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...

Descripción completa

Detalles Bibliográficos
Autores principales: 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.
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