# Global properties of proton-proton collisions at = 100 TeV

###### Abstract

The global properties of the final states produced in hadronic interactions of protons at centre-of-mass energies of future hadron colliders (such as FCC-hh at CERN, and SppC in China), are studied. The predictions of various Monte Carlo (MC) event generators used in collider physics (pythia 6, pythia 8, and phojet) and in ultrahigh-energy cosmic-rays studies (epos, and qgsjet) are compared. Despite their different underlying modeling of hadronic interactions, their predictions for proton-proton (p-p) collisions at = 100 TeV are quite similar. The average of all MC predictions (except phojet) for the different observables are: (i) p-p inelastic cross sections = 105 2 mb; (ii) total charged multiplicity = 150 20; (iii) charged particle pseudorapidity density at midrapidity ; (iv) energy density at midrapidity GeV, and GeV at the edge of the central region; and (v) average transverse momenta at midrapidities GeV/c. At midrapidity, epos and qgsjet-ii predict larger per-event multiplicity probabilities at very low () and very high () particle multiplicities, whereas pythia 6 and 8 feature higher yields in the intermediate region 30–80. These results provide useful information for the estimation of the detector occupancies and energy deposits from pileup collisions at the expected large FCC-hh/SppC luminosities.

## I Introduction

The Future Circular Collider (FCC) is a post-LHC project in a new 100-km tunnel under consideration at CERN,
that would provide hadron and collisions at much higher energies and luminosities than studied so
far. Its key scientific goals are the complete exploration of the Higgs sector of the Standard
Model (SM), and a significant extension in searches of physics beyond the SM via direct or indirect
measurements Mangano16a ; Mangano16b ; Mangano16c . The FCC-hh will deliver proton-proton (p-p) collisions at a centre-of-mass (c.m.) energy of
= 100 TeV with integrated luminosities at the level of several 100 fb per year or
above Benedikt:2015poa . Ongoing studies exist on the detector requirements needed to carry out the
planned measurements under running conditions involving simultaneous p-p collisions per bunch crossing. Similar studies are under consideration
in the context of the Super proton-proton Collider (SppC) promoted by IHEP in ChinaCEPC-SPPCStudyGroup:2015csa .
This work presents a study of the average properties of multiparticle production in p-p collisions at FCC-hh/SppC energies,
of usefulness, among others, for the estimation of the expected occupancies and energy deposits in the planned FCC-hh/SppC detectors.

Inclusive particle production in high-energy hadronic collisions receives contributions from
“soft” and “hard” interactions, loosely separated by the virtuality of the underlying -channel exchanges. Soft (hard) processes involve partons of virtualities typically
below (above) a scale 1–2 GeV. Semihard parton-parton scatterings around ,
dominate the inelastic hadron production cross sections for c.m. energies above a few
hundreds GeV, whereas soft scatterings dominate at lower energies ( 20 GeV) where few hadrons
with low transverse momenta are produced. On the one hand, hard processes
can be theoretically described within perturbative Quantum Chromodynamics (pQCD) in a collinear-factorized
approach through the convolution of parton distribution functions (PDFs) and matrix elements for the underlying
parton-parton collisions subprocesses. The scattered quarks and gluons produce then collimated bunches of final-state
hadrons (jets) through a parton branching process dominated by perturbative splittings described by the
Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equations dglap1 ; dglap2 ; dglap3 , followed by non-perturbative
hadronization when the parton virtuality is below . On the other hand, soft processes have
momenta exchanges not far from 0.2 GeV and, although they cannot be treated within pQCD,
basic quantum field-theory principles — such as unitarity and analyticity of scattering amplitudes as implemented in
Gribov’s Reggeon Field Theory (RFT) Gribov:1968fc and exemplified e.g. in the original Dual Parton
Model Capella:1992yb — give a decent account of their cross sections in terms of the exchange of
virtual quasi-particle states (Pomerons and Reggeons).
Given the extended composite nature of hadrons, even at asymptotically large energies, a non-negligible
fraction of inelastic p-p interactions involve soft “peripheral” scatterings.
The Pomeron () contribution, identified perturbatively with a colour-singlet multigluon exchange,
dominates over those from secondary Reggeons (virtual mesons)
and is responsible for diffractive dissociation accounting for a noticeable fraction, about a fourth, of the
total inelastic cross section at high energies Donnachie:2002en ; Khachatryan:2015gka .

The general-purpose Monte Carlo (MC) models used in high-energy collider physics, such as
pythia 6 Sjostrand:2006za , pythia 8 Sjostrand:2007gs , herwig++ Bahr:2008pv ,
and sherpa Gleisberg:2008ta , are fully based on a pQCD framework which then incorporates soft
diffractive scatterings in a more or less ad hoc manner. In contrast, MC models commonly used in
cosmic-ray physics d'Enterria:2011kw such as epos Werner:2005jf ; Pierog:2009zt ; Pierog:2013ria ,
qgsjet 01 Kalmykov:1993qe ; Kalmykov:1997te ,
qgsjet-ii Ostapchenko:2005nj ; Ostapchenko:2004ss ; Ostapchenko:2007qb ; Ostapchenko:2010vb and
sibyll Ahn:2009wx , as well as phojet Engel:1994vs ; Engel:1995yda ; Engel:1995sb
mostly used for collider environments, are fully-based on the RFT approach. The latter MCs start off from a
construction of the hadron-hadron elastic scattering amplitude to determine the total, elastic and inelastic
(including diffractive) cross sections, extended to include hard processes via “cut (hard) Pomerons” (also known as “parton ladder”) diagrams.

At increasingly larger c.m. energies, the inelastic cross section receives major contributions from the region
of low parton fractional momenta (), where the
gluon distribution rises very fast. As a matter of fact, at = 100 TeV the partonic cross section
saturates the total inelastic cross section (i.e. 100 mb) at
momenta 10 GeV/c, 50 times larger than . Such a “divergent” behaviour (taking
place well above the infrared regime) is solved by reinterpreting this observation as a consequence of
the increasing number of multiparton
interactions (MPI) occurring in a single p-p collision. Multiple scattering is naturally incorporated in the
RFT models through the “eikonalization” of multi-Pomeron exchanges that unitarize the cross sections, whereas
pythia eikonalises multiparton exchanges, supplemented with an impact-parameter (Glauber-like) description of
the proton Sjostrand:1987su .
The energy evolution of such MPI and low- effects is implemented phenomenologically in all MCs through a
transverse momentum cutoff of a few GeV that tames the fastly-rising minijet cross section
(e.g. in pythia the cutoff is introduced through a multiplicative factor). This
regulator is often defined so as to run with c.m. energy following a slow power-law (or logarithmic)
dependence, closely mimicking the “saturation scale” that controls the onset of non-linear
(gluon fusion) effects saturating the growth of the PDFs as 0 Gribov:1984tu .
Last but not least, all MC generators, both based on pQCD or RFT alike, use parton-to-hadron fragmentation
approaches fitted to the experimental data — such as the Lund string Andersson:1983ia , area law Artru:1974hr or cluster
hadronization Marchesini:1991ch models — to hadronize the coloured degrees of freedom once their
virtuality evolves below .

In this paper, we compare the basic properties of the so-called “minimum bias” (MB) observables characterizing the final states produced in proton-proton collisions at = 100 TeV, predicted by pQCD- and RFT-based hadronic interaction models. The MB term refers commonly to inelastic interactions experimentally measured using a generic minimum-bias trigger that accepts a large fraction of the particle production cross section by requiring a minimum activity in one or various detectors. In some cases we present also results for the so-called “non single-diffractive” (NSD) events, mimicking the typical experimental requirement of a two-arm trigger with particles in opposite hemispheres to eliminate backgrounds from beam-gas collisions and cosmic-rays. Such NSD topology reduces significantly the detection rate of (single) diffractive collisions characterized by the survival of one of the colliding protons and particle production in just one hemisphere. The phenomenological setup of our study is described in Section II, the predictions of the different MCs for basic inclusive particle production observables — such as the inelastic cross section , the particle and energy densities as a function of pseudorapidity and , the per-event multiplicity distribution , and the transverse momentum distribution (and associated mean transverse momenta ) — are presented in Section III, and the main conclusions are summarized in Section IV.

## Ii Theoretical setup

The basic ingredients of the pythia 6 and 8 event generators are leading-order (LO) pQCD matrix elements, complemented with initial- and final-state parton radiation (ISR and FSR), folded with PDFs (interfaced here via the lhapdf v6.1.6 package Bourilkov:2006cj ), and the Lund string model for parton hadronization. The decomposition of the inelastic cross section into non-diffractive and diffractive components is based on a Regge model Schuler:1993wr . In this work we use the pythia event generator in two flavours: the Fortran version 6.428 Sjostrand:2006za , as well as the C++ version pythia 8.17 Sjostrand:2007gs . We consider two different “tunes” of the parameters governing the non-perturbative and semihard dynamics: ISR and FSR showering, MPI, beam-remnants, FS colour-reconnection, and hadronization. For pythia 6.4 we use the Perugia-350 tune Skands:2010ak , whereas for pythia 8 we use the Monash 2013 tune (Tune:ee=7; Tune:pp=14) Skands:2014pea . Both sets of parameters (Table 1) have been obtained from recent (2011 and 2013 respectively) analysis of MB, underlying-event (UE), and/or Drell-Yan data in p-p collisions at = 7 TeV.

Version | Tuning | Diffraction | Semihard dynamics | Initial state | Final state | ||||
---|---|---|---|---|---|---|---|---|---|

(PYTUNES) | power | transv. overlap | colour reconnection | hadronization | |||||

6.428 | Perugia 2011 (350) | Regge-based Schuler:1993wr | 7 TeV | 2.93 GeV | 0.265 | CTEQ5L | strong | Lund model fits (2011) | |

8.170 | Monash 2013 (14) | improved Rasmussen:2015iid | 7 TeV | 2.28 GeV | 0.215 | NNPDF2.3 LO | strong | Lund model fits (2013) |

For the initial-state, pythia 6 (Perugia 350) uses the CTEQ5L parton densities Lai:1999wy and
pythia 8 (Monash) the NNPDF2.3 LO set Ball:2013hta , whereas for the description of the transverse parton
density, both models use an exponential-of-power profile of the p-p overlap function, , with slightly
different exponents ( = 1.7 and 1.85 respectively). The pythia 6 choice results in a broader p-p overlap
which thereby enhances the fluctuations in the number of MPI relative to the Monash-2013 choice.
The energy evolution of the MPI cutoff is driven by , with the parameters quoted in Table 1.
Given that the generation of additional parton-parton interactions in the UE is suppressed below , a
higher scaling power implies a slower increase of the overall hadronic activity. Thus,
the Monash tune results in a slower evolution of , yielding larger MPI activity at 100 TeV compared to
the Perugia tune.
The treatment of diffraction has improved in pythia 8 compared to 6. In the former, a diffractive system is
viewed as a Pomeron-proton collision, including hard scatterings subject to all the same ISR/FSR
and MPI dynamics as for a “normal” parton-parton process Rasmussen:2015iid .
For the final-state, the two tunes have strong final-state colour reconnections (implemented through different
models Skands:2007zg ; Sjostrand:2014zea ), which act to reduce the number of final-state
particles (for a given value) or, equivalently, lower the value that is required to reach
a given average final-state multiplicity.
The Lund hadronization parameters for light- and heavy-quarks have been updated in pythia 8
compared to pythia 6 by refitting updated sets of LEP and SLD data Skands:2014pea .

The RFT-based models used in this work differ in various approximations for the collision configurations (e.g. the distributions for the number of cut Pomerons, and for the energy-momentum partition among them), the treatment of diffractive and semihard dynamics, the details of particle production from string fragmentation, and the incorporation or not of other final-state effects (Table 2). Whereas the RFT approach is applied using only Pomerons and Reggeons in the case of qgsjet and phojet, epos extends it to include partonic constituents Drescher:2000ha . In the latter case, this is done with an exact implementation of energy sharing between the different constituents of a hadron at the amplitude level. The evolution of the parton ladders from the projectile and the target side towards the centre (small ) is governed by the DGLAP equations. For the minijet production cutoff, phojet uses dependence of the form , whereas epos and qgsjet-ii use a fixed value of . The latter MC resums dynamically low- effects through enhanced diagrams corresponding to multi-Pomeron interactions Ostapchenko:2005nj ; Ostapchenko:2006vr ; Ostapchenko:2006nh . In that framework, high mass diffraction and parton saturation are related to each other, being governed by the chosen multi-Pomeron vertices, leading to impact-parameter and density-dependent saturation at low momenta Ostapchenko:2005yj . LHC data were used to tune the latest qgsjet-ii-04 release Ostapchenko:2010vb shown here. epos on the other hand, uses the wealth of RHIC proton-proton and nucleus-nucleus data to parametrize the low- behaviour of the parton densities in a more phenomenological way Werner:2005jf (correcting the amplitude used for both cross section and particle production). The epos MC is run with the LHC tune Pierog:2013ria which includes collective final-state string interactions which result in an extra radial flow of the final hadrons produced in more central p-p collisions. Among all the MC models presented here, phojet is the only one which does not take into account any retuning using LHC data (its last parameter update dates from year 2000).

Model (version) | Diffraction | Semihard dynamics | Final state | |
---|---|---|---|---|

Evolution | ||||

epos-lhc Pierog:2013ria | effective diffractive | 2.0 GeV | power-law corr. of | collective flow + area law hadronization |

qgsjet-ii-04 Ostapchenko:2005nj ; Ostapchenko:2004ss ; Ostapchenko:2007qb | cut-enhanced graphs + G.-W. Good:1960ba | 1.6 GeV | enhanced -graphs | simplified string hadronization |

phojet 1.12 Engel:1994vs ; Engel:1995yda | G.-W. model Good:1960ba | 2.5 GeV | hadronization via pythia 6.115 |

The results are presented, in the case of pythia 6 and 8, for primary charged particles, defined as all
charged particles produced in the collision including the products of strong and electromagnetic decays but
excluding products of weak decays, obtained by decaying all unstable particles^{*}^{*}*pythia 6.4:
MSTJ(22)=2,PARJ(71)=10. pythia 8: ParticleDecays:limitTau0 = on, ParticleDecays:tau0Max = 10.
for which 10 mm. For the RFT MCs, unless stated otherwise, the results correspond to the primary
charged hadrons (with the same requirement) but without charged leptons which, nonetheless,
represent a very small correction (amounting to about 1.5% of the total charged yield, mostly from the Dalitz
decay). Unless explicitly stated, no requirement on the minimum of the particles is applied in
any of the results presented.

## Iii Results

### iii.1 Inelastic p-p cross section

The most inclusive quantity measurable in p-p collisions is the total hadronic cross section and its separation into elastic and inelastic (and, in particular, diffractive) components. In both pythia 6 and 8, the total hadronic cross section is calculated using the Donnachie-Landshoff parametrisation Donnachie:1992ny , including Pomeron and Reggeon terms, whereas the elastic and diffractive cross sections are calculated using the Schuler-Sjöstrand model Schuler:1993wr . The predictions for the inelastic cross sections in p-p at = 100 TeV, obtained simply from , yield basically the same value, mb, for both pythia 6 and 8. The RFT-based MCs, based on amplitudes, predict slightly lower values: mb for epos-lhc, qgsjet-ii and phojet respectively. The dependence of the inelastic cross section predictions is shown in Fig. 1 together with the available data from p- (UA5 Alner:1986iy , E710 Amos:1991bp and CDF Abe:1993xy ) and p-p (ALICE Abelev:2012sea , ATLASAad:2011eu ; atlas13TeV , CMS Chatrchyan:2012nj ; cms13TeV , TOTEM Antchev:2011vs ; Antchev:2013iaa ; Antchev:2013paa ) colliders, as well as the AUGER result at = 57 TeV derived from cosmic-ray data Auger:2012wt . Interestingly, all model curves cross at about 60 TeV, and predict about the same inelastic cross section at the nominal FCC-hh/SppC p-p c.m. energy of 100 TeV. A simple average among all predictions yields mb, whereas larger differences in the energy evolution of appear above the 300 TeV, i.e. around and above the maximum energy observed so far in high-energy cosmic rays impinging on Earth atmosphere d'Enterria:2011kw . The expected increase in the inelastic p-p cross section at 100 TeV is about 45% compared to the LHC results at 13 TeV ( = 73.1 7.7 mb atlas13TeV , and (preliminary) 71.3 3.5 mb cms13TeV ).

### iii.2 Particle pseudorapidity density

Figure 2 shows the distribution of the number of charged particles produced in p-p collisions at 100 TeV per unit of pseudorapidity as a function of pseudorapidity (), predicted by the
different models in the range (the beam rapidity at = 100 TeV is ).
The left plot shows the NSD distribution^{†}^{†}†In pythia 6 and 8 this is achieved by directly
switching off single-diffractive contributions via: MSUB(92)=MSUB(93)=0, and
SoftQCD:singleDiffraction=off. For phojet, epos-lhc and qgsjet-ii only events MC-tagged as non-diffractive
or double diffractive are included., and the right one shows the inclusive inelastic
distribution which, including lower-multiplicity diffractive interactions, has a smaller average number of
particles produced. All models (except phojet) predict about 10 charged particles at midrapidity ().

Taking an unweighted average of all the predictions (except phojet which is systematically lower by 40%), we obtain: and . The width of the central pseudorapidity “plateau” covers 10 units from to . At forward rapidities (equivalent to small ) pythia 6 and phojet predict noticeably “thinner” distributions than the rest, due to lower underlying gluon densities at , than those from the NNPDF 2.3 LO set used in pythia 8 Skands:2014pea . A significant fraction of the particles produced issue from the fragmentation of partons from semihard MPI, the hardest partonic collision in the MB event producing only a small fraction of them. The fact that the phojet particle yields are about 40% lower than the rest of MCs is indicative of missing multiparton contributions in this event generator.

The c.m. energy evolution of the charged hadron pseudorapidity density at predicted by the different
models in the range = 10 GeV–800 TeV is presented in Fig. 3 compared
to the existing NSD (left panel) and inelastic (right panel) data measured at SpS
(UA1 Albajar:1989an , and UA5 Alner:1986xu ), Tevatron (CDF Abe:1989td ; Abe:1988yu ) and
LHC (ALICE Aamodt:2010ft ; Aamodt:2010pp ; Adam:2015pza , ATLAS Aad:2010ac and
CMS Khachatryan:2010xs ; Khachatryan:2010us ; Khachatryan:2015jna ) colliders. The expected increase in particle multiplicity
at midrapidity at 100 TeV is about a factor of two compared to the LHC results at 13 TeV
( = 5.31 0.18 Adam:2015pza ,
5.49 0.17 Khachatryan:2015jna ). As aforementioned, the NSD selection has
central densities which are about 15% larger than those obtained with the less-biased INEL trigger, which has less
particles produced on average as it includes (most of) diffractive production. All models (except phojet,
whose results are not actually trustable beyond 75 TeV Ralph ) more or less reproduce
the available experimental data up to LHC, and show a very similar trend with up to FCC-hh/SppC
energies. Beyond 100 TeV, however, epos-lhc tends to produce higher yields than the rest of MCs.
It is worth to notice that, thanks to the LHC data, the differences among model predictions have been
considerably reduced in comparison to the results of the pre-LHC models discussed in d'Enterria:2011kw .

The FCC-hh experiments aim at fully tracking coverage in the central region. The total number of charged particles expected in the tracker system is obtained by integrating the distributions over that interval, which yields an average of =10 100. For the expected FCC-hh pileups, in the range , this value implies that the trackers would sustain on average a total number of 20–100 thousand tracks per bunch crossing. Such a value is of the same order of magnitude as a single central Pb-Pb collision at LHC energies Adam:2015ptt , and thus perfectly manageable for the high-granularity FCC-hh tracker designs. Further integrating the distributions over all pseudorapidities, one obtains the total number of charged particles produced in an average p-p collision at 100 TeV. The epos, pythia 8 and qgsjet-ii models predict the largest total charged multiplicities, = 161 (184), 160 (170), 152 (172) respectively; followed by pythia 6, ; and phojet, .

### iii.3 Energy pseudorapidity density

Figure 4 shows the distributions of energy density as a function of pseudorapidity for the total energy (left) and for the energy carried by charged particles above a minimum MeV/c (right). phojet predicts the lowest energy produced at all rapidities (consistent with the lower particle yields produced by the model), whereas pythia 8 predicts the highest. At , the total energy produced per unit rapidity is 9.9, 12.2, 12.6, 13.7 and 15.6 GeV for phojet, qgsjet-ii, pythia 6, epos-lhc and pythia 8 respectively. The same values at the forward edges of typical detector coverages () are 410, 525, 670, 700 and 760 GeV for phojet, pythia 6, qgsjet-ii, epos-lhc and pythia 8 respectively. The trend for pythia 6 is to predict a smaller relative increase of energy density as a function of rapidity compared to the rest of models due, again, to a more relatively depleted underlying gluon density at the increasingly lower values probed at forward .

### iii.4 Multiplicity distribution

The multiplicity distribution , i.e. the probability to produce charged particles in a p-p event, provides important differential constraints on the internal details of the hadronic interaction models. Figure 5 shows the distribution for charged particles

produced at central rapidities (within ) in inelastic p-p collisions at the FCC-hh/SppC. The tail of the distribution (right) gives information on the relative contribution of multiparton scatterings (multi-Pomeron exchanges), whereas the low multiplicity part (left) is mostly sensitive to the contributions from diffraction (single Pomeron exchanges). The various MCs considered predict quite different distributions at both ends of the spectrum. The RFT-based models epos-lhc and qgsjet-ii predict both higher yields at very low () and very high () particle multiplicities, whereas pythia 6 and 8 feature higher yields in the intermediate region 30–80. phojet clearly produces too many particles within 10–40, but much fewer at high multiplicities compared to the rest of models (which is, again, indicative of missing MPI contributions in this MC generator).

### iii.5 Transverse momentum distribution

Figure 6 (left) shows the -differential distributions of charged particles at midrapidity (within ) in p-p collisions at 100 TeV predicted by all models.

All spectra have been absolutely normalized at their value at GeV/c to be able to easily compare their shapes. Both pythia 6 and 8 feature the largest yields at the high- end of the distributions (not shown here), qgsjet-ii features the “softest” spectrum, whereas epos shows higher yields in the region 1–5 GeV/c, due to collective partonic flow boosting the semihard region of the spectra, but then progressively falls below the pure-pQCD pythia MC generators. The phojet spectrum has a more convex shape, being comparatively depleted at intermediate 1–3 GeV/c but rising at its tail. Studying the -evolution of the average of the spectra provides useful (integrated) information. At high energies, the peak of the perturbative cross section comes from interactions between partons whose transverse momentum is around the saturation scale, , producing (mini)jets of a few GeV which fragment into lower- hadrons. As explained in the introduction, pythia and phojet MCs have an energy-dependent cutoff that mimics the power-law evolution of , while epos and qgsjet have a fixed cutoff and low- saturation is implemented through corrections to the multi-Pomeron dynamics. The different behaviours are seen in the -evolution of the average shown in Fig. 6 (right). All MCs, but qgsjet-ii, predict a (slow) power-law-like increase of with energy. Both pythia 6 and 8 — whose dynamics is fully dominated by (mini)jet production — predict a higher than the rest of models, yielding GeV/c at 100 TeV to be compared with = 0.73, 0.71 and 0.67 GeV/c from phojet, epos-lhc and qgsjet-ii respectively. Above 20 TeV, qgsjet-ii predicts a flattening of whereas the epos-lhc evolution continues to rise due to final-state collective flow which increases with increasing multiplicity.

## Iv Summary

In summary, the global properties of the final states produced in hadronic interactions of protons at
centre-of-mass energies of the of the CERN Future Circular Collider and of the IHEP Super proton-proton Collider,
have been studied with various Monte Carlo event
generators used in collider physics (pythia 6, pythia 8, and phojet) and in ultrahigh-energy cosmic-rays
studies (epos, and qgsjet). Despite their different underlying modeling of hadronic interactions,
their predictions for proton-proton collisions at = 100 TeV are quite similar (excluding
phojet, whose parameters have not been retuned with the collider data in the last 15 years).
Table 3 lists the basic kinematical observables predicted for p-p at 100 TeV by all MC
generators considered.

pythia 6 | pythia 8 | epos-lhc | qgsjet II | phojet | Average | |

(mb) | ||||||

131 (150) | 160 (170) | 161 (184) | 152 (172) | 101 (121) | 150 (170) 20 | |

(GeV) | ||||||

(GeV) | ||||||

0.30 0.03 | ||||||

0.015 0.05 | ||||||

(GeV/c) |

The averages of all MC predictions (except phojet) for the different observables are:
(i) p-p inelastic cross sections = 105 2 mb (to be compared with
72 mb at the LHC(13 TeV), i.e. a 45% increase),
(ii) total charged multiplicity = 150 (170) 20,
(iii) charged particle pseudorapidity density at midrapidity
(to be compared with the LHC(13 TeV) result of = 5.4 0.2, i.e. an increase of
80%), and for the NSD selection,
(iv) energy density at midrapidity GeV,
and energy density at the edge of the central region GeV, and
(v) average transverse momenta at midrapidities GeV/c (to be compared with = 0.55 0.16
at the LHC(8 TeV), i.e. a 40% increase).
The per-event multiplicity probabilities , have been also compared: epos-lhc and
qgsjet-ii both predict higher yields at very low () and very high ()
particle multiplicities, whereas pythia 6 and 8 feature higher yields in the intermediate region 30–80. These results are useful to estimate the expected detector occupancies and energy
deposits from pileup collisions at high luminosities of relevance for planned FCC-hh/SppC detector designs.

#### Acknowledgments —

We are grateful to Peter Skands for useful discussions and feedback to a previous version of this document, and to Ralph Engel for valuable discussions.

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