QCD at LHC with ATLAS Theodota Lagouri Aristotle University of Thessaloniki (on behalf of the ATLAS collaboration) EPS July 2003, Aachen, Germany

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Outline  LHC and ATLAS  Jet physics  Measurement of the α S at very large scales  Photon Physics  Lepton Physics  Background processes: minimum-bias and hard diffractive scattering events  Beauty production and QCD  Summary

EPS July 2003 QCD at LHC with ATLASTh. Lagouri LHC (Large Hadron Collider): p-p collisions at √s = 14TeV bunch crossing every 25 ns (40 MHz)  low-luminosity: L ≈ 2 x cm -2 s -1 ( L ≈ 10 fb -1 /year)  high-luminosity: L ≈ cm -2 s -1 ( L ≈ 100 fb -1 /year) Mass reach up to ~ 5 TeV Processσ (nb)Events/year ( L = 10 fb -1 ) Inclusive bb 5 x 10 5 ~ Inclusive jet p T > 200 GeV 100~ 10 9 Inclusive tt 0.8~ 10 7 Inclusive jet E T > 2 TeV ~10 -8 ~ 10 3 Test QCD predictions and perform precision measurements. Production cross section and dynamics are largely controlled by QCD. - - large statistics: small statistical error! -

EPS July 2003 QCD at LHC with ATLASTh. Lagouri ATLAS: A Toroidal LHC AparatuS ~44m ~22m 7,000 tons Multi-purpose detector coverage up to |η| = 5; design to operate at L= cm -2 s -1 Most of the QCD related measurements are expected to be performed during the “low-luminosity” stage. Inner Detector (tracker) Si pixel & strip detectors + TRT; 2 T magnetic field; coverage up to |η|< 2.5. Calorimetry highly granular LAr EM calorimeter ( | η |< 3.2); hadron calorimeter – scintillator tile - LAr for endcap&forward ( | η |< 4.9). Muon Spectrometer air-core toroid system (| η | < 2.7). Jet energy scale: precision of 1% ( W → jj; Z ( ll) + jets) Absolute luminosity: precision ≤ 5% ( machine, optical theorem, rate of known processes) Lepton precision: 0.1% ( or better )

EPS July 2003 QCD at LHC with ATLASTh. Lagouri LHC Parton Kinematics  Essentially all physics at LHC are connected to the interactions of quarks and gluons (small & large transferred momentum).  Accurate measurements of SM cross sections at the LHC will further constrain the pdf’s.  The kinematic acceptance of the LHC detectors allows a large range of x and Q 2 to be probed LHC coverage: | y | < 5.  This requires a solid understanding of QCD.

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Jet physics Test of pQCD in an energy regime never probed! Jet E T N events > 1 TeV4 x 10 5 > 2 TeV3 x 10 3 > 3 TeV40 At the LHC the statistical uncertainties on the jet cross-section will be small. Systematic errors :  jet algorithm (how to best define a jet),  calorimeter response (jet energy scale),  jet trigger efficiency,  luminosity (dominant uncertainty 5% -10% ),  the underlying event. The measurement of di-jets and their properties (E T and η 1,2 ) can be used to constrain p.d.f.’s. - α S (M Z ) measurement with 10% accuracy ( can be reduced by using the 3-jet to 2-jet production ) α S measurement at very large scales (O(1 TeV)). L = 30 fb -1 ● 0 < |η| < 1 ○ 1 < |η| < 2 ■ 2 < |η| < 3 dσ/dE T [nb/GeV] E T Jet [GeV] Inclusive Jet Cross-Section  The measurement of jet production will allow to access small distances due to large cross-section.  The statistical uncertainties will be small: A 30 fb -1 integrated luminosity amounts to 4x10 5 events with E T > 1 TeV, 3000 events with E T >2 TeV and ~40 with E T > 3 TeV.  The expected statistics at large jet E T values implies a desirable control of the systematic uncertainties to a precision better than 1% for E T < 1 TeV and to ~10% for E T of ~3 TeV. Multi-jet production is important for several physics studies: tt production with hadronic final states Higgs production in association with tt and bb Search for R-parity violating SUSY (8 – 12 jets). α S (M Z ) measurement with 10% accuracy ( can be reduced by using the 3-jet to 2-jet production ) α S measurement at very large scales (O(1 TeV)).

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Jet Physics Di-jet Production  1. Triple differential cross-section The measurement of di-jets and their properties can be used to constrain the parton densities inside the proton and in various kinematic regions in Q 2 and x.  2. Di-jet invariant mass For an integrated luminosity of 300 fb -1, the available statistics should allow a measurement of masses up to 10 TeV/c 2. Q 2 [GeV 2 ]

EPS July 2003 QCD at LHC with ATLASTh. Lagouri However, measurements of α S (M Z ) will not be able to compete with precision measurements from e + e - and DIS ( gluon distribution ). Differential cross-section for inclusive jet production (NLO ) E CM = 14 TeV, -1.5 < η jet < 1.5 A and B are calculated at NLO with input p.d.f.’s. Fitting this expression to the measured inclusive cross- section gives for each E T bin a value of α S (E T ). Systematic uncertainties :  p.d.f. set ( ±3%),  parametrization of A and B,  renormalization and factorization scale ( ±7%). Verification of the running of α S : check of QCD at the smallest distance scales yet uncovered :  α S = at 100 GeV  α S ~ at 4 TeV Determination of α s

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Understanding photon production:  Higgs signals (H→γγ) & background;  prompt-photon can be used to study the underlying parton dynamics;  gluon density in the proton, f g (x) ATLAS : high granularity calorimeters ( |η| < 3.2 ) allow good background rejection. Isolation cut : reduces background from fragmentation ( π 0 ) qg→γq qq→γg - Production mechanism: dominant (QCD Compton scattering) p T γ > 40 GeV Photon Physics Low luminosity run: the photon efficiency is more than 80% ( LAr calorimeter ). Background : mainly related to fragmentation (non-perturbative QCD) ( requires good knowledge of α s ) ( cone isolation) |η||η|

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Photon Physics  Direct photon measurements can provide important constraints on parton distributions, especially on the gluon distribution in the proton. The advantage of photon measurements is the better energy determination in comparison to jet measurements, thus avoiding the jet definition ambiguities.  The expected ratio of the inclusive photon cross-section has a value of about 1.5x  A rejection larger than 3x10 3 can be achieved while retaining an efficiency of more than 80% for photons with E T >40 GeV.  Photons with E T >40 GeV (Q 2 >10 3 GeV 2 ) allow to reach values of Bjorken-x down to 5x10 -4 (for |  | 500 GeV are expected for 30 fb -1  Effects of soft gluon emission can be studied directly by measuring the production of pairs of photons. At LHC it will be possible to study the photon pair production up to 1 TeV invariant mass of the pair with reasonable statistics.

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Lepton Physics Drell-Yan production  The measurement of Drell-Yan lepton pair production and the production of W and Z bosons (with a leptonic decay to electrons or muons) will allow one to constrain the quark and anti-quark densities of the proton at a scale given by the invariant mass of the lepton pair over a wide range in Bjorken x.  The jet rejection factors of the order of 10 5 can be achieved, having an efficiency of ~70% for electrons from W(Z) decays. W/Z production  In contract to the case of proton anti-proton collisions, at the LHC there is no rapidity asymmetry for the produced W’s. However, the shape of the rapidity distributions is different for W + and W -, where the total cross-section is larger for W + than for W -. It is a direct consequence of the parton distribution functions responsible for W + and W - production.  Z-production: 3x10 -4 < x< 0.1 at Q 2 = 8x10 3 GeV 2  During 1 year at low luminosity about 10 8 (10 7 ) events with W-> e (Z-> e + e - ) will be produced.

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Properties of Minimum-Bias Events and Hard Diffractive Scattering  An extension of the ATLAS detector in the forward region (beyond pseudo-rapidities of |  |=5) is presently under study, in order to increase the acceptance for charged particles from inelastic interactions (possibly including a momentum measurement) and to provide tagging and measurement of leading protons from elastic and diffractive interactions.  A detailed understanding of the structure of minimum bias events is needed in order to reduce dependencies on models used to determine their effects at the design luminosity.  Each minimum bias event is expected to contribute from charged particles only about GeV per unit rapidity and unit azimuth to the transverse energy.

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Beauty production and QCD  B production measurements offer an important probe of pQCD  Full NLO calculation available in QCD  Tevatron single b production results show factor ~2 cross-section discrepancy between NLO QCD and data  Tevatron has measured b-b correlations which are more sensitive to production mechanisms, however the precision was limited by statistics  ATLAS at LHC will further contribute tests of QCD and investigate cause of theory-data discrepancy at hadron interactions  b-b correlations  We investigate angular correlations in b-b production  Using J/  (  )-  angle measurements, b  J/  X, b   X  The ATLAS detector performance is very good for these channels

EPS July 2003 QCD at LHC with ATLASTh. Lagouri ATLAS b-b correlations in B d  J/  K 0 s, B 0 s  J/ , b  X  Efficiency does not drop at small  <1. No selection cuts requiring model dependent corrections  Including backgrounds shown before/after application of K/  rejection  B 0 s more difficult than B d because of correlated background from K  --

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Summary  The LHC will provide a big sample of events with high p T signatures for QCD studies. It will extend the kinematic range to larger values of Q 2, the hard scale of the partonic process, reaching scales of the order of TeV 2. The fraction of the proton momentum attributed to a parton will allow access to 10 -5, while keeping the scale above 100 GeV 2, in contrast to HERA measurements, where these small momentum fractions are only reached for hard scales close to or even below 1 GeV 2.  Candidate signatures to provide constraints on the quark and anti-quark distributions are the production of W and Z bosons via the Drell-Yan process as well as lepton pair production in general. On the other hand, the production of direct photons, of jets and of top quarks can be used to get information on the gluon distribution.  The study of diffractive processes, which allow to access the hard and soft regime of QCD at the same time, presents a significant experimental challenge in the LHC environment and given the limited angular acceptance of the detectors.

EPS July 2003 QCD at LHC with ATLASTh. Lagouri Summary  The high beauty production rate at LHC will allow one to extend b-production measurements up to transverse momenta of several hundred GeV. Correlations between b and b quarks and events with more than one heavy-quark pair, that were difficult to access in previous experiments due to limited statistics, will be investigated in detail.  ATLAS can exploit the large statistics of b quark decays at the LHC to make precise b production measurements. Good prospects for measurements of b-b correlations in muon channels. Two exclusive channels studied so far: B d  J/  K 0 s, B 0 s  J/  looking for additional muon.  A precise knowledge and understanding of QCD processes is important for the studies of the Higgs boson(s) and searches for new physics beyond the SM, where QCD represents a large part of the background. - -