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China ATLAS Status report. HAN Liang Univ. of Sci. & Tech. of China On behalf of China ATLAS collaborate. The LHC Machine and Experiments. pp at 14 TeV, 10 34 cm -2 s -1. High Energy factor 7 increase w.r.t. present accelerator Tevatron
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China ATLAS Status report HAN Liang Univ. of Sci. & Tech. of China On behalf of China ATLAS collaborate
The LHC Machine and Experiments pp at 14 TeV, 1034cm-2s-1 High Energy factor 7 increase w.r.t. present accelerator Tevatron High Luminosity Nevents/(s*T) factor 100 increase
ATLAS Experiment and China Cluster Length ~ 46 m Diameter ~ 25 m Weight ~ 7000Ts Channel ~ 108 Cable ~ 3000km • Muon spectrometer • air-core toroids, • MDT+RPC+TGC+CSC • s/pT ~ 2-7 % • |h|<2.5 (precise phys.) • EM Calorimetry • Pb-LAr • s/E ~ 10%/√E(GeV)1% • |h|<3.2, |h| < 2.5 (fine granularity) • Inner Tracker: • + vertex • + b-tagging • + pT & Q of track • Calorimeter(EM+HD): • + E of e/g • + E of hadron jet • + MET of n(c0) • Muon(outmost tracker): • + pT & Q m • Inner detector (B=2 T) • Si pixels and strips • Transition Radiation Detector (e/ sep) • s/pT ~ 0.05% pT(GeV)0.1%; • |h| < 2.5, B=2 T(central solenoid) • Hadron Calorimeter • Fe/scintillator (central), Cu/W-LAr (fwd) • s/E ~ 50%/√E(GeV)3%, up to ||<3
Institution of High Energy Physics (IHEP): • Shandong University (SDU): • Univ. of Science & Technology of China (USTC): • Nanjing University (NJU): • Higgs search and property study • LCG Teir2 construction • electron energy calibration and ID study • W helicity measurement in top decay • top spin correlation in pair production • single top measurement • WZ production and TGC anomalous coupling • R-parity violation SUSY • single top measurement
Higgs production@ LHC q q q q
Higgs search@ ATLAS -- SM Higgs (114-190GeV) discovery @ 10 fb-1 -- easy and fast for mH >140 GeV with HWW* channel -- more strength on mH<140 GeV with Htt, Hgg
MVA HMatrix: 8 variables_dijet 10 variables_dijet Photon/jet discrimination in Hgg(IHEP) -- Signal : gluon fusion production s(ggHgg)50fbin 95-130GeV mass region -- Background : • irreducible photon pairs continuum sgg1pb/GeV • reducible background s(g+j)103×sgg , s(j+j)106×sgg -- MVA discriminator studies: MVA Fisher: 8 variables_dijet 10 variables_dijet
Top Yukawa coupling in ttH(HWW*) (IHEP) -- Precise Yukawa couplings of heaviest fermion, in the intermediate ~160GeV mass gt -- Cross section measurement coupling constant gt extraction
Signal: same-signed 2L + 3L -- Topology and 2L/3L signal channel : • Same-signed 2L/3L • (from Higgs and top) • >=4 high pT jets • Missing ET for >=2n -- irreducible background : tt(1l/2l)+X(W,Z,jets) • lepton in heavy flavor e.g. bc+ln(W*) decay signal same-signed “L” • overwhelming QCD ISR and pileup signal “jet” Isolation ofLis crucial
Calorimeter Isolation: • The total energy deposited in the calorimeter around the lepton in a cone size of 0.2 should smaller than 10GeV • Tracker Isolation: • The maximum pt of extra tracks in ID around the lepton in a cone size of 0.2 should smaller than 2 GeV Isolation in Calorimeter and tracker Isolated lepton Uniso. lepton Lepton Calo track Calorimeter Cone size 0.2 Clusters around the lepton Inner detector Tracks around the lepton Electron Muon
Theoretical uncertainties -- Uncertainty on Pythia ttH signal : PDF, Q2, ISR/FSR, fragmentation
2L+3L combined prediction @ ATLAS 30fb-1 -- Accuracy on combined σttH×BRHWW -- Accuracy on coupling gt 47.4% (@160GeV) 23.7% (@160GeV)
WH(WW*) measurement (IHEP) -- Complementary to heavy Higgs discovery: what if discovered via HZZ4l channel, while WH is absent? -- Measure cross-section to probe Higgs-gauge boson couplings -- Combined 2L+2j and 3L channel
Preliminary results -- Normalized to 30 fb-1 • accepted in ATLAS CSC-NOTE • WH coupling measurement in progress
Physics of top quark pair production Mass W helicity Charge CP violation Width Anomalous coupling Production cross section Heavy resonance decay Spin correlation Branching ratios CKM :|Vtb| Rare decays
spin=1/2 1/2 1 W polarization and top-pair spin correlation (SDU) -- W helicity in top: σtt@LHC~850pb, Br(tWb)~100% governed by V-A in SM SM prediction(NLO): F0=0.695 FL=0.304 FR=0.001
-- top-pair spin correlation: where NLO SM prediction:
Single lepton channel analysis -- high BR with moderate background -- in situ W and top mass(transverse) constraints (730pb-1) (220pb-1) * *due to unknown discrepancy between fast and full simulation NLO SM prediction:
Di-lepton channel analysis -- rare BR with rare background -- need to solve equations for missing ET of 2n
Single top measurement (NJU) t-channel (~247pb) W+t channel (~66pb) s-channel (~11pb) • The only known way to directly measure CKM matrix element Vtb • Try to distinguish s-channel from t-channel production mode to test SM
t-channel cut based analysis results • Processes muon channel electron channel nEvt to L=fb-1 • t-channel 3.83±0.15% 3.10±0.14% 1668 • t-ch (τ)l 1.48±0.23% 0.36±0.11% • s-channel 1.84±0.11% 1.14±0.08% 34 • s-chan (τ)l 0.39±0.12% 0.39±0.12% • W+t channel 0.85±0.07% 0.61±0.02% 136 • W+t chan (τ)l 0.18±0.08% 0.20±0.08% • ttl+jets 0.95±0.03% 0.69±0.02% 4173 • tt(τ)l+j 0.35±0.04% 0.22±0.03% • tte + e 1.83±0.12% • ttμ+μ 3.07±0.16% • ttμ+e 2.10±0.09% • ttμ+τ 3.18±0.11% • tt e +τ 2.41±0.10% • ttτ+τ 0.74±0.08% S/B = 1668/4343 = 38.4%, S/ √ S+B = 21.5
s-channel cut based analysis results • Processes muon channel electron channel nEvt to L=fb-1 • s-channel 2.47±0.12% 1.49±0.10% 46 • s-ch (τ)l 0.71±0.16% 0.64±0.15% • t-channel 0.22±0.04% 0.14±0.03% 84 • t-chan (τ)l 0.04±0.04% 0.00±0.00% • W+t channel 0.10±0.03% 0.08±0.03% 11 • W+t chan (τ)l 0.00±0.00% 0.00±0.00% • ttl+jets 0.09±0.01% 0.08±0.01% 646 • tt(τ)l+j 0.04±0.01% 0.02±0.01% • tte + e 0.34±0.05% • ttμ+μ 0.48±0.06% • ttμ+e 0.33±0.04% • ttμ+τ 0.69±0.05% • tt e +τ 0.54±0.05% • ttτ+τ 0.24±0.04% S/B = 46/741 = 6.2%, S/ √ S+B = 1.64
WZ cross-section and TGC measurement (USTC) SM NLO : • Phys. Rev. D41, 2782(1990). • Phys. Rev. D47, 940(1993). • Phys. Rev. D60, 114037(1999). • Phys. Rev. D60, 113006(1999) • Unique measurement on WWZ TGC -- non-SM anomalousas with form factor as -- Enhancement on production + excess at W/Z high pT spectrum • WZllln search channel : -- eee, eem, emm and mmm combined, Br~1.5% -- high pT isolated lepton + MET + di-lepton invariant mass around Z -- background Z(ll)+X and ZZ(4l)
WZ Observation @ 1fb-1 -- Simple straight cut results
R-parity violating sneutrio em resonance (USTC) Parity in SUSY can be partially violated in generic super-potential: -- Tri-linear on-spontaneous B- & L-number violation interactions stable proton -- Bi-linear couplings neutrino mass for oscillation -- Constraints from indirect low energy experiments With hypothesis: 1) degenerate M=100GeV 2) single coupling dominance l13k l31k LLE in tenn l312, l321 < 0.07 LQD in tpn l’311 < 0.12 Reference: hep-ph/9906224; Phys. Rept. 420, 1(2005)
Expected result @ 1fb-1 -- Phenomenology in collider physics • Y. B. Sun et al., Commun. Theor. Phys. 44, 107 (2005) • L. L.Yang et al., Phys. Rev. D 72, 074026 (2005) • S.M. Wang et al.,Phys. Rev. D 74, 057902 (2006) • H. K.Dreiner et al., Phys. Rev. D 75, 035003 (2007) • Y. Q. Chen et al., J. High Energy Phys. 05 (2007) 068 • S.M. Wang et al., Chinese Phys. Lett. Vol.25, No.1(2008)58 -- Results of measured at Tevatron/D0 expected at ATLAS/LHC PRL 100,241803 10-20 folded improvement on RPV parameter sensitivity would be expected @ATLAS
Prepare for Commissioning Run -- Full Dress Rehearsal Complete test on DAQ test by physics processes after Event Filters, e.g. Trigger ”e25i” single e (pT>20GeV) di-e (pT>20GeV,df>2)
-- Combined Test Beam 2004: to calibrate electron energy linearity (IHEP) • CTB2004 is the first beam test integrating all sub detector • All sub detectors are the final prototype of ATLAS detector • First dedicated runs for energy <10GeV particles
Summary -- Physics analyses are beginning to take shape, channels cover top, Higgs, EW and SUSY -- Stay tuned for the commissioning run: understanding detector, e.g. e/g efficiency, fake rate, energy scale and resolution, trigger performance etc is the 1st priority -- China LCG Tier2 construction is in good progress; need push university-level distributed Tier3 to be on line in time. -- Young graduates are heartly welcomed to join the team and enjoy yourself in the game for next 10-15 years.
ttH(HWW) Cut flow 2L 3L
Pileup event effects Significance=S/sqrt(B): 3.0 2.4 ( -20% ! )
Physics and Performance Goal of 2008 run (L=100pb-1)
Pier-Olivier DeViveiros Fast G4 Simulationimportant for reducing systematic errors Fast G4 simulation and full simulation Jet pT spectra (in GeV) in release 13.0.30.3 ttbar events Full Sim Fast G4 Sim Full Sim Fast G4 Sim
How to quickly access data? • Tier-2 in China is badly needed • Before the tier-2 is ready (in two years?), the best way seems to send people to France under the FCPPL frame.
总 结 • LHC 物理研究意义重大;中国应加强对LHC物理研究的投入(人力和经费)。 • 中国组出色完成了LHC各个实验探测器建造任务,为参加物理分析取得了“参赛权”。 • 尽管物理分析起步较晚,ATLAS/CMS/LHCb 中国组仍在Higgs、SUSY、味物理(top和b物理)、电弱理论和QCD检验等各个方面取得了良好进展,其中ATLAS中国组有四个分析被合作组接受包括在即将正式发表的CSC Note里(尤其是ttH分析由高能所成员任召集人),CMS中国组有一个分析列入已正式发表的Physics TDR。 • 我们迫切需要 Tier-2 尽快在国内建成。