Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at
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Charged jet production cross sections in p–Pb collisions at hmlsrc">he MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si1.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=401774e964d685e61d2f08793341b088">height="17" width="103" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S037026931500564X-si1.gif">hContainer hidden">hCode">h altimg="si1.gif" overflow="scroll">shvariant="normal">NN=5.02 TeVh> measured with the ALICE detector at the LHC are presented. Using the anti-hmlsrc">hImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si2.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=048998ea66ecfc276a65840ff350cbc7" title="Click to view the MathML source">kThContainer hidden">hCode">h altimg="si2.gif" overflow="scroll">khvariant="normal">Th> algorithm, jets have been reconstructed in the central rapidity region from charged particles with resolution parameters hmlsrc">hImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si3.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=eb13754e81be5a20aeb5ea79e7bb4f5d" title="Click to view the MathML source">R=0.2hContainer hidden">hCode">h altimg="si3.gif" overflow="scroll">R=0.2h> and hmlsrc">hImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si25.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=712ba53204ae700960f35bc6ce5fcf2d" title="Click to view the MathML source">R=0.4hContainer hidden">hCode">h altimg="si25.gif" overflow="scroll">R=0.4h>. The reconstructed jets have been corrected for detector effects and the underlying event background. To calculate the nuclear modification factor, hmlsrc">hImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si5.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=486b5d917d715b728c288b58a5267bb5" title="Click to view the MathML source">RpPbhContainer hidden">hCode">h altimg="si5.gif" overflow="scroll">Rhvariant="normal">pPbh>, of charged jets in p–Pb collisions, a pp reference was constructed by scaling previously measured charged jet spectra at hmlsrc">he MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si6.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=faa3cfb6cd777c391a5fbd6d6367f144">height="17" width="69" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S037026931500564X-si6.gif">hContainer hidden">hCode">h altimg="si6.gif" overflow="scroll">s=7 TeVh>. In the transverse momentum range hmlsrc">he MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si7.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=b127f0f18ef01fb86dd2783070bc52ec">height="16" width="158" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S037026931500564X-si7.gif">hContainer hidden">hCode">h altimg="si7.gif" overflow="scroll">20phvariant="normal">T,h="0.2em">hvariant="normal">chh="0.25em">hvariant="normal">jet120 GeVhy="false">/ch>, hmlsrc">hImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si5.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=486b5d917d715b728c288b58a5267bb5" title="Click to view the MathML source">RpPbhContainer hidden">hCode">h altimg="si5.gif" overflow="scroll">Rhvariant="normal">pPbh> is found to be consistent with unity, indicating the absence of strong nuclear matter effects on jet production. Major modifications to the radial jet structure are probed via the ratio of jet production cross sections reconstructed with the two different resolution parameters. This ratio is found to be similar to the measurement in pp collisions at hmlsrc">he MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si6.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=faa3cfb6cd777c391a5fbd6d6367f144">height="17" width="69" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S037026931500564X-si6.gif">hContainer hidden">hCode">h altimg="si6.gif" overflow="scroll">s=7 TeVh> and to the expectations from PYTHIA pp simulations and NLO pQCD calculations at hmlsrc">he MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S037026931500564X&_mathId=si1.gif&_user=111111111&_pii=S037026931500564X&_rdoc=1&_issn=03702693&md5=401774e964d685e61d2f08793341b088">height="17" width="103" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S037026931500564X-si1.gif">hContainer hidden">hCode">h altimg="si1.gif" overflow="scroll">shvariant="normal">NN=5.02 TeVh>.

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