cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.78231.v1/t13
title: "Table 13" of "Flow dominance and factorization of transverse momentum correlations in Pb-Pb collisions at the LHC"

description: $v_{4}$ coefficients estimatEd from the flow ansatz in the range $0.9 \leq |\Delta\eta| \leq 1.9$.
description: CERN-LHC. ALICE Measurement of charged particles differential transverse momentum correlation function, $\Delta p_{\rm T}\Delta p_{\rm T}$, in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV. The correlations are reported as a function of the relative pseudorapidity and azimuthal angle difference, $\Delta\varphi$. The $\Delta\varphi$ dependence is found to be largely independent of $\Delta\eta$ at $\Delta\eta &gt; 0.9$. $\Delta p_{\rm T}\Delta p_{\rm T}$ exhibits a strong dependence on collision centrality that is qualitatively similar to that of number correlations, R2, previously reported. In 0-5% most central Pb--Pb collisions the two particle transverse momentum correlation function exhibits a cleartwo hump structure at the 'away-side', an indication of the dominance of triangular flow. Detailed comparison of R2 and $\Delta p_{\rm T}\Delta p_{\rm T}$ correlation functions utilizing Fourier decomposition show that the $\Delta p_{\rm T}\Delta p_{\rm T}$ correlations at $\Delta\eta &gt; 0.9$ can be well reproduced by the flow ansatz, assuming that all the correlations are dominated by the anisotropic flow.
DOI: 10.17182/hepdata.78231.v1/t14
title: "Table 14" of "Flow dominance and factorization of transverse momentum correlations in Pb-Pb collisions at the LHC"

description: $v_{2}[P_2]$ coefficients vs pair separation in pseudorapidity in 0-5% centrality.
description: CERN-LHC. ALICE Measurement of charged particles differential transverse momentum correlation function, $\Delta p_{\rm T}\Delta p_{\rm T}$, in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV. The correlations are reported as a function of the relative pseudorapidity and azimuthal angle difference, $\Delta\varphi$. The $\Delta\varphi$ dependence is found to be largely independent of $\Delta\eta$ at $\Delta\eta &gt; 0.9$. $\Delta p_{\rm T}\Delta p_{\rm T}$ exhibits a strong dependence on collision centrality that is qualitatively similar to that of number correlations, R2, previously reported. In 0-5% most central Pb--Pb collisions the two particle transverse momentum correlation function exhibits a cleartwo hump structure at the 'away-side', an indication of the dominance of triangular flow. Detailed comparison of R2 and $\Delta p_{\rm T}\Delta p_{\rm T}$ correlation functions utilizing Fourier decomposition show that the $\Delta p_{\rm T}\Delta p_{\rm T}$ correlations at $\Delta\eta &gt; 0.9$ can be well reproduced by the flow ansatz, assuming that all the correlations are dominated by the anisotropic flow.
DOI: 10.17182/hepdata.78231.v1/t15
title: "Table 15" of "Flow dominance and factorization of transverse momentum correlations in Pb-Pb collisions at the LHC"

description: $v_{2}[R_2]$ coefficients vs pair separation in pseudorapidity in 0-5% centrality.
description: CERN-LHC. ALICE Measurement of charged particles differential transverse momentum correlation function, $\Delta p_{\rm T}\Delta p_{\rm T}$, in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV. The correlations are reported as a function of the relative pseudorapidity and azimuthal angle difference, $\Delta\varphi$. The $\Delta\varphi$ dependence is found to be largely independent of $\Delta\eta$ at $\Delta\eta &gt; 0.9$. $\Delta p_{\rm T}\Delta p_{\rm T}$ exhibits a strong dependence on collision centrality that is qualitatively similar to that of number correlations, R2, previously reported. In 0-5% most central Pb--Pb collisions the two particle transverse momentum correlation function exhibits a cleartwo hump structure at the 'away-side', an indication of the dominance of triangular flow. Detailed comparison of R2 and $\Delta p_{\rm T}\Delta p_{\rm T}$ correlation functions utilizing Fourier decomposition show that the $\Delta p_{\rm T}\Delta p_{\rm T}$ correlations at $\Delta\eta &gt; 0.9$ can be well reproduced by the flow ansatz, assuming that all the correlations are dominated by the anisotropic flow.
DOI: 10.17182/hepdata.78231.v1/t16
title: "Table 16" of "Flow dominance and factorization of transverse momentum correlations in Pb-Pb collisions at the LHC"

description: $v_{3}[P_2]$ coefficients vs pair separation in pseudorapidity in 0-5% centrality.
description: CERN-LHC. ALICE Measurement of charged particles differential transverse momentum correlation function, $\Delta p_{\rm T}\Delta p_{\rm T}$, in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV. The correlations are reported as a function of the relative pseudorapidity and azimuthal angle difference, $\Delta\varphi$. The $\Delta\varphi$ dependence is found to be largely independent of $\Delta\eta$ at $\Delta\eta &gt; 0.9$. $\Delta p_{\rm T}\Delta p_{\rm T}$ exhibits a strong dependence on collision centrality that is qualitatively similar to that of number correlations, R2, previously reported. In 0-5% most central Pb--Pb collisions the two particle transverse momentum correlation function exhibits a cleartwo hump structure at the 'away-side', an indication of the dominance of triangular flow. Detailed comparison of R2 and $\Delta p_{\rm T}\Delta p_{\rm T}$ correlation functions utilizing Fourier decomposition show that the $\Delta p_{\rm T}\Delta p_{\rm T}$ correlations at $\Delta\eta &gt; 0.9$ can be well reproduced by the flow ansatz, assuming that all the correlations are dominated by the anisotropic flow.
DOI: 10.17182/hepdata.78231.v1/t17
title: "Table 17" of "Flow dominance and factorization of transverse momentum correlations in Pb-Pb collisions at the LHC"

description: $v_{3}[R_2]$ coefficients vs pair separation in pseudorapidity in 0-5% centrality.
description: CERN-LHC. ALICE Measurement of charged particles differential transverse momentum correlation function, $\Delta p_{\rm T}\Delta p_{\rm T}$, in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV. The correlations are reported as a function of the relative pseudorapidity and azimuthal angle difference, $\Delta\varphi$. The $\Delta\varphi$ dependence is found to be largely independent of $\Delta\eta$ at $\Delta\eta &gt; 0.9$. $\Delta p_{\rm T}\Delta p_{\rm T}$ exhibits a strong dependence on collision centrality that is qualitatively similar to that of number correlations, R2, previously reported. In 0-5% most central Pb--Pb collisions the two particle transverse momentum correlation function exhibits a cleartwo hump structure at the 'away-side', an indication of the dominance of triangular flow. Detailed comparison of R2 and $\Delta p_{\rm T}\Delta p_{\rm T}$ correlation functions utilizing Fourier decomposition show that the $\Delta p_{\rm T}\Delta p_{\rm T}$ correlations at $\Delta\eta &gt; 0.9$ can be well reproduced by the flow ansatz, assuming that all the correlations are dominated by the anisotropic flow.
DOI: 10.17182/hepdata.78231.v1/t18
title: "Table 18" of "Flow dominance and factorization of transverse momentum correlations in Pb-Pb collisions at the LHC"

description: $v_{4}[P_2]$ coefficients vs pair separation in pseudorapidity in 0-5% centrality.
description: CERN-LHC. ALICE Measurement of charged particles differential transverse momentum correlation function, $\Delta p_{\rm T}\Delta p_{\rm T}$, in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV. The correlations are reported as a function of the relative pseudorapidity and azimuthal angle difference, $\Delta\varphi$. The $\Delta\varphi$ dependence is found to be largely independent of $\Delta\eta$ at $\Delta\eta &gt; 0.9$. $\Delta p_{\rm T}\Delta p_{\rm T}$ exhibits a strong dependence on collision centrality that is qualitatively similar to that of number correlations, R2, previously reported. In 0-5% most central Pb--Pb collisions the two particle transverse momentum correlation function exhibits a cleartwo hump structure at the 'away-side', an indication of the dominance of triangular flow. Detailed comparison of R2 and $\Delta p_{\rm T}\Delta p_{\rm T}$ correlation functions utilizing Fourier decomposition show that the $\Delta p_{\rm T}\Delta p_{\rm T}$ correlations at $\Delta\eta &gt; 0.9$ can be well reproduced by the flow ansatz, assuming that all the correlations are dominated by the anisotropic flow.
DOI: 10.17182/hepdata.78231.v1/t19
title: "Table 19" of "Flow dominance and factorization of transverse momentum correlations in Pb-Pb collisions at the LHC"

description: $v_{4}[R_2]$ coefficients vs pair separation in pseudorapidity in 0-5% centrality.
description: CERN-LHC. ALICE Measurement of charged particles differential transverse momentum correlation function, $\Delta p_{\rm T}\Delta p_{\rm T}$, in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV. The correlations are reported as a function of the relative pseudorapidity and azimuthal angle difference, $\Delta\varphi$. The $\Delta\varphi$ dependence is found to be largely independent of $\Delta\eta$ at $\Delta\eta &gt; 0.9$. $\Delta p_{\rm T}\Delta p_{\rm T}$ exhibits a strong dependence on collision centrality that is qualitatively similar to that of number correlations, R2, previously reported. In 0-5% most central Pb--Pb collisions the two particle transverse momentum correlation function exhibits a cleartwo hump structure at the 'away-side', an indication of the dominance of triangular flow. Detailed comparison of R2 and $\Delta p_{\rm T}\Delta p_{\rm T}$ correlation functions utilizing Fourier decomposition show that the $\Delta p_{\rm T}\Delta p_{\rm T}$ correlations at $\Delta\eta &gt; 0.9$ can be well reproduced by the flow ansatz, assuming that all the correlations are dominated by the anisotropic flow.
DOI: 10.17182/hepdata.78254.v1/t1
title: "Table 1" of "Measurement of electroweak-induced production of W gamma with two jets in pp collisions at sqrt(s)=8 TeV and constraints on anomalous quartic gauge couplings"

description: Summary of the measured and predicted observables.
description: CERN-LHC. A measurement of electroweak-induced production of W gamma and two jets is performed, where the W boson decays leptonically. The data used in the analysis correspond to an integrated luminosity of 19.7 fb^-1 collected by the CMS experiment in center-of-mass energy 8 TeV proton-proton collisions produced at the LHC. Candidate events are selected with exactly one muon or electron, missing transverse momentum, one photon, and two jets with large rapidity separation. 

The fiducial region is defined as:
- pTj1 &gt; 30 GeV, |etaj1| &lt; 4.7
- pTj2 &gt; 30 GeV, |etaj1| &lt; 4.7
- mjj &gt; 700 GeV, |deltaetaJJ| &gt; 2.4
- ptLepton &gt; 20 GeV and |etaLepton| &lt; 2.4
- ptGamma &gt; 20 GeV and |etaGamma| &lt; 1.4442
- missing transverse energy &gt; 20 GeV
- deltaR(jj,lj,jgamma,lgamma) &gt; 0.4
DOI: 10.17182/hepdata.78254.v1/t2
title: "Table 2" of "Measurement of electroweak-induced production of W gamma with two jets in pp collisions at sqrt(s)=8 TeV and constraints on anomalous quartic gauge couplings"

description: Observed and expected shape-based exclusion limits for the aQGC parameters at 95% CL, without any form factors.
description: CERN-LHC. A measurement of electroweak-induced production of W gamma and two jets is performed, where the W boson decays leptonically. The data used in the analysis correspond to an integrated luminosity of 19.7 fb^-1 collected by the CMS experiment in center-of-mass energy 8 TeV proton-proton collisions produced at the LHC. Candidate events are selected with exactly one muon or electron, missing transverse momentum, one photon, and two jets with large rapidity separation. 

The fiducial region is defined as:
- pTj1 &gt; 30 GeV, |etaj1| &lt; 4.7
- pTj2 &gt; 30 GeV, |etaj1| &lt; 4.7
- mjj &gt; 700 GeV, |deltaetaJJ| &gt; 2.4
- ptLepton &gt; 20 GeV and |etaLepton| &lt; 2.4
- ptGamma &gt; 20 GeV and |etaGamma| &lt; 1.4442
- missing transverse energy &gt; 20 GeV
- deltaR(jj,lj,jgamma,lgamma) &gt; 0.4
DOI: 10.17182/hepdata.78261.v1/t1
title: "Table 1" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t5
title: "Table 5" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t2
title: "Table 2" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t3
title: "Table 3" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t4
title: "Table 4" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t6
title: "Table 6" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t7
title: "Table 7" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t8
title: "Table 8" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t9
title: "Table 9" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t10
title: "Table 10" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t11
title: "Table 11" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t12
title: "Table 12" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t13
title: "Table 13" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity independent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.
DOI: 10.17182/hepdata.78261.v1/t14
title: "Table 14" of "A glimpse of gluons through deeply virtual compton scattering on the proton"

description: Beam helicity dependent cross sections. The first systematic uncertainty is the combined correlated systematic uncertainty, the second is the point-to-point systematic uncertainty to add quadratically to the statistical uncertainty.
description: Jefferson Laboratory, Hall A. Measurements of the beam-helicity dependent and independent cross section of photon electroproduction on unpolarized proton. At xB=0.36, we perform measurements for Q**2 values of 1.5, 1.75 and 2 GeV**2. Each Q**2 value was measured with two beam energies. We provide four bins in squared momentum transfer to the proton, ranging from -0.18 to -0.36 GeV**2, except for Q**2=1.5 GeV**2 for which t ranges from -0.18 to -0.30 GeV**2.