The Madgraph/MadEvent generator: an update.

Size: px
Start display at page:

Download "The Madgraph/MadEvent generator: an update."

Transcription

1 The Madgraph/MadEvent generator: an update. The Web Generation Fabio Maltoni UCL Tim Stelzer UIUC

2 Yuri Dokshitzer, Lyon, 5 hours ago

3 Outline Motivation Current Status Standard Model Matrix Element and Feynman Diagram Protons, Jets, Les Houches and user specified Models Integration / Event Generation Examples Outlook

4 Motivation A large amount of time and energies are devoted to produce tree-level Monte Carlo data sets These are the key to many foreseeable measurements Most of it is a solved problem => no fame! It involves both theorists and experimentalists Automatize the full procedure => free us!

5 Big Picture User requests any process (leťs say in the SM): process ppp ppp > e+ >b b~ ve h jjjjjj jj j QCD order 0 36 QED order 0 23 MadGraph/MadEvent Returns: List all contributing sub processes Feynman diagrams for each sub process Self-Contained Fortran Package Integrates to get the cross section Generates unit-weighted events Les Houches ready

6 How can I generate events? 1. Log on to the web page and input the process 2. Download the code and run it 3. Check your results with a browser It seems easy, but is it really? Leťs see!!

7 How can I generate events? 1. Log on to the web page and input the process 2. Download the code and run it 3. Check your results with a browser It seems easy, but is it really? Leťs see!!

8 Flexibility User defined models: - Standard Model - MSSM (Plehn and Rainwater) - Higgs EFT NEW!

9 Flexibility II Given a model the user can choose the order of the QCD and QED couplings Include multi-particle labels for protons and Jets: pp > W+ W- b b~ j Require / Exclude particles in a process: pp > tt~ >W+ W- b b~ j //Z Example: Spin correlations can be included exactly for any process!

10 Example: pp>ttbb pp t th t tb b is an important discovery mode for a light LHC Backgrounds are large and difficult to curb!

11 Example: pp>ttbb In collaboration with CompHEP (Boos) Amp 2 = A QCD 2 α 4 S + A EM 2 α 2 Sα 2 EM But what about interference? +2α 3 Sα EM Re(A QCD A EM ) Iťs negative and large (~20%)!

12 MadGraph Capabilities Good news: Matrix elements generated minutes All sub processes identified and calculated Extendable to new models Large number of particles Color information for showers (see later!) Limitations: Must integrate over phase space. Maximum 9999 diagrams/sub process (W+5j)

13 MadEvent Integration and Event Generation Automatization of integration of all sub processes Hard problem because matrix elements are sharply peaked All previous Monte Carlo methods cannot be adapted to the general-purpose phylosophy

14 Single-Diagram-Enhanced summary Key Idea Any single diagram is easy to integrate Divide integration into pieces, based on diagrams Get N independent integrals Errors add in quadrature so no extra cost No need to calculate weight function from other channels. Can optimize # of points for each one independently Parallel in nature What about interference? Never creates new peaks, so we re OK!

15 Single diagram information The integration diagram-by-diagram offers unforseen insights on the process Each diagram is not a gauge-invariant quantity => the corresponding integral is not physical by itself. Anyway, its topology is invariant and can give useful information on the dominant kinematic configuration.

16 Single diagram information Example: gg b bh w/o cuts on the b-jets Q: What are the dominant contributions? 8 diagrams in total Hints to the use of the right scale and/or to b-pdf to resum possibly large log m b m h

17 Integrates cross section and generates unweighted events for any tree-level processes Events are stored in the Les Houches format: Interfaces for PYTHIA and HERWIG are available! Advantages Can handle general problem Parallel in nature => use a PC cluster! Limitations: MadEvent Capabilities - Factorial growth of the Feynman diagrams: Example: W+5 jets (7,000 diagrams w/ hundreds sub processes) Yuri said: It grows like MAD...

18 W+jets: MC4LHC comparison

19 Just a few recent applications Samples for ME-PS matching studies of Mrenna- Richardson: e+ e- > n jets and pp>w + n jets Single top at CDF and D0 (signal and background) ATLAS: WBF studies (B. Mellado) CMS PTDR, Backgrounds for: - Charged Higgs - Radion searches - gg H WW

20 Just a few recent applications Z+(1,2) jets are known at NLO. (Campbell & Ellis, MCFM) Z+ n jets is known at LO+PS matching. (Alpgen or Madgraph + Pythia, Sherpa) PATRIOT=MADGRAPH+PYTHIA The (N)NLO calculations are necessary to fix the normalization and test the distributions. LO+PS works very well in (Z,W)+jets both relative rates.

21 The Decay routine A new routine has been added to MadEvent It allows to decay unstable particles off-line Implemented decays for Higgs,W, Z, top, tau in various channels. Example: pp t th with t bjj, t bl ν l, h b b

22 Latest developments Web based generation: User inputs cuts/parameters Code runs in parallel on farms (US and IT). Returns cross section, plots, root file, and events! Advantages Reduces overhead to getting results Reduce computing cost by load leveling Events can easily be shared/stored Centralize maintenance Come tomorrow to the tutorial and see this working!!

23 To Do: 1. Update the documentation and officially release the latest version. 2. Release of SMADGRAPH and its embedding in MadEvent. 3. Open up the web production to the experimental groups. 4. Produce fully showered and hadronized events directly from the web. 5. Create fully inclusive samples from the web...

24 Summary Madgraph/MadEvent is stable (V3.80) Written in the good old Fortran 77 + sch + Perl Generates unweighted parton-level events in the Les Houches Accord (and also root format). Codes for specific processes are generated on air upon user request and stored in DB Pythia and Herwig interfaces are available Code is maintained and under continuos improvement (SUSY, new models...) Web generator and event repository available ~400 registrations and 10k requestes fullfilled

25 Conclusions MadGraph/MadEvent are available Generate events for ANY tree-level process Multi-purpose philosophy entails: flexibility => huge range of applications immediate response to new questions/needs one framework for all => no overhead/no errors more time to do real analsys! Present and Near future: The original Available Now! Available Soon!

MadGraph5. Olivier Mattelaer CP3/FNRS

MadGraph5. Olivier Mattelaer CP3/FNRS MadGraph5 Olivier Mattelaer CP3/FNRS MG5: J. Alwall / M. herquet / F. Maltoni / OM /T. Stelzer ALOHA: P. Aquino / W. Link / F. Maltoni / OM / T. Stelzer UFO: C. Degrande / C. Duhr / B. Fuks / D. Grellsheid/

More information

MG/ME tutorial: running the code and gridpack preparation

MG/ME tutorial: running the code and gridpack preparation MG/ME tutorial: running the code and gridpack preparation S.de Visscher Université catholique de Louvain On Behalf of the MG/ME Team *** CMS A. M. C. U. a. T. S. - CERN - 15/12/08 1 Plan GridPack and multi-jet

More information

New Developments in MadGraph/MadEvent

New Developments in MadGraph/MadEvent SLAC-PUB-14697 New Developments in MadGraph/MadEvent J. Alwall, P. Artoisenet, S. de Visscher, C. Duhr, R. Frederix, M. Herquet and O. Mattelaer SLAC, Stanford University, Menlo Park, CA 94025, E-mail:

More information

Simulations of Beyond Standard Model Physics in Herwig++

Simulations of Beyond Standard Model Physics in Herwig++ Simulations of Beyond Standard Model Physics in Herwig++ Martyn Gigg IPPP, Durham University IOP HEPP Conference, Lancaster, 2nd April 2008 Outline Basics of event generation, Outline of method for inclusion

More information

MonteCarlo s for Top Physics

MonteCarlo s for Top Physics MonteCarlo s for Top Physics Fabio Maltoni Center for Particle Physics and Phenomenology Université Catholique de Louvain European Physical Society, HEP 2007, Manchester 19th July Outline From top physics

More information

Understanding the backgrounds to WW->H at the LHC: the Zeppenfeld plots

Understanding the backgrounds to WW->H at the LHC: the Zeppenfeld plots Understanding the backgrounds to WW->H at the LHC: the Zeppenfeld plots Ben Cooper University College London Joey Huston Michigan State University -Monte Carlo studies here -Comparisons to data next meeting

More information

Understanding Top and Its Backgrounds

Understanding Top and Its Backgrounds Understanding Top and Its Backgrounds Maximizing the Chances of Finding New Physics in Run2 Stephen Mrenna Computing Division Fermilab and MCTP University of Michigan Top Quark Symposium 2005 Stephen Mrenna

More information

Higgs Production at LHC

Higgs Production at LHC Higgs Production at LHC Vittorio Del Duca INFN Torino Havana 3 April 2006 1 In proton collisions at 14 TeV, and for the Higgs is produced mostly via M H > 100 GeV gluon fusion gg H largest rate for all

More information

Jet Matching at Hadron Colliders. Johan Alwall National Taiwan University

Jet Matching at Hadron Colliders. Johan Alwall National Taiwan University Jet Matching at Hadron Colliders Johan Alwall National Taiwan University IPMU Focus week, Tokyo, Japan, 12 Nov 2009 Why jet matching? Many (all) interesting New Physics signals at hadron colliders include

More information

W/Z production with 2b at NLO

W/Z production with 2b at NLO W/Z production with b at NLO Laura Reina Eugene, September 9 Motivations: main background to W H/ZH associated production; single-top production; H/A + b b and other signals of new physics; t t production;

More information

Bound-State Effects on Kinematical Distributions of Top-Quarks at Hadron Colliders

Bound-State Effects on Kinematical Distributions of Top-Quarks at Hadron Colliders 1 Bound-State Effects on Kinematical Distributions of Top-Quarks at Hadron Colliders Hiroshi YOKOYA (CERN-Japan Fellow) based on arxiv:1007.0075 in collaboration with Y. Sumino (Tohoku univ.) 2 Outline

More information

Introduction to MadGraph/MadEvent:

Introduction to MadGraph/MadEvent: Introduction to MadGraph/MadEvent: an informal tutorial Florian Bonnet INFN - Sezione di Padova January 21st 2011 What I will do Why using MadGraph/MadEvent (MG/ME) Getting familiar with the MG/ME environment

More information

Some New Particles beyond the Standard Model

Some New Particles beyond the Standard Model Journal of Applied Mathematics and Physics, 2014, 2, 55-60 Published Online April 2014 in SciRes. http://www.scirp.org/journal/jamp http://dx.doi.org/10.4236/jamp.2014.25008 Some New Particles beyond the

More information

Calculation of the p p t t Higgs cross section at the LHC and potential background analysis

Calculation of the p p t t Higgs cross section at the LHC and potential background analysis Calculation of the p p t t Higgs cross section at the LHC and potential background analysis DESY SUMMER STUDENT PROGRAM 2007 Angeliki Koutsoukou- Argyraki * ABSTRACT In this report we present the cross

More information

W/Z+jet results from the Tevatron

W/Z+jet results from the Tevatron W/Z+jet results from the Tevatron Dmitry Bandurin Florida State University On behalf of D0 and CDF Collaborations Moriond QCD 2012, March 15, La Thuile, Italy Precision QCD tests Photon, W, Z etc. p parton

More information

W/Z + jets and W/Z + heavy flavor production at the LHC

W/Z + jets and W/Z + heavy flavor production at the LHC W/Z + jets and W/Z + heavy flavor production at the LHC A. Paramonov (ANL) on behalf of the ATLAS and CMS collaborations Moriond QCD 2012 Motivation for studies of jets produced with a W or Z boson Standard

More information

Towards a more accurate prediction of W +b jets with an automatized approach to one-loop calculations

Towards a more accurate prediction of W +b jets with an automatized approach to one-loop calculations Towards a more accurate prediction of W +b jets with an automatized approach to one-loop calculations Laura Reina Loops and Legs in Quantum Field Theory Wernigerode, April 2012 Outline Motivations: W +b-jet

More information

Using MadGraph/MadEvent/PYTHIA/PGS

Using MadGraph/MadEvent/PYTHIA/PGS Using MadGraph/MadEvent/PYTHIA/PGS Ian-Woo Kim Seoul National University SNU, Mar 20, 2007 Ian-Woo Kim (SNU) MadGraph/MadEvent/PYTHIA/PGS SNU 03/2007 1 / 18 Introduction MadGraph/MadEvent is a Feynman

More information

NLM introduction and wishlist

NLM introduction and wishlist 1. NLM introduction and wishlist he LHC will be a very complex environment with most of the interesting physics signals, and their backgrounds, consisting of multi-parton (and lepton/photon) final states.

More information

MC(4BSM) Overview. Kentarou Mawatari,

MC(4BSM) Overview. Kentarou Mawatari, MC(4BSM) Overview Kentarou Mawatari, 1. History of MC4BSM 2. BSM workflow at the LHC 3. Beyond LO+PS 4. Summary and outlook disclaimer (Who am I?) I m a pheno person. I m a heavy user of MC tools, but

More information

How to turn a hep-ph paper into a simulation: Introduction. M. E. Peskin May 2007

How to turn a hep-ph paper into a simulation: Introduction. M. E. Peskin May 2007 How to turn a hep-ph paper into a simulation: Introduction M. E. Peskin May 2007 in memory of Maurice Jacob If you have a model that makes sense and should be tested in detail, experimenters will ask,

More information

Recent developments in the POWHEG BOX

Recent developments in the POWHEG BOX Recent developments in the POWHEG BOX Emanuele Re IPPP, Durham University Standard Model @ LHC Durham, 12 April 2011 in collaboration with S. Alioli, K. Hamilton, P. Nason and C. Oleari Outline Quick description

More information

Tools for LHC. MadGraph/MadEvent. Ian-Woo Kim, Ji-Hun Kim. Seoul National University. SNU, Mar 31, 2007

Tools for LHC. MadGraph/MadEvent. Ian-Woo Kim, Ji-Hun Kim. Seoul National University. SNU, Mar 31, 2007 Tools for LHC MadGraph/MadEvent Ian-Woo Kim, Ji-Hun Kim Seoul National University SNU, Mar 31, 2007 Ian-Woo Kim (SNU) Tools for LHC SNU 03/2007 1 / 30 Introduction We are facing with the exciting era with

More information

Precision Calculations for Collider Physics

Precision Calculations for Collider Physics SFB Arbeitstreffen März 2005 Precision Calculations for Collider Physics Michael Krämer (RWTH Aachen) Radiative corrections to Higgs and gauge boson production Combining NLO calculations with parton showers

More information

Precision Jet Physics At the LHC

Precision Jet Physics At the LHC Precision Jet Physics At the LHC Matthew Schwartz Harvard University JETS AT THE LHC An (almost) universal feature of SUSY is and Source: Atlas TDR SIGNAL VS. BACKGROUND Source: Atlas TDR Can we trust

More information

Sherpa, Event Generator for the LHC. Stefan Höche Dresden University of Technology

Sherpa, Event Generator for the LHC. Stefan Höche Dresden University of Technology Sherpa, Event Generator for the LHC Stefan Höche Dresden University of Technology Outline Introduction Matrix Elements in Sherpa Merging ME s with the Parton Shower Simulation results vs. Data Conclusion

More information

New particle Searches in the dijet final state at 13TeV with the ATLAS detector

New particle Searches in the dijet final state at 13TeV with the ATLAS detector New particle Searches in the dijet final state at 13TeV with the ATLAS detector Mohammad Atif August 21, 2015 1 INTRODUCTION Summer Project at CERN Supervised by Dr. Caterina Doglioni. In Standard Model

More information

PDFs for Event Generators: Why? Stephen Mrenna CD/CMS Fermilab

PDFs for Event Generators: Why? Stephen Mrenna CD/CMS Fermilab PDFs for Event Generators: Why? Stephen Mrenna CD/CMS Fermilab 1 Understanding Cross Sections @ LHC: many pieces to the puzzle LO, NLO and NNLO calculations K-factors Benchmark cross sections and pdf correlations

More information

SM/BSM physics with GoSam

SM/BSM physics with GoSam Physik-Institut SM/BSM physics with GoSam Nicolas Greiner On behalf of the GoSam collaboration Monte Carlo Tools for Physics Beyond the Standard Model -- 20-24.7.2016 Beijing Outline q Very brief introduction

More information

Measurements of the production of a vector boson in association with jets in the ATLAS and CMS detectors

Measurements of the production of a vector boson in association with jets in the ATLAS and CMS detectors Measurements of the production of a vector boson in association with s in the ALAS and CMS detectors Vieri Candelise University of rieste and INFN rieste, Via Valerio 2, 3428, rieste, Italy Abstract. he

More information

Measurement of W-boson Mass in ATLAS

Measurement of W-boson Mass in ATLAS Measurement of W-boson Mass in ATLAS Tai-Hua Lin on behalf of the ATLAS collaboration Blois 2017, France Outline Motivation for W mass measurement Measurement Strategy Method: Monte Carlo Templates Fits

More information

MadGraph/MadEvent v4: The new web generation

MadGraph/MadEvent v4: The new web generation slac-pub-12603 hep-ph/0706.2334 June 2007 Preprint typeset in JHEP style - HYPER VERSION CP3-07-17 MadGraph/MadEvent v4: The new web generation Johan Alwall Stanford Linear Accelerator Center, Stanford

More information

Early SUSY Searches in Events with Leptons with the ATLAS-Detector

Early SUSY Searches in Events with Leptons with the ATLAS-Detector Early SUSY Searches in Events with Leptons with the ATLAS-Detector Timo Müller Johannes Gutenberg-Universität Mainz 2010-29-09 EMG Annual Retreat 2010 Timo Müller (Universität Mainz) Early SUSY Searches

More information

A program for Matrix Element

A program for Matrix Element A program for Matrix Element Olivier Mattelaer University of Illinois at Urbana Champaign May 20 2013 Olivier Mattelaer 1 Aims of this seminar Motivate Monte-Carlo Physics Describe the methods Advertise

More information

Results on top physics by CMS

Results on top physics by CMS EPJ Web of Conferences 95, 04069 (2015) DOI: 10.1051/ epjconf/ 20159504069 C Owned by the authors, published by EDP Sciences, 2015 Results on top physics by CMS Silvano Tosi 1,2,a, on behalf of the CMS

More information

Precision QCD at the Tevatron. Markus Wobisch, Fermilab for the CDF and DØ Collaborations

Precision QCD at the Tevatron. Markus Wobisch, Fermilab for the CDF and DØ Collaborations Precision QCD at the Tevatron Markus Wobisch, Fermilab for the CDF and DØ Collaborations Fermilab Tevatron - Run II Chicago Ecm: 1.8 1.96 TeV more Bunches 6 36 Bunch Crossing 3500 396ns CDF Booster Tevatron

More information

Accelerating Particle Discoveries Through Computation. Igor Volobouev TTU Department of Physics

Accelerating Particle Discoveries Through Computation. Igor Volobouev TTU Department of Physics Accelerating Particle Discoveries Through Computation Igor Volobouev TTU Department of Physics Measurements in HEP Hadronic showers EM showers Eperimental High Energy Physics (HEP) studies particle reactions

More information

QCD Phenomenology at High Energy

QCD Phenomenology at High Energy QCD Phenomenology at High Energy CERN Academic Training Lectures 18-21 February 2008 Lecture 5: Matching Fixed Order Matrix Elements with Parton Showers ME-PS Matching Two rather different objectives:

More information

MadGolem: Automated NLO predictions for SUSY and beyond

MadGolem: Automated NLO predictions for SUSY and beyond David López-Val D. Gonçalves Netto (MPI, Munich), T. Plehn (Heidelberg U.), I. Wigmore (Edinburgh U.), K. Mawatari (Vrije U.) together with ITP - Universität Heidelberg SUSY 2013, Trieste (Italy) - August

More information

PoS(ACAT08)110. Standard SANC Modules. Vladimir Kolesnikov DLNP,Joint Institute for Nuclear Research (JINR)

PoS(ACAT08)110. Standard SANC Modules. Vladimir Kolesnikov DLNP,Joint Institute for Nuclear Research (JINR) E-mail: kolesnik@numail.jinr.ru Anton Andonov Bishop Konstantin Preslavsky University, Shoumen, Bulgaria Andrey Arbuzov BLTP,Joint Institute for Nuclear Research (JINR) Dmitry Bardin Serge Bondarenko BLTP,Joint

More information

Bound-state effects in ttbar production at the LHC

Bound-state effects in ttbar production at the LHC 1 Bound-state effects in ttbar production at the LHC Hiroshi YOKOYA (National Taiwan University) based on works in collaboration with K.Hagiwara(KEK) and Y.Sumino(Tohoku U) GGI workshop, Firenze, 2011.09.28

More information

SUSY MADGRAPH, MADEVENT

SUSY MADGRAPH, MADEVENT SUSY MADGRAPH, MADEVENT Tilman Plehn MPI München & University of Edinurh Madraph/Madevent approach proof of power y LHC examples all under rapid development in name of: J. Alwall, K. Haiwara, F. Maltoni,

More information

t th production at the LHC

t th production at the LHC t th production at the LHC Laura Reina Spring Institute 04: High-energy physics after LHC Run I March 04 Outline Motivations for t th studies. First results coming from LHC s Run I data, most expected

More information

Les Houches and Monte Carlos

Les Houches and Monte Carlos Les Houches and Monte Carlos Much of the time during meeting was spent developing a generic process interface from matrix element to Monte Carlo programs This interface allows: arbitrary hard subprocesses

More information

Differential Top Cross-section Measurements

Differential Top Cross-section Measurements Differential op Cross-section Measurements ALPS207 Obergurgl Michael Fenton on behalf of the ALAS Collaboration University of Glasgow m.fenton.@research.gla.ac.uk April 8, 207 Michael Fenton Differential

More information

Physics at Hadron Colliders

Physics at Hadron Colliders Physics at Hadron Colliders Part 2 Standard Model Physics Test of Quantum Chromodynamics - Jet production - W/Z production - Production of Top quarks Precision measurements -W mass - Top-quark mass QCD

More information

Maria Fiascaris (University of Oxford) ATLAS UK Meeting, Durham 10/01/08

Maria Fiascaris (University of Oxford) ATLAS UK Meeting, Durham 10/01/08 Summary W/Z + Jets Analyses Maria Fiascaris (University of Oxford) Aim and Motivations Work of the W/Z + jets Csc Note Group Goal: Measure W/Z+jets cross section in function of Jet Multiplicity and Leading

More information

Proton anti proton collisions at 1.96 TeV currently highest centre of mass energy

Proton anti proton collisions at 1.96 TeV currently highest centre of mass energy Tevatron & Experiments 2 Proton anti proton collisions at 1.96 TeV currently highest centre of mass energy Tevatron performing very well 6.5 fb 1 delivered (per experiment) 2 fb 1 recorded in 2008 alone

More information

Higgs-related SM Measurements at ATLAS

Higgs-related SM Measurements at ATLAS Higgs-related SM Measurements at ATLAS Junjie Zhu University of Michigan 2 nd MCTP Spring Symposium on Higgs Boson Physics Outline Introduction Isolated γγ cross section (37 pb -1, Phys. Rev. D 85, 012003

More information

Physics at Hadron Colliders Part II

Physics at Hadron Colliders Part II Physics at Hadron Colliders Part II Marina Cobal Università di Udine 1 The structure of an event One incoming parton from each of the protons enters the hard process, where then a number of outgoing particles

More information

Top Quark Production at the LHC. Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations

Top Quark Production at the LHC. Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations Top Quark Production at the LHC Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations Phys. Rev. D 83 (2011) 091503, Phys. Rev. D 82 (2010) 054018, Phys. Rev. D 81 (2010) 054028, Comput.

More information

Top production measurements using the ATLAS detector at the LHC

Top production measurements using the ATLAS detector at the LHC Top production measurements using the ATLAS detector at the LHC INFN, Sezione di Bologna and University of Bologna E-mail: romano@bo.infn.it This paper is an overview of recent results on top-quark production

More information

Recent developments on Perturbative QCD (Part I)

Recent developments on Perturbative QCD (Part I) Recent developments on Perturbative QCD (Part I) Jianwei Qiu Iowa State University/Argonne National Laboratory 威海高能物理前沿暑期论坛 (Weihai Summer Topic Seminar On the Frontiers of High Energy Physics) 山东大学 -

More information

Higgs Searches - Overview. Kétévi A. Assamagan BNL

Higgs Searches - Overview. Kétévi A. Assamagan BNL Higgs Searches - Overview Kétévi A. Assamagan BNL Outline SM Higgs MSSM Higgs Mass and coupling measurements Les Houches, June 11, 2009 Ketevi A. Assamagan 2 Improvement in Higgs Studies at the LHC Many

More information

QCD at CDF. Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration

QCD at CDF. Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration QCD at CDF Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration Jet Inclusive Cross-Section Underlying event studies Jet Shapes Specific processes _ W+Jets, γ + γ, γ + b/c, b-jet / bb jet Diffraction

More information

Multi-Particle Processes at the LHC with HELAC

Multi-Particle Processes at the LHC with HELAC Multi-Particle Processes at the LHC with HELAC Malgorzata Worek ITP, Karlsruhe University Dresden 29th May 2008 Outline of the Talk Introduction Particle Physics Today The Large Hadron Collider The Higgs

More information

Stefano Carignano 12/2010. Phenomenology of particle production in pp collisions

Stefano Carignano 12/2010. Phenomenology of particle production in pp collisions Phenomenology of particle production in pp collisions Stefano Carignano 12/2010 Outline Some very basic stuff Modeling interactions in pp collisions Strings and hadronization Motivation pp collisions provide

More information

The simplest observations. How do we know we made a W boson? Easier: How do we know we made a Z boson? Let s consider pp Z + e + e...

The simplest observations. How do we know we made a W boson? Easier: How do we know we made a Z boson? Let s consider pp Z + e + e... The simplest observations How do we know we made a W boson? Easier: How do we know we made a Z boson? Let s consider pp Z + e + e.... Trigger on events with 2 electrons, require two isolated moderate-p

More information

Joseph Lykken Fermilab

Joseph Lykken Fermilab Joseph Lykken Fermilab LHC Theory Initiative Fellows Meeting, 30 April 2008 Monte Carlo Tools for Beyond the Standard Model Physics 3rd workshop: MARCH 10-11, 2008 (CERN) Note: both days will be full days.

More information

Constraining total width of Higgs boson at the LHC. Kajari Mazumdar Tata Institute of Fundamental Research Mumbai

Constraining total width of Higgs boson at the LHC. Kajari Mazumdar Tata Institute of Fundamental Research Mumbai Constraining total width of Higgs boson at the LHC Kajari Mazumdar Tata Institute of Fundamental Research Mumbai DAE-BRNS symposium, IIT, Guwahati December 10, 2014 After the discovery in 2012, the principal

More information

arxiv: v1 [hep-ex] 24 Oct 2017

arxiv: v1 [hep-ex] 24 Oct 2017 Production of electroweak bosons in association with jets with the ATLAS detector arxiv:1710.08857v1 [hep-ex] 24 Oct 2017 S. Spagnolo on behalf of the ATLAS Collaboration INFN Lecce and Dip. di Matematica

More information

Top quark at LHC. M. Villa. Bologna, oggi

Top quark at LHC. M. Villa. Bologna, oggi Top quark at LHC M. Villa Bologna, oggi 1 Outline Top quark characteristics Top production and decay Measurements 2 Outline Top quark characteristics Top production and decay Measurements 3 Top quark I.D.

More information

Theoretical Predictions For Top Quark Pair Production At NLO QCD

Theoretical Predictions For Top Quark Pair Production At NLO QCD Theoretical Predictions For Top Quark Pair Production At NLO QCD Malgorzata Worek Wuppertal Uni. HP2: High Precision for Hard Processes, 4-7 September 2012, MPI, Munich 1 Motivations Successful running

More information

Recent QCD results from ATLAS

Recent QCD results from ATLAS Recent QCD results from ATLAS PASCOS 2013 Vojtech Pleskot Charles University in Prague 21.11.2013 Introduction / Outline Soft QCD: Underlying event in jet events @7TeV (2010 data) Hard double parton interactions

More information

The LHC Higgs Cross Section Working Group: Results and Future Goals. Higgs Hunting Chiara Mariotti, INFN Torino

The LHC Higgs Cross Section Working Group: Results and Future Goals. Higgs Hunting Chiara Mariotti, INFN Torino The LHC Higgs Cross Section Working Group: Results and Future Goals Higgs Hunting 2010 --- Chiara Mariotti, INFN Torino 1 Outline Why precision Higgs physics now The status of the theoretical calculation

More information

CMS Physics Analysis Summary

CMS Physics Analysis Summary Available on the CERN CDS information server CMS PAS EXO-11-009 CMS Physics Analysis Summary Contact: cms-pag-conveners-exotica@cern.ch 01/05/06 Search for Contact Interactions in µ + µ Events in pp Collisions

More information

GoSam: Automated One Loop Calculations within and beyond the SM

GoSam: Automated One Loop Calculations within and beyond the SM GoSam: Automated One Loop Calculations within and beyond the SM Nicolas Greiner Max-Planck Institute for Physics in collaboration with G.Cullen,H.vanDeurzen,G.Heinrich,G.Luisoni,P.Mastrolia,E.Mirabella,G.Ossola,T.Peraro,J.Schlenk,

More information

High p T physics at the LHC Lecture III Standard Model Physics

High p T physics at the LHC Lecture III Standard Model Physics High p T physics at the LHC Lecture III Standard Model Physics Miriam Watson, Juraj Bracinik (University of Birmingham) Warwick Week, April 2011 1. LHC machine 2. High PT experiments Atlas and CMS 3. Standard

More information

arxiv: v1 [hep-ex] 18 Jul 2016

arxiv: v1 [hep-ex] 18 Jul 2016 Top quark mass measurements with the experiment at the LHC arxiv:67.4972v [hep-ex] 8 Jul 26 Deutsches Elektronen-Synchrotron DESY E-mail: simon.spannagel@desy.de Measurements of the top quark mass are

More information

Single-Top at the Tevatron

Single-Top at the Tevatron Single-Top at the Tevatron Bernd Stelzer University of Toronto on behalf of the CDF and DØD Collaborations 15 th International Conference on Hadron Collider Physics, Michigan State University, 14-18 June

More information

Top production at the Tevatron

Top production at the Tevatron Top production at the Tevatron Bob Hirosky University of Virginia for the CDF and D0 Collaborations Moriond Moriond QCD 2017 1 Top production at the Tevatron Top mass from differential cross section Polarization

More information

What to do with Multijet Events?

What to do with Multijet Events? DØ note 4465 2004-06-03 What to do with Multijet Events? T. Hebbeker RWTH Aachen ABSTRACT Multijet events are frequently produced in p p collisions. Events with several jets might indicate physics beyond

More information

Measurement of t-channel single top quark production in pp collisions

Measurement of t-channel single top quark production in pp collisions Measurement of t-channel single top quark production in pp collisions (on behalf of the CMS collaboration) INFN-Napoli & Università della Basilicata E-mail: Francesco.Fabozzi@cern.ch Measurements of t-channel

More information

The Monte Carlo Event Generator AcerMC and package AcerDET

The Monte Carlo Event Generator AcerMC and package AcerDET The Monte Carlo Event Generator AcerMC and package AcerDET B. Kersevan,, E. Richter-Was,, Faculty of Mathematics and Physics, University of Ljubljana, Jadranska 9, SI-00, Slovenia Experimental Particle

More information

Anomalous Gauge Couplings. Abstract

Anomalous Gauge Couplings. Abstract Anomalous Gauge Couplings Kristina Krylova Department of Physics, University at Buffalo; REU at Wayne State University (Dated: 9 August, 2) Abstract With the Large Hadron Collider s successful operation

More information

Vector boson + jets at NLO vs. LHC data

Vector boson + jets at NLO vs. LHC data Vector boson + jets at NLO vs. LHC data Lance Dixon (SLAC) for the BlackHat collaboration Z. Bern, LD, G. Diana, F. Febres Cordero, S. Höche, H. Ita, D. Kosower, D. Maître, K. Ozeren LHC Theory Workshop

More information

PROSPECTS FOR MEASURING HIGGS CP VIOLATION AT FUTURE COLLIDERS

PROSPECTS FOR MEASURING HIGGS CP VIOLATION AT FUTURE COLLIDERS PROSPECTS FOR MEASURING HIGGS CP VIOLATION AT FUTURE COLLIDERS Felix Yu Johannes Gutenberg University, Mainz U. of Massachusetts, Amherst, Amherst Center for Fundamental Interactions The CP Nature of the

More information

Introduction. The LHC environment. What do we expect to do first? W/Z production (L 1-10 pb -1 ). W/Z + jets, multi-boson production. Top production.

Introduction. The LHC environment. What do we expect to do first? W/Z production (L 1-10 pb -1 ). W/Z + jets, multi-boson production. Top production. Introduction. The LHC environment. What do we expect to do first? W/Z production (L 1-10 pb -1 ). W/Z + jets, multi-boson production. Top production. Early discoveries? Conclusions. 2 First collisions

More information

Yu Gao Mitchell Institute for Fundamental physics and Astronomy Texas A&M University

Yu Gao Mitchell Institute for Fundamental physics and Astronomy Texas A&M University Probing Light Nonthermal Dark Matter @ LHC Yu Gao Mitchell Institute for Fundamental physics and Astronomy Texas A&M University Outline Minimal extension to SM for baryogenesis & dark matter Current constraints

More information

Recent Advances in QCD Event Generators

Recent Advances in QCD Event Generators Durham University Recent Advances in QCD Event Generators Peter Richardson IPPP, Durham University Bonn Seminar 27 th January 1 Introduction Monte Carlo event generators are essential for experimental

More information

La ricerca dell Higgs Standard Model a CDF

La ricerca dell Higgs Standard Model a CDF La ricerca dell Higgs Standard Model a CDF Melisa Rossi INFN-TS Giornata di seminari INFN Trieste - 7 Luglio 2009 FNAL: Fermi National Accelerator Lab Tevatron currently provides the highest energy proton-antiproton

More information

ME/PS Matching Studies in DØ

ME/PS Matching Studies in DØ ME/PS Matching Studies in DØ Daniel Wicke (Fermilab) Outline Introduction MLM CKKW Summary Revision : 1.11 TeV4LHC, 1-Dec-4 1 Introduction Parton shower models good in describing jet evolution, i.e. for

More information

EW theoretical uncertainties on the W mass measurement

EW theoretical uncertainties on the W mass measurement EW theoretical uncertainties on the W mass measurement Luca Barze 1, Carlo Carloni Calame 2, Homero Martinez 3, Guido Montagna 2, Oreste Nicrosini 3, Fulvio Piccinini 3, Alessandro Vicini 4 1 CERN 2 Universita

More information

CTEQ6.6 pdf s etc. J. Huston Michigan State University

CTEQ6.6 pdf s etc. J. Huston Michigan State University CTEQ6.6 pdf s etc J. Huston Michigan State University 1 Parton distribution functions and global fits Calculation of production cross sections at the LHC relies upon knowledge of pdf s in the relevant

More information

Higgs in the light of Hadron Collider limits: impact on a 4th generation

Higgs in the light of Hadron Collider limits: impact on a 4th generation Higgs in the light of Hadron Collider limits: impact on a 4th generation Jack Gunion U.C. Davis Saclay, June 6, 2011 Outline Review of Experimental Status. Eliminating a 4th generation for a light SM-like

More information

Powheg in Herwig++ for SUSY

Powheg in Herwig++ for SUSY Powheg in Herwig++ for SUSY Alix Wilcock IPPP, Durham University 27/04/205 Based on work done with P. Richardson, S. Plätzer and B. Fuks Acronyms SUSY = Supersymmetry Want SUSY to solve the hierarchy problem

More information

Constraints on Higgs-boson width using H*(125) VV events

Constraints on Higgs-boson width using H*(125) VV events Constraints on Higgs-boson width using H*(125) VV events Roberto Covarelli ( University / INFN of Torino ) on behalf of the CMS and ATLAS collaborations 25th International Workshop on Weak Interactions

More information

Computerpraktikum zur Vorlesung Teilchenphysik für Fortgeschrittene

Computerpraktikum zur Vorlesung Teilchenphysik für Fortgeschrittene Institut für Experimentelle Kernphysik (EKP) Prof. Dr. M. Feindt, Dr. M. Kreps, Dr. T. Kuhr C. Hackstein, D. Zander, Dr. A. Zupanc 19. November 2009 Computerpraktikum zur Vorlesung Teilchenphysik für Fortgeschrittene

More information

Higgs properties from experiments. Bruno Mansoulié (CEA-IRFU-Saclay)

Higgs properties from experiments. Bruno Mansoulié (CEA-IRFU-Saclay) Higgs properties from experiments Bruno Mansoulié (CEA-IRFU-Saclay) Contents m H : m(gg) and m(zz*) G H (limits): direct (gg), invisible, interferometry (ZZ*) Spin/CP: gg, WW*, ZZ* Higgs couplings Signal

More information

arxiv:hep-ph/ v1 13 Mar 2002

arxiv:hep-ph/ v1 13 Mar 2002 Higgs couplings at the LHC Dieter Zeppenfeld Department of Physics, University of Wisconsin, Madison, WI 53706, USA (Dated: November 2, 2018) The observation of a SM-like Higgs boson in multiple channels

More information

QCD in gauge-boson production at the LHC "

QCD in gauge-boson production at the LHC QCD in gauge-boson production at the LHC " " Matthias Schott " on behalf of the ATLAS and CMS Collaborations" Prof. Dr. Matthias Schott What can we learn " from those tests?" Inclusive and differential

More information

Recent Results from the Tevatron

Recent Results from the Tevatron Recent Results from the Tevatron Simona Rolli Tufts University (on behalf of the CDF and D0 Collaborations) PPC 2010: IV INTERNATIONAL WORKSHOP ON THE INTERCONNECTION BETWEEN PARTICLE PHYSICS AND COSMOLOGY

More information

Top quark pair cross section measurements at the Tevatron experiments and ATLAS. Flera Rizatdinova (Oklahoma State University)

Top quark pair cross section measurements at the Tevatron experiments and ATLAS. Flera Rizatdinova (Oklahoma State University) Top quark pair cross section measurements at the Tevatron experiments and ATLAS (Oklahoma State University) Outline Introduction: Large Hadron Collider (LHC) and major experiments on it ATLAS detector

More information

ECFA workshop report. Current status of LCGrace. 3nd LC Physics Study Group Meeting. Yoshiaki Yasui Nov. Montpellier France

ECFA workshop report. Current status of LCGrace. 3nd LC Physics Study Group Meeting. Yoshiaki Yasui Nov. Montpellier France 3nd LC Physics Study Group Meeting Yoshiaki Yasui ECFA workshop report 13-16 Nov. Montpellier France Current status of LCGrace Event generator for the Higgs study ECFA workshop(13-16 Nov.2003) Report 185

More information

Double Parton Scattering in CMS. Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x th June 2017 Bari, Italy

Double Parton Scattering in CMS. Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x th June 2017 Bari, Italy Double Parton Scattering in CMS Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x 2017 17th June 2017 Bari, Italy Outline Introduction to DPS DPS measurements with CMS 2b +

More information

Stop pair production at the LHC with Validation figures. C. Degrande, B. Fuks, V. Hirschi, J. Proudom & H.S. Shao

Stop pair production at the LHC with Validation figures. C. Degrande, B. Fuks, V. Hirschi, J. Proudom & H.S. Shao Stop pair production at the LHC with amc@nlo Validation figures C. Degrande, B. Fuks, V. Hirschi, J. Proudom & H.S. Shao November, 0 χ (m,m χ ) = (500, 00) GeV, LO (m,m ) = (00, 50) GeV, LO χ χ (m,m χ

More information

Theory Summary of the SM and NLO Multi-leg WG

Theory Summary of the SM and NLO Multi-leg WG Theory Summary of the SM and NLO Multi-leg WG Departamento de Física Teórica y del Cosmos Universidad de Granada Les Houches June 17th 2009 Theory Summary of the SM and NLO Multi-leg WG Departamento de

More information

HIGGS Bosons at the LHC

HIGGS Bosons at the LHC ATLAS HIGGS Bosons at the LHC Standard Model Higgs Boson - Search for a light Higgs at the LHC - Vector boson fusion - Comparison to the Tevatron potential Measurement of Higgs boson parameters The MSSM

More information

In The Dawn of The LHC Era

In The Dawn of The LHC Era In The Dawn of The LHC Era Tao Han University of Wisconsin Madison LHC Panel Discussion SUSY 06, UC-Irvine, June 15, 2006 In The Dawn of The LHC Era Tao Han University of Wisconsin Madison LHC Panel Discussion

More information

Studies of top pair production in the fully hadronic channel at LHC with CMS

Studies of top pair production in the fully hadronic channel at LHC with CMS Studies of top pair production in the fully hadronic channel at LHC with CMS Claudia Ciocca University of Bologna CMS Collaboration DIS 2006 XIV International Workshop on Deep Inelastic Scattering Tsukuba,

More information