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{
"@context": "https://schema.org/",
"@id": 262777,
"@type": "ScholarlyArticle",
"creator": [
{
"@type": "Person",
"affiliation": "CERN",
"name": "CERN \u0130\u015fbirli\u011fi"
}
],
"datePublished": "2022-01-01",
"description": "<p>The first results on K$^{\u204e}$(892)$^{\u00b1}$ resonance production in inelastic pp collisions at LHC energies of $\\sqrt{s}=5.02$, 8, and 13 TeV are presented. The K$^{\u204e}$(892)$^{\u00b1}$ has been reconstructed via its hadronic decay channel ${K}^{\u204e}$(892)${}^{\u00b1}\\to {K}_{S}^{0}+{\\pi }^{\u00b1}$ with the ALICE detector. Measurements of transverse momentum distributions, ${p}_{T}$-integrated yields, and mean transverse momenta for charged K$^{\u204e}$(892) are found to be consistent with previous ALICE measurements for neutral K$^{\u204e}$(892) within uncertainties. For ${p}_{T}>1$ GeV/c the K$^{\u204e}$(892)$^{\u00b1}$ transverse momentum spectra become harder with increasing centre-of-mass energy from 5.02 to 13 TeV, similar to what previously observed for charged kaons and pions. For ${p}_{T}<1$ GeV/c the K$^{\u204e}$(892)$^{\u00b1}$ yield does not evolve significantly and the abundance of K$^{\u204e}$(892)$^{\u00b1}$ relative to K is rather independent of the collision energy. The transverse momentum spectra, measured for K$^{\u204e}$(892)$^{\u00b1}$ at midrapidity in the interval 0 < ${p}_{T}<15$ GeV/c, are not well described by predictions of different versions of PYTHIA 6, PYTHIA 8 and EPOS-LHC event generators. These generators reproduce the measured ${p}_{T}$-integrated K$^{\u204e\u00b1}$/K ratios and describe well the momentum dependence for ${p}_{T}<2$ GeV/c.</p>",
"headline": "Measurement of K (892) production in inelastic pp collisions at the LHC",
"identifier": 262777,
"image": "https://aperta.ulakbim.gov.tr/static/img/logo/aperta_logo_with_icon.svg",
"license": "http://www.opendefinition.org/licenses/cc-by",
"name": "Measurement of K (892) production in inelastic pp collisions at the LHC",
"url": "https://aperta.ulakbim.gov.tr/record/262777"
}
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