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Charged K* multiplicity dependent analysis in pp collisions at $\sqrt{s} =$ 13 TeV with ALICE (ANA-1237)

K$^{*\pm}$/K$^0_{s}$ double ratio: high multiplicity K$^{*\pm}$/K$^0_{s}$ $p$\textsubscript{T} spectrum divided by the low multiplicity one
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
Double_ratio_0.eps
Figure image (.pdf)
Double_ratio_0.pdf
K$^{*\pm}$ and K$^{*0}$ $p_{\rm T}$-integrated yields
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
dNdy_vsKzero.eps
Figure image (.pdf)
dNdy_vsKzero.pdf
K$^{*\pm}$ and K$^{*0}$ mean $p_{\rm T}$ spectra
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
meanpT_vsKzero.eps
Figure image (.pdf)
meanpT_vsKzero.pdf
K$^{*\pm}$ and K$^{*0}$ $p$\textsubscript{T} spectra
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
pTspectra_vsKzero_0.eps
Figure image (.pdf)
pTspectra_vsKzero_0.pdf
K$^0_{s}\pi^{\pm}$ invariant mass distribution after the uncorrelated background subtraction
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
Inv_Mass_after_0.eps
Figure image (.pdf)
Inv_Mass_after_0.pdf
K$^0_{s}$ $\pi^{\pm}$ invariant mass distribution
Energy
13 TeV
System
p-p
Scope: PWG
PWG-LF (Light Flavour Spectra)
Figure image (.eps)
Inv_Mass_before_0.eps
Figure image (.pdf)
Inv_Mass_before_0.pdf