cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.111055.v1/t6
title: "$\frac{\tau_{2}}{\tau_{1}}$ with Soft Drop in pp" of "First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV"

description: The $\tau_{2}/\tau_{1}$ (with Soft Drop) fully corrected data distributions for jetsin the jet transverse momentum range 40-60 GeV/c in pp collisions
description: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
DOI: 10.17182/hepdata.111055.v1/t7
title: "$\frac{\tau_{2}}{\tau_{1}}$ with $k_{T}$ reclustering in Pb-Pb" of "First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV"

description: The $\tau_{2}/\tau_{1}$ (with $k_{T}$) fully corrected data distributions for recoil jetsin the jet transverse momentum range 40-60 GeV/c in PbPb collisions
description: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
DOI: 10.17182/hepdata.111055.v1/t8
title: "$\frac{\tau_{2}}{\tau_{1}}$ with CA reclustering in Pb-Pb" of "First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV"

description: The $\tau_{2}/\tau_{1}$ (with C/A) fully corrected data distributions for recoil jetsin the jet transverse momentum range 40-60 GeV/c in PbPb collisions
description: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
DOI: 10.17182/hepdata.111055.v1/t9
title: "$\frac{\tau_{2}}{\tau_{1}}$ with Soft Drop in Pb-Pb" of "First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV"

description: The $\tau_{2}/\tau_{1}$ (with Soft Drop) fully corrected data distributions for recoil jetsin the jet transverse momentum range 40-60 GeV/c in PbPb collisions
description: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
DOI: 10.17182/hepdata.129148.v1/t1
title: "Table 1" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: The p$_{T}$ distribution of K*(892)$^{\pm}$ in inelastic pp collisions at
$\sqrt{s} = 13$ TeV. The data were collected in 2015 with an integrated luminosity of 0.92 nb$^{-1}$.
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.129148.v1/t2
title: "Table 2" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: The p$_{T}$ distribution of K*(892)$^{\pm}$ in inelastic pp collisions at
$\sqrt{s} = 8$ TeV. The data were collected in 2012 with an integrated luminosity of 1.25 nb$^{-1}$.
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.129148.v1/t3
title: "Table 3" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: The p$_{T}$ distribution of K*(892)$^{\pm}$ in inelastic pp collisions at
$\sqrt{s} = 5$ TeV. The data were collected in 2015 with an integrated luminosity of 2.12 nb$^{-1}$.
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.129148.v1/t4
title: "Table 4" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: The p$_{T}$ distribution of K$^{*\pm}$/K$^{*0}$ in inelastic pp collisions at
$\sqrt{s} = 13$ TeV. The p$_{T}$ distribution of K$^{*0}$ is taken from [3]. The systematic uncertanty due to global tracking, primary pions, material budget and hadronic interaction cross section are equal for charged and neutral K*, thus they cancel out in the propagation of the uncertainty to the final ratio.
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.129148.v1/t5
title: "Table 5" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: The p$_{T}$ distribution of K$^{*\pm}$/K$*^{0}$ in inelastic pp collisions at
$\sqrt{s} = 8$ TeV. The p$_{T}$ distribution of K$^{*0}$ is taken from [17]. The systematic uncertanty due to global tracking, primary pions, material budget and hadronic interaction cross section are equal for charged and neutral K*, thus they cancel out in the propagation of the uncertainty to the final ratio.
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.129148.v1/t6
title: "Table 6" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: The p$_{T}$ distribution of K$^{*\pm}$/K$*^{0}$ in inelastic pp collisions at
$\sqrt{s} = 5.02$ TeV. The p$_{T}$ distribution of K$^{*0}$ is taken from [11]. The systematic uncertanty due to global tracking, primary pions, material budget and hadronic interaction cross section are equal for charged and neutral K*, thus they cancel out in the propagation of the uncertainty to the final ratio.
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.129148.v1/t7
title: "Table 7" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: Ratio of p$_{T}$ distribution of K$^{*\pm}$ at $\sqrt{s} = 13$ TeV to the same distribution at $\sqrt{s} = 5.02$ TeV. The systematic uncertanty due to material budget and hadronic interaction cross section are equal for the two energies, thus they cancel out in the propagation of the uncertainty to the final ratio.
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.129148.v1/t10
title: "Table 10" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: The p$_{T}$ distribution of K$^{*\pm}$/K in inelastic pp collisions at
$\sqrt{s} = 5.02$ TeV. The p$_{T}$ distribution of K is taken from [33].
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.129148.v1/t8
title: "Table 8" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: Ratio of p$_{T}$ distribution of K$^{*\pm}$ at $\sqrt{s} = 8$ TeV to the same distribution at $\sqrt{s} = 5.02$ TeV. The systematic uncertanty due to material budget and hadronic interaction cross section are equal for the two energies, thus they cancel out in the propagation of the uncertainty to the final ratio.
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.129148.v1/t9
title: "Table 9" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: The p$_{T}$ distribution of K$^{*\pm}$/K in inelastic pp collisions at
$\sqrt{s} = 13$ TeV. The p$_{T}$ distribution of K is taken from [3].
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.