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ItemPseudorapidity distribution of charged hadrons in proton–proton collisions at √s=13 TeV( 2015-12-17) Khachatryan, V. ; Sirunyan, A. M. ; Tumasyan, A. ; Adam, W. ; Asilar, E. ; Bergauer, T. ; Brandstetter, J. ; Brondolin, E. ; Dragicevic, M. ; Erö, J. ; Flechl, M. ; Friedl, M. ; Frühwirth, R. ; Ghete, V. M. ; Hartl, C. ; Hörmann, N. ; Hrubec, J. ; Jeitler, M. ; Knünz, V. ; König, A. ; Krammer, M. ; Krätschmer, I. ; Liko, D. ; Matsushita, T. ; Mikulec, I. ; Rabady, D. ; Rahbaran, B. ; Rohringer, H. ; Schieck, J. ; Schöfbeck, R. ; Strauss, J. ; Treberer-Treberspurg, W. ; Waltenberger, W. ; Wulz, C. E. ; Mossolov, V. ; Shumeiko, N. ; Suarez Gonzalez, J. ; Alderweireldt, S. ; Cornelis, T. ; De Wolf, E. A. ; Janssen, X. ; Knutsson, A. ; Lauwers, J. ; Luyckx, S. ; Van De Klundert, M. ; Van Haevermaet, H. ; Van Mechelen, P. ; Van Remortel, N. ; Van Spilbeeck, A. ; Abu Zeid, S. ; Blekman, F. ; D'Hondt, J. ; Daci, N. ; De Bruyn, I. ; Deroover, K. ; Heracleous, N. ; Keaveney, J. ; Lowette, S. ; Moreels, L. ; Olbrechts, A. ; Python, Q. ; Strom, D. ; Tavernier, S. ; Van Doninck, W. ; Van Mulders, P. ; Van Onsem, G. P. ; Van Parijs, I. ; Barria, P. ; Brun, H. ; Caillol, C. ; Clerbaux, B. ; De Lentdecker, G. ; Fasanella, G. ; Favart, L. ; Grebenyuk, A. ; Karapostoli, G. ; Lenzi, T. ; Léonard, A. ; Maerschalk, T. ; Marinov, A. ; Perniè, L. ; Randle-conde, A. ; Reis, T. ; Seva, T. ; Vander Velde, C. ; Vanlaer, P. ; Yonamine, R. ; Zenoni, F. ; Zhang, F. ; Beernaert, K. ; Benucci, L. ; Cimmino, A. ; Crucy, S. ; Dobur, D. ; Fagot, A. ; Garcia, G. ; Gul, M. ; Mccartin, J. ; Ocampo Rios, A. A. ; Poyraz, D.The pseudorapidity distribution of charged hadrons in pp collisions at s=13 TeV is measured using a data sample obtained with the CMS detector, operated at zero magnetic field, at the CERN LHC. The yield of primary charged long-lived hadrons produced in inelastic pp collisions is determined in the central region of the CMS pixel detector (|η| < 2) using both hit pairs and reconstructed tracks. For central pseudorapidities (|η| < 0.5), the charged-hadron multiplicity density is dNch/dη||η| < 0.5=5.49±0.01(stat)±0.17(syst), a value obtained by combining the two methods. The result is compared to predictions from Monte Carlo event generators and to similar measurements made at lower collision energies.