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$\Xi$ baryon production vs multiplicity and effective energy in pp $\sqrt{s}$ = 13 TeV

Description

This includes $p_{\text{T}}$ spectra in ($\sqrt{s}$ - ZDC) effective energy classes, normalised yields and Pythia8 simulation studies.

$\Xi^{-}$ + $\bar{\Xi}^{+}$ $p_{\text{T}}$-spectra in ($\sqrt{s}$ - ZDC) and V0M classes in pp collisions at $\sqrt{s}$ = 13 TeV
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiCorrectedpTSpectra_ZDCV0M_LevyTsallis_1.eps
Figure image (.pdf)
XiCorrectedpTSpectra_ZDCV0M_LevyTsallis_1.pdf
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields to multiplicity (self-normalised to INEL>0) as a function of the average charged particle multiplicity
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiNormYieldsvsNch_V0MZDC_pp13TeV.eps
Figure image (.pdf)
XiNormYieldsvsNch_V0MZDC_pp13TeV.pdf
Ratio $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields to multiplicity (self-normalised to INEL>0) as a function of the percentile selection
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiNormYieldsvsperc_ZDCV0M_pp13TeV_2.eps
Figure image (.pdf)
XiNormYieldsvsperc_ZDCV0M_pp13TeV_2.pdf
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity as a function of the particle multiplicity
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiAvYieldsvsNch_V0MSel_pp13TeV_1.eps
Figure image (.pdf)
XiAvYieldsvsNch_V0MSel_pp13TeV_1.pdf
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity self-normalised to INEL>0 as a function of the charged particle multiplicity at midrapidity
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiNormYieldsvsNch_V0MSel_pp13TeV_1.eps
Figure image (.pdf)
XiNormYieldsvsNch_V0MSel_pp13TeV_1.pdf
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity as a function of the charged particle multiplicity at midrapidity
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiAvYieldsvsNch_ZDCSel_pp13TeV_1.eps
Figure image (.pdf)
XiAvYieldsvsNch_ZDCSel_pp13TeV_1.pdf
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity (self-normalised to INEL>0) as a function of the charged particle multiplicity at midrapidity
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiNormYieldsvsNch_ZDCSel_pp13TeV_1.eps
Figure image (.pdf)
XiNormYieldsvsNch_ZDCSel_pp13TeV_1.pdf
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity as a function of the percentile estimator
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiAvYieldsvsperc_V0MSel_pp13TeV_0.eps
Figure image (.pdf)
XiAvYieldsvsperc_V0MSel_pp13TeV_0.pdf
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity (self-normalised to INEL>0) as a function of the percentile estimator
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiNormYieldsvsperc_V0MSel_pp13TeV_1.eps
Figure image (.pdf)
XiNormYieldsvsperc_V0MSel_pp13TeV_1.pdf
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity as a function of the percentile estimator
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiAvYieldsvsperc_ZDCSel_pp13TeV_0.eps
Figure image (.pdf)
XiAvYieldsvsperc_ZDCSel_pp13TeV_0.pdf
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity (self-normalised to INEL>0) as a function of the percentile estimator
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
XiNormYieldsvsperc_ZDCSel_pp13TeV_0.eps
Figure image (.pdf)
XiNormYieldsvsperc_ZDCSel_pp13TeV_0.pdf
Expected correlation between average charged multiplicity at midrapidity and effective energy in V0M and ($\sqrt{s}$ - ZDC) standalone selections
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
SimNchvsEffEn_V0MZDCStandalone_pp13TeV_2.eps
Figure image (.pdf)
SimNchvsEffEn_V0MZDCStandalone_pp13TeV_2.pdf
Expected correlation between average charged multiplicity at midrapidity and effective energy in V0M and ($\sqrt{s}$ - ZDC) combined selections
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
SimNchvsEffEn_V0MZDCSel_pp13TeV_1.eps
Figure image (.pdf)
SimNchvsEffEn_V0MZDCSel_pp13TeV_1.pdf