cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.78399.v1/t7
title: "Table 7" of "Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings"

description: The expected number of events passing the final event selection in the WW/WZ-&gt;lvJ channel, in each pT(J) bin of the signal region (SR). The expected number of background and signal events are given, together with the number of events observed in data. The numbers correspond to Figures 7(b). The BSM numbers do not include the SM WV contribution, so the SM and BSM WV numbers should be added together. The numbers correspond to the raw event yields, not divided by the bin widths. The six bins in the SR have the following bin boundaries: (100, 200, 300, 400, 500, 600, 700, +inf) GeV. No control region is used for the WW/WZ-&gt;lvJ channel.
description: CERN-LHC. This paper presents a study of the production of WW or WZ boson pairs, with one W boson decaying to electron-neutrino or muon-neutrino and one W or Z boson decaying hadronically. The analysis uses 20.2 fb-1 of sqrt(s)=8 TeV pp collision data, collected by the ATLAS detector at the Large Hadron Collider. Cross-sections for WW/WZ production are measured in high-pT fiducial regions defined close to the experimental event selection. The cross-section is measured for the case where the hadronically decaying boson is reconstructed as two resolved jets (WV-&gt;lvjj), and the case where it is reconstructed as a single jet (WV-&gt;lvJ). For the description of the WV-&gt;lvjj and WV-&gt;lvJ fiducial phase spaces, refer to section 8.1 and 8.2 of the paper.
The transverse momentum distribution of the hadronically decaying boson is used to search for new physics. Observations are consistent with the Standard Model predictions, and 95% confidence intervals are calculated for parameters describing anomalous triple gauge-boson couplings (aTGCs). The aTGC search is done applying the same selection used for cross section measurement, plus an additional requirement for the jet-jet invariant mass (single jet mass) to be close to the W mass: 65 GeV &lt; m_jj &lt; 95 GeV (65 GeV &lt; m_J &lt; 95 GeV).
DOI: 10.25345/c5dz03f4w
title: MassIVE MSV000099748 - Ketogenic diet and ketone body supplementation in polycystic kidney disease models
title: Project description: Metabolic changes induced by a ketogenic diet were investigated in the kidneys and serum of a polycystic kidney disease model using Han:SPRD rats and wild-type controls. The ketogenic diet started at week 3 until week 8. The ketogenic diet (#F3666 diet; Bio-Serv) consisted of approximately 91% fat, 2% carbohydrates, and 5% protein as a caloric ratio. Additionally, in the Pkd1rc/rc mice, the effect of beta-hydroxybutyrate supplements was tested. BHB supplementation started at 3 weeks of age for 12 weeks in total. The diet contained 10% sodium D-BHB. Sample processing protocol: All samples were processed with all procedures performed on ice. First, 30 uL of each sample was aliquoted into V-bottom 96-well plates on ice. Then, 120 uL of an ice-cold acetonitrile-methanol (1:1) mixture was added to each well. For kidney tissue samples, tissues were weighed, and acetonitrile-methanol-water (2:2:1) mixture was added before homogenizing in a bullet blender. Serum and urine samples were sonicated for 5 minutes in ice water and then stored at -20 C for 2 hours. Kidney tissue samples were transferred to an Eppendorf tube without the beads and stored for 2 hours at -20 C. Next, the serum samples were centrifuged for 1 hour at 4 C (4347 rpm), while the kidney tissue samples were centrifuged for 20 minutes at 4 C (18,000 rpm). The supernatant was transferred to a new plate and dried in a vacuum centrifuge (Labconco) at 8 C. Before analysis, the dried extracts were resuspended by adding ice-cold acetonitrile-water (1:1), followed by 20 minutes of sonication in ice water and subsequent centrifugation at 4 C for 1.5 hours at 4347 rpm. The final supernatant was transferred to a new plate. For serum, 100 uL of acetonitrile-water (1:1) was used for resuspension. Kidney tissue sample volumes were normalized to tissue mass. For the targeted metabolomics, an ultra-high-pressure liquid chromatography system (1290 Infinity II, Agilent Technologies) coupled to a triple quadrupole (QQQ) mass spectrometer (Agilent 6495C, San Diego, Agilent Technologies) was used. Agilent MassHunter Workstation Data Acquisition (Version 10.1) was used for data acquisition. Metabolites were determined based on specific transitions, as well as retention times of authentic standards. Metabolite signals without sufficient peak shape, signal-to-noise ratio, or inconsistent retention time (+/-0.1 min) were removed.
DOI: 10.17182/hepdata.78401.v1/t1
title: "Table 1" of "Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector"

description: Measured cross sections for isolated-photon plus jet production as a function of $E_{\rm T}^{\gamma}$.
description: The dynamics of isolated-photon production in association with a jet in proton-proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of $3.2$~fb$^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R=0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon-jet invariant mass and the scattering angle in the photon-jet centre-of-mass system. Tree-level plus parton-shower predictions from SHERPA and PYTHIA as well as next-to-leading-order QCD predictions from JETPHOX and SHERPA are compared to the measurements.

Information about bin-to-bin correlation of the systematic uncertainties:
The following uncertaintes are not correlated bin-to-bin:
sysPhotonRES, sysPhotonID, sysEtisoGap, sysPhotonInvertVar, sysEtisoUpperLimit, sysEtisoMC and sysMCStat.

The different components of the sysPhotonES and sysJetES uncertainties (only the total uncertainty is given here) are fully correlated bin-to-bin.
DOI: 10.17182/hepdata.78401.v1/t2
title: "Table 2" of "Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector"

description: Measured cross sections for isolated-photon plus jet production as a function of $p_{\rm T}^{\rm jet-lead}$.
description: The dynamics of isolated-photon production in association with a jet in proton-proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of $3.2$~fb$^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R=0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon-jet invariant mass and the scattering angle in the photon-jet centre-of-mass system. Tree-level plus parton-shower predictions from SHERPA and PYTHIA as well as next-to-leading-order QCD predictions from JETPHOX and SHERPA are compared to the measurements.

Information about bin-to-bin correlation of the systematic uncertainties:
The following uncertaintes are not correlated bin-to-bin:
sysPhotonRES, sysPhotonID, sysEtisoGap, sysPhotonInvertVar, sysEtisoUpperLimit, sysEtisoMC and sysMCStat.

The different components of the sysPhotonES and sysJetES uncertainties (only the total uncertainty is given here) are fully correlated bin-to-bin.
DOI: 10.17182/hepdata.78401.v1/t3
title: "Table 3" of "Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector"

description: Measured cross sections for isolated-photon plus jet production as a function of $\Delta\phi^{\rm \gamma-jet\ lead}$.
description: The dynamics of isolated-photon production in association with a jet in proton-proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of $3.2$~fb$^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R=0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon-jet invariant mass and the scattering angle in the photon-jet centre-of-mass system. Tree-level plus parton-shower predictions from SHERPA and PYTHIA as well as next-to-leading-order QCD predictions from JETPHOX and SHERPA are compared to the measurements.

Information about bin-to-bin correlation of the systematic uncertainties:
The following uncertaintes are not correlated bin-to-bin:
sysPhotonRES, sysPhotonID, sysEtisoGap, sysPhotonInvertVar, sysEtisoUpperLimit, sysEtisoMC and sysMCStat.

The different components of the sysPhotonES and sysJetES uncertainties (only the total uncertainty is given here) are fully correlated bin-to-bin.
DOI: 10.17182/hepdata.78401.v1/t4
title: "Table 4" of "Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector"

description: Measured cross sections for isolated-photon plus jet production as a function of $m^{\gamma-\rm jet}$.
description: The dynamics of isolated-photon production in association with a jet in proton-proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of $3.2$~fb$^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R=0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon-jet invariant mass and the scattering angle in the photon-jet centre-of-mass system. Tree-level plus parton-shower predictions from SHERPA and PYTHIA as well as next-to-leading-order QCD predictions from JETPHOX and SHERPA are compared to the measurements.

Information about bin-to-bin correlation of the systematic uncertainties:
The following uncertaintes are not correlated bin-to-bin:
sysPhotonRES, sysPhotonID, sysEtisoGap, sysPhotonInvertVar, sysEtisoUpperLimit, sysEtisoMC and sysMCStat.

The different components of the sysPhotonES and sysJetES uncertainties (only the total uncertainty is given here) are fully correlated bin-to-bin.
DOI: 10.17182/hepdata.78401.v1/t5
title: "Table 5" of "Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector"

description: Measured cross sections for isolated-photon plus jet production as a function of $|\cos\theta^{\star}|$.
description: The dynamics of isolated-photon production in association with a jet in proton-proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of $3.2$~fb$^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R=0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon-jet invariant mass and the scattering angle in the photon-jet centre-of-mass system. Tree-level plus parton-shower predictions from SHERPA and PYTHIA as well as next-to-leading-order QCD predictions from JETPHOX and SHERPA are compared to the measurements.

Information about bin-to-bin correlation of the systematic uncertainties:
The following uncertaintes are not correlated bin-to-bin:
sysPhotonRES, sysPhotonID, sysEtisoGap, sysPhotonInvertVar, sysEtisoUpperLimit, sysEtisoMC and sysMCStat.

The different components of the sysPhotonES and sysJetES uncertainties (only the total uncertainty is given here) are fully correlated bin-to-bin.
DOI: 10.17182/hepdata.78402.v1/t2
title: "Table 1" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Observed and predicted mTtot distribution in the b-veto category of the 1l1tau_h channel. Despite listing this as an exclusive final state (as there must be no b-jets), there is no explicit selection on the presence of additional light-flavour jets. Please note that the bin content is divided by the bin width in the paper figure, but not in the HepData table. In the paper, the first bin is cut off at 60 GeV for aesthetics but contains underflows down to 50 GeV as in the HepData table. The last bin includes overflows. The combined prediction for A and H bosons with masses of 300, 500 and 800 GeV and $\tan\beta$ = 10 in the hMSSM scenario are also provided.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.78402.v1/t3
title: "Table 2" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Observed and predicted mTtot distribution in the b-tag category of the 1l1tau_h channel. Despite listing this as an exclusive final state (as there must be at least one b-jets), there is no explicit selection on the presence of additional light-flavour jets. Please note that the bin content is divided by the bin width in the paper figure, but not in the HepData table. In the paper, the first bin is cut off at 60 GeV for aesthetics but contains underflows down to 50 GeV as in the HepData table. The last bin includes overflows. The combined prediction for A and H bosons with masses of 300, 500 and 800 GeV and $\tan\beta$ = 10 in the hMSSM scenario are also provided.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.78402.v1/t10
title: "Table 10" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Observed and expected 95% CL upper limits on the Higgs boson production cross section times ditau branching fraction as a function of the boson mass and the relative strength of the b-associated production.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.78402.v1/t4
title: "Table 3" of "Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Observed and predicted mTtot distribution in the b-veto category of the 2tau_h channel. Despite listing this as an exclusive final state (as there must be no b-jets), there is no explicit selection on the presence of additional light-flavour jets. Please note that the bin content is divided by the bin width in the paper figure, but not in the HepData table. The last bin includes overflows. The combined prediction for A and H bosons with masses of 300, 500 and 800 GeV and $\tan\beta$ = 10 in the hMSSM scenario are also provided.
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"