Measurement of the 3-jet to 2-jet Cross Sections Ratio in pp Collisions at 7TeV Update : Pythia8 tune 2C P.Kokkas, I.Papadopoulos, C.Fountas University.

Slides:



Advertisements
Similar presentations
PPR Meeting - May 16, 2003 Andrea Dainese 1 Measurement of D 0 production in pp Andrea Dainese University of Padova.
Advertisements

Low-x and PDF studies at LHC Sept 2008 A M Cooper-Sarkar, Oxford At the LHC high precision (SM and BSM) cross section predictions require precision Parton.
ZEUS high Q 2 e + p NC measurements and high-x cross sections A.Caldwell Max Planck Institute for Physics On behalf of the ZEUS Collaboration Allen Caldwell.
Interjet Energy Flow. Patrick Ryan, Univ. of Wisconsin Collaboration Meeting, June 6, Patrick Ryan University of Wisconsin Claire Gwenlan Oxford.
Measurement of the inclusive jet cross section in p+p collisions at E CM =200 GeV Mike Miller (MIT) For the STAR collaboration.
Low-p T Multijet Cross Sections John Krane Iowa State University MC Workshop Oct , Fermilab Part I: Data vs MC, interpreted as physics Part II:
Jet and Jet Shapes in CMS
Precision Measurement of F 2 with H1 Workshop on DIS and QCD, Florence, Max Klein for the H1 Collaboration Towards today The Measurement Results.
ISR/FSR Tomonobu Tomura (University of Tsukuba). 2 Introduction ISR/FSR is becoming one of the dominant sources of systematic uncertainties for in-situ.
Dimuon Channel ( Z  μμ ) L uminosity ~180 pb -1 (recorded) 2 isolated muons with both having matching central tracks |η μ | 15 GeV 65.0 < M μ 1 μ 2
Interjet Energy Flow at ZEUS. Patrick Ryan. Univ. of Wisconsin DPF, Aug. 27, Patrick Ryan University of Wisconsin Aug. 27, 2004 Interjet Energy.
November 1999Rick Field - Run 2 Workshop1 We are working on this! “Min-Bias” Physics: Jet Evolution & Event Shapes  Study the CDF “min-bias” data with.
T-CHANNEL MODELING UNCERTAINTIES AND FURTHER QUESTIONS TO TH AND NEW FIDUCIAL MEASUREMENTS Julien Donini, Jose E. Garcia, Dominic Hirschbuehl, Luca Lista,
4/10/12 Contribution in ATLAS Collaboration 1 Talk “Multi-jet balance for high pT jet calibration” presented on ATLAS Hadronic Calibration Workshop 2011(SLAC.
Darren Price – Monte Carlo onia simulations at ATLAS QWG Workshop – 20/10/2007Page 1 Monte Carlo quarkonium simulations at A TLAS Darren Price, LANCASTER.
CDF Joint Physics Group June 27, 2003 Rick FieldPage 1 PYTHIA Tune A versus Run 2 Data  Compare PYTHIA Tune A with Run 2 data on the “underlying event”.
H → ZZ →  A promising new channel for high Higgs mass Sara Bolognesi – Torino INFN and University Higgs meeting 23 Sept – CMS Week.
Unfolding jet multiplicity and leading jet p T spectra in jet production in association with W and Z Bosons Christos Lazaridis University of Wisconsin-Madison.
A measurement of the Ratio of Tree over Two Jet Cross Sections with CMS at 7TeV P.Kokkas, I.Papadopoulos, C.Fountas, I.Evangelou, N.Manthos University.
2012 Tel Aviv, October 15, 2012 Rick Field – Florida/CDF/CMSPage 1 Rick Field University of Florida Outline of Talk CMS at the LHC CDF Run 2 
Cambridge 19 th April1 Comparisons between Event Generators and Data Peter Richardson IPPP, Durham University.
16/04/2004 DIS2004 WGD1 Jet cross sections in D * photoproduction at ZEUS Takanori Kohno (University of Oxford) on behalf of the ZEUS Collaboration XII.
Ratio of Three over Two Jet Cross Sections: Update 36 pb -1 P.Kokkas, I.Papadopoulos, C.Fountas University of Ioannina, Greece QCD High p T Meeting 17.
Victor Ryabov (PNPI) for the PHENIX Collaboration QM2005 Budapest Aug,06, First measurement of the  - meson production with PHENIX experiment at.
Fermilab MC Workshop April 30, 2003 Rick Field - Florida/CDFPage 1 The “Underlying Event” in Run 2 at CDF  Study the “underlying event” as defined by.
Update ON the Study of Subjet Multiplicity at CMS 7TeV Manuk Zubin Mehta, Manjit Kaur Panjab University, Chandigarh 11/27/
Hadronic Event Shapes at 7 TeV with CMS Detector S,Banerjee, G. Majumdar, MG + ETH, Zurich CMS PAS QCD M. Guchait DAE-BRNS XIX High Energy Physics.
1 Hadronic Event Shape Variables in pp collision at 7 TeV Introduction Data-set and Event Selection Comparison of Basic Jet Objects in Data and MC Event.
Update : Ratio of Three over Two Jet Cross Sections P.Kokkas, I.Papadopoulos, C.Fountas, I.Evangelou, N.Manthos University of Ioannina, Greece Senior Editor.
Itamar Roth, Ehud Duchovni Group meeting 19/01/15 1.
Predictions of Diffractive and Total Cross Sections at LHC Confirmed by Measurements Konstantin Goulianos / Robert Ciesielski The Rockefeller University.
Hadron Structure 2009 Factorisation in diffraction Alice Valkárová Charles University, Prague Representing H1 and ZEUS experiments Hadron structure.
1 TOP MASS MEASUREMENT WITH ATLAS A.-I. Etienvre, for the ATLAS Collaboration.
Ti Results: Energy and system dependence Conclusions Ridge Jet Figure 1: Sample di-hadron correlation showing the jet-like correlation and the ridge [1]
The Underlying Event in Jet Physics at TeV Colliders Arthur M. Moraes University of Glasgow PPE – ATLAS IOP HEPP Conference - Dublin, 21 st – 23 rd March.
Jet Studies at CDF Anwar Ahmad Bhatti The Rockefeller University CDF Collaboration DIS03 St. Petersburg Russia April 24,2003 Inclusive Jet Cross Section.
Jet + Isolated Photon Triple Differential Cross Section Nikolay Skachkov: “Photon2007”, Paris, 9-13 July 2007 DO Measurement of Triple Differential Photon.
1 Arnold Pompoš, SUSY03, Tucson, Arizona, June 5-10, 2003.
Charged Particle Multiplicity, Michele Rosin U. WisconsinQCD Meeting May 13, M. Rosin, D. Kçira, and A. Savin University of Wisconsin L. Shcheglova.
Update on Diffractive Dijets Analysis Hardeep Bansil University of Birmingham Soft QCD / Diffraction WG Meeting 31/03/2014.
ATLAS Higgs Search Strategy and Sources of Systematic Uncertainty Jae Yu For the ATLAS Collaboration 23 June, 2010.
Update on Diffractive Dijets Hardeep Bansil University of Birmingham 12/07/2013.
Π 0 and η meson production in pp collisions at 0.9, 2.76 and 7 TeV measured with ALICE LHC on the march November 2011 Boris Polishchuk (IHEP, Protvino),
Kinematics of Top Decays in the Dilepton and the Lepton + Jets channels: Probing the Top Mass University of Athens - Physics Department Section of Nuclear.
A measurement of the Ratio of Three over Two Jet Cross Sections with CMS at 7TeV 70 nb -1 P.Kokkas, I.Papadopoulos, C.Fountas, I.Evangelou, N.Manthos University.
Costas Foudas, Imperial College, Jet Production at High Transverse Energies at HERA Underline: Costas Foudas Imperial College
Improved measurements of the b quark mass at LEP María José Costa (IFIC-València) ICHEP 2002 Amsterdam Motivations to measure m b at M Z. Observables sensitive.
Update on Diffractive Dijet Production Search Hardeep Bansil University of Birmingham 23/07/2012.
Jet + Isolated Photon Triple Differential Cross Section Nikolay Skachkov: “Photon2007”, Paris, 9-13 July 2007 DO Measurement of Triple Differential Photon.
UED Observables at the LHC. UED Observables at the LHC? Level 1 Discovery Potential –4 leptons + missing energy –Neutral LKP escapes detection Level 2.
Two particle correlations: from RHIC to LHC Francesco Noferini Bologna University INFN – sez. Bologna ALICE-TOF Tuesday, May 16th Villasimius (Italy) HOT.
1 Unfolding Study 07/11/12. 2 RooUnfold Using the RooUnfold In this study we make response.
What can we learn from high-p T azimuthal correlations of neutral strange baryons and mesons at RHIC ? Jana Bielcikova (Yale University) for the STAR Collaboration.
Joshua Moss (Ohio State University) on behalf of the ATLAS Collaboration ICHEP 2012, Melbourne 6 July 2012 ATLAS Electroweak measurements of W and Z properties.
(members of the group) Underlying CMS F.Ambroglini, D.Acosta, P.Bartalini, A.De Roeck, L.Fanò, R. Field, K.Kotov, E.Izaguirre, A.Vilela.
Erik Devetak Oxford University 18/09/2008
Multilepton production at HERA
Charged Current Cross Sections with polarised lepton beam at ZEUS
Introduction and analysis method
Decomposing p+p Events at √s = 200 GeV with STAR
“Min-Bias” and the “Underlying Event” at CDF
Rick Field – Florida/CDF/CMS
ATLAS 2.76 TeV inclusive jet measurement and its PDF impact A M Cooper-Sarkar PDF4LHC Durham Sep 26th 2012 In 2011, 0.20 pb-1 of data were taken at √s.
Charged Current Cross Sections with polarised lepton beam at ZEUS
“Min-Bias” & “Underlying Event” at the Tevatron and the LHC
Rick Field – Florida/CDF/CMS
The Underlying Event in Hard Scattering Processes
PYTHIA 6.2 “Tunes” for Run II
Heavy Quarkonium production in p-Pb collisions at LHCb
Presentation transcript:

Measurement of the 3-jet to 2-jet Cross Sections Ratio in pp Collisions at 7TeV Update : Pythia8 tune 2C P.Kokkas, I.Papadopoulos, C.Fountas University of Ioannina, Greece High p T meeting 25 Feb 2011

Final Result P.Kokkas, Univ. of Ioannina2 The measured ratio rises with H T as the phase space opens up for a third jet to be emitted, as a result of the 50 GeV p T selection cut. The ratio R 32 reaches a plateau of ≈0.8 which is most sensitive to α s, although its exact value depends upon p T and y cuts as well as the jet finding algorithm. The error bars represent the statistical uncertainty. The yellow band indicates the size of the combined systematic error. Shown also in the same plot, are the predictions of the six MC generators considered in this analysis.

Final Result P.Kokkas, Univ. of Ioannina3 The figure on the left shows the ratio of MC R 32 over Data R 32. The yellow band represents the combined statistical and systematic uncertainty of the data. The predictions of Madgraph agree with the data throughout the H T range of the measurement. The prediction of Alpgen is consistently lower than those of Madgraph and underestimate the measurement for H T <1.5 TeV. The predictions of Pythia6, Pythia8 and Herwig++ are in agreement with the measurement for H T >0.5 TeV, but they overestimate the data for lower values of H T. In the kinematic range of this measurement Madgraph describes best the R 32 data.