LHC HI WG: Kickoff - HI Weekly Update Dennis Perepelitsa & Dominik Derendarz June 24, 2021 - CERN Indico
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בס"ד LHC HI WG: Kickoff (!) ATLAS perspective, wishes (!!), proposals, and views on the working group HI Weekly Update Zvi Citron Dennis Perepelitsa & Dominik Derendarz LHC HI WG: 7 July 2021
Getting Our House in Order • Most basic function of such a forum is resolving tensions within the community • Place to systematically and comprehensively review • Tensions (or disagreements) in data/results • Tensions (or disagreements) in planning priorities with shared implications Zvi Citron 2 LHC HI WG: 7 July 2021
EW Bosons as Standard Candles (Have We/They Failed?) • Tension in results is clear CMS 1.7 nb-1 (5.02 TeV PbPb) 0.6 • Probably not some ‘trivial’ Z boson R AA ATLAS 1.6 0.55 60 < mll < 120 GeV Pb+Pb, sNN=5.02 TeV, 0.49 nb-1 1.4 pp , s=5.02 TeV, 25 pb-1 0.5 |yZ| < 2.1 measurement issue 1 1 N (nb) 1.2 0.45 • Origin not yet understood Nevt TAA Z 0.4 - 1 Z/γ * → l+l 0.35 0.8 0-90% data 0.3 Data HG-Pythia (isospin corrected) 0.6 W- 0.25 HG-PYTHIA scaled by 0-90% Z + 0.4 W Model 1.2 0 20 40 60 80 100 Data 0 20 40 60 80 100 1 0.8 Centrality [%] 0 20 40 60 80 0−90 Centrality (%) Zvi Citron 3 LHC HI WG: 7 July 2021
inel = 70m ATLAS W ATLAS W + ATLAS Z data inel = 41.5 1.2 1.2 Fitted inel uncertainty nn RPbPb with nn RPbPb with nn 1.0 1.0 Broad Implications EPPS16 EPPS16 min.bias min.bias 0.8 0.8 ATLAS W ATLAS W + ATLAS Z data 4 0.6 K.Eskola AA et al [PRL 125, 212301 (2020)] Original T uncertainty 0.6 • ATLAS results mean HG-Pythia model p p 1.4 s = 5.02 TeV 1.4 s = 5.02 TeV inel = 41.5mb inel = 70mb ATLAS W ATLAS W + ATLAS Z data 1.2 1.2 Fitted inel nn uncertainty is incomplete/wrong • May suggest modification of σNN EPPS16 EPPS16 RPbPb with nn RPbPb with nn min.bias min.bias 1.0 1.0 EPPS16 EPPS16 • CMS results mean strong min.bias min.bias 0.8 0.8 ATLAS W ATLAS W + ATLAS Z data confirmation of HG-Pythia model EPPS16 EPPS16 min.bias min.bias Original TAA uncertainty 0.6 0.6 1.4 0 ps10 20 30 = 5.02 TeV 40 50 60 70 80 90 100 1.4 0 ps10 20 30 = 5.02 TeV 40 50 60 70 80 90 100 • à This is not a Z boson issue, this is inel = 41.5mb Centrality [%] Centrality [%] a baseline for HI interpretation issue inel = 70mb The centrality-dependent nuclear modification ratios for W ± and FIG. 3. 1.2 1.2 Z boson production in Pb+Pb collisions from ATLAS inel [37, 38] compared to NNLO pQCD calculation with EPPS16 nuclear modification with the nominal value of nn = 70.0 mb inel (left) and with the nuclear-suppressed value nn = EPPS16 41.5 mb (right). EPPS16 RPbPb with nn RPbPb with nn min.bias min.bias 1.0 1.0 (close-to) minimum-bias collisions. The impact, however, IV. MINIJETS WITH SHADOWING 0.8 grows towards more peripheral centrality classes, see Ta- 0.8 exp ALICE ble I. To illustrate this, Fig. 3 compares the centrality dependent RPbPb before and after rescaling the data by EPPS16 min.bias To study the plausibility of the obtained suppression inel 0.6 EPPS16 min.bias in 0.6 , we calculate its value in an eikonal model for minijet hTAA ( pp https://doi.org/10.1 inel )i/hTAA ( nninel )i using the fitted nninel . The left- nn production with nuclear shadowing. The model is based hand panels016/j.physletb.2019. show the original ATLAS data including the 0 10 20 30 40 50 60 70 80 90 100 on a similar0 10setup 20as 30 in Ref.40 [57] 50 but60 in70 the 80 eikonal 90 func- 100 quoted hT 04.047 AA i uncertainties, and in the right-hand panels tion we include only the contribution from the hard mini- the data have been rescaled Centrality [%] and the uncertainties follow pCentrality [%] inel jet cross section jet ( snn , p0 , [Q]), calculated at lead- from the nn fit. The striking e↵ect is that the mysteri- ing order in pQCD. The transverse-momentum cuto↵ p FIG. 3. The ous rise centrality-dependent towards more peripheralnuclear modification collisions ratios for W ± and Z boson production in the original p in Pb+Pb collisions from ATLAS0 [37, data38] compared becomes to NNLOwith compatible pQCD calculationcentrality a negligible with EPPS16 (which de- nuclear depends on modification with thes , scale choice nn nominal value of Q and inel the pro- nn = 70.0 mb Zvi Citron (left) and with inel ton thickness) and the width of the assumed Gaussian pendence, the the nuclear-suppressed central values indicatingvalue nn = a perhaps 41.5 mb (right). mildly proton thickness function we fix so that the model repro- 4 decreasing trend towards peripheral bins. As discussed LHC HI WG: 7 July 2021 duces inel = 70 mb matching the COMPETE analysis pp
because of the worse energy eightresolution of electrons measurements compared per track. Theseto muons. silicon In simulated detectors events are comple- in Ref. [23]. these selections correspond to 90%bybackground mented rejection, andtracker, the transition-radiation result inwhich a small efficiency enables loss radially Events with a Z boson candidate are selected by requiring for Z bosons, which is taken care oftrack extended withreconstruction the applied corrections. up to |η| =Candidates 2.0. resulting from exactly two opposite-charge muons or electrons, at least one of this background account for 0.6 The(0.7)% of the dimuon calorimeter system (dielectron) covers the yield before subtraction. pseudorapidity range |η|The < which is matched to a lepton selected at trigger level. The dilepton Centrality – Cart or Horse? other backgrounds considered are Z ! t + t , tt production, and the production of W bosons 4.9. Within the region |η| < 3.2, electromagnetic (EM) calorime- invariant mass must satisfy the requirement 66 < m$$ < 116 GeV decaying to a lepton thattry is combined is provided with another by barrel lepton and originating endcap from a hadron high-granularity decay. liquid-argon consistent with previous ATLAS measurements. A total of 5347 Z Z The expected yields are calculated as functions (LAr) sampling of centrality, calorimeters, with anpT ,additional or yZ using appropriate thin LAr presam- MC boson candidates are found in the muon channel and 4047 in the samples. These backgrounds plercontribute covering |less η|
Compatible (Unified?) Centrality Treatment • Whether or not my guess is correct, points to a need for a compatible or even unified centrality treatment • Clear definitions and goals for centrality classification • (I don’t claim this will be trivial) • Once ‘vocabulary’ is shared well positioned for more possibilities: • pA collisions • Light ion collisions • EW boson based centrality (?) Zvi Citron 6 LHC HI WG: 7 July 2021
➤ ATLAS uses full Run 2 (2015+2018) run of Pb+Pb at 5.02 TeV ➤ CMS has a measurement based on 2015 data only ➤ Important: difference in the kinematic phase space: CMS: pT>2 GeV, ATLAS: pT>2.5 GeV will Go Out for a Stroll … require an extrapolation correction ➤ About 2 sigma difference with Standard Model predictions ➤ Combination analysis is ongoing as part of the HonexComb project [more] ➤ Could be improved with the unpublished CMS 2018 data ➤ Opens a door for the combination of differential cross sections • Once our house is in order we can go out for a walk à Clear target is data combination, e.g. LbyL Combination analysis is ongoing as part of the HonexComb project [JHEP 03 (2021) 243] [Phys. Lett. B 797 (2019) 134826] Zvi Citron 7 LHC HI WG: 7 July 2021
Go Out for a Stroll …5 [JHEP 03 (2021) 243] • Once our house is in order we can go out for a walk à Clear target is data combination, e.g. LbyL Also set limits on ALP s Zvi Citron 8 LHC HI WG: 7 July 2021
A Combination Paradigm? • LbyL is too good of an example! • [HonexComb exists to focus on finding these - LbyL is 2nd case, total charm was 1st ] • Examples ripe for combination or in tension from ATLAS measurements next slides • Some wishlist items : • Top quark pairs • Tau pair production in UPC • Should also consider to what extent this changes how we approach and chose the analyses that further the HI program • There are of course downsides to too much cooperation between independent experiments Zvi Citron 9 LHC HI WG: 7 July 2021
Exclusive Di-Leptons: → + − • Baseline measurement for UPC • Statistical uncertainties dominate at high m and high aco-planarity Zvi Citron 10 LHC HI WG: 7 July 2021
Inclusive Jets v2, central collisions 2 ATLAS, ATLAS-CONF-2020-019 Inclusive Jet v2 in central PbPb Tension observed between Tension observed between ALICE results and the other ALICE results and the other experiments experiments, as those results are Would bedata, used to constraint greatitto clarify will be … great to clarified the tension with ALICE and other experiments. Zvi Citron 11 LHC HI WG: 7 July 2021
A Shared Interpretation-Oriented Paradigm? • Besides the cases of direct comparison there is room for improvement in how we go from measurement , and specifically multiple measurements, to interpretation • Centrality as discussed • Bulk property measurements typically have plenty of statistics, no large blatant tensions between experiments, “ahead of theory”, where do we go forward? Can we develop common interpretation- oriented approach • Important example: Template method for 2PC used only by ATLAS • Similar measurements are sometimes still difficult/impossible to directly compare Zvi Citron 12 LHC HI WG: 7 July 2021
Photon-Jet Asymmetry Analysis approach, in PbPb, pp procedure and observables 3 • CMS compares reco-level PbPb w/smeared pp • ATLAS compares fully unfolded • Similar story elsewhere (e.g. di-jets) • It would be great if the philosophy behind the analysis could be discussed, à find common ground to make the comparison possible/easier. Zvi Citron 13 LHC HI WG: 7 July 2021
Light Ions (sooner) • Many of these concerns/opportunities converge for upcoming Oxygen running • [See Anne’s nice talk at OO workshop for review of ATLAS perspective] • Small system flow and related physics questions, require good handle on geometry description, inter-experiment clarity on centrality and related crucial • Similar issues for understanding onset of jet quenching + need for compatibility in places where we haven’t always had it Zvi Citron 14 LHC HI WG: 7 July 2021
Light Ions (later) p • It’s distant but post Run Year 2021 4 Systems, sNN Time Pb–Pb 5.5 TeV 3 weeks running L 2.3 nb (and any changes of course before int 1 then) will need some level 1 week of pp 5.5 TeV common 3 pb (ALICE), 300buy 1 in from pb (ATLAS, 1 CMS),the 25 pb community 1 (LHCb) 1 2022 Pb–Pb 5.5 TeV 5 weeks 3.9 nb • Requires common physics1 week case/questions O–O, p–O 500 µb and 200 µb and forum to express them 1 1 2023 p–Pb 8.8 TeV 3 weeks 0.6 pb 1 (ATLAS, CMS), 0.3 pb 1 (ALICE, LHCb) pp 8.8 TeV few days 1.5 pb 1 (ALICE), 100 pb 1 (ATLAS, CMS, LHCb) 2027 Pb–Pb 5.5 TeV 5 weeks 3.8 nb 1 pp 5.5 TeV 1 week 3 pb 1 (ALICE), 300 pb 1 (ATLAS, CMS), 25 pb 1 (LHCb) 2028 p–Pb 8.8 TeV 3 weeks 0.6 pb 1 (ATLAS, CMS), 0.3 pb 1 (ALICE, LHCb) pp 8.8 TeV few days 1.5 pb 1 (ALICE), 100 pb 1 (ATLAS, CMS, LHCb) 2029 Pb–Pb 5.5 TeV 4 weeks 3 nb 1 Run-5 Intermediate AA 11 weeks e.g. Ar–Ar 3–9 pb 1 (optimal species to be defined) pp reference 1 week Zvi Citron 15 LHC HI WG: 7 July 2021
Summary • Some existing tensions linger and understanding them matters! • Data combination can help us with important measurements • We should consider where coordinating in general approach (i.e. beyond one particular measurement) can help us, especially for reaching meaningful intepretations • Upcoming (and future) light ion running at the LHC is an especially good opportunity to implement these ideas and make use of this forum Zvi Citron 16 LHC HI WG: 7 July 2021
Backups Zvi Citron 17 LHC HI WG: 7 July 2021
ATLAS-ALICE Tension in PbPb v2 from 4- cumulants v2{4} ATLAS 0.08 Pb+Pb sNN = 2.76 TeV 0.06 ATLAS ALICE 0.04 0.2 < p < 3 GeV, |η| < 1 T 50 100 150 200 250 300 〈Nch(|η| < 1)〉 Zvi Citron 18 LHC HI WG: 7 July 2021
Inclusive JetR RAA Inclusive Jets R=0.4 jets AA 1 CMS arXiv:2102.13080 ATLAS arXiv:1805.05635 Hint of a tension, but still consistent within uncertainties. Zvi Citron 19 LHC HI WG: 7 July 2021
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