Cargando…
Measurement of inclusive forward neutron production cross section in proton-proton collisions at $\sqrt{s} = 13$~TeV with the LHCf Arm2 detector
In this paper, we report the measurement relative to the production of forward neutrons in proton-proton collisions at $ \sqrt{s}=13 $ TeV obtained using the LHCf Arm2 detector at the Large Hadron Collider. The results for the inclusive differential production cross section are presented as a functi...
Autores principales: | , , , , , , , , , , , , , , , , , , , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2018
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP11(2018)073 http://cds.cern.ch/record/2636348 |
_version_ | 1780959870178033664 |
---|---|
author | Adriani, O. Berti, E. Bonechi, L. Bongi, M. D'Alessandro, R. Detti, S. Haguenauer, M. Itow, Y. Kasahara, K. Makino, Y. Masuda, K. Menjo, H. Muraki, Y. Ohashi, K. Papini, P. Ricciarini, S. Sako, T. Sakurai, N. Sato, K. Shinoda, M. Suzuki, T. Tamura, T. Tiberio, A. Torii, S. Tricomi, A. Turner, W.C. Ueno, M. Zhou, Q.D. |
author_facet | Adriani, O. Berti, E. Bonechi, L. Bongi, M. D'Alessandro, R. Detti, S. Haguenauer, M. Itow, Y. Kasahara, K. Makino, Y. Masuda, K. Menjo, H. Muraki, Y. Ohashi, K. Papini, P. Ricciarini, S. Sako, T. Sakurai, N. Sato, K. Shinoda, M. Suzuki, T. Tamura, T. Tiberio, A. Torii, S. Tricomi, A. Turner, W.C. Ueno, M. Zhou, Q.D. |
author_sort | Adriani, O. |
collection | CERN |
description | In this paper, we report the measurement relative to the production of forward neutrons in proton-proton collisions at $ \sqrt{s}=13 $ TeV obtained using the LHCf Arm2 detector at the Large Hadron Collider. The results for the inclusive differential production cross section are presented as a function of energy in three different pseudorapidity regions: η > 10.76, 8.99 < η < 9.22 and 8.81 < η < 8.99. The analysis was performed using a data set acquired in June 2015 that corresponds to an integrated luminosity of 0.194 nb$^{−1}$. The measurements were compared with the predictions of several hadronic interaction models used to simulate air showers generated by Ultra High Energy Cosmic Rays. None of these generators showed good agreement with the data for all pseudorapidity intervals. For η > 10.76, no model is able to reproduce the observed peak structure at around 5 TeV and all models underestimate the total production cross section: among them, QGSJET II-04 shows the smallest deficit with respect to data for the whole energy range. For 8.99 < η < 9.22 and 8.81 < η < 8.99, the models having the best overall agreement with data are SIBYLL 2.3 and EPOS-LHC, respectively: in particular, in both regions SIBYLL 2.3 is able to reproduce the observed peak structure at around 1.5–2.5 TeV. |
id | cern-2636348 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2018 |
record_format | invenio |
spelling | cern-26363482022-06-30T11:30:33Zdoi:10.1007/JHEP11(2018)073http://cds.cern.ch/record/2636348engAdriani, O.Berti, E.Bonechi, L.Bongi, M.D'Alessandro, R.Detti, S.Haguenauer, M.Itow, Y.Kasahara, K.Makino, Y.Masuda, K.Menjo, H.Muraki, Y.Ohashi, K.Papini, P.Ricciarini, S.Sako, T.Sakurai, N.Sato, K.Shinoda, M.Suzuki, T.Tamura, T.Tiberio, A.Torii, S.Tricomi, A.Turner, W.C.Ueno, M.Zhou, Q.D.Measurement of inclusive forward neutron production cross section in proton-proton collisions at $\sqrt{s} = 13$~TeV with the LHCf Arm2 detectorParticle Physics - Experimenthep-exIn this paper, we report the measurement relative to the production of forward neutrons in proton-proton collisions at $ \sqrt{s}=13 $ TeV obtained using the LHCf Arm2 detector at the Large Hadron Collider. The results for the inclusive differential production cross section are presented as a function of energy in three different pseudorapidity regions: η > 10.76, 8.99 < η < 9.22 and 8.81 < η < 8.99. The analysis was performed using a data set acquired in June 2015 that corresponds to an integrated luminosity of 0.194 nb$^{−1}$. The measurements were compared with the predictions of several hadronic interaction models used to simulate air showers generated by Ultra High Energy Cosmic Rays. None of these generators showed good agreement with the data for all pseudorapidity intervals. For η > 10.76, no model is able to reproduce the observed peak structure at around 5 TeV and all models underestimate the total production cross section: among them, QGSJET II-04 shows the smallest deficit with respect to data for the whole energy range. For 8.99 < η < 9.22 and 8.81 < η < 8.99, the models having the best overall agreement with data are SIBYLL 2.3 and EPOS-LHC, respectively: in particular, in both regions SIBYLL 2.3 is able to reproduce the observed peak structure at around 1.5–2.5 TeV.In this paper, we report the measurement relative to the production of forward neutrons in proton-proton collisions at $\mathrm{\sqrt{s} = 13~TeV}$ obtained using the LHCf Arm2 detector at the Large Hadron Collider. The results for the inclusive differential production cross section are presented as a function of energy in three different pseudorapidity regions: $\eta > 10.76$, $8.99 < \eta < 9.22$ and $8.81 < \eta < 8.99$. The analysis was performed using a data set acquired in June 2015 that corresponds to an integrated luminosity of $\mathrm{0.194~nb^{-1}}$. The measurements were compared with the predictions of several hadronic interaction models used to simulate air showers generated by Ultra High Energy Cosmic Rays. None of these generators showed good agreement with the data for all pseudorapidity intervals. For $\eta > 10.76$, no model is able to reproduce the observed peak structure at around $\mathrm{5~TeV}$ and all models underestimate the total production cross section: among them, QGSJET II-04 shows the smallest deficit with respect to data for the whole energy range. For $8.99 < \eta < 9.22$ and $8.81 < \eta < 8.99$, the models having the best overall agreement with data are SIBYLL 2.3 and EPOS-LHC, respectively: in particular, in both regions SIBYLL 2.3 is able to reproduce the observed peak structure at around $\mathrm{1.5-2.5~TeV}$.arXiv:1808.09877CERN-EP-2018-239oai:cds.cern.ch:26363482018-08-28 |
spellingShingle | Particle Physics - Experiment hep-ex Adriani, O. Berti, E. Bonechi, L. Bongi, M. D'Alessandro, R. Detti, S. Haguenauer, M. Itow, Y. Kasahara, K. Makino, Y. Masuda, K. Menjo, H. Muraki, Y. Ohashi, K. Papini, P. Ricciarini, S. Sako, T. Sakurai, N. Sato, K. Shinoda, M. Suzuki, T. Tamura, T. Tiberio, A. Torii, S. Tricomi, A. Turner, W.C. Ueno, M. Zhou, Q.D. Measurement of inclusive forward neutron production cross section in proton-proton collisions at $\sqrt{s} = 13$~TeV with the LHCf Arm2 detector |
title | Measurement of inclusive forward neutron production cross section in proton-proton collisions at $\sqrt{s} = 13$~TeV with the LHCf Arm2 detector |
title_full | Measurement of inclusive forward neutron production cross section in proton-proton collisions at $\sqrt{s} = 13$~TeV with the LHCf Arm2 detector |
title_fullStr | Measurement of inclusive forward neutron production cross section in proton-proton collisions at $\sqrt{s} = 13$~TeV with the LHCf Arm2 detector |
title_full_unstemmed | Measurement of inclusive forward neutron production cross section in proton-proton collisions at $\sqrt{s} = 13$~TeV with the LHCf Arm2 detector |
title_short | Measurement of inclusive forward neutron production cross section in proton-proton collisions at $\sqrt{s} = 13$~TeV with the LHCf Arm2 detector |
title_sort | measurement of inclusive forward neutron production cross section in proton-proton collisions at $\sqrt{s} = 13$~tev with the lhcf arm2 detector |
topic | Particle Physics - Experiment hep-ex |
url | https://dx.doi.org/10.1007/JHEP11(2018)073 http://cds.cern.ch/record/2636348 |
work_keys_str_mv | AT adrianio measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT bertie measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT bonechil measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT bongim measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT dalessandror measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT dettis measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT haguenauerm measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT itowy measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT kasaharak measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT makinoy measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT masudak measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT menjoh measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT murakiy measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT ohashik measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT papinip measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT ricciarinis measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT sakot measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT sakurain measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT satok measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT shinodam measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT suzukit measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT tamurat measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT tiberioa measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT toriis measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT tricomia measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT turnerwc measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT uenom measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector AT zhouqd measurementofinclusiveforwardneutronproductioncrosssectioninprotonprotoncollisionsatsqrts13tevwiththelhcfarm2detector |