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2011 QCD and High Energy Interactio
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Proceedings of the XLVIth RENCONTRE
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2011 RENCONTRES DE MORIOND The XLVI
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Foreword Contents 1. Higgs Searches
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1. Higgs
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95% CL Limit/SM 10 1 Tevatron Run I
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Events/5 GeV 6 10 5 10 4 10 3 10 2
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Events / 0.5 CDF Run II Preliminary
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For the most sensitive sub-channel
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Table 1: Table listing the various
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various SM Higgs mass hypotheses. T
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constraints on parameters are given
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Figure 2: Invariant mass of the ele
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Figure 4: CDF Exclusion limits for
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Table 1: Main phases of 2010 commis
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Table 4: Parameter list for early (
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luminosity of 1.2×10 33 cm −2 s
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2 QCD Analysis settings HERA PDFs a
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min 2 - 2 20 15 10 5 0 H1 and ZEUS
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SM σ / σ 95% CL Limit on 3 10 2 1
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NNLO σ/ σSM 95% CL Upper Bound on
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the report of this working group. I
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2.3 The impact of different PDF par
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SUSY Searches at the Tevatron Ph. G
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on the quality (loose or tight) and
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SUSY searches at ATLAS N. Barlow, o
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channel. These results are combined
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Figure 2: The top left plot shows t
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2010 data. Analysis techniques for
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as main discriminator between event
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sign leptons is particularly intere
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N of events 5 10 DATA 10 4 3 10 10
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) [pb] ν e → B(W’ × σ 10 1 -
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2 Searches in the dijet final state
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ing that the neutrinos were the onl
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The Quasi-Classical Model in SU(N)
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g (γ µ kµ) γ µ Aa µ g (pk)
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3. Top
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of their vertex with respect to the
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of about 9%. 3.1 Differential Cross
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Figure 5: Summary of most recent CD
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the minimum number of jets identifi
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where f’s are probability functio
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hood technique, with a simultaneous
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momentum direction of the b quark f
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Events 200 150 100 50 -1 DØ L=5.4
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after all corrections in the M t¯t
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for prompt J/ψ under the fully tra
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2 Events / 20 MeV/c 50 40 30 20 10
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ATLAS - consists of four parts (mon
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5 D mesons High cross-sections of D
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μ +X') [nb/GeV] → b+X → (pp T
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GeV) μ |
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HEAVY FLAVOUR IN A NUTSHELL Robert
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Figure 1: Overlapping constraints o
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Figure 3: Constraints on new physic
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RECENT B PHYSICS RESULTS FROM THE T
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(IP) distributions are fitted separ
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decays CDF extracts Using a 5.94 fb
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Search for B 0 s → µ+ µ − and
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- Page 133 and 134: CHARMLESS HADRONIC B-DECAYS AT BABA
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- Page 170 and 171: Figure 1: The π 0 recoil mass spec
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- Page 174 and 175: conservation. This second principle
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- Page 196 and 197: Figure 1: Helix string parametrizat
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- Page 202 and 203: Figure 1: Rapidity of the vector bo
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- Page 222 and 223: Figure 3: Leading jet pT in Z/γ
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events / 5 GeV data/MC 5 10 4 10 10
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2 Events/2GeV/c 50 40 30 20 10 CMS
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The results of two new measurements
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The measurement of the differential
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p p i k j l a b c d p p Figure 1: (
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§ ¨ ©© ¥ ¤ £ ¢
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process, gain better insight into t
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d η d N ch . 1/ N ev Ratio 1.8 1.6
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space-time region emitting bosons w
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and Aridane is generated. Pythia is
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ALEPH 91 - 206 GeV Event Shapes JAD
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g q (LO) Z g q Z g (NLO) “LO type
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atio to LO (x µ=1) 3 2.5 2 1.5 1 p
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We then apply the Borel transformat
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Figure 1: (a) M dependence of fπ f
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then results in overall finite inte
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0.002 0 −0.002 −0.004 σNS −
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can be traced back to the different
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σ(W - )B W [nb] 4.4 4.3 4.2 4.1 4
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is compactified to S1 with an anti-
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√ 2 3 MKK mass ✻ ✻ ❄ ✻
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chiral phase transition for Nc > 3,
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2. L.McLerranandR.D. Pisarski, Nucl
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Figure 1: The pp mass spectrum for
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the ηπ 0 mass spectrum recoiling
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is a cylindrical TPC. It has a leng
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GeV/c) µ dy ( T /dp 2 σJ/ ψ d 10
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a unique phase δp for all P-wave f
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events with a subsequent π ± →
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HADRONIC FINAL STATES AND DIFFRACTI
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gap (LRG) between the reaction prod
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(a) (b) (c) Figure 2: a) Reduced cr
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The branch-point λ only depends on
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Figure 2: The rate of rise λ, defi
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The AdS Graviton/Pomeron Descriptio
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Figure 2: In the left, with the BPS
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anticipation of LHC measurements, M
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After Moriond-2011, ATLAS reported
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forward region is not well describe
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7. S. Catani, M. Ciafaloni and F. H
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FIRST MEASUREMENTS IN PB-PB COLLISI
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2 v {4} 2 v 0.3 0.25 0.2 0.15 0.1 0
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TWO-, THREE-, AND JET-HADRON CORREL
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3 Di-Jets through Correlations To e
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Forward Physics in d+Au Collisions:
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Figure 2: (a) Rapidity of a second
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Measurement of jet quenching with I
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CP I 2.5 2.0 1.5 1.0 0.5 0.0 Near s
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Jet Reconstruction and Jet Quenchin
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[GeV] T, leading Subtracted E 140 1
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Studies of Jet Quenching in HI Coll
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0.15), is plotted as a function of
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JET QUENCHING FROM RHIC TO LHC B.G.
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This value was previously obtained
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ELECTRICAL CONDUCTIVITY OF QUARK MA
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References 1. D.E. Kharzeev, L.D. M
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In p+p collisions, in which there i
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is significantly larger than both p
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2 CMS and data taking CMS 5 is a ge
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divided by the expected nuclear ove
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Heavy-flavour production in pp and
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Figure 3: Invariant mass distributi
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Direct Photons and Photon-Hadron Co
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Figure 2: Fraction of direct photon
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Probing nuclear parton densities an
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3 Heavy Quark Energy Loss in γ + Q
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MEASUREMENTS OF Xmax AND TESTS OF H
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82 +25 −21 g/cm2 /decade in the e
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8. Conference Summary
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1 Introduction Most of the LHC resu
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Figure 4: Inclusive electron (left)
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Another domain where Tevatron is st
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3 High Density Matter The one-month
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Figure 15: Yield of high-PT hadrons
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difference related to the amplitude
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List of Participants
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Family name First name Institution