cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.165281.v1/t7
title: "Figure 5a" of "Vector boson scattering and anomalous quartic couplings in final states with $\ellν$qq or $\ell\ell$qq plus jets using proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distributions of M(WV) for the data and post-fit backgrounds (stacked histograms), in the SRs of the electron (left) and muon (right) channels in the merged regime. The template for one signal hypothesis is shown overlaid as a red solid line. The overflow is included in the last bin. The lower panels show the ratios of the data to the pre-fit background prediction and post-fit background yield as red open squares and blue points, respectively. The gray band in the lower panels indicates the systematic component of the post-fit background uncertainty. The vertical bars on the data points represent statistical uncertainties. The last bin includes overflow.
description: A measurement is presented of the electroweak vector boson scattering production of ZV (V = W, Z) boson pairs associated with two jets in proton-proton collisions at a center-of-mass energy of 13 TeV. The data, corresponding to an integrated luminosity of 138 fb$^{-1}$, were collected at the CERN LHC with the CMS detector during the 2016--2018 data-taking period. The analysis targets final states with a pair of isolated electrons or muons from Z boson decays and three or four jets, depending on the momentum of the vector boson that decays into quarks. Signal strength is measured for events characterized by a large invariant mass of two forward jets with a wide pseudorapidity gap between them. The electroweak production of ZV in association with two jets is measured with an observed (expected) significance of 1.3 (1.8) standard deviations. A combination of the analyses of ZV channel and the previously published WV channel in the lepton plus jets final state places constraints on effective field theory parameters that describe anomalous electroweak production of WW, WZ, and ZZ boson pairs in association with two jets. Several world best limits are set on anomalous quartic gauge couplings in terms of dimension-8 standard model effective field theory operators.
DOI: 10.17182/hepdata.165281.v1/t10
title: "Measured EW ZV signal strength" of "Vector boson scattering and anomalous quartic couplings in final states with $\ellν$qq or $\ell\ell$qq plus jets using proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Measured and expected signal strength μ for EW ZV production.
description: A measurement is presented of the electroweak vector boson scattering production of ZV (V = W, Z) boson pairs associated with two jets in proton-proton collisions at a center-of-mass energy of 13 TeV. The data, corresponding to an integrated luminosity of 138 fb$^{-1}$, were collected at the CERN LHC with the CMS detector during the 2016--2018 data-taking period. The analysis targets final states with a pair of isolated electrons or muons from Z boson decays and three or four jets, depending on the momentum of the vector boson that decays into quarks. Signal strength is measured for events characterized by a large invariant mass of two forward jets with a wide pseudorapidity gap between them. The electroweak production of ZV in association with two jets is measured with an observed (expected) significance of 1.3 (1.8) standard deviations. A combination of the analyses of ZV channel and the previously published WV channel in the lepton plus jets final state places constraints on effective field theory parameters that describe anomalous electroweak production of WW, WZ, and ZZ boson pairs in association with two jets. Several world best limits are set on anomalous quartic gauge couplings in terms of dimension-8 standard model effective field theory operators.
DOI: 10.17182/hepdata.165281.v1/t8
title: "Figure 5b" of "Vector boson scattering and anomalous quartic couplings in final states with $\ellν$qq or $\ell\ell$qq plus jets using proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distributions of M(WV) for the data and post-fit backgrounds (stacked histograms), in the SRs of the electron (left) and muon (right) channels in the merged regime. The template for one signal hypothesis is shown overlaid as a red solid line. The overflow is included in the last bin. The lower panels show the ratios of the data to the pre-fit background prediction and post-fit background yield as red open squares and blue points, respectively. The gray band in the lower panels indicates the systematic component of the post-fit background uncertainty. The vertical bars on the data points represent statistical uncertainties. The last bin includes overflow.
description: A measurement is presented of the electroweak vector boson scattering production of ZV (V = W, Z) boson pairs associated with two jets in proton-proton collisions at a center-of-mass energy of 13 TeV. The data, corresponding to an integrated luminosity of 138 fb$^{-1}$, were collected at the CERN LHC with the CMS detector during the 2016--2018 data-taking period. The analysis targets final states with a pair of isolated electrons or muons from Z boson decays and three or four jets, depending on the momentum of the vector boson that decays into quarks. Signal strength is measured for events characterized by a large invariant mass of two forward jets with a wide pseudorapidity gap between them. The electroweak production of ZV in association with two jets is measured with an observed (expected) significance of 1.3 (1.8) standard deviations. A combination of the analyses of ZV channel and the previously published WV channel in the lepton plus jets final state places constraints on effective field theory parameters that describe anomalous electroweak production of WW, WZ, and ZZ boson pairs in association with two jets. Several world best limits are set on anomalous quartic gauge couplings in terms of dimension-8 standard model effective field theory operators.
DOI: 10.17182/hepdata.165281.v1/t9
title: "EFT limits on quartic operators" of "Vector boson scattering and anomalous quartic couplings in final states with $\ellν$qq or $\ell\ell$qq plus jets using proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL intervals on the parameters of quartic operators in the WV and ZV channels, and their combination.
description: A measurement is presented of the electroweak vector boson scattering production of ZV (V = W, Z) boson pairs associated with two jets in proton-proton collisions at a center-of-mass energy of 13 TeV. The data, corresponding to an integrated luminosity of 138 fb$^{-1}$, were collected at the CERN LHC with the CMS detector during the 2016--2018 data-taking period. The analysis targets final states with a pair of isolated electrons or muons from Z boson decays and three or four jets, depending on the momentum of the vector boson that decays into quarks. Signal strength is measured for events characterized by a large invariant mass of two forward jets with a wide pseudorapidity gap between them. The electroweak production of ZV in association with two jets is measured with an observed (expected) significance of 1.3 (1.8) standard deviations. A combination of the analyses of ZV channel and the previously published WV channel in the lepton plus jets final state places constraints on effective field theory parameters that describe anomalous electroweak production of WW, WZ, and ZZ boson pairs in association with two jets. Several world best limits are set on anomalous quartic gauge couplings in terms of dimension-8 standard model effective field theory operators.
DOI: 10.17182/hepdata.165429.v1/t1
title: "$W^+ \to \mu^+ \nu_{\mu}$ $d\sigma/dp_T$" of "Measurement of the $W \to μν_μ$ cross-sections as a function of the muon transverse momentum in $pp$ collisions at 5.02 TeV"

description: The measured differential cross sections ($d\sigma/dp_T$) for $W^+$. The first systematic uncertainty is statistical and the second is systematic.
description: The $pp \to W^{\pm}(\to \mu^{\pm}\nu_{\mu})X$ cross-sections are measured at a
proton-proton centre-of-mass energy $\sqrt{s} = 5.02$ TeV using a dataset
corresponding to an integrated luminosity of $100\,\mathrm{pb}^{-1}$ recorded
by the LHCb experiment.

Considering muons in the pseudorapidity range $2.2 &lt; \eta &lt; 4.4$, the
cross-sections are measured differentially in twelve intervals of muon
transverse momentum between $28 &lt; p_{T} &lt; 52$ GeV. Integrated over $p_{T}$,
the measured cross-sections are

$$
 \sigma(W^+ \to \mu^+\nu_{\mu}) = 300.9 \pm 2.4 \,(\mathrm{stat})
 \pm 3.8 \,(\mathrm{syst}) \pm 6.0 \,(\mathrm{lumi})\,\mathrm{pb},
$$

$$
 \sigma(W^- \to \mu^-\nu_{\mu}) = 236.9 \pm 2.1 \,(\mathrm{stat})
 \pm 2.7 \,(\mathrm{syst}) \pm 4.7 \,(\mathrm{lumi})\,\mathrm{pb}.
$$

These integrated results are consistent with theoretical predictions.
This analysis introduces a new method to determine the $W$ boson mass using the
measured differential cross-sections corrected for detector effects. The
measurement is performed on this statistically limited dataset as a proof of
principle and yields

$$
 m_W = 80369 \pm 130 \,(\mathrm{exp}) \pm 33 \,(\mathrm{theo})\,\mathrm{MeV}.
$$
DOI: 10.17182/hepdata.165429.v1/t2
title: "$W^- \to \mu^- \nu_{\mu}$ $d\sigma/dp_T$" of "Measurement of the $W \to μν_μ$ cross-sections as a function of the muon transverse momentum in $pp$ collisions at 5.02 TeV"

description: The measured differential cross sections ($d\sigma/dp_T$) for $W^-$. The first systematic uncertainty is statistical and the second is systematic.
description: The $pp \to W^{\pm}(\to \mu^{\pm}\nu_{\mu})X$ cross-sections are measured at a
proton-proton centre-of-mass energy $\sqrt{s} = 5.02$ TeV using a dataset
corresponding to an integrated luminosity of $100\,\mathrm{pb}^{-1}$ recorded
by the LHCb experiment.

Considering muons in the pseudorapidity range $2.2 &lt; \eta &lt; 4.4$, the
cross-sections are measured differentially in twelve intervals of muon
transverse momentum between $28 &lt; p_{T} &lt; 52$ GeV. Integrated over $p_{T}$,
the measured cross-sections are

$$
 \sigma(W^+ \to \mu^+\nu_{\mu}) = 300.9 \pm 2.4 \,(\mathrm{stat})
 \pm 3.8 \,(\mathrm{syst}) \pm 6.0 \,(\mathrm{lumi})\,\mathrm{pb},
$$

$$
 \sigma(W^- \to \mu^-\nu_{\mu}) = 236.9 \pm 2.1 \,(\mathrm{stat})
 \pm 2.7 \,(\mathrm{syst}) \pm 4.7 \,(\mathrm{lumi})\,\mathrm{pb}.
$$

These integrated results are consistent with theoretical predictions.
This analysis introduces a new method to determine the $W$ boson mass using the
measured differential cross-sections corrected for detector effects. The
measurement is performed on this statistically limited dataset as a proof of
principle and yields

$$
 m_W = 80369 \pm 130 \,(\mathrm{exp}) \pm 33 \,(\mathrm{theo})\,\mathrm{MeV}.
$$
DOI: 10.17182/hepdata.165429.v1/t3
title: "Statistical correlation matrix for $W^+$" of "Measurement of the $W \to μν_μ$ cross-sections as a function of the muon transverse momentum in $pp$ collisions at 5.02 TeV"

description: The correlation matrix corresponding to the statistical uncertainties on the differential cross-section ($d\sigma/dp_T$) fit results for $W^+$. To combine with $W^-$, use the rows and columns ordered as $W^+$ and then $W^-$. Assume no correlation in the statistical uncertainties between $W^+$ and $W^-$ (zero entries in the off-diagonal blocks).
description: The $pp \to W^{\pm}(\to \mu^{\pm}\nu_{\mu})X$ cross-sections are measured at a
proton-proton centre-of-mass energy $\sqrt{s} = 5.02$ TeV using a dataset
corresponding to an integrated luminosity of $100\,\mathrm{pb}^{-1}$ recorded
by the LHCb experiment.

Considering muons in the pseudorapidity range $2.2 &lt; \eta &lt; 4.4$, the
cross-sections are measured differentially in twelve intervals of muon
transverse momentum between $28 &lt; p_{T} &lt; 52$ GeV. Integrated over $p_{T}$,
the measured cross-sections are

$$
 \sigma(W^+ \to \mu^+\nu_{\mu}) = 300.9 \pm 2.4 \,(\mathrm{stat})
 \pm 3.8 \,(\mathrm{syst}) \pm 6.0 \,(\mathrm{lumi})\,\mathrm{pb},
$$

$$
 \sigma(W^- \to \mu^-\nu_{\mu}) = 236.9 \pm 2.1 \,(\mathrm{stat})
 \pm 2.7 \,(\mathrm{syst}) \pm 4.7 \,(\mathrm{lumi})\,\mathrm{pb}.
$$

These integrated results are consistent with theoretical predictions.
This analysis introduces a new method to determine the $W$ boson mass using the
measured differential cross-sections corrected for detector effects. The
measurement is performed on this statistically limited dataset as a proof of
principle and yields

$$
 m_W = 80369 \pm 130 \,(\mathrm{exp}) \pm 33 \,(\mathrm{theo})\,\mathrm{MeV}.
$$
DOI: 10.17182/hepdata.165429.v1/t4
title: "Statistical correlation matrix for $W^-$" of "Measurement of the $W \to μν_μ$ cross-sections as a function of the muon transverse momentum in $pp$ collisions at 5.02 TeV"

description: The correlation matrix corresponding to the statistical uncertainties on the differential cross-section ($d\sigma/dp_T$) fit results for $W^-$. To combine with $W^+$ results (Fig8a), use the rows and columns ordered as $W^+$ and then $W^-$. Assume no correlation in the statistical uncertainties between $W^+$ and $W^-$ (zero entries in the off-diagonal blocks).
description: The $pp \to W^{\pm}(\to \mu^{\pm}\nu_{\mu})X$ cross-sections are measured at a
proton-proton centre-of-mass energy $\sqrt{s} = 5.02$ TeV using a dataset
corresponding to an integrated luminosity of $100\,\mathrm{pb}^{-1}$ recorded
by the LHCb experiment.

Considering muons in the pseudorapidity range $2.2 &lt; \eta &lt; 4.4$, the
cross-sections are measured differentially in twelve intervals of muon
transverse momentum between $28 &lt; p_{T} &lt; 52$ GeV. Integrated over $p_{T}$,
the measured cross-sections are

$$
 \sigma(W^+ \to \mu^+\nu_{\mu}) = 300.9 \pm 2.4 \,(\mathrm{stat})
 \pm 3.8 \,(\mathrm{syst}) \pm 6.0 \,(\mathrm{lumi})\,\mathrm{pb},
$$

$$
 \sigma(W^- \to \mu^-\nu_{\mu}) = 236.9 \pm 2.1 \,(\mathrm{stat})
 \pm 2.7 \,(\mathrm{syst}) \pm 4.7 \,(\mathrm{lumi})\,\mathrm{pb}.
$$

These integrated results are consistent with theoretical predictions.
This analysis introduces a new method to determine the $W$ boson mass using the
measured differential cross-sections corrected for detector effects. The
measurement is performed on this statistically limited dataset as a proof of
principle and yields

$$
 m_W = 80369 \pm 130 \,(\mathrm{exp}) \pm 33 \,(\mathrm{theo})\,\mathrm{MeV}.
$$
DOI: 10.17182/hepdata.165429.v1/t5
title: "Systematic correlation matrix for $W^{\pm}$ (combined)" of "Measurement of the $W \to μν_μ$ cross-sections as a function of the muon transverse momentum in $pp$ collisions at 5.02 TeV"

description: The correlation matrix corresponding to all of the systematic uncertainties on the differential cross-section ($d\sigma/dp_T$) fit results for $W^+$ and $W^-$ combined together, with rows and columns ordered as $W^+$ and then $W^-$.
description: The $pp \to W^{\pm}(\to \mu^{\pm}\nu_{\mu})X$ cross-sections are measured at a
proton-proton centre-of-mass energy $\sqrt{s} = 5.02$ TeV using a dataset
corresponding to an integrated luminosity of $100\,\mathrm{pb}^{-1}$ recorded
by the LHCb experiment.

Considering muons in the pseudorapidity range $2.2 &lt; \eta &lt; 4.4$, the
cross-sections are measured differentially in twelve intervals of muon
transverse momentum between $28 &lt; p_{T} &lt; 52$ GeV. Integrated over $p_{T}$,
the measured cross-sections are

$$
 \sigma(W^+ \to \mu^+\nu_{\mu}) = 300.9 \pm 2.4 \,(\mathrm{stat})
 \pm 3.8 \,(\mathrm{syst}) \pm 6.0 \,(\mathrm{lumi})\,\mathrm{pb},
$$

$$
 \sigma(W^- \to \mu^-\nu_{\mu}) = 236.9 \pm 2.1 \,(\mathrm{stat})
 \pm 2.7 \,(\mathrm{syst}) \pm 4.7 \,(\mathrm{lumi})\,\mathrm{pb}.
$$

These integrated results are consistent with theoretical predictions.
This analysis introduces a new method to determine the $W$ boson mass using the
measured differential cross-sections corrected for detector effects. The
measurement is performed on this statistically limited dataset as a proof of
principle and yields

$$
 m_W = 80369 \pm 130 \,(\mathrm{exp}) \pm 33 \,(\mathrm{theo})\,\mathrm{MeV}.
$$
DOI: 10.17182/hepdata.166008.v1/t1
title: "R(J/psi) ratio of branching fractions" of "Measurement of the ratio of the B$_\mathrm{c}^+$$\to$ J/$ψ$$τ^+ν_τ$ and B$_\mathrm{c}^+$$\to$ J/$ψ$$μ^+ν_μ$ branching fractions using three-prong $τ$ lepton decays"

description: Measured R(J/psi) ratio
description: CERN-LHC-CMS. Measurement of the ratio of the $\mathrm{B}_\mathrm{c}^{+}$ to $\mathrm{J}/\psi\tau^{+}\nu$ and $\mathrm{B}_\mathrm{c}^{+}$ to $\mathrm{J}/\psi\mu\nu$ branching fractions using three-prong tau lepton decays.
DOI: 10.15468/dl.kq7y5b
title: Occurrence Download

description: A dataset containing 0 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Adoncholaimus parvus",
 "HasCoordinate is true",
 "HasGeospatialIssue is false"
 ]
}

 The dataset includes 0 records from 0 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0016069-251025141854904/datasets/export for details.
DOI: 10.17182/hepdata.166316.v1/t1
title: "Meas. 1:Forward cross section vs. $p_T^{\eta}$" of "Cross sections of $\eta$ mesons in $p$ $+$ $p$ collisions at forward rapidity at $\sqrt{s}=500$ GeV and central rapidity at $\sqrt{s}=510$ GeV"

description: The invariant differential cross section of $\eta$ mesons at forward rapidity in pp collisions at center-of-mass energy 500 GeV.
description: We present the first measurements of the forward and midrapidity $\eta$ meson cross sections from $p+p$ collisions at $\sqrt{s} = 500$ GeV and $510$ GeV, respectively. We also report the midrapidity $\eta/\pi^0$ ratio at 510 GeV. The forward cross section is measured differentially in $\eta$ meson transverse momentum ($p_T$) from 1.0 to 6.5 GeV/c for pseudorapidity $3.0 &lt; |\eta| &lt; 3.8$. The midrapidity cross section is measured from 3.5 to 44 GeV/c for pseudorapidity $|\eta| &lt; 0.35$. Both cross sections serve as critical inputs to an updated global analysis of the $\eta$ meson fragmentation functions
DOI: 10.17182/hepdata.166316.v1/t2
title: "Meas. 2:Midrapidity cross section vs. $p_T^{\eta}$" of "Cross sections of $\eta$ mesons in $p$ $+$ $p$ collisions at forward rapidity at $\sqrt{s}=500$ GeV and central rapidity at $\sqrt{s}=510$ GeV"

description: The invariant differential cross section of $\eta$ mesons at central rapidity in pp collisions at center-of-mass energy 510 GeV.
description: We present the first measurements of the forward and midrapidity $\eta$ meson cross sections from $p+p$ collisions at $\sqrt{s} = 500$ GeV and $510$ GeV, respectively. We also report the midrapidity $\eta/\pi^0$ ratio at 510 GeV. The forward cross section is measured differentially in $\eta$ meson transverse momentum ($p_T$) from 1.0 to 6.5 GeV/c for pseudorapidity $3.0 &lt; |\eta| &lt; 3.8$. The midrapidity cross section is measured from 3.5 to 44 GeV/c for pseudorapidity $|\eta| &lt; 0.35$. Both cross sections serve as critical inputs to an updated global analysis of the $\eta$ meson fragmentation functions
DOI: 10.17182/hepdata.166316.v1/t3
title: "Meas. 3:Midrapidity $\eta/\pi^0$ ratio vs. $p_T$" of "Cross sections of $\eta$ mesons in $p$ $+$ $p$ collisions at forward rapidity at $\sqrt{s}=500$ GeV and central rapidity at $\sqrt{s}=510$ GeV"

description: The ratio of $\eta$ to $\pi^0$ cross sections at central rapidity in pp collisions at center-of-mass energy 510 GeV.
description: We present the first measurements of the forward and midrapidity $\eta$ meson cross sections from $p+p$ collisions at $\sqrt{s} = 500$ GeV and $510$ GeV, respectively. We also report the midrapidity $\eta/\pi^0$ ratio at 510 GeV. The forward cross section is measured differentially in $\eta$ meson transverse momentum ($p_T$) from 1.0 to 6.5 GeV/c for pseudorapidity $3.0 &lt; |\eta| &lt; 3.8$. The midrapidity cross section is measured from 3.5 to 44 GeV/c for pseudorapidity $|\eta| &lt; 0.35$. Both cross sections serve as critical inputs to an updated global analysis of the $\eta$ meson fragmentation functions
DOI: 10.17182/hepdata.166316.v1/t4
title: "Sys. corr 1:Forward cross section vs. $p_T^{\eta}$" of "Cross sections of $\eta$ mesons in $p$ $+$ $p$ collisions at forward rapidity at $\sqrt{s}=500$ GeV and central rapidity at $\sqrt{s}=510$ GeV"

description: Correlation matrix for the correlated systematic uncertainties of the forward rapidity $\eta$ meson cross section.
description: We present the first measurements of the forward and midrapidity $\eta$ meson cross sections from $p+p$ collisions at $\sqrt{s} = 500$ GeV and $510$ GeV, respectively. We also report the midrapidity $\eta/\pi^0$ ratio at 510 GeV. The forward cross section is measured differentially in $\eta$ meson transverse momentum ($p_T$) from 1.0 to 6.5 GeV/c for pseudorapidity $3.0 &lt; |\eta| &lt; 3.8$. The midrapidity cross section is measured from 3.5 to 44 GeV/c for pseudorapidity $|\eta| &lt; 0.35$. Both cross sections serve as critical inputs to an updated global analysis of the $\eta$ meson fragmentation functions
DOI: 10.17182/hepdata.166316.v1/t5
title: "Sys. corr 2:Midrapidity cross section vs. $p_T^{\eta}$" of "Cross sections of $\eta$ mesons in $p$ $+$ $p$ collisions at forward rapidity at $\sqrt{s}=500$ GeV and central rapidity at $\sqrt{s}=510$ GeV"

description: Correlation matrix for the correlated systematic uncertainties of the central rapidity $\eta$ meson cross section.
description: We present the first measurements of the forward and midrapidity $\eta$ meson cross sections from $p+p$ collisions at $\sqrt{s} = 500$ GeV and $510$ GeV, respectively. We also report the midrapidity $\eta/\pi^0$ ratio at 510 GeV. The forward cross section is measured differentially in $\eta$ meson transverse momentum ($p_T$) from 1.0 to 6.5 GeV/c for pseudorapidity $3.0 &lt; |\eta| &lt; 3.8$. The midrapidity cross section is measured from 3.5 to 44 GeV/c for pseudorapidity $|\eta| &lt; 0.35$. Both cross sections serve as critical inputs to an updated global analysis of the $\eta$ meson fragmentation functions
DOI: 10.17182/hepdata.92073.v1/t34
title: "Table 34" of "A measurement of soft-drop jet observables in $pp$ collisions with the ATLAS detector at $\sqrt{s} = 13$ TeV"

description: Data from FigAux 4f. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ &gt; 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
description: Unfolded soft drop jet mass distributions for dijet events.
DOI: 10.17182/hepdata.140262.v1/t17
title: "Figure 10a" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 10a
description: No data abstract available.
DOI: 10.15468/dl.put3rx
title: Occurrence Download

description: A dataset containing 2312 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Country is Canada",
 "OccurrenceStatus is Present",
 "TaxonKey is Taricha granulosa"
 ]
}

 The dataset includes 2312 records from 28 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0016071-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.13140/rg.2.2.13199.66722
title: Propuesta de Flora para la reintroducción en rios Isidro Fabela, Estado de méxico al norte del Bosque de agua. (Anexo)
DOI: 10.34740/kaggle/dsv/13616391
title: Peer-to-Peer Boliviano (BOB) Exchange Data
DOI: 10.57967/hf/6879
title: sys-scan-linux-synthetic
DOI: 10.15468/dl.zdsct6
title: Occurrence Download

description: A dataset containing 0 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Thalassomonhystera leptosoma",
 "HasCoordinate is true",
 "HasGeospatialIssue is false"
 ]
}

 The dataset includes 0 records from 0 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0016072-251025141854904/datasets/export for details.