cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.25549/vercoutere-ouc110609874
title: 9 scenes with captions depicting Robin Hood themes

description: Nine rectangles (three across and three down) with cursive writing describing each scene with "The Story of Robin Hood" written in the right margin. "Sherwood Forest" - green trees with a brown path; "Barrel (for garbage in Sherwood Forest signifies 'transformation'" - green trees with brown path and black barrel with a lid in the foreground; "King Richard the Lion Hearted" - one male dressed in black from crotch to nose in front of ten men dressed in green knee long suits and caps with black belts, white leggings, and black shoes; "Approach to the castle where horses can go" across two panels - green trees with brown path leading to a blue street and yellow and blue building; two yellow buildings with blue, brown, and black details next to a blue sidewalk next to a blue street; "Nottingham Castle" - gray stone castle walls with a round turret in one corner; "In the Castle" - gray stone walls; "Rooms in the Castle" - Gray stone walls, gray floor, dark gray furniture with curved legs and two doors; "Maid Marian" - side view of one male from buttocks up dressed in a dark gray coat standing with a female from knees to neck dressed in black spotted dress. See description of 001 for OT notes.
DOI: 10.17182/hepdata.105273.v1/t34
title: "Table 18" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 11.00 &lt; q2 &lt; 12.50 GeV2/c4
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105273.v1/t35
title: "Table 19" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 15.00 &lt; q2 &lt; 17.00 GeV2/c4
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105273.v1/t36
title: "Table 20" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 17.00 &lt; q2 &lt; 19.00 GeV2/c4
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105273.v1/t37
title: "Table 21" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 1.10 &lt; q2 &lt; 6.00 GeV2/c4
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105273.v1/t38
title: "Table 22" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 15.00 &lt; q2 &lt; 19.00 GeV2/c4
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105278.v1/t1
title: "Figure 1 (200GeV)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: Fractions of the next-to-leading-order cross section for inclusive jet production arising from quark-quark, quark-gluon and gluon-gluon scattering in pp collisions (200GeV)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105278.v1/t2
title: "Figure 1 (500GeV)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: Fractions of the next-to-leading-order cross section for inclusive jet production arising from quark-quark, quark-gluon and gluon-gluon scattering in pp collisions (500GeV)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105278.v1/t3
title: "Figure 2 (JP0)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: The upper panel shows the jet yield vs detector jet pT in data and simulation for each of the three trigger categories. The lower three panels show the relative differences between data and simulation (JP0)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105278.v1/t4
title: "Figure 2 (JP1)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: The upper panel shows the jet yield vs detector jet pT in data and simulation for each of the three trigger categories. The lower three panels show the relative differences between data and simulation (JP1)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105278.v1/t5
title: "Figure 2 (JP2)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: The upper panel shows the jet yield vs detector jet pT in data and simulation for each of the three trigger categories. The lower three panels show the relative differences between data and simulation (JP2)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105278.v1/t6
title: "Figure 3 (data, 8.0 GeV/c)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: Distributions of the charged hadrons within the jets as a function of the hadron longitudinal momentum fraction,z, for two typical detector jet pT bins
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105278.v1/t7
title: "Figure 3" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: Distributions of the charged hadrons within the jets as a function of the hadron longitudinal momentum fraction,z, for two typical detector jet pT bins
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.25549/vercoutere-ouc110611213
title: 2 running antelope

description: Two running black antelope with white bellies in a tan desert landscape with brown and black scrubby shrubs. Colorful mountains and sky above with curved bands of pink, yellow, green, black, tan, gray, purple, orange, and blue
DOI: 10.17182/hepdata.105273.v1/t17
title: "Fig 4g" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: The optimised observable P6' versus q2. The first (second) error bars represent the statistical (total) uncertainties.
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105278.v1/t10
title: "Figure 4 (data, 34.4GeV/c)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: Distributions of the charged hadrons within the jets as a function of the hadron longitudinal momentum transverse to the thrust axis,jT, for two typical detector jet pT bins (data, 34.4GeV/c)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105278.v1/t11
title: "Figure 4 (simulation, 34.4GeV/c)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: Distributions of the charged hadrons within the jets as a function of the hadron longitudinal momentum transverse to the thrust axis,jT, for two typical detector jet pT bins (simulation, 34.4GeV/c)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105278.v1/t8
title: "Figure 4 (data, 8GeV/c)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: Distributions of the charged hadrons within the jets as a function of the hadron longitudinal momentum transverse to the thrust axis,jT, for two typical detector jet pT bins (data, 8GeV/c)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105278.v1/t9
title: "Figure 4 (simulation, 8GeV/c)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: Distributions of the charged hadrons within the jets as a function of the hadron longitudinal momentum transverse to the thrust axis,jT, for two typical detector jet pT bins (simulation, 8GeV/c)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.
DOI: 10.17182/hepdata.105273.v1/t18
title: "Fig 4h" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: The optimised observable P8' versus q2. The first (second) error bars represent the statistical (total) uncertainties.
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105273.v1/t19
title: "Table 3" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 0.10 &lt; q2 &lt; 0.98 GeV2/c4
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105278.v1/t12
title: "Figure 5 (JP0, 34.4GeV/c)" of "Longitudinal double-spin asymmetry for inclusive jet and dijet production in $pp$ collisions at $\sqrt{s} = 510$ GeV"

description: The upper panel shows the electromagnetic fraction distribution for jets in a low-pT bin. The lower panel shows the electromagnetic fraction distributions in a higher pT bin for each of the three jet categories (JP0, 34.4GeV/c)
description: We report the first measurement of the inclusive jet and the dijet longitudinal double-spin asymmetries, ALL, at midrapidity in polarized pp collisions at a center-of-mass energy s√=510 GeV. The inclusive jet ALL measurement is sensitive to the gluon helicity distribution down to a gluon momentum fraction of x≈0.015, while the dijet measurements, separated into four jet-pair topologies, provide constraints on the x dependence of the gluon polarization. Both results are consistent with previous measurements made at s√=200 GeV in the overlapping kinematic region, x&gt;0.05, and show good agreement with predictions from recent next-to-leading order global analyses.