cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.95826.v1/t191
title: "m2l4q for gluon-gluon fusion, llWW, mA 760 mH 640" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The m2l4q mass distribution for the m4q window defined for (mA, mH) = (760, 640) GeV with gluon-gluon fusion production is shown for the llWW channel. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (760, 640) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t192
title: "m2l4q for gluon-gluon fusion, llWW, mA 760 mH 650" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The m2l4q mass distribution for the m4q window defined for (mA, mH) = (760, 650) GeV with gluon-gluon fusion production is shown for the llWW channel. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (760, 650) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t193
title: "m2l4q for gluon-gluon fusion, llWW, mA 770 mH 660" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The m2l4q mass distribution for the m4q window defined for (mA, mH) = (770, 660) GeV with gluon-gluon fusion production is shown for the llWW channel. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (770, 660) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t194
title: "m2l4q for gluon-gluon fusion, llWW, mA 780 mH 670" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The m2l4q mass distribution for the m4q window defined for (mA, mH) = (780, 670) GeV with gluon-gluon fusion production is shown for the llWW channel. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (780, 670) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t195
title: "m2l4q for gluon-gluon fusion, llWW, mA 780 mH 680" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The m2l4q mass distribution for the m4q window defined for (mA, mH) = (780, 680) GeV with gluon-gluon fusion production is shown for the llWW channel. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (780, 680) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t196
title: "m2l4q for gluon-gluon fusion, llWW, mA 790 mH 690" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The m2l4q mass distribution for the m4q window defined for (mA, mH) = (790, 690) GeV with gluon-gluon fusion production is shown for the llWW channel. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (790, 690) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.3535/n0r-xp9-1h3
title: Carex acutiformis Ehrh.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95826.v1/t197
title: "m2l4q for gluon-gluon fusion, llWW, mA 800 mH 700" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The m2l4q mass distribution for the m4q window defined for (mA, mH) = (800, 700) GeV with gluon-gluon fusion production is shown for the llWW channel. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (800, 700) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95866.v1/t1
title: " Pi0 & IDP - Hadron 5 &lt; pT,trigger &lt; 7 GeV/c" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side charged hadron yield per π 0 trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1 & Away-side isolated direct photon trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.17182/hepdata.95866.v1/t2
title: " Pi0 & IDP - Hadron 7 &lt; pT,trigger &lt; 9 GeV/c" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side charged hadron yield per π 0 trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1 & Away-side isolated direct photon trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.17182/hepdata.95866.v1/t3
title: " Pi0 & IDP - Hadron 9 &lt; pT,trigger &lt; 12 GeV/c" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side charged hadron yield per π 0 trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1 & Away-side isolated direct photon trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.17182/hepdata.95866.v1/t4
title: " Pi0 & IDP - Hadron 12 &lt; pT,trigger &lt; 15 GeV/c" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side charged hadron yield per π 0 trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1 & Away-side isolated direct photon trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.17182/hepdata.95866.v1/t5
title: " Pi0 & IDP - Hadron 5 &lt; pT,t &lt; 7" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side charged hadron yield per π 0 trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1 & Away-side isolated direct photon trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.17182/hepdata.95866.v1/t6
title: " Pi0 - Hadron 7 &lt; pT,t &lt; 9" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side charged hadron yield per π 0 trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.3535/dl5-809-hvz
title: Rumex acetosella L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/mpw-kfy-465
title: Koeleria macrantha (Ledeb.) Schult.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95866.v1/t10
title: " Isolated Direct Photon - Hadron 12 &lt; pT,t &lt; 15" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side isolated direct photon trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.17182/hepdata.95866.v1/t7
title: " Isolated Direct Photon - Hadron 7 &lt; pT,t &lt; 9" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side isolated direct photon trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.17182/hepdata.95866.v1/t8
title: " Pi0 & IDP - Hadron 9 &lt; pT,t &lt; 12" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side charged hadron yield per π 0 trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1 & Away-side isolated direct photon trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.17182/hepdata.95866.v1/t9
title: " Pi0 - Hadron 12 &lt; pT,t &lt; 15" of "High p_T Direct Photon and pi^0 Triggered Azimuthal Jet Correlations in sqrt(s)=200 GeV p+p Collisions"

description: Away-side charged hadron yield per π 0 trigger as a function of xE, which is equivalent to zT in the collinear limit cos(∆φ) = 1.
description: BNL-RHIC. Correlations of charged hadrons of 1&lt; pT&lt;10 Gev/cwith highpTdirect photons andπ0mesonsin the range 5&lt; pT&lt;15 Gev/care used to study jet fragmentation in theγ+jet and dijet channels,respectively. The magnitude of the partonic transverse momentum,kT, is obtained by comparingto a model incorporating a GaussiankTsmearing. The sensitivity of the associated charged hadronspectra to the underlying fragmentation function is testedand the data are compared to calculationsusing recent global fit results. The shape of the direct photon-associated hadron spectrum as well asits charge asymmetry are found to be consistent with a sampledominated by quark-gluon Comptonscattering. No significant evidence of fragmentation photon correlated production is observed withinexperimental uncertainties.
DOI: 10.17182/hepdata.95877.v1/t1
title: "Fig1" of "Medium modification of jet fragmentation in Au+Au collisions at sqrt(s_NN)=200 GeV measured in direct photon-hadron correlations"

description: Direct photon-hadron pair per-trigger yields vs Delta-phi (Au+Au and p+p)
description: BNL-RHIC. The jet fragmentation function is measured with direct photon-hadron correlations inp+pandAu+Au collisions at√sNN= 200 GeV. ThepTof the photon is an excellent approximation to theinitialpTof the jet and the ratiozT=phT/pγTis used as a proxy for the jet fragmentation function.A statistical subtraction is used to extract the direct photon-hadron yields in Au+Au collisionswhile a photon isolation cut is applied inp+p.IAA, the ratio of jet fragment yield in Au+Au tothat inp+p, indicates modification of the jet fragmentation function.Suppression, most likely dueto energy loss in the medium, is seen at highzT. The fragment yield at lowzTis enhanced at largeangles. Such a trend is expected from redistribution of the lost energy into increased production oflow-momentum particles.