cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.15468/dl.pb78uu
title: Occurrence Download

description: A dataset containing 10 records in GBIF matching the query:
SELECT scientificName, eventDate
 FROM occurrence
 WHERE "year" &gt;= 2020
 LIMIT 10

 The dataset's 10 records were derived from 25737 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0031013-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.6084/m9.figshare.29109194
title: CTCF_diff_2

description: NU1 cells Chipseq data
DOI: 10.15468/dl.ny8cjj
title: Occurrence Download

description: A dataset containing 22870 species occurrences available in GBIF matching the query:
{
 "and" : [
 "CoordinateUncertaintyInMeters 0.0-5090.0",
 "DistanceFromCentroidInMeters is greater than or equal to 500.0",
 "Geometry POLYGON((-2.09416 44.9102,4.20065 39.13996,25.06678 34.53542,55.72485 35.11828,54.67571 59.30667,19.70454 70.90545,3.79265 61.69637,5.83264 56.39241,3.38465 54.76042,1.98581 50.97188,-2.32731 50.44731,-6.05756 47.88275,-2.09416 44.9102))",
 "HasCoordinate is true",
 "OccurrenceStatus is Present",
 "TaxonKey is Pelophylax lessonae (Camerano, 1882)",
 "VerbatimScientificName is Pelophylax lessonae",
 "Year 2000-2024"
 ]
}

 The dataset includes 22870 records from 15 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0009557-250515123054153/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.6075/j0zc838s
title: Airborne radio occultation observations retrieved during atmospheric river reconnaissance 2018 field campaign, version 1. In Global Navigation Satellite System (GNSS) Airborne Radio Occultation (ARO) Observations from the Atmospheric River Reconnaissance Field Campaigns

description: Multi-GNSS airborne radio occultation observations were retrieved from the NOAA G-IV aircraft during the 2018 atmospheric river reconnaissance campaign.
description: NetCDF version number: netcdf4_classic (4.9.2).

Processing algorithm and data format version: 0003.0026.
DOI: 10.6075/j0tm7bhm
title: Airborne radio occultation observations retrieved during atmospheric river reconnaissance 2019 field campaign, version 1. In Global Navigation Satellite System (GNSS) Airborne Radio Occultation (ARO) Observations from the Atmospheric River Reconnaissance Field Campaigns

description: Multi-GNSS airborne radio occultation observations were retrieved from the NOAA G-IV aircraft during the 2019 atmospheric river reconnaissance campaign.
description: NetCDF version number: netcdf4_classic (4.9.2).

Processing algorithm and data format version: 0003.0026.
DOI: 10.6075/j0k35v1f
title: Airborne radio occultation observations retrieved during atmospheric river reconnaissance 2021 field campaign, version 1. In Global Navigation Satellite System (GNSS) Airborne Radio Occultation (ARO) Observations from the Atmospheric River Reconnaissance Field Campaigns

description: Multi-GNSS airborne radio occultation observations were retrieved from the NOAA G-IV aircraft during the 2021 atmospheric river reconnaissance campaign.
description: NetCDF version number: netcdf4_classic (4.9.2).

Processing algorithm and data format version: 0003.0026.
DOI: 10.6075/j0pv6krf
title: Airborne radio occultation observations retrieved during atmospheric river reconnaissance 2020 campaign, version 1. In Global Navigation Satellite System (GNSS) Airborne Radio Occultation (ARO) Observations from the Atmospheric River Reconnaissance Field Campaigns

description: Multi-GNSS airborne radio occultation observations were retrieved from the NOAA G-IV aircraft during the 2020 atmospheric river reconnaissance campaign.
description: NetCDF version number: netcdf4_classic (4.9.2).

Processing algorithm and data format version: 0003.0026.
DOI: 10.6075/j09p321j
title: Airborne radio occultation observations retrieved during atmospheric river reconnaissance 2023 field campaign, version 1. In Global Navigation Satellite System (GNSS) Airborne Radio Occultation (ARO) Observations from the Atmospheric River Reconnaissance Field Campaigns

description: NetCDF version number: netcdf4_classic (4.9.2).

Processing algorithm and data format version: 0003.0026.
description: Multi-GNSS airborne radio occultation observations were retrieved from the NOAA G-IV and AFRC WC-130s aircraft during the 2023 atmospheric river reconnaissance campaign.
DOI: 10.6075/j0348krp
title: Global Navigation Satellite System (GNSS) Airborne Radio Occultation (ARO) Observations from the Atmospheric River Reconnaissance Field Campaigns

description: The airborne radio occultation (ARO) technique is based on precise measurements of Global Navigation Satellite System (GNSS) signal delays collected from a receiver onboard an aircraft as GNSS satellites set or rise. The excess signal delay induced by propagation through the atmosphere can be converted to ray path refractive bending, which is further interpreted in terms of the refractive index, pressure, temperature, and moisture of a stratified atmosphere. ARO inherits the advantages of high vertical resolution and all-weather capability of spaceborne RO observations and has the additional advantage of continuous and dense sampling of the targeted storm area. The horizontal drift of the representative tangent point retrieval coordinate is an important characteristic of ARO profiles, which greatly extends the sensing area from underneath the aircraft to both sides of the flight track (up to 500 km). This ARO dataset complements the dropsonde, flight level meteorological, and Doppler radar observations by providing simultaneous measurements at no additional expendable cost in the reconnaissance flights. Atmospheric Rivers (ARs) are narrow filaments of high moisture flux responsible for most of the horizontal transport of water vapor from the tropics to mid-latitudes. Improving forecasts of ARs through numerical weather prediction (NWP) is important for increasing the resilience of the western US to flooding and droughts. The AR Reconnaissance (AR Recon) program is a collaborative effort of the Center for Western Weather and Water Extremes (CW3E) and the National Oceanic and Atmospheric Administration (NOAA) National Center for Environmental Prediction (NCEP), involving several domestic and international partners, that focuses on atmospheric dynamics, the predictability of ARs, airborne instrumentation, and data assimilation in numerical weather modeling.
DOI: 10.6075/j0fb53bj
title: Airborne radio occultation observations retrieved during atmospheric river reconnaissance 2022 field campaign, version 1. In Global Navigation Satellite System (GNSS) Airborne Radio Occultation (ARO) Observations from the Atmospheric River Reconnaissance Field Campaigns

description: NetCDF version number: netcdf4_classic (4.9.2).

Processing algorithm and data format version: 0003.0026.
description: Multi-GNSS airborne radio occultation observations were retrieved from the NOAA G-IV aircraft during the 2022 atmospheric river reconnaissance campaign.
DOI: 10.17182/hepdata.77905.v1/t54
title: "Table 54" of "Azimuthally differential pion femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV"

description: An estimate of freeze-out eccentricity $2
 R^{2}_{\mathrm side,2}/R^{2}_{\mathrm side,0}$ for different $k_{\mathrm T}$ ranges vs.
 initial state eccentricity from Monte Carlo Glauber
 model for six centrality ranges, 0-5%,
 5-10%, 10-20%, 20-30%, 30-40%, and 40-50%.
description: No description provided.
DOI: 10.17182/hepdata.77905.v1/t55
title: "Table 55" of "Azimuthally differential pion femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV"

description: An estimate of freeze-out eccentricity $2
 R^{2}_{\mathrm side,2}/R^{2}_{\mathrm side,0}$ for different $k_{\mathrm T}$ ranges vs.
 initial state eccentricity from Monte Carlo Glauber
 model for six centrality ranges, 0-5%,
 5-10%, 10-20%, 20-30%, 30-40%, and 40-50%.
description: No description provided.
DOI: 10.17182/hepdata.79482.v1/t4
title: "Table 4" of "Constraining the magnitude of the Chiral Magnetic Effect with Event Shape Engineering in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76$ TeV"

description: $v_2\{EP\}$ with $|\Delta\eta| &gt; 2.0$ as a function of centrality for shape selected events (20-30% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
description: In ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow $v_2$ reflects fluctuations in the shape of the initial state of the system. This allows us to systematically study events corresponding to the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two- and three-particle correlations in Pb—Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV. The two-particle correlator $\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$, calculated for different combinations of charges $\alpha$ and $\beta$, is almost independent of $v_2$ (for a given centrality), while the three-particle correlator $\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_2) \rangle$ scales almost linearly both with the event $v_2$ and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on $v_2$ points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.
DOI: 10.17182/hepdata.79482.v1/t5
title: "Table 5" of "Constraining the magnitude of the Chiral Magnetic Effect with Event Shape Engineering in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76$ TeV"

description: $v_2\{EP\}$ with $|\Delta\eta| &gt; 2.0$ as a function of centrality for shape selected events (30-40% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
description: In ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow $v_2$ reflects fluctuations in the shape of the initial state of the system. This allows us to systematically study events corresponding to the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two- and three-particle correlations in Pb—Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV. The two-particle correlator $\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$, calculated for different combinations of charges $\alpha$ and $\beta$, is almost independent of $v_2$ (for a given centrality), while the three-particle correlator $\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_2) \rangle$ scales almost linearly both with the event $v_2$ and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on $v_2$ points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.
DOI: 10.5064/f6g2petf/puqcrx
title: Moore-et-al_MD_0321_Governor Larry Hogan - Official Website for the Governor of Maryland_24.pdf
DOI: 10.17182/hepdata.72903.v1/t1
title: "Table 1" of "Centrality dependence of charged jet production in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: pp reference spectrum, obtained by scaling down the measured charged jets at 7 TeV to 5.02 TeV for R = 0.2 jets.
description: CERN-LHC. Measurements of charged jet production as a function of centrality are presented for p-Pb collisions recorded at $\sqrt{s_{\rm NN}} = 5.02$ TeV with the ALICE detector. Centrality classes are determined via the energy deposit in neutron calorimeters at zero degree, close to the beam direction, to minimise dynamical biases of the selection. The corresponding number of participants or binary nucleon-nucleon collisions is determined based on the particle production in the Pb-going rapidity region. Jets have been reconstructed in the central rapidity region from charged particles with the anti-$k_{\rm T}$ algorithm for resolution parameters $R = 0.2$ and $R = 0.4$ in the transverse momentum range 20 to 120 GeV/$c$. The reconstructed jet momentum and yields have been corrected for detector effects and underlying-event background.
DOI: 10.17182/hepdata.72903.v1/t2
title: "Table 2" of "Centrality dependence of charged jet production in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: $p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 0-20%.
description: CERN-LHC. Measurements of charged jet production as a function of centrality are presented for p-Pb collisions recorded at $\sqrt{s_{\rm NN}} = 5.02$ TeV with the ALICE detector. Centrality classes are determined via the energy deposit in neutron calorimeters at zero degree, close to the beam direction, to minimise dynamical biases of the selection. The corresponding number of participants or binary nucleon-nucleon collisions is determined based on the particle production in the Pb-going rapidity region. Jets have been reconstructed in the central rapidity region from charged particles with the anti-$k_{\rm T}$ algorithm for resolution parameters $R = 0.2$ and $R = 0.4$ in the transverse momentum range 20 to 120 GeV/$c$. The reconstructed jet momentum and yields have been corrected for detector effects and underlying-event background.
DOI: 10.17182/hepdata.72903.v1/t3
title: "Table 3" of "Centrality dependence of charged jet production in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: $p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 20-40%.
description: CERN-LHC. Measurements of charged jet production as a function of centrality are presented for p-Pb collisions recorded at $\sqrt{s_{\rm NN}} = 5.02$ TeV with the ALICE detector. Centrality classes are determined via the energy deposit in neutron calorimeters at zero degree, close to the beam direction, to minimise dynamical biases of the selection. The corresponding number of participants or binary nucleon-nucleon collisions is determined based on the particle production in the Pb-going rapidity region. Jets have been reconstructed in the central rapidity region from charged particles with the anti-$k_{\rm T}$ algorithm for resolution parameters $R = 0.2$ and $R = 0.4$ in the transverse momentum range 20 to 120 GeV/$c$. The reconstructed jet momentum and yields have been corrected for detector effects and underlying-event background.
DOI: 10.17182/hepdata.72903.v1/t4
title: "Table 4" of "Centrality dependence of charged jet production in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: $p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector, centrality 40-60%.
description: CERN-LHC. Measurements of charged jet production as a function of centrality are presented for p-Pb collisions recorded at $\sqrt{s_{\rm NN}} = 5.02$ TeV with the ALICE detector. Centrality classes are determined via the energy deposit in neutron calorimeters at zero degree, close to the beam direction, to minimise dynamical biases of the selection. The corresponding number of participants or binary nucleon-nucleon collisions is determined based on the particle production in the Pb-going rapidity region. Jets have been reconstructed in the central rapidity region from charged particles with the anti-$k_{\rm T}$ algorithm for resolution parameters $R = 0.2$ and $R = 0.4$ in the transverse momentum range 20 to 120 GeV/$c$. The reconstructed jet momentum and yields have been corrected for detector effects and underlying-event background.
DOI: 10.17182/hepdata.77905.v1/t56
title: "Table 56" of "Azimuthally differential pion femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV"

description: An estimate of freeze-out eccentricity $2
 R^{2}_{\mathrm side,2}/R^{2}_{\mathrm side,0}$ for different $k_{\mathrm T}$ ranges vs.
 initial state eccentricity from Monte Carlo Glauber
 model for six centrality ranges, 0-5%,
 5-10%, 10-20%, 20-30%, 30-40%, and 40-50%.
description: No description provided.
DOI: 10.17182/hepdata.79482.v1/t6
title: "Table 6" of "Constraining the magnitude of the Chiral Magnetic Effect with Event Shape Engineering in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76$ TeV"

description: $v_2\{EP\}$ with $|\Delta\eta| &gt; 2.0$ as a function of centrality for shape selected events (40-50% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
description: In ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow $v_2$ reflects fluctuations in the shape of the initial state of the system. This allows us to systematically study events corresponding to the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two- and three-particle correlations in Pb—Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV. The two-particle correlator $\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$, calculated for different combinations of charges $\alpha$ and $\beta$, is almost independent of $v_2$ (for a given centrality), while the three-particle correlator $\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_2) \rangle$ scales almost linearly both with the event $v_2$ and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on $v_2$ points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.
DOI: 10.17182/hepdata.79482.v1/t7
title: "Table 7" of "Constraining the magnitude of the Chiral Magnetic Effect with Event Shape Engineering in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76$ TeV"

description: $v_2\{EP\}$ with $|\Delta\eta| &gt; 2.0$ as a function of centrality for shape selected events (50-60% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
description: In ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow $v_2$ reflects fluctuations in the shape of the initial state of the system. This allows us to systematically study events corresponding to the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two- and three-particle correlations in Pb—Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV. The two-particle correlator $\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$, calculated for different combinations of charges $\alpha$ and $\beta$, is almost independent of $v_2$ (for a given centrality), while the three-particle correlator $\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_2) \rangle$ scales almost linearly both with the event $v_2$ and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on $v_2$ points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.
DOI: 10.17182/hepdata.79482.v1/t8
title: "Table 8" of "Constraining the magnitude of the Chiral Magnetic Effect with Event Shape Engineering in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76$ TeV"

description: $v_2\{EP\}$ with $|\Delta\eta| &gt; 2.0$ as a function of centrality for shape selected events (60-70% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
description: In ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow $v_2$ reflects fluctuations in the shape of the initial state of the system. This allows us to systematically study events corresponding to the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two- and three-particle correlations in Pb—Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV. The two-particle correlator $\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$, calculated for different combinations of charges $\alpha$ and $\beta$, is almost independent of $v_2$ (for a given centrality), while the three-particle correlator $\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_2) \rangle$ scales almost linearly both with the event $v_2$ and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on $v_2$ points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.
DOI: 10.17182/hepdata.72903.v1/t10
title: "Table 10" of "Centrality dependence of charged jet production in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: $p_{\rm T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector, centrality 40-60%.
description: CERN-LHC. Measurements of charged jet production as a function of centrality are presented for p-Pb collisions recorded at $\sqrt{s_{\rm NN}} = 5.02$ TeV with the ALICE detector. Centrality classes are determined via the energy deposit in neutron calorimeters at zero degree, close to the beam direction, to minimise dynamical biases of the selection. The corresponding number of participants or binary nucleon-nucleon collisions is determined based on the particle production in the Pb-going rapidity region. Jets have been reconstructed in the central rapidity region from charged particles with the anti-$k_{\rm T}$ algorithm for resolution parameters $R = 0.2$ and $R = 0.4$ in the transverse momentum range 20 to 120 GeV/$c$. The reconstructed jet momentum and yields have been corrected for detector effects and underlying-event background.