bar{c} + X}) / \sigma( {\rm pp} \rightarrow {\rm W^- + c + X}) $ are measured inclusively and differentially as functions of the absolute pseudorapidity and of the transverse momentum of the lepton from the W boson decay.The results are compared with theoretical predictions.The impact of these measurements on the determination of the strange quark distribution is assessed.
DOI: 10.17182/hepdata.114364.v1/t3
title: "Table 3" of "Measurements of the associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s}$ = 8 TeV"

description: Measured diferential cross sections $\sigma(W^- + c) + \sigma(W^+ + \overline{c})$ as a function of the absolute value of the pseudorapidity of the lepton from the W decay.
description: Measurements of the associated production of a W boson and a charm (c) quark in proton-proton collisions at a centre-of-mass energy of 8 TeV is reported. The analysis uses a data sample corresponding to a total integrated luminosity of 19.7 {\rm fb}$^{-1}$ collected by theCMS detector at the LHC. The W bosons are identified through their leptonic decays to an electron or a muon, and a neutrino. Charm quark jets are selectedusing distinctive signatures of charm hadron decays.The product of the cross section and branching fraction $ \sigma({\rm pp} \rightarrow {\rm W + c + X}) B({\rm W}\rightarrow \ell \nu)$, where $\ell =$ e or $\mu$, and the cross section ratio $ \sigma({\rm pp} \rightarrow {\rm W^+ + \bar{c} + X}) / \sigma( {\rm pp} \rightarrow {\rm W^- + c + X}) $ are measured inclusively and differentially as functions of the absolute pseudorapidity and of the transverse momentum of the lepton from the W boson decay.The results are compared with theoretical predictions.The impact of these measurements on the determination of the strange quark distribution is assessed.
DOI: 10.17182/hepdata.114364.v1/t4
title: "Table 4" of "Measurements of the associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s}$ = 8 TeV"

description: Measured diferential cross sections as a function of the transverse momentum of the lepton from the W decay.
description: Measurements of the associated production of a W boson and a charm (c) quark in proton-proton collisions at a centre-of-mass energy of 8 TeV is reported. The analysis uses a data sample corresponding to a total integrated luminosity of 19.7 {\rm fb}$^{-1}$ collected by theCMS detector at the LHC. The W bosons are identified through their leptonic decays to an electron or a muon, and a neutrino. Charm quark jets are selectedusing distinctive signatures of charm hadron decays.The product of the cross section and branching fraction $ \sigma({\rm pp} \rightarrow {\rm W + c + X}) B({\rm W}\rightarrow \ell \nu)$, where $\ell =$ e or $\mu$, and the cross section ratio $ \sigma({\rm pp} \rightarrow {\rm W^+ + \bar{c} + X}) / \sigma( {\rm pp} \rightarrow {\rm W^- + c + X}) $ are measured inclusively and differentially as functions of the absolute pseudorapidity and of the transverse momentum of the lepton from the W boson decay.The results are compared with theoretical predictions.The impact of these measurements on the determination of the strange quark distribution is assessed.
DOI: 10.17182/hepdata.114364.v1/t5
title: "Table 5" of "Measurements of the associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s}$ = 8 TeV"

description: Measured diferential cross sections ratio $R=\sigma(W^+ + \overline{c}) / \sigma(W^- + c)$ as a function of the absolute value of the pseudorapidity of the lepton from the W decay.
description: Measurements of the associated production of a W boson and a charm (c) quark in proton-proton collisions at a centre-of-mass energy of 8 TeV is reported. The analysis uses a data sample corresponding to a total integrated luminosity of 19.7 {\rm fb}$^{-1}$ collected by theCMS detector at the LHC. The W bosons are identified through their leptonic decays to an electron or a muon, and a neutrino. Charm quark jets are selectedusing distinctive signatures of charm hadron decays.The product of the cross section and branching fraction $ \sigma({\rm pp} \rightarrow {\rm W + c + X}) B({\rm W}\rightarrow \ell \nu)$, where $\ell =$ e or $\mu$, and the cross section ratio $ \sigma({\rm pp} \rightarrow {\rm W^+ + \bar{c} + X}) / \sigma( {\rm pp} \rightarrow {\rm W^- + c + X}) $ are measured inclusively and differentially as functions of the absolute pseudorapidity and of the transverse momentum of the lepton from the W boson decay.The results are compared with theoretical predictions.The impact of these measurements on the determination of the strange quark distribution is assessed.
DOI: 10.25549/vercoutere-ouc110611141
title: Abstract pencil sketch

description: Sketch of indistinguishable objects. OT notes on reverse side: seemed very tense
DOI: 10.15468/dl.4a3bu2
title: Occurrence Download

description: A dataset containing 2 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((-94.19666 -3.58488,-58.80334 -3.58488,-58.80334 10.58488,-94.19666 10.58488,-94.19666 -3.58488))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Brasso-Cattleya"
 ]
}

 The dataset includes 2 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015939-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.114364.v1/t6
title: "Table 6" of "Measurements of the associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s}$ = 8 TeV"

description: Measured diferential cross sections ratio $R=\sigma(W^+ + \overline{c}) / \sigma(W^- + c)$ as a function of the transverse momentum of the lepton from the W decay.
description: Measurements of the associated production of a W boson and a charm (c) quark in proton-proton collisions at a centre-of-mass energy of 8 TeV is reported. The analysis uses a data sample corresponding to a total integrated luminosity of 19.7 {\rm fb}$^{-1}$ collected by theCMS detector at the LHC. The W bosons are identified through their leptonic decays to an electron or a muon, and a neutrino. Charm quark jets are selectedusing distinctive signatures of charm hadron decays.The product of the cross section and branching fraction $ \sigma({\rm pp} \rightarrow {\rm W + c + X}) B({\rm W}\rightarrow \ell \nu)$, where $\ell =$ e or $\mu$, and the cross section ratio $ \sigma({\rm pp} \rightarrow {\rm W^+ + \bar{c} + X}) / \sigma( {\rm pp} \rightarrow {\rm W^- + c + X}) $ are measured inclusively and differentially as functions of the absolute pseudorapidity and of the transverse momentum of the lepton from the W boson decay.The results are compared with theoretical predictions.The impact of these measurements on the determination of the strange quark distribution is assessed.
DOI: 10.17182/hepdata.114365.v1/t1
title: "$1\sigma$ Limits" of "Updated MiniBooNE Neutrino Oscillation Results with Increased Data and New Background Studies"

description: The frequentist $1\sigma$ confidence region in $\sin^2(2\theta)$ $\Delta m^2$ for a 2-neutrino muon-to-electron oscillation fit.
description: The MiniBooNE experiment at Fermilab reports a total excess of $638.0\pm 132.8$ electron-like events ($4.8\sigma$) from a data sample corresponding to $18.75\times 10^{20}$ protons-on-target in neutrino mode, which is a $46\%$ increase in the data sample with respect to previously published results, and $11.27\times 10^{20}$ protons-on-target in antineutrino mode. The additional statistics allow several studies to address questions on the source of the excess. First, we provide two-dimensional plots in visible energy and cosine of the angle of the outgoing lepton, which can provide valuable input to models for the event excess. Second, we test whether the excess may arise from photons that enter the detector from external events or photons exiting the detector from $\pi_0$ decays in two model independent ways. Beam timing information shows that almost all of the excess is in time with neutrinos that interact in the detector. The radius distribution shows that the excess is distributed throughout the volume, while tighter cuts on the fiducial volume increase the significance of the excess. We conclude that models of the event excess based on entering and exiting photons are disfavored.

The data release is intended to enable the oscillation fit for three different data-set combinations, the neutrino-mode data fit, the antineutrino-mode data fit, and the combined neutrino- plus antineutrino-mode data fit. In all cases the data is fit above a reconstructed neutrino energy of $200~\text{MeV}$. The neutrino-mode and the combined fit are released for the first time in conjunction with the 2020 neutrino oscillation paper (arXiv:2006.16883), while the antineutrino-mode fit is a re-release of the information from the 2018 neutrino oscillation paper (arXiv:1207.4809).

Files and numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/nue/). Original data release files are available as additional resources.
DOI: 10.17182/hepdata.114365.v1/t2
title: "$90\%$ Limits" of "Updated MiniBooNE Neutrino Oscillation Results with Increased Data and New Background Studies"

description: The frequentist $90\%$ confidence region in $\sin^2(2\theta)$ $\Delta m^2$ for a 2-neutrino muon-to-electron oscillation fit.
description: The MiniBooNE experiment at Fermilab reports a total excess of $638.0\pm 132.8$ electron-like events ($4.8\sigma$) from a data sample corresponding to $18.75\times 10^{20}$ protons-on-target in neutrino mode, which is a $46\%$ increase in the data sample with respect to previously published results, and $11.27\times 10^{20}$ protons-on-target in antineutrino mode. The additional statistics allow several studies to address questions on the source of the excess. First, we provide two-dimensional plots in visible energy and cosine of the angle of the outgoing lepton, which can provide valuable input to models for the event excess. Second, we test whether the excess may arise from photons that enter the detector from external events or photons exiting the detector from $\pi_0$ decays in two model independent ways. Beam timing information shows that almost all of the excess is in time with neutrinos that interact in the detector. The radius distribution shows that the excess is distributed throughout the volume, while tighter cuts on the fiducial volume increase the significance of the excess. We conclude that models of the event excess based on entering and exiting photons are disfavored.

The data release is intended to enable the oscillation fit for three different data-set combinations, the neutrino-mode data fit, the antineutrino-mode data fit, and the combined neutrino- plus antineutrino-mode data fit. In all cases the data is fit above a reconstructed neutrino energy of $200~\text{MeV}$. The neutrino-mode and the combined fit are released for the first time in conjunction with the 2020 neutrino oscillation paper (arXiv:2006.16883), while the antineutrino-mode fit is a re-release of the information from the 2018 neutrino oscillation paper (arXiv:1207.4809).

Files and numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/nue/). Original data release files are available as additional resources.