cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.61627.v1/t37
title: "Table 37" of "Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector"

description: The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.3 &lt;= |y| &lt; 0.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.
description: CERN-LHC. This paper reports the measurement of inclusive jet cross sections in proton-proton collisions at a centre-of-mass energy of 2.76 TeV using a data sample of integrated luminosity of 0.20 pb-1 collected in 2011. Jets are identified using the anti-kt algorithm with two radius parameters (0.4 and 0.6). The cross sections are presented as a function of the jet transverse momentum and rapidity covering jets from 20-430 GeV in transverse momentum and |rapidity| &lt; 4.4. The data are also compared with previous ATLAS 7 TeV cross sections as functions of PT and XT. The main tables below show the results correlated and uncorrelated systematic errors individually combined, as presented in the plots in the paper. The first table below gives access to the complete tables with the various sources of systematic error individually presented. Correlations over the rapidity bins and to the 7 TeV data are shown in table 1 of the paper and repeated below. 

Note added (27 JUN 2014):
The central values of the (2.76 TeV)/(7 TeV) cross-section ratios reported in Tables 15-42 below should be multiplied by a factor of 1/1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") for the 7 TeV cross sections increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details. The 7 TeV Lumi uncertainty is added in quadrature to the 2.76 TeV Lumi uncertainty (2.7%) in the cross-section ratios, leading to a slight increase in the Lumi uncertainty on the cross-section ratios from sqrt(2.7**2+3.4**2)=4.3% to sqrt(2.7**2+3.5**2)=4.4%.
DOI: 10.17182/hepdata.61627.v1/t38
title: "Table 38" of "Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector"

description: The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 0.8 &lt;= |y| &lt; 1.2 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.
description: CERN-LHC. This paper reports the measurement of inclusive jet cross sections in proton-proton collisions at a centre-of-mass energy of 2.76 TeV using a data sample of integrated luminosity of 0.20 pb-1 collected in 2011. Jets are identified using the anti-kt algorithm with two radius parameters (0.4 and 0.6). The cross sections are presented as a function of the jet transverse momentum and rapidity covering jets from 20-430 GeV in transverse momentum and |rapidity| &lt; 4.4. The data are also compared with previous ATLAS 7 TeV cross sections as functions of PT and XT. The main tables below show the results correlated and uncorrelated systematic errors individually combined, as presented in the plots in the paper. The first table below gives access to the complete tables with the various sources of systematic error individually presented. Correlations over the rapidity bins and to the 7 TeV data are shown in table 1 of the paper and repeated below. 

Note added (27 JUN 2014):
The central values of the (2.76 TeV)/(7 TeV) cross-section ratios reported in Tables 15-42 below should be multiplied by a factor of 1/1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") for the 7 TeV cross sections increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details. The 7 TeV Lumi uncertainty is added in quadrature to the 2.76 TeV Lumi uncertainty (2.7%) in the cross-section ratios, leading to a slight increase in the Lumi uncertainty on the cross-section ratios from sqrt(2.7**2+3.4**2)=4.3% to sqrt(2.7**2+3.5**2)=4.4%.
DOI: 10.17182/hepdata.61627.v1/t39
title: "Table 39" of "Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector"

description: The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 1.2 &lt;= |y| &lt; 2.1 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.
description: CERN-LHC. This paper reports the measurement of inclusive jet cross sections in proton-proton collisions at a centre-of-mass energy of 2.76 TeV using a data sample of integrated luminosity of 0.20 pb-1 collected in 2011. Jets are identified using the anti-kt algorithm with two radius parameters (0.4 and 0.6). The cross sections are presented as a function of the jet transverse momentum and rapidity covering jets from 20-430 GeV in transverse momentum and |rapidity| &lt; 4.4. The data are also compared with previous ATLAS 7 TeV cross sections as functions of PT and XT. The main tables below show the results correlated and uncorrelated systematic errors individually combined, as presented in the plots in the paper. The first table below gives access to the complete tables with the various sources of systematic error individually presented. Correlations over the rapidity bins and to the 7 TeV data are shown in table 1 of the paper and repeated below. 

Note added (27 JUN 2014):
The central values of the (2.76 TeV)/(7 TeV) cross-section ratios reported in Tables 15-42 below should be multiplied by a factor of 1/1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") for the 7 TeV cross sections increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details. The 7 TeV Lumi uncertainty is added in quadrature to the 2.76 TeV Lumi uncertainty (2.7%) in the cross-section ratios, leading to a slight increase in the Lumi uncertainty on the cross-section ratios from sqrt(2.7**2+3.4**2)=4.3% to sqrt(2.7**2+3.5**2)=4.4%.
DOI: 10.17182/hepdata.61627.v1/t41
title: "Table 41" of "Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector"

description: The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.8 &lt;= |y| &lt; 3.6 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.
description: CERN-LHC. This paper reports the measurement of inclusive jet cross sections in proton-proton collisions at a centre-of-mass energy of 2.76 TeV using a data sample of integrated luminosity of 0.20 pb-1 collected in 2011. Jets are identified using the anti-kt algorithm with two radius parameters (0.4 and 0.6). The cross sections are presented as a function of the jet transverse momentum and rapidity covering jets from 20-430 GeV in transverse momentum and |rapidity| &lt; 4.4. The data are also compared with previous ATLAS 7 TeV cross sections as functions of PT and XT. The main tables below show the results correlated and uncorrelated systematic errors individually combined, as presented in the plots in the paper. The first table below gives access to the complete tables with the various sources of systematic error individually presented. Correlations over the rapidity bins and to the 7 TeV data are shown in table 1 of the paper and repeated below. 

Note added (27 JUN 2014):
The central values of the (2.76 TeV)/(7 TeV) cross-section ratios reported in Tables 15-42 below should be multiplied by a factor of 1/1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") for the 7 TeV cross sections increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details. The 7 TeV Lumi uncertainty is added in quadrature to the 2.76 TeV Lumi uncertainty (2.7%) in the cross-section ratios, leading to a slight increase in the Lumi uncertainty on the cross-section ratios from sqrt(2.7**2+3.4**2)=4.3% to sqrt(2.7**2+3.5**2)=4.4%.
DOI: 10.25505/fiz.icsd.cc2bchrz
title: CSD 2156011: Experimental Crystal Structure Determination

description: Related Article: Wen Fa Chen, Bin Wen Liu, Shao Min Pei, Xiao Ming Jiang, Guo Cong Guo
|2023|Adv. Sci.|10|2207630|doi:10.1002/advs.202207630
description: An entry from the Inorganic Crystal Structure Database, the world’s repository for inorganic crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the joint CCDC and FIZ Karlsruhe Access Structures service and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.5517/ccdc.csd.cc27qtsl
title: CCDC 2077520: Experimental Crystal Structure Determination

description: Related Article: Siti Nabilla Aliya Mohd Nizar, Mohd Mustaqim Rosli, Siti Azrah Mohamad Samsuri, Ibrahim Abdul Razak, Suhana Arshad|2024|Phys.Scr.|99|015917|doi:10.1088/1402-4896/ad11c5
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.17182/hepdata.61627.v1/t35
title: "Table 35" of "Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector"

description: The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 &lt;= |y| &lt; 4.4 for anti-kt jets with R = 0.4 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.
description: CERN-LHC. This paper reports the measurement of inclusive jet cross sections in proton-proton collisions at a centre-of-mass energy of 2.76 TeV using a data sample of integrated luminosity of 0.20 pb-1 collected in 2011. Jets are identified using the anti-kt algorithm with two radius parameters (0.4 and 0.6). The cross sections are presented as a function of the jet transverse momentum and rapidity covering jets from 20-430 GeV in transverse momentum and |rapidity| &lt; 4.4. The data are also compared with previous ATLAS 7 TeV cross sections as functions of PT and XT. The main tables below show the results correlated and uncorrelated systematic errors individually combined, as presented in the plots in the paper. The first table below gives access to the complete tables with the various sources of systematic error individually presented. Correlations over the rapidity bins and to the 7 TeV data are shown in table 1 of the paper and repeated below. 

Note added (27 JUN 2014):
The central values of the (2.76 TeV)/(7 TeV) cross-section ratios reported in Tables 15-42 below should be multiplied by a factor of 1/1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") for the 7 TeV cross sections increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details. The 7 TeV Lumi uncertainty is added in quadrature to the 2.76 TeV Lumi uncertainty (2.7%) in the cross-section ratios, leading to a slight increase in the Lumi uncertainty on the cross-section ratios from sqrt(2.7**2+3.4**2)=4.3% to sqrt(2.7**2+3.5**2)=4.4%.
DOI: 10.17182/hepdata.61627.v1/t40
title: "Table 40" of "Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector"

description: The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 2.1 &lt;= |y| &lt; 2.8 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.
description: CERN-LHC. This paper reports the measurement of inclusive jet cross sections in proton-proton collisions at a centre-of-mass energy of 2.76 TeV using a data sample of integrated luminosity of 0.20 pb-1 collected in 2011. Jets are identified using the anti-kt algorithm with two radius parameters (0.4 and 0.6). The cross sections are presented as a function of the jet transverse momentum and rapidity covering jets from 20-430 GeV in transverse momentum and |rapidity| &lt; 4.4. The data are also compared with previous ATLAS 7 TeV cross sections as functions of PT and XT. The main tables below show the results correlated and uncorrelated systematic errors individually combined, as presented in the plots in the paper. The first table below gives access to the complete tables with the various sources of systematic error individually presented. Correlations over the rapidity bins and to the 7 TeV data are shown in table 1 of the paper and repeated below. 

Note added (27 JUN 2014):
The central values of the (2.76 TeV)/(7 TeV) cross-section ratios reported in Tables 15-42 below should be multiplied by a factor of 1/1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") for the 7 TeV cross sections increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details. The 7 TeV Lumi uncertainty is added in quadrature to the 2.76 TeV Lumi uncertainty (2.7%) in the cross-section ratios, leading to a slight increase in the Lumi uncertainty on the cross-section ratios from sqrt(2.7**2+3.4**2)=4.3% to sqrt(2.7**2+3.5**2)=4.4%.
DOI: 10.17182/hepdata.61627.v1/t42
title: "Table 42" of "Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector"

description: The measured ratio of inclusive jet cross sections at sqrt(s)=2.76 TeV to the one at sqrt(s)=7 TeV in the rapidity bin 3.6 &lt;= |y| &lt; 4.4 for anti-kt jets with R = 0.6 as a function of the jet PT. The first (sys) error is the combined correlated systematic error and the second the combined uncorrelated systematic error, excluding the luminosity uncertainty. Also shown are the multiplicative non-perturbative corrections, NPcorr.
description: CERN-LHC. This paper reports the measurement of inclusive jet cross sections in proton-proton collisions at a centre-of-mass energy of 2.76 TeV using a data sample of integrated luminosity of 0.20 pb-1 collected in 2011. Jets are identified using the anti-kt algorithm with two radius parameters (0.4 and 0.6). The cross sections are presented as a function of the jet transverse momentum and rapidity covering jets from 20-430 GeV in transverse momentum and |rapidity| &lt; 4.4. The data are also compared with previous ATLAS 7 TeV cross sections as functions of PT and XT. The main tables below show the results correlated and uncorrelated systematic errors individually combined, as presented in the plots in the paper. The first table below gives access to the complete tables with the various sources of systematic error individually presented. Correlations over the rapidity bins and to the 7 TeV data are shown in table 1 of the paper and repeated below. 

Note added (27 JUN 2014):
The central values of the (2.76 TeV)/(7 TeV) cross-section ratios reported in Tables 15-42 below should be multiplied by a factor of 1/1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") for the 7 TeV cross sections increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details. The 7 TeV Lumi uncertainty is added in quadrature to the 2.76 TeV Lumi uncertainty (2.7%) in the cross-section ratios, leading to a slight increase in the Lumi uncertainty on the cross-section ratios from sqrt(2.7**2+3.4**2)=4.3% to sqrt(2.7**2+3.5**2)=4.4%.
DOI: 10.25505/fiz.icsd.cc2bchs0
title: CSD 2156012: Experimental Crystal Structure Determination

description: Related Article: Wen Fa Chen, Bin Wen Liu, Shao Min Pei, Xiao Ming Jiang, Guo Cong Guo
|2023|Adv. Sci.|10|2207630|doi:10.1002/advs.202207630
description: An entry from the Inorganic Crystal Structure Database, the world’s repository for inorganic crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the joint CCDC and FIZ Karlsruhe Access Structures service and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.17182/hepdata.61628.v1/t1
title: "Table 1" of "Long-range angular correlations of $\rm \pi$, K and p in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The Fourier coefficients V2(2PC,sub) extracted for all charged particles as a function of PT from the correlation in the 0-20% multiplicity class after subraction of the correlation from the 60-100% event class.
description: CERN-LHC. Measurements of angular correlations between unidentified charged trigger particles and various species of charged associated partices (all charged, pions, kaon, protons and antiprotons) produced from proton-lead collisions at a nucleon-nucleon centre-of-mass energy of 5.02 TeV in the transverse momentum range 0.3-4 GeV/c. The correlations, expressed as associated yield per trigger particle, are obtained in the lab. pseudorapidity range |eta|&lt;0.8. Fourier coefficients are extracted from the long-range correlations projected onto the azimuthal angle difference and studied as a function of PT and in intervals of event multiplicity. This record tabulates the values of the Fourier coefficient V2 extracted using two methods refered to as 2PC, the two-particle correlation method, and SP, the scalar product method. See the text of the paper for details. In figure 4 the per trigger yield measured in high multiplicity events is subtracted from that of low multiplicity events to reduce correaltions due to jets.
DOI: 10.17182/hepdata.61628.v1/t2
title: "Table 2" of "Long-range angular correlations of $\rm \pi$, K and p in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The Fourier coefficients V2(2PC,sub) extracted for charged pions as a function of PT from the correlation in the 0-20% multiplicity class after subraction of the correlation from the 60-100% event class.
description: CERN-LHC. Measurements of angular correlations between unidentified charged trigger particles and various species of charged associated partices (all charged, pions, kaon, protons and antiprotons) produced from proton-lead collisions at a nucleon-nucleon centre-of-mass energy of 5.02 TeV in the transverse momentum range 0.3-4 GeV/c. The correlations, expressed as associated yield per trigger particle, are obtained in the lab. pseudorapidity range |eta|&lt;0.8. Fourier coefficients are extracted from the long-range correlations projected onto the azimuthal angle difference and studied as a function of PT and in intervals of event multiplicity. This record tabulates the values of the Fourier coefficient V2 extracted using two methods refered to as 2PC, the two-particle correlation method, and SP, the scalar product method. See the text of the paper for details. In figure 4 the per trigger yield measured in high multiplicity events is subtracted from that of low multiplicity events to reduce correaltions due to jets.
DOI: 10.17182/hepdata.61628.v1/t3
title: "Table 3" of "Long-range angular correlations of $\rm \pi$, K and p in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The Fourier coefficients V2(2PC,sub) extracted for charged kaons as a function of PT from the correlation in the 0-20% multiplicity class after subraction of the correlation from the 60-100% event class.
description: CERN-LHC. Measurements of angular correlations between unidentified charged trigger particles and various species of charged associated partices (all charged, pions, kaon, protons and antiprotons) produced from proton-lead collisions at a nucleon-nucleon centre-of-mass energy of 5.02 TeV in the transverse momentum range 0.3-4 GeV/c. The correlations, expressed as associated yield per trigger particle, are obtained in the lab. pseudorapidity range |eta|&lt;0.8. Fourier coefficients are extracted from the long-range correlations projected onto the azimuthal angle difference and studied as a function of PT and in intervals of event multiplicity. This record tabulates the values of the Fourier coefficient V2 extracted using two methods refered to as 2PC, the two-particle correlation method, and SP, the scalar product method. See the text of the paper for details. In figure 4 the per trigger yield measured in high multiplicity events is subtracted from that of low multiplicity events to reduce correaltions due to jets.
DOI: 10.17182/hepdata.61628.v1/t4
title: "Table 4" of "Long-range angular correlations of $\rm \pi$, K and p in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The Fourier coefficients V2(2PC,sub) extracted for (anti)protons as a function of PT from the correlation in the 0-20% multiplicity class after subraction of the correlation from the 60-100% event class.
description: CERN-LHC. Measurements of angular correlations between unidentified charged trigger particles and various species of charged associated partices (all charged, pions, kaon, protons and antiprotons) produced from proton-lead collisions at a nucleon-nucleon centre-of-mass energy of 5.02 TeV in the transverse momentum range 0.3-4 GeV/c. The correlations, expressed as associated yield per trigger particle, are obtained in the lab. pseudorapidity range |eta|&lt;0.8. Fourier coefficients are extracted from the long-range correlations projected onto the azimuthal angle difference and studied as a function of PT and in intervals of event multiplicity. This record tabulates the values of the Fourier coefficient V2 extracted using two methods refered to as 2PC, the two-particle correlation method, and SP, the scalar product method. See the text of the paper for details. In figure 4 the per trigger yield measured in high multiplicity events is subtracted from that of low multiplicity events to reduce correaltions due to jets.