cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.60001.v1/t5
title: "Table 5" of "Measurement of prompt J/psi and beauty hadron production cross sections at mid-rapidity in pp collisions at sort(s)= 7 TeV"

description: The integrated cross section for J/PSI from b-hadrons in the |y| region &lt; 0.9 as a function of PT. 
The the second (sys) error is the extrapolation systematic error.
description: CERN-LHC. Measurement of the differential and integrated cross sections for prompt and non-prompt J/PSI production in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data cover the mid-rapidity region with |y|&lt;0.9 and are presented as a function of PT. The data is obtained from a sample of integrated luminosity 5.6nb-1 with J/PSI particles identified through their decay to electron pairs. The sample is separated into prompt and non-prompt production through determining the fraction of J/PSIs from the decay of long-lived b-hadrons.
DOI: 10.17182/hepdata.60001.v1/t6
title: "Table 6" of "Measurement of prompt J/psi and beauty hadron production cross sections at mid-rapidity in pp collisions at sort(s)= 7 TeV"

description: The cross section for b-bbar production in the |y| region &lt; 0.9 integrated over PT. 
The the second (sys) error is the extrapolation systematic error.
description: CERN-LHC. Measurement of the differential and integrated cross sections for prompt and non-prompt J/PSI production in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data cover the mid-rapidity region with |y|&lt;0.9 and are presented as a function of PT. The data is obtained from a sample of integrated luminosity 5.6nb-1 with J/PSI particles identified through their decay to electron pairs. The sample is separated into prompt and non-prompt production through determining the fraction of J/PSIs from the decay of long-lived b-hadrons.
DOI: 10.17182/hepdata.60001.v1/t7
title: "Table 7" of "Measurement of prompt J/psi and beauty hadron production cross sections at mid-rapidity in pp collisions at sort(s)= 7 TeV"

description: The cross section for b-bbar production integrated over PT and rapidity. 
The the second (sys) error is the extrapolation systematic error.
description: CERN-LHC. Measurement of the differential and integrated cross sections for prompt and non-prompt J/PSI production in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data cover the mid-rapidity region with |y|&lt;0.9 and are presented as a function of PT. The data is obtained from a sample of integrated luminosity 5.6nb-1 with J/PSI particles identified through their decay to electron pairs. The sample is separated into prompt and non-prompt production through determining the fraction of J/PSIs from the decay of long-lived b-hadrons.
DOI: 10.17182/hepdata.60017.v1/t1
title: "Table 1" of "Search for diphoton events with large missing transverse momentum in 7 TeV proton-proton collision data with the ATLAS detector"

description: Observeded limit on gluino mass as function of LSP mass for the GGM model.
description: CERN-LHC. This paper reports the results of a search for diphoton events with substantial missing transverse momentum produced in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample used has an integrated luminosity of 4.8 fb-1 and the results are interpreted in the contect of three models: 
A general model of gauge-mediated supersymmetry breaking (GGM) 
A minimal model of gauge-mediated supersymmetry breaking (SPS8) 
A model with one universal extra dimension (UED) 
See the text of the paper for details.
DOI: 10.17182/hepdata.60017.v1/t2
title: "Table 2" of "Search for diphoton events with large missing transverse momentum in 7 TeV proton-proton collision data with the ATLAS detector"

description: Limit on squark mass as function of LSP mass for the GGM model.
description: CERN-LHC. This paper reports the results of a search for diphoton events with substantial missing transverse momentum produced in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample used has an integrated luminosity of 4.8 fb-1 and the results are interpreted in the contect of three models: 
A general model of gauge-mediated supersymmetry breaking (GGM) 
A minimal model of gauge-mediated supersymmetry breaking (SPS8) 
A model with one universal extra dimension (UED) 
See the text of the paper for details.
DOI: 10.17182/hepdata.60017.v1/t3
title: "Table 3" of "Search for diphoton events with large missing transverse momentum in 7 TeV proton-proton collision data with the ATLAS detector"

description: Cross section limit for the SPS8 model.
description: CERN-LHC. This paper reports the results of a search for diphoton events with substantial missing transverse momentum produced in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample used has an integrated luminosity of 4.8 fb-1 and the results are interpreted in the contect of three models: 
A general model of gauge-mediated supersymmetry breaking (GGM) 
A minimal model of gauge-mediated supersymmetry breaking (SPS8) 
A model with one universal extra dimension (UED) 
See the text of the paper for details.
DOI: 10.17182/hepdata.60017.v1/t4
title: "Table 4" of "Search for diphoton events with large missing transverse momentum in 7 TeV proton-proton collision data with the ATLAS detector"

description: Cross section x BR limit for the UED model.
description: CERN-LHC. This paper reports the results of a search for diphoton events with substantial missing transverse momentum produced in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample used has an integrated luminosity of 4.8 fb-1 and the results are interpreted in the contect of three models: 
A general model of gauge-mediated supersymmetry breaking (GGM) 
A minimal model of gauge-mediated supersymmetry breaking (SPS8) 
A model with one universal extra dimension (UED) 
See the text of the paper for details.
DOI: 10.17182/hepdata.60018.v1/t1
title: "Table 1" of "Measurement of Bose-Einstein Correlations in pp Collisions at sqrt(s)=0.9 and 7 TeV"

description: The double ratio R_double at 900 and 7000 GeV.
description: CERN-LHC. Measurments of the Bose-Einstein correlations (BEC) between pairs of identical particles produced in proton-proton collisions at centre-of-mass energies of 0.9 and 7 TeV. The data used are minimum-bias events (4.2M at 0.9 TeV and 2.7M at 7 TeV) with charged particles required to have |eta| &lt; 2.4 and PT &gt; 200MeV. The following is a definition of the quantity measured:

R_double is defined as ratio between (DN/DQ)/(DNref/DQ) and the equivalent quantity from simulated Monte Carlo events (without BEC effects), where N is the number of 'real' events and Nref the number 'reference' events derived from combining identical particles from different events with similar charged particle multiplicites and in similar pseudorapidity regions. Q is the Lorentz-invariant quantity equal to the square-root of the negative squared difference in four momentum of the two identical particles. Assuming the particles to be predominantly pions, this is equal to the square-root of the difference in the squared invariant mass of the two particles and 4*the pion mass squared.

The data shows an enhancement of the number of pairs of same-sign charged particles with small relative momentum, the dependence of which is studied on kinematic and topological features.
DOI: 10.17182/hepdata.60018.v1/t2
title: "Table 2" of "Measurement of Bose-Einstein Correlations in pp Collisions at sqrt(s)=0.9 and 7 TeV"

description: The double ratio R_double at 7000 GeV in different bins of charged particle multiplicity and kT.
description: CERN-LHC. Measurments of the Bose-Einstein correlations (BEC) between pairs of identical particles produced in proton-proton collisions at centre-of-mass energies of 0.9 and 7 TeV. The data used are minimum-bias events (4.2M at 0.9 TeV and 2.7M at 7 TeV) with charged particles required to have |eta| &lt; 2.4 and PT &gt; 200MeV. The following is a definition of the quantity measured:

R_double is defined as ratio between (DN/DQ)/(DNref/DQ) and the equivalent quantity from simulated Monte Carlo events (without BEC effects), where N is the number of 'real' events and Nref the number 'reference' events derived from combining identical particles from different events with similar charged particle multiplicites and in similar pseudorapidity regions. Q is the Lorentz-invariant quantity equal to the square-root of the negative squared difference in four momentum of the two identical particles. Assuming the particles to be predominantly pions, this is equal to the square-root of the difference in the squared invariant mass of the two particles and 4*the pion mass squared.

The data shows an enhancement of the number of pairs of same-sign charged particles with small relative momentum, the dependence of which is studied on kinematic and topological features.
DOI: 10.17182/hepdata.60018.v1/t3
title: "Table 3" of "Measurement of Bose-Einstein Correlations in pp Collisions at sqrt(s)=0.9 and 7 TeV"

description: The double ratio R_double at 7000 GeV in different bins of charged particle multiplicity and kT.
description: CERN-LHC. Measurments of the Bose-Einstein correlations (BEC) between pairs of identical particles produced in proton-proton collisions at centre-of-mass energies of 0.9 and 7 TeV. The data used are minimum-bias events (4.2M at 0.9 TeV and 2.7M at 7 TeV) with charged particles required to have |eta| &lt; 2.4 and PT &gt; 200MeV. The following is a definition of the quantity measured:

R_double is defined as ratio between (DN/DQ)/(DNref/DQ) and the equivalent quantity from simulated Monte Carlo events (without BEC effects), where N is the number of 'real' events and Nref the number 'reference' events derived from combining identical particles from different events with similar charged particle multiplicites and in similar pseudorapidity regions. Q is the Lorentz-invariant quantity equal to the square-root of the negative squared difference in four momentum of the two identical particles. Assuming the particles to be predominantly pions, this is equal to the square-root of the difference in the squared invariant mass of the two particles and 4*the pion mass squared.

The data shows an enhancement of the number of pairs of same-sign charged particles with small relative momentum, the dependence of which is studied on kinematic and topological features.
DOI: 10.17182/hepdata.60018.v1/t4
title: "Table 4" of "Measurement of Bose-Einstein Correlations in pp Collisions at sqrt(s)=0.9 and 7 TeV"

description: The double ratio R_double at 7000 GeV in different bins of charged particle multiplicity and kT.
description: CERN-LHC. Measurments of the Bose-Einstein correlations (BEC) between pairs of identical particles produced in proton-proton collisions at centre-of-mass energies of 0.9 and 7 TeV. The data used are minimum-bias events (4.2M at 0.9 TeV and 2.7M at 7 TeV) with charged particles required to have |eta| &lt; 2.4 and PT &gt; 200MeV. The following is a definition of the quantity measured:

R_double is defined as ratio between (DN/DQ)/(DNref/DQ) and the equivalent quantity from simulated Monte Carlo events (without BEC effects), where N is the number of 'real' events and Nref the number 'reference' events derived from combining identical particles from different events with similar charged particle multiplicites and in similar pseudorapidity regions. Q is the Lorentz-invariant quantity equal to the square-root of the negative squared difference in four momentum of the two identical particles. Assuming the particles to be predominantly pions, this is equal to the square-root of the difference in the squared invariant mass of the two particles and 4*the pion mass squared.

The data shows an enhancement of the number of pairs of same-sign charged particles with small relative momentum, the dependence of which is studied on kinematic and topological features.
DOI: 10.17182/hepdata.60018.v1/t5
title: "Table 5" of "Measurement of Bose-Einstein Correlations in pp Collisions at sqrt(s)=0.9 and 7 TeV"

description: The double ratio R_double at 7000 GeV in different bins of charged particle multiplicity.
description: CERN-LHC. Measurments of the Bose-Einstein correlations (BEC) between pairs of identical particles produced in proton-proton collisions at centre-of-mass energies of 0.9 and 7 TeV. The data used are minimum-bias events (4.2M at 0.9 TeV and 2.7M at 7 TeV) with charged particles required to have |eta| &lt; 2.4 and PT &gt; 200MeV. The following is a definition of the quantity measured:

R_double is defined as ratio between (DN/DQ)/(DNref/DQ) and the equivalent quantity from simulated Monte Carlo events (without BEC effects), where N is the number of 'real' events and Nref the number 'reference' events derived from combining identical particles from different events with similar charged particle multiplicites and in similar pseudorapidity regions. Q is the Lorentz-invariant quantity equal to the square-root of the negative squared difference in four momentum of the two identical particles. Assuming the particles to be predominantly pions, this is equal to the square-root of the difference in the squared invariant mass of the two particles and 4*the pion mass squared.

The data shows an enhancement of the number of pairs of same-sign charged particles with small relative momentum, the dependence of which is studied on kinematic and topological features.
DOI: 10.17182/hepdata.60018.v1/t6
title: "Table 6" of "Measurement of Bose-Einstein Correlations in pp Collisions at sqrt(s)=0.9 and 7 TeV"

description: Parameters of the fit to the double ratio R_double at 900 GeV.
description: CERN-LHC. Measurments of the Bose-Einstein correlations (BEC) between pairs of identical particles produced in proton-proton collisions at centre-of-mass energies of 0.9 and 7 TeV. The data used are minimum-bias events (4.2M at 0.9 TeV and 2.7M at 7 TeV) with charged particles required to have |eta| &lt; 2.4 and PT &gt; 200MeV. The following is a definition of the quantity measured:

R_double is defined as ratio between (DN/DQ)/(DNref/DQ) and the equivalent quantity from simulated Monte Carlo events (without BEC effects), where N is the number of 'real' events and Nref the number 'reference' events derived from combining identical particles from different events with similar charged particle multiplicites and in similar pseudorapidity regions. Q is the Lorentz-invariant quantity equal to the square-root of the negative squared difference in four momentum of the two identical particles. Assuming the particles to be predominantly pions, this is equal to the square-root of the difference in the squared invariant mass of the two particles and 4*the pion mass squared.

The data shows an enhancement of the number of pairs of same-sign charged particles with small relative momentum, the dependence of which is studied on kinematic and topological features.
DOI: 10.17182/hepdata.60018.v1/t7
title: "Table 7" of "Measurement of Bose-Einstein Correlations in pp Collisions at sqrt(s)=0.9 and 7 TeV"

description: Parameters of the fit to the double ratio R_double at 7000 GeV.
description: CERN-LHC. Measurments of the Bose-Einstein correlations (BEC) between pairs of identical particles produced in proton-proton collisions at centre-of-mass energies of 0.9 and 7 TeV. The data used are minimum-bias events (4.2M at 0.9 TeV and 2.7M at 7 TeV) with charged particles required to have |eta| &lt; 2.4 and PT &gt; 200MeV. The following is a definition of the quantity measured:

R_double is defined as ratio between (DN/DQ)/(DNref/DQ) and the equivalent quantity from simulated Monte Carlo events (without BEC effects), where N is the number of 'real' events and Nref the number 'reference' events derived from combining identical particles from different events with similar charged particle multiplicites and in similar pseudorapidity regions. Q is the Lorentz-invariant quantity equal to the square-root of the negative squared difference in four momentum of the two identical particles. Assuming the particles to be predominantly pions, this is equal to the square-root of the difference in the squared invariant mass of the two particles and 4*the pion mass squared.

The data shows an enhancement of the number of pairs of same-sign charged particles with small relative momentum, the dependence of which is studied on kinematic and topological features.
DOI: 10.17182/hepdata.60030.v1/t1
title: "Table 1" of "Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA"

description: The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0003 and Q^2=3.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.
description: DESY-HERA. Measurements of the reduced cross section in the process
 E P --&gt; E X Y where Y is a proton or low mass excitation with mass &lt; 1.6 GeV.
 The analysis covers the phase space region 3 &lt; Q^2 &lt; 1600 GeV^2, 
 |t| &lt; 1.0 GeV^2 and the longitudinal momentum fraction of the incident proton
 carried by the colourless exchange, X(POMERON) &lt; 0.05. The data is presented 
 as functions of X(POMERON), Q^2 and BETA=X/X(POMERON).
DOI: 10.17182/hepdata.60030.v1/t2
title: "Table 2" of "Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA"

description: The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0003 and Q^2=5.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.
description: DESY-HERA. Measurements of the reduced cross section in the process
 E P --&gt; E X Y where Y is a proton or low mass excitation with mass &lt; 1.6 GeV.
 The analysis covers the phase space region 3 &lt; Q^2 &lt; 1600 GeV^2, 
 |t| &lt; 1.0 GeV^2 and the longitudinal momentum fraction of the incident proton
 carried by the colourless exchange, X(POMERON) &lt; 0.05. The data is presented 
 as functions of X(POMERON), Q^2 and BETA=X/X(POMERON).
DOI: 10.17182/hepdata.60030.v1/t3
title: "Table 3" of "Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA"

description: The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0003 and Q^2=6.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.
description: DESY-HERA. Measurements of the reduced cross section in the process
 E P --&gt; E X Y where Y is a proton or low mass excitation with mass &lt; 1.6 GeV.
 The analysis covers the phase space region 3 &lt; Q^2 &lt; 1600 GeV^2, 
 |t| &lt; 1.0 GeV^2 and the longitudinal momentum fraction of the incident proton
 carried by the colourless exchange, X(POMERON) &lt; 0.05. The data is presented 
 as functions of X(POMERON), Q^2 and BETA=X/X(POMERON).
DOI: 10.17182/hepdata.60030.v1/t4
title: "Table 4" of "Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA"

description: The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0003 and Q^2=8.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.
description: DESY-HERA. Measurements of the reduced cross section in the process
 E P --&gt; E X Y where Y is a proton or low mass excitation with mass &lt; 1.6 GeV.
 The analysis covers the phase space region 3 &lt; Q^2 &lt; 1600 GeV^2, 
 |t| &lt; 1.0 GeV^2 and the longitudinal momentum fraction of the incident proton
 carried by the colourless exchange, X(POMERON) &lt; 0.05. The data is presented 
 as functions of X(POMERON), Q^2 and BETA=X/X(POMERON).
DOI: 10.17182/hepdata.60030.v1/t5
title: "Table 5" of "Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA"

description: The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0003 and Q^2=12.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.
description: DESY-HERA. Measurements of the reduced cross section in the process
 E P --&gt; E X Y where Y is a proton or low mass excitation with mass &lt; 1.6 GeV.
 The analysis covers the phase space region 3 &lt; Q^2 &lt; 1600 GeV^2, 
 |t| &lt; 1.0 GeV^2 and the longitudinal momentum fraction of the incident proton
 carried by the colourless exchange, X(POMERON) &lt; 0.05. The data is presented 
 as functions of X(POMERON), Q^2 and BETA=X/X(POMERON).
DOI: 10.17182/hepdata.60030.v1/t6
title: "Table 6" of "Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA"

description: The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=3.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.
description: DESY-HERA. Measurements of the reduced cross section in the process
 E P --&gt; E X Y where Y is a proton or low mass excitation with mass &lt; 1.6 GeV.
 The analysis covers the phase space region 3 &lt; Q^2 &lt; 1600 GeV^2, 
 |t| &lt; 1.0 GeV^2 and the longitudinal momentum fraction of the incident proton
 carried by the colourless exchange, X(POMERON) &lt; 0.05. The data is presented 
 as functions of X(POMERON), Q^2 and BETA=X/X(POMERON).
DOI: 10.17182/hepdata.60030.v1/t7
title: "Table 7" of "Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA"

description: The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=5.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.
description: DESY-HERA. Measurements of the reduced cross section in the process
 E P --&gt; E X Y where Y is a proton or low mass excitation with mass &lt; 1.6 GeV.
 The analysis covers the phase space region 3 &lt; Q^2 &lt; 1600 GeV^2, 
 |t| &lt; 1.0 GeV^2 and the longitudinal momentum fraction of the incident proton
 carried by the colourless exchange, X(POMERON) &lt; 0.05. The data is presented 
 as functions of X(POMERON), Q^2 and BETA=X/X(POMERON).
DOI: 10.17182/hepdata.60030.v1/t8
title: "Table 8" of "Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA"

description: The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=6.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.
description: DESY-HERA. Measurements of the reduced cross section in the process
 E P --&gt; E X Y where Y is a proton or low mass excitation with mass &lt; 1.6 GeV.
 The analysis covers the phase space region 3 &lt; Q^2 &lt; 1600 GeV^2, 
 |t| &lt; 1.0 GeV^2 and the longitudinal momentum fraction of the incident proton
 carried by the colourless exchange, X(POMERON) &lt; 0.05. The data is presented 
 as functions of X(POMERON), Q^2 and BETA=X/X(POMERON).
DOI: 10.17182/hepdata.60030.v1/t10
title: "Table 10" of "Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA"

description: The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=12.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.
description: DESY-HERA. Measurements of the reduced cross section in the process
 E P --&gt; E X Y where Y is a proton or low mass excitation with mass &lt; 1.6 GeV.
 The analysis covers the phase space region 3 &lt; Q^2 &lt; 1600 GeV^2, 
 |t| &lt; 1.0 GeV^2 and the longitudinal momentum fraction of the incident proton
 carried by the colourless exchange, X(POMERON) &lt; 0.05. The data is presented 
 as functions of X(POMERON), Q^2 and BETA=X/X(POMERON).