- Page 1 and 2: 2009 QCD and High Energy Interactio
- Page 3 and 4: Proceedings of the XLIVth RENCONTRE
- Page 5 and 6: 2009 RENCONTRES DE MORIOND The XLIV
- Page 7 and 8: Foreword Contents 1. LHC and LHC de
- Page 9: 11. Heavy Ions The RHIC beam energy
- Page 13 and 14: ALICE COMMISSIONING: GETTING READY
- Page 15 and 16: Figure 2: Performance of the TPC me
- Page 17 and 18: COMMISSIONING OF THE ATLAS DETECTOR
- Page 19 and 20: Figure 2: (Left) Trigger timing dis
- Page 21 and 22: Commissioning of the CMS Detector M
- Page 23 and 24: In the DTs the worst resolution val
- Page 25 and 26: THE LHCB COMMISSIONING S. DE CAPUA
- Page 27 and 28: due to the limited capacity of the
- Page 29: References 1. LHCb collaboration, A
- Page 32 and 33: line in which the cable travels, re
- Page 34 and 35: • The QPS snapshot method which u
- Page 39 and 40: Searches for a low mass SM Higgs at
- Page 41 and 42: Number of Events 4.5 4 3.5 3 2.5 2
- Page 43 and 44: SEARCHES FOR A HIGH MASS STANDARD M
- Page 45 and 46: Table 1: Number of expected and obs
- Page 47 and 48: SEARCHES FOR BSM HIGGS AT THE TEVAT
- Page 49 and 50: s c → + H with all b) + H → B(t
- Page 51 and 52: HIGGS SEARCHES AT CMS AND ATLAS J.
- Page 53 and 54: Luminosity [fb −1 ] 10 9 8 7 6 5
- Page 55 and 56: LIGHT HIGGS SEARCHES AT THE LHC USI
- Page 57 and 58: dN/dm [arbitrary units] 16000 12000
- Page 59 and 60: Higgs and Beyond the Standard Model
- Page 61 and 62: •Mass&widthininvisibledecays:Deta
- Page 63 and 64: attheLHCwithforwardprotontaggers[25
- Page 65 and 66: HIGGSBOUNDS a : CONFRONTING ARBITRA
- Page 67 and 68: Figure 1: Coverage of the LEP Higgs
- Page 69 and 70: ALL-ORDER CORRECTIONS TO HIGGS BOSO
- Page 71 and 72: [fb] j σ 600 500 400 300 200 100 0
- Page 73 and 74: STRONGLY INTERACTING GAUGE BOSON SY
- Page 75 and 76: where mZZ is the invariant mass of
- Page 77: 3. Light Mesons
- Page 80 and 81: spectrum with background components
- Page 82 and 83: 4 Conclusions The KLOE data set, to
- Page 84 and 85: TABLE I: The branching fractions of
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FIG. 6: The K 0 SK ± π ∓ (a) an
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4. Heavy Flavours
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Figure 1: The representation of the
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Figure 3: Standard Model (left) and
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References 1. KLOE Collaboration, J
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Events/(0.005 GeV) 500 400 300 200
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) -1 (ps 0.6 0.4 0.2 0.0 -0.2 -0.4
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oppositely-charged tracks are requi
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2 Events per 0.010 GeV/c 2 Events p
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anching fraction of B + → Λ ¯
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3.3 Study of ¯ B → Ξc ¯ Λ −
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een done for B0 decays to the V V f
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1 - CL 1.0 0.8 0.6 0.4 0.2 CKM f i
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1.1 X(3872) Amongst the other state
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(and averaged) Υ − ηb hyperfine
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M 2 (π + ψ’), GeV 2 /c 4 Events
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Table 1: Properties of Y (1 −−
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which then decays to Υ(1S), ii) in
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Figure 3: The center of mass energy
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2 Candidates/5 MeV/c 2 Candidates/5
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decay. For each trial, the most sig
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4. chiral extrapolation to the phys
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apex of the CKM unitarity triangle.
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to update measurements of the branc
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We searched for all the above γ+ p
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2 Bottomonium Hyperfine Splitting i
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References 1. A. Pineda and F.J. Yn
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Table 1: D 0/+ semileptonic branchi
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Figure 2: Missing-mass-squared dist
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Table 1: The measured branching fra
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and 3.872 GeV. We observe an anomal
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2 B 0 s ) 2 Events / ( 5 MeV/c 80 6
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Table 1: The branching fractions (B
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(pb/GeV) µ T / dp d σ 10 1 (a) -1
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cc HERA F2 - x = 0.00003 (× 4 20 (
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2 Events/10 MeV/c CMS Preliminary 9
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ATLAS developed a strategy for the
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ÌÎ × Ð ÑÓÐ ÓÖ ÒÙØÖÒÓ
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× Û ÛÓÙÐ Ø×Ø Ø Ø ÁÄ
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form of the Kähler potential, K =
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4 Cosmological vacuum selection 9 T
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NON-SUSY SEARCHES AT THE TEVATRON A
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Figure 2: Key distributions for the
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MODEL INDEPENDENT SEARCHES FOR NEW
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state shows an excess of data compa
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Searches for new phenomena at CMS a
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[GeV] 1/2 m 1000 800 600 400 200 ~
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Multi-muon events at CDF F. Ptochos
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which tracks are required to have h
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(cm) s d 2 1.5 1 0.5 0 0.5 1 d (cm)
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Search for Excess Dimuon Production
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ε( µ ) / 0.5 GeV/c 1 0.95 0.9 0.8
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6. Top
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(1) dileptons, kinematic based appr
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Theoretical computation mt (GeV) NL
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just four years ago. Improved metho
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Table 1: Recent mt measurements by
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Table 2: Measurements of MW using t
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Figure 1: The three SM single top p
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[pb] l, top dσ/d p T -2 10 -3 10 -
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2 Motivation Studies of single top
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DØ estimates the significance of t
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2 Properties of Top Quark Pair Prod
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4 Conclusions A number of propertie
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2 ∆ χ 12 10 8 6 4 2 0 LEP exclus
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[GeV] ± H M 700 600 500 400 300 20
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one another by swapping one t → W
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Events/4 GeV 250 200 150 100 50 ATL
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integrated luminosity. With Ldt =
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6 σ[pb] 5 4 3 2 1 0 0.1 1 µ/mt p
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4 Conclusions In this talk we discu
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(FCNC), can alter this branching ra
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C.L. that range from 48 times the S
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RECENT RESULTS ON JET PHYSICS AT TH
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Figure 3: (left) The measured integ
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PHOTON+JET PRODUCTION AT √ s=1.96
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(pb/GeV) jet dy dy dp T 3 d 3 1
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Jet Studies at CMS and ATLAS Konsta
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the QCD predictions at transverse m
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Monte Carlo methods for robust erro
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Monte Carlo replicas 100 10 1 0.1 0
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Aspects of Jet Production with PHEN
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Figure 3: Example of a di-hadron co
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Jet physics and strong coupling at
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σσ σ σ σ σ
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W/Z+Jets and W/Z+Heavy Flavor Jets
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[1 / GeV] * jet) Z/ γ nd d σ d p
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DIBOSON PRODUCTION CROSS SECTIONS A
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TGCs are −1.09 < ∆κZ < 1.40,
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LEPTON STUDIES WITH ATLAS AND CMS E
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Events/GeV 3500 3000 2500 2000 1500
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Multi-jet cross sections at NLO wit
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dσ / dE T [ pb / GeV ] 10 -1 10 -2
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Two-loop multi-gluon amplitudes in
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So the matching between Wilson loop
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HIGHER-ORDER QCD CORRECTIONS FOR VE
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The universal exponent GN contains
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MEASUREMENT OF THE UNDERLYING EVENT
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Average Charged pT versus Charged M
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MINIMUM BIAS AND UNDERLYING EVENT S
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Table 1: Efficiencies of selected A
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4 Conclusion The revised LHC progra
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2.1 Charmonia constrains to the had
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this suppression can be attributed
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The second harmonic term (v2) means
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shows the comparison of invariant c
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oadening BT and BW, C-parameter C a
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10 −2 assuming partially correlat
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ÁÆÄÍÁÆÌÀÄÇÆÁÌÍÁÆÄ
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xf 1 2 2 Q = 10 GeV 0.8 ZEUS-JETS F
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HIGH Q 2 CROSS SECTIONS, ELECTROWEA
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Unpolarised neutral and charged cur
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Selected Recent HERMES results on P
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2 sin(+S ) h UT 2 sin(+S ) h UT 0.2
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Recent Spin Results from STAR Andre
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and simulation agree well over a la
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SPIN RESULTS FROM THE PHENIX DETECT
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LL A 0.1 0.08 0.06 0.04 0.02 0 Run2
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DIFFRACTION PHYSICS AND LUMINOSITY
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The luminosity is also reduced if t
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DIFFRACTIVE W AND Z PRODUCTION AT T
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3 Diffractive W and Z Measurement T
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DIFFRACTION AT H1 AND ZEUS P. J. LA
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z⋅singlet(z) z⋅singlet(z) 0.2 0
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Introduction Recent results of the
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the very high correlation (-0.93) o
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9. Lattice
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guidance for BSM strongly coupled t
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z , ψ 2 ξ 1 2 z , ψ 3 3 3 λ χ
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For many years calculations were pe
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with the hadron spectrum observed i
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troublesome is the latter. We have
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which is an essential ingredient fo
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where H is the radiator function, d
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1400 1200 1000 800 600 400 ¾( e e
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THE TOTEM EXPERIMENT AT THE LHC G.
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3 Physics Programme The physics goa
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JETS IN THE FORWARD REGION AT THE L
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to all orders in αs. The approach
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Investigation of Hadronic Interacti
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[VEM] µ S 30 25 20 15 10 5 0 0 200
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Forward physics : from SPS to LHC,
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inelastic cross section (mb) 700 60
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11. Heavy Ions
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uncertainties canceling, to first o
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local parity violation in strong in
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AA I 2 1.8 1.6 1.4 1.2 1 0.8 0.6 0.
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hadronic calorimeter, so only neutr
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of 0 < ηtrig < 1.5. Associated par
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In Fig. 3(b), the integrated ridge
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Figure 1: (Color online) Left panel
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limit to free streaming of particle
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9 8 7 6 5 4 3 2 0.4 0.6 0.8 1.0 1.2
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1.2 1.0 0.8 0.6 0.4 0.2 0.0 χ l /T
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2 The Model To describe the J/ψ pr
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We have used PHENIX measurements of
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particle production due to the fact
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10 9 8 7 6 5 4 3 2 1 0 parton dN d
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• Decomposition of the correlatio
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C(k*) 1.4 1.35 1.3 1.25 1.2 1.15 1.
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z)]ûλφi(z,ρ)/ √ 2Ei (hereafte
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m2 D . Approximately such a chromom
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at t = −∞ and ends in a vacuum
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In heavy ion collisions this curren
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Tevatron will provide a contingency
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with respect to the amount of data
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MORIOND 2009, QCD AND HIGH ENERGY I
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nium and bottomonium spectroscopy a
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π + π− decay planes in the meso
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hard scattering process which can b
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scale, lepton energy resolutions, r
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tb tqb W tt Event
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π0 ALL 0.06 0.04 0.02 0 −0.02 GR
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ThePHENIXexperiment has measured as
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massspectruminmultijet+E miss T fin
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epresentsthefirstexclusionbeyondthe
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50. E.G.Ferreiro,Coldnuclearmattere
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2.0 1.5 1.0 0.5 0.0 ρ K* φ mass [
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Jäger 22 discussed pp → V V jj,
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2 ∆ χ 12 10 8 6 4 2 0 LEP exclus
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5 Beyond the Standard Model Two kin
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and in designing experimental analy
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arXiv:0902.2245 [hep-th]. 50. Z. Be
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Martinez Mario ICREA - IFAE Spain m