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CERN İşbirliği
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<identifier identifierType="URL">https://aperta.ulakbim.gov.tr/record/107153</identifier>
<creators>
<creator>
<creatorName>CERN İşbirliği</creatorName>
<affiliation>CERN</affiliation>
</creator>
</creators>
<titles>
<title>Performance Of The Atlas Track Reconstruction Algorithms In Dense Environments In Lhc Run 2</title>
</titles>
<publisher>Aperta</publisher>
<publicationYear>2017</publicationYear>
<dates>
<date dateType="Issued">2017-01-01</date>
</dates>
<resourceType resourceTypeGeneral="Text">Journal article</resourceType>
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<alternateIdentifier alternateIdentifierType="url">https://aperta.ulakbim.gov.tr/record/107153</alternateIdentifier>
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<relatedIdentifiers>
<relatedIdentifier relatedIdentifierType="DOI" relationType="IsIdenticalTo">10.1140/epjc/s10052-017-5225-7</relatedIdentifier>
</relatedIdentifiers>
<rightsList>
<rights rightsURI="http://www.opendefinition.org/licenses/cc-by">Creative Commons Attribution</rights>
<rights rightsURI="info:eu-repo/semantics/openAccess">Open Access</rights>
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<descriptions>
<description descriptionType="Abstract"><p>With the increase in energy of the Large Hadron Collider to a centre-of-mass energy of 13 $\text{TeV}$ for Run 2, events with dense environments, such as in the cores of high-energy jets, became a focus for new physics searches as well as measurements of the Standard Model. These environments are characterized by charged-particle separations of the order of the tracking detectors sensor granularity. Basic track quantities are compared between 3.2 fb ${}^{-1}$ of data collected by the ATLAS experiment and simulation of proton–proton collisions producing high-transverse-momentum jets at a centre-of-mass energy of 13 $\text{TeV}$ . The impact of charged-particle separations and multiplicities on the track reconstruction performance is discussed. The track reconstruction efficiency in the cores of jets with transverse momenta between 200 and 1600 $\text{GeV}$ is quantified using a novel, data-driven, method. The method uses the energy loss, $\phantom{\rule{0.333333em}{0ex}}\text{d}E/dx$ , to identify pixel clusters originating from two charged particles. Of the charged particles creating these clusters, the measured fraction that fail to be reconstructed is $0.061±0.006\phantom{\rule{4pt}{0ex}}\text{(stat.)}±0.014\phantom{\rule{4pt}{0ex}}\text{(syst.)}$ and $0.093±0.017\phantom{\rule{4pt}{0ex}}\text{(stat.)}±0.021\phantom{\rule{4pt}{0ex}}\text{(syst.)}$ for jet transverse momenta of 200–400 $\text{GeV}$ and 1400–1600 $\text{GeV}$ , respectively.</p></description>
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