cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.116374.v1/t26
title: "Figure 9b (expected limit contour)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Contour of the region excluded with 95% CL (expected).
description: No data abstract available.
DOI: 10.17182/hepdata.116374.v1/t27
title: "Figure 9b (observed limit contour)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Contour of the region excluded with 95% CL (observed).
description: No data abstract available.
DOI: 10.17182/hepdata.116374.v1/t28
title: "Figure 9c (expected upper limit)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: 95% CL expected upper limit on top squark cross section for the mixed decay model.
description: No data abstract available.
DOI: 10.17182/hepdata.116374.v1/t29
title: "Figure 9c (observed upper limit)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: 95% CL observed upper limit on top squark cross section for the mixed decay model.
description: No data abstract available.
DOI: 10.17182/hepdata.116374.v1/t30
title: "Figure 9c (expected limit contour)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Contour of the region excluded with 95% CL (expected).
description: No data abstract available.
DOI: 10.17182/hepdata.116374.v1/t31
title: "Figure 9c (observed limit contour)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Contour of the region excluded with 95% CL (observed).
description: No data abstract available.
DOI: 10.17182/hepdata.116374.v1/t32
title: "Figure 10a (expected limit)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: 95% CL expected limit on $\sigma/\sigma_{theory}$ for a fermionic DM particle with m = 1 GeV, as a function of the mediator mass for a scalar.
description: No data abstract available.
DOI: 10.17182/hepdata.116374.v1/t33
title: "Figure 10a (observed limit)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: 95% CL observed limit on $\sigma/\sigma_{theory}$ for a fermionic DM particle with m = 1 GeV, as a function of the mediator mass for a scalar.
description: No data abstract available.
DOI: 10.17182/hepdata.116374.v1/t34
title: "Figure 10b (expected limit)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: 95% CL expected limit on $\sigma/\sigma_{theory}$ for a fermionic DM particle with m = 1 GeV, as a function of the mediator mass for a pseudoscalar.
description: No data abstract available.
DOI: 10.25549/vercoutere-ouc110611937
title: Woven wall hanging with horizontal stripes

description: Gray warp with horizonal (weft) stripes in different colors including gray, looped mauve on both sides of gold with metallic gold thread, followed by turquoise with "dashed" lines of two strands, followed by mauve and gold stripes in a regular pattern over the length of the weaving. Different weaving patterns including twill and plain.
DOI: 10.17182/hepdata.116374.v1/t22
title: "Figure 9a (expected limit contour)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Contour of the region excluded with 95% CL (expected).
description: No data abstract available.
DOI: 10.17182/hepdata.116374.v1/t35
title: "Figure 10b (observed limit)" of "Combined searches for the production of supersymmetric top quark partners in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: 95% CL observed limit on $\sigma/\sigma_{theory}$ for a fermionic DM particle with m = 1 GeV, as a function of the mediator mass for a pseudoscalar.
description: No data abstract available.
DOI: 10.17182/hepdata.116547.v1/t1
title: "Table 1" of "Observation and measurement of forward proton scattering in association with lepton pairs produced via the photon fusion mechanism at ATLAS"

description: The measured fiducial cross sections. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity, the second is the luminosity
description: CERN-LHC. Measurement of proton-tagged dielectron and dimuon production via photon fusion in proton collisions at a centre-of mass energy of 13.0 TeV. The data sample after event selection, collected during 2017, has a total integrated luminosity of 14.6 fb-1 with 19 candidate electron pairs and 23 muon pairs. The cross sections are measured in this fiducual region is defined as: - PT of electrons &gt; 18 GeV - PT of muons &gt; 15 GeV - ETA of electrons: |eta|&lt;2.47 - ETA of muons: |eta|&lt;2.4 - PT of dilepton system &lt; 5 GeV - acoplanrity of dilepton system &lt; 0.01 - dilepton mass &gt; 20 GeV AND ( dilepton mass &lt; 70 GeV OR &gt; dilepton mass 105 GeV) - (xill+ &gt; 0.035 GeV AND xill+ &lt; 0.08) OR (xill- &gt; 0.035 GeV AND xill- &lt; 0.08)
DOI: 10.17182/hepdata.116551.v1/t2
title: "Table_T02" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.3275 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t3
title: "Table_T03" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.3486 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t5
title: "Table_T05" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.3897 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t1
title: "Table_T01" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.3062 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t4
title: "Table_T04" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.3693 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t6
title: "Table_T06" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.4098 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.25549/vercoutere-ouc110611938
title: Woven wall hanging with horizontal stripes

description: Gray warp with horizonal (weft) stripes in different colors including gray, looped mauve on both sides of gold with metallic gold thread, followed by turquoise with "dashed" lines of two strands, followed by mauve and gold stripes in a regular pattern over the length of the weaving. Different weaving patterns including twill and plain.
DOI: 10.17182/hepdata.116551.v1/t10
title: "Table_T10" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.4875 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t12
title: "Table_T12" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.5249 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t13
title: "Table_T13" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.5432 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t14
title: "Table_T14" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.5614 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t8
title: "Table_T08" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.4492 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t9
title: "Table_T09" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.4685 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t11
title: "Table_T11" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.5063 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t15
title: "Table_T15" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.5793 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t16
title: "Table_T16" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.5970 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t17
title: "Table_T17" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.6146 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t18
title: "Table_T18" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.6319 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t20
title: "Table_T20" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.6660 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t7
title: "Table_T07" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.4296 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. The systematic uncertainty
is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%).
By adding all contributions in quadrature, a total systematic uncertainty of less
than 6% is obtained. The experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.