Proposal for the LHC Run 3 Addressing Cosmic Ray physics with forward measurements in proton – proton and proton – light nuclei collisions at LHC

The LHCf experiment was originally designed to measure neutral particles produced at very high pseudo-rapidity (η > 8.4) in p+ p collisions at an energy of 14 TeV in the center of mass frame and in p+A collision. Since the first activities at the LHC in 2009, the LHCf detectors have taken data in different conditions involving proton and ions with different energies. The measurements carried out so far concern p + p collisions at √ s=0.9, 2.76, 7 and 13 TeV and p+ Pb collisions at √ sNN=5 TeV and 8 TeV. These cases correspond to proton collisions in the laboratory frame with an equivalent energy ranging from 1014 eV to almost 1017 eV, thus covering a large energy range which is significant for the study of the highest energy cosmic-rays interactions with the atmosphere. These data are extremely useful for the calibration of hadronic interaction models used for the study of the development of atmospheric showers, the so called Extensive Air Showers (EAS), produced by extremely energetic cosmic-ray (CR) particles interacting with the atmospheric gas. Because of the characteristics of these collisions, the study of the p + p system only at LHC is not enough to have a complete picture of the real processes going on in the Earth atmosphere, where interactions involve mainly nitrogen and oxygen nuclei. The dynamic of p + N collisions can differ in many important aspects with respect to the more simple case of p+p interactions. For example, a significant reduction in the cross section in p+A with respect to p+p collisions, due to nuclear screening effects, has been found in previous measurements performed at smaller values of pseudo-rapidity and lower energy than the LHC; this reduction has been later confirmed by LHCf itself by comparing p+ p with p+ Pb interactions. In this document we propose to install the LHCf detectors for the p+p run at √ s=14 TeV and for the eventual proton light ion run that is under discussion after the first year of the LHC Run3. The main purpose of this proposal is to get a better understanding of the nuclear effects in a pseudo-rapidity and energy configuration that is very significant for CR physics, with the aim to reduce the systematic uncertainties still present in the High Energy hadronic interaction models. As an additional by-product, we can extend at 14 TeV the measurements already carried out by LHCf at smaller center of mass energies; thanks to the improved DAQ system, which allows more than the double of the previous DAQ rate, and to a more sophisticated trigger scheme, allowing to operate at a luminosity 10 times higher than before, we can significantly increase the statistics of our measurements. This will give us the opportunity to measure also the spectra of neutral hadrons others than π0 very forward produced in the p+ p and p+Light Ion collisions.

[1]  K. Sato,et al.  Recent results from the LHCf and RHICf experiments , 2019, EPJ Web of Conferences.

[2]  I. Vitev,et al.  Future physics opportunities for high-density QCD at the LHC with heavy-ion and proton beams , 2018, 1812.06772.

[3]  K. Sato,et al.  Measurement of inclusive forward neutron production cross section in proton-proton collisions at s=13$$ \sqrt{s}=13 $$ TeV with the LHCf Arm2 detector , 2018, Journal of High Energy Physics.

[4]  A. Martin,et al.  Total π + p cross section extracted from the leading neutron spectra at the LHC. , 2017, 1705.03685.

[5]  M. Haguenauer,et al.  Measurement of forward photon production cross-section in proton-proton collisions at √{ s } = 13TeV with the LHCf detector , 2017, 1703.07678.

[6]  J. G. Contreras,et al.  LHC forward physics , 2016, 1611.05079.

[7]  S. Ostapchenko,et al.  Constraining high energy interaction mechanisms by studying forward hadron production at the LHC , 2016, 1608.07791.

[8]  A. Perrot,et al.  Measurements of longitudinal and transverse momentum distributions for neutral pions in the forward-rapidity region with the LHCf detector , 2015, 1507.08764.

[9]  A. Perrot,et al.  Measurement of very forward neutron energy spectra for 7 TeV proton-proton collisions at the Large Hadron Collider , 2015, 1503.03505.

[10]  A. Perrot,et al.  Transverse-momentum distribution and nuclear modification factor for neutral pions in the forward-rapidity region in proton-lead collisions at s NN =5.02 TeV , 2014, 1403.7845.

[11]  A. Perrot,et al.  Measurement of zero degree inclusive photon energy spectra for s=900GeV proton–proton collisions at LHC , 2012, 1207.7183.

[12]  M. Haguenauer,et al.  Measurement of forward neutral pion transverse momentum spectra for √ s = 7TeV proton-proton collisions at the LHC , 2012, 1205.4578.

[13]  K. Kampert,et al.  Measurements of the Cosmic Ray Composition with Air Shower Experiments , 2011, 1201.0018.

[14]  D. Macina,et al.  Measurement of zero degree single photon energy spectra for √s=7 TeV proton-proton collisions at LHC , 2011, 1104.5294.

[15]  S. Ostapchenko,et al.  Monte Carlo treatment of hadronic interactions in enhanced Pomeron scheme: I. QGSJET-II model , 2010, 1010.1869.

[16]  G. Castellini,et al.  The construction and testing of the silicon position sensitive modules for the LHCf experiment at CERN , 2010 .

[17]  D. A. Faus,et al.  The LHCf detector at the CERN Large Hadron Collider , 2008 .

[18]  S. Mrenna,et al.  PYTHIA 6.4 Physics and Manual , 2006, hep-ph/0603175.

[19]  S. Roesler,et al.  Antiparticle to particle production ratios in hadron-hadron and d-Au collisions in the DPMJET-III Monte Carlo model , 2005, hep-ph/0505035.

[20]  S. Klein,et al.  Exclusive vector meson production in relativistic heavy ion collisions , 1999, hep-ph/9902259.

[21]  T. Stanev,et al.  Sophia Monte-carlo Simulations of Photohadronic Processes in Astrophysics Title of Program: Sophia 2.0 Catalog Number: Program Obtainable from A. M Ucke R(e N ) = 1 8e 2 N N , 2007 .

[22]  Raffaello D'Alessandro,et al.  LHCf experiment : Technical Design Report , 2006 .