cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.58497.v1/t4
title: "Table 4" of "Rapidity gap cross sections measured with the ATLAS detector in pp collisions at sqrt(s) = 7 TeV"

description: The inelastic cross section differential in the forward rapidity gap size, DELTA(C=RAPGAP) for a maximum observed particle transverse momentum of 800 MeV in the gap.
description: CERN-LHC. Measurement of the pseudorapidity gap distributions in proton-proton collisions at a centre-of-mass energy of 7 TeV with a minumim bias data sample of integrated luminosity 7.1 mub-1. The pseudorapidity gap variable , denoted here as DELTA(C=RAPGAP), is defined as the larger of the pseudorapidity regions extending to the limits of the ATLAS detector sensitivity at eta=+-4.9, in which no final state particles are observed above a transverse momentum threshold, PT(CUT). The measurements span the region in DELTA(C=RAPGAP) from 0 to 8 for PT(CUT) from 200 to 800 MeV. 
 
In the tables the last nine columns show the following percentage uncertainties: 
 
dpy6: uncertainty due to modelling of final state particle production.
dpho: uncertainty due to modelling of the xi_X and xi_Y and t dependencies.
de+: the upward uncertainty due to variations in the relative energy scales.
de-: the downward uncertainty due to variations in the relative energy scales.
dsd: the upward uncertainty due to the enhancing of the SS/DD cross section ratio.
ddd: the downward uncertainty dur to the reducing of the SS/DD cross section ratio.
dcd: the uncertainty om the variation of the CD cross section in the unfolding procedure.
dmat: the uncertainty in the amount of dead material in the tracking region.
dmbts the uncertainty in the minumum bias trigger system response

The overall systematic errors reported are the quadratic sum of the positive and negative elements of these individual systematic errors, including the 3.4% luminosity uncertainty. The errors in dpy6, dpho, dcd, dmat and dmbts are treated symmetrically and the errors in de+ and dsd are included in the positive error and de- and ddd in the negative, except where the sign of the error is negative in which case they are included in the opposite polarity error 

Note added 12/2/2014:
The cross section values reported in the tables should be multiplied by factor 1.0187 to take into account the updated value of the integrated luminosity for ATLAS 2010 data taking period. The uncertainty on the global normalisation ('Lumi') increases slightly from 3.4% to 3.5%.See Eur.Phys.J. C73 (2013) 2518 for more detail.
DOI: 10.17182/hepdata.58497.v1/t5
title: "Table 5" of "Rapidity gap cross sections measured with the ATLAS detector in pp collisions at sqrt(s) = 7 TeV"

description: The inelastic cross section excluding diffractive processes with xi_X &lt; xi_cut, obtained by integration of the differential cross section from gap sizes zero to a variable maximum. Here xi_X is the variable (M_X)**2/S and for SD data DELTA(C=RAPGAP)~=-ln(xi_X). The errors shown are the total errors excluding the 3.4% luminosity uncertainty.
description: CERN-LHC. Measurement of the pseudorapidity gap distributions in proton-proton collisions at a centre-of-mass energy of 7 TeV with a minumim bias data sample of integrated luminosity 7.1 mub-1. The pseudorapidity gap variable , denoted here as DELTA(C=RAPGAP), is defined as the larger of the pseudorapidity regions extending to the limits of the ATLAS detector sensitivity at eta=+-4.9, in which no final state particles are observed above a transverse momentum threshold, PT(CUT). The measurements span the region in DELTA(C=RAPGAP) from 0 to 8 for PT(CUT) from 200 to 800 MeV. 
 
In the tables the last nine columns show the following percentage uncertainties: 
 
dpy6: uncertainty due to modelling of final state particle production.
dpho: uncertainty due to modelling of the xi_X and xi_Y and t dependencies.
de+: the upward uncertainty due to variations in the relative energy scales.
de-: the downward uncertainty due to variations in the relative energy scales.
dsd: the upward uncertainty due to the enhancing of the SS/DD cross section ratio.
ddd: the downward uncertainty dur to the reducing of the SS/DD cross section ratio.
dcd: the uncertainty om the variation of the CD cross section in the unfolding procedure.
dmat: the uncertainty in the amount of dead material in the tracking region.
dmbts the uncertainty in the minumum bias trigger system response

The overall systematic errors reported are the quadratic sum of the positive and negative elements of these individual systematic errors, including the 3.4% luminosity uncertainty. The errors in dpy6, dpho, dcd, dmat and dmbts are treated symmetrically and the errors in de+ and dsd are included in the positive error and de- and ddd in the negative, except where the sign of the error is negative in which case they are included in the opposite polarity error 

Note added 12/2/2014:
The cross section values reported in the tables should be multiplied by factor 1.0187 to take into account the updated value of the integrated luminosity for ATLAS 2010 data taking period. The uncertainty on the global normalisation ('Lumi') increases slightly from 3.4% to 3.5%.See Eur.Phys.J. C73 (2013) 2518 for more detail.
DOI: 10.17182/hepdata.58503.v1/t1
title: "Table 1" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: B-jet cross section from the 'jet' analysis.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t2
title: "Table 2" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: B-jet cross section from the 'muon' analysis.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t3
title: "Table 3" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: B-jet cross section extrapolated from the 'muon' analysis.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t4
title: "Table 4" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 0.0 to 0.5, using a jet resolution R value of 0.5.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t6
title: "Table 6" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 1.0 to 1.5, using a jet resolution R value of 0.5.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t10
title: "Table 10" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: Inclusive b-jet differential cross sections in the |rapidity| range 0.0 to 2.4, using a jet resolution R value of 0.5.
Extrapolated result from muuon visible range PT(MU) &gt; 9 GeV and |pseudorapidity(MU)| &lt; 2.4.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t11
title: "Table 11" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: Inclusive b-jet (with muon) differential cross sections in the PT range greater than 30 GeV, using a jet resolution R value of 0.5. Muon visible range corresponds to PT(MU) &gt; 9 GeV and |pseudorapidity(MU)| &lt; 2.4.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t12
title: "Table 12" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: Inclusive b-jet differential cross sections in the PT range greater than 30 GeV, using a jet resolution R value of 0.5. Extrapolated result from muon visible range PT(MU) &gt; 9 GeV and |pseudorapidity(MU)| &lt; 2.4.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t5
title: "Table 5" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 0.5 to 1.0, using a jet resolution R value of 0.5.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t7
title: "Table 7" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 1.5 to 2.0, using a jet resolution R value of 0.5.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t8
title: "Table 8" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: Inclusive b-jet double-differential cross sections and their ratio to inclusive jet cross sections in the |rapidity| range 2.0 to 2.2, using a jet resolution R value of 0.5.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58503.v1/t9
title: "Table 9" of "Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV"

description: Inclusive b-jet (with muon) differential cross sections in the |rapidity| range 0.0 to 2.4, using a jet resolution R value of 0.5. Muon visible range corresponds to PT(MU) &gt; 9 GeV and |pseudorapidity(MU)| range 0.0 to 2.4.
description: CERN LHC. Measurement of the inclusive b-jet production cross section in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement is performed with two different analyses: a 'jet' analysis that selects events with b-jets using a sample with integrated luminosity 34 pb-1, and a 'muon' analysis requiring a b-jet with a muon using a sample with integrated luminosity 3 pb-1. In both, b-jets are identified from the secondary vertex of the b-jet using the anti-kt algorithm with a jet clustering distance of 0.5. The cross section is presented as a function of jet transverse momentum in the range 18 to 200 GeV for several jet rapidity intervals. Results are also given for the b-jet to inclusive-jet ratio. To compare the results from the two methods the data from the 'muon' analysis is extrapolated to the same visible phase-space as the 'jet' analysis using PYTHIA.
DOI: 10.17182/hepdata.58516.v1/t1
title: "Table 1" of "Search for scalar bottom pair production with the ATLAS detector in pp Collisions at sqrt{s} = 7 TeV"

description: Observed 95% CL exclusion limit in the sbottom-neutralino mass plane.
description: CERN-LHC. Search for pair production of the scalar partners of bottom quarks in proton-proton collisions at a centre-of-mass energy of 7 TeV with a data set of integrated total luminosity of 2.05 fb-1. Events with large missing transverse momentum and two jets in the final state, where both jets have a b-quark signature, are studied. The data is interpreted in the context of an R-parity conserving MSSM scenario. assuming that the scalar bottom decays exclusively into a bottom quark and a neutralino. 95% CL upper limits are presented in the sbottom-neutralino mass plane both with the renormalization and factorization scale = mu, and also varying it by factors of 2 up and down (ie mu/2 and 2*mu). These are compared with the expected limits.
DOI: 10.17182/hepdata.58516.v1/t2
title: "Table 2" of "Search for scalar bottom pair production with the ATLAS detector in pp Collisions at sqrt{s} = 7 TeV"

description: Observed 95% CL exclusion limit in the sbottom-neutralino mass plane with the renormalization and factorization scales set to mu/2.
description: CERN-LHC. Search for pair production of the scalar partners of bottom quarks in proton-proton collisions at a centre-of-mass energy of 7 TeV with a data set of integrated total luminosity of 2.05 fb-1. Events with large missing transverse momentum and two jets in the final state, where both jets have a b-quark signature, are studied. The data is interpreted in the context of an R-parity conserving MSSM scenario. assuming that the scalar bottom decays exclusively into a bottom quark and a neutralino. 95% CL upper limits are presented in the sbottom-neutralino mass plane both with the renormalization and factorization scale = mu, and also varying it by factors of 2 up and down (ie mu/2 and 2*mu). These are compared with the expected limits.
DOI: 10.17182/hepdata.58516.v1/t3
title: "Table 3" of "Search for scalar bottom pair production with the ATLAS detector in pp Collisions at sqrt{s} = 7 TeV"

description: Observed 95% CL exclusion limit in the sbottom-neutralino mass plane with the renormalization and factorization scales set to 2*mu.
description: CERN-LHC. Search for pair production of the scalar partners of bottom quarks in proton-proton collisions at a centre-of-mass energy of 7 TeV with a data set of integrated total luminosity of 2.05 fb-1. Events with large missing transverse momentum and two jets in the final state, where both jets have a b-quark signature, are studied. The data is interpreted in the context of an R-parity conserving MSSM scenario. assuming that the scalar bottom decays exclusively into a bottom quark and a neutralino. 95% CL upper limits are presented in the sbottom-neutralino mass plane both with the renormalization and factorization scale = mu, and also varying it by factors of 2 up and down (ie mu/2 and 2*mu). These are compared with the expected limits.
DOI: 10.17182/hepdata.58516.v1/t4
title: "Table 4" of "Search for scalar bottom pair production with the ATLAS detector in pp Collisions at sqrt{s} = 7 TeV"

description: Expected 95% CL exclusion limit in the sbottom-neutralino mass plane.
description: CERN-LHC. Search for pair production of the scalar partners of bottom quarks in proton-proton collisions at a centre-of-mass energy of 7 TeV with a data set of integrated total luminosity of 2.05 fb-1. Events with large missing transverse momentum and two jets in the final state, where both jets have a b-quark signature, are studied. The data is interpreted in the context of an R-parity conserving MSSM scenario. assuming that the scalar bottom decays exclusively into a bottom quark and a neutralino. 95% CL upper limits are presented in the sbottom-neutralino mass plane both with the renormalization and factorization scale = mu, and also varying it by factors of 2 up and down (ie mu/2 and 2*mu). These are compared with the expected limits.
DOI: 10.15468/dl.2va2kq
title: Occurrence Download

description: A dataset containing 239 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Reseda inodora"
 ]
}

 The dataset includes 239 records from 51 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015224-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.