MadGraph/MadEvent Automatically Calculate 1-Loop Cross Sections !

Slides:



Advertisements
Similar presentations
N =4 Supersymmetric Gauge Theory, Twistor Space, and Dualities David A. Kosower Saclay Lectures Fall Term 2004.
Advertisements

1 Top Production Processes at Hadron Colliders By Paul Mellor.
Bonn 23 rd Feb1 Simulations of BSM Signals Peter Richardson IPPP, Durham University.
1 Bruce Knuteson University of Chicago A Monte Carlo Wishlist 1.Incremental 2.Global.
Les Houches 14 th June1 Matching Matrix Elements and Parton Showers Peter Richardson IPPP, Durham University.
Physics with ATLAS and CMS Are there new symmetries or extra-dimensions? What is dark matter? Where does mass come from? The two big multi-purpose experiments.
QFTHEP04 - St. Petersburg – June 2004 Alessandro Ballestrero 1 E. Accomando A. Ballestrero A. Belhouari E. Maina INFN and Dip. Fisica Teorica Torino.
Introducing II MadGraph Automated Tree-Level Feynman Diagram and Helicity Amplitude Generation +
MadGraph + MadEvent Automated Tree-Level Feynman Diagram, Helicity Amplitude, and Event Generation + Tim Stelzer Fabio Maltoni.
MadGraph + MadEvent Automated Tree-Level Feynman Diagram, Helicity Amplitude, and Event Generation + Tim Stelzer Fabio Maltoni.
Jets and QCD resummation Albrecht Kyrieleis. BFKL at NLO Gaps between Jets.
Evaluating Semi-Analytic NLO Cross-Sections Walter Giele LoopFest 2006 SLAC 06/21/06 Nigel Glover and W.G.: hep-ph/ Giulia Zanderighi, Nigel Glover.
Measurement of α s at NNLO in e+e- annihilation Hasko Stenzel, JLU Giessen, DIS2008.
Benedikt Biedermann | Numerical evaluation of one-loop QCD amplitudes | DESY 2011 Numerical Evaluation of one-loop QCD Amplitudes Benedikt Biedermann Humboldt-Universität.
Irakli Chakaberia Final Examination April 28, 2014.
1 A Preliminary Model Independent Study of the Reaction pp  qqWW  qq ℓ qq at CMS  Gianluca CERMINARA (SUMMER STUDENT)  MUON group.
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.
Efficient Integration of Large Stiff Systems of ODEs Using Exponential Integrators M. Tokman, M. Tokman, University of California, Merced 2 hrs 1.5 hrs.
Outline 3  PWA overview Computational challenges in Partial Wave Analysis Comparison of new and old PWA software design - performance issues Maciej Swat.
The last talk in session-3. Full one-loop electroweak radiative corrections to single photon production in e + e - ACAT03, Tsukuba, 4 Dec LAPTH.
Th.Diakonidis - ACAT2010 Jaipur, India1 Calculating one loop multileg processes A program for the case of In collaboration with B.Tausk ( T.Riemann & J.
Cargese Summer School July 2010Tim Stelzer MadGraph/MadEvent 5.
The SAMPER project (Semi-numerical AMPlitude EvaluatoR) W. Giele, TeV4LHC, 20/10/05 Giulia Zanderighi, Keith Ellis and Walter Giele. hep-ph/ hep-ph/
CompHEP development for distributed calculation of particle processes at LHC
Computational Methods in Particle Physics: On-Shell Methods in Field Theory David A. Kosower University of Zurich, January 31–February 14, 2007 Lecture.
Electroweak Correction for the Study of Higgs Potential in LC LAPTH-Minamitateya Collaboration LCWS , Stanford U. presented by K.Kato(Kogakuin.
Benedikt Biedermann | Numerical evaluation of one-loop QCD amplitudes | ACAT 2011 Numerical Evaluation of one-loop QCD Amplitudes Benedikt Biedermann Humboldt-Universität.
V MCnet network meeting Durham, 15 January 2009 Luca D’ Errico Updates of my work.
12004, TorinoAram Kotzinian Monte Carlo Event Generators The basic lepton-quark scattering processes have well defined cross section formulae within the.
Models Experiment Bridging the Gap Tim Stelzer Fabio Maltoni + CP 3.
1 Higgs, Top and Boson Boson Scattering Six fermion simulations at the LHC E. Maina U. Torino MCWG Frascati Feb 27, 2006.
Top mass error predictions with variable JES for projected luminosities Joshua Qualls Centre College Mentor: Michael Wang.
Experience with CalcHEP H. S. Goh Univ. of Arizona very little West Coast LHC Theory Network -- UC Irvine May
Peter Uwer *) Universität Karlsruhe *) Financed through Heisenberg fellowship and SFB-TR09 LoopFest VII May, 2008, Buffalo NLO QCD corrections to WW +
DIS Conference, Madison WI, 28 th April 2005Jeff Standage, York University Theoretical Motivations DIS Cross Sections and pQCD The Breit Frame Physics.
SHERPA Simulation for High Energy Reaction of PArticles.
1 Update on tt-bar signal and background simulation Stan Bentvelsen.
Physics 842, February 2006 Bogdan Popescu Presentation based on “Introduction to Elementary Particles” by David Griffiths WEAK INTERACTION (1)
Peter Uwer *) Universität Karlsruhe *) Funded through Heisenberg fellowship and SFB-TR09 Radcor 07 —— October 1-5, 2007, Galileo Galilei Institute, Florence.
Slava Bunichev, Moscow State University in collaboration with A.Kryukov.
Six-Fermion Production at ILC with Grcft Calculation of the Six-Fermion Production at ILC with Grcft -New algorithm for Grace- KEK Minamitateya group Yoshiaki.
Modern Approach to Monte Carlo’s (L1) The role of resolution in Monte Carlo’s (L1) Leading order Monte Carlo’s (L1) Next-to-Leading order Monte Carlo’s.
Vector boson scattering at CMS (LHC)
IFIC. 1/15 Why are we interested in the top quark? ● Heaviest known quark (plays an important role in EWSB in many models) ● Important for quantum effects.
David Farhi (Harvard University) Work in progress with Ilya Feige, Marat Freytsis, Matthew Schwartz SCET Workshop, 3/27/2014.
Modern Approach to Monte Carlo’s (L1) The role of resolution in Monte Carlo’s (L1) Leading order Monte Carlo’s (L1) Next-to-Leading order Monte Carlo’s.
Higgs boson production in association with a photon in Vector Boson Fusion at LHC Emidio Gabrielli Uppsala University and Helsinki Institute of Physics.
Session 3 J. Fujimoto KEK May 27, Feynman Diagram Calculations automatization tree level loop level multi-loop Event Generators.
Viktor Veszpremi Purdue University, CDF Collaboration Tev4LHC Workshop, Oct , Fermilab ZH->vvbb results from CDF.
MadGraph/MadEvent 4.0 The New Web Generation Fabio Maltoni (UCL) Tim Stelzer (UIUC) Michel Herquet (UCL) Johan Alwall (UCL) Simon de Visscher (UCL) Rikkert.
MadGraph/MadEvent 4.0 SUSY, 2HDM and more
QCD CORRECTIONS TO bb →h h
Automated Tree-Level Feynman Diagram and Event Generation
More Precision, Less Work
Particle Physics Tour with CalcHEP
First Evidence for Electroweak Single Top Quark Production
Derivation of Electro-Weak Unification and Final Form of Standard Model with QCD and Gluons  1W1+  2W2 +  3W3.
QCD Radiative Corrections for the LHC
Evaluating Semi-Analytic NLO Cross-Sections
B Tagging Efficiency and Mistag Rate Measurement in ATLAS
Announcements Exam Details: Today: Problems 6.6, 6.7
Introduction to state of the art calculations for LHC

Di-jet production in gg collisions in OPAL
Lecture 2: Invariants, cross-section, Feynman diagrams
Zhao Li IHEP-CAS 2016-June-17, CPHEPII
Monte-Carlo event generation for CEPC
Measurement of b-jet Shapes at CDF
UED KK-quark decays in pandora
Presentation transcript:

MadGraph/MadEvent Automatically Calculate 1-Loop Cross Sections ! + MadGraph/MadEvent Automatically Calculate 1-Loop Cross Sections ! Can ? Not Yet! Tim Stelzer Fabio Maltoni

Outline Why am I here? MadGraph MadEvent Topology Generation Diagram/Amplitude Generation MadEvent Single Diagram Enhanced MC 02

Why Am I Here? Currently MadGraph/MadEvent Soon it could Generates Born Level s Uses Helicity Amplitudes Generates Color-Connected Amps Efficient Single-Diagram Integration Soon it could Subtraction of Reals 1-loop diagrams 1-loop helicity amplitudes?? Zoltan Trocsanyi 4

MadGraph Matrix Element / Feynman Diagrams Inspired by FeynArts. Fortran computer program that: Generates fortran helicity code (HELAS) to calculate tree level matrix elements Includes color/symmetry factors Creates postscript file of Feynman diagrams. Here tell story of creating. Francis saying calculate 150 diagrams and see if it’s interesting. Perhaps show example? 05

MadGraph Example pp -> W+ + 3 jets Enter Process: pp > e+ ve jjj Enter QCD Order: 3 Enter QED Order: 2 (…… wait 2 minutes) Generated 53 sub processes 06

Topologies Start with 3 external line topology Add external line to 1 2 Start with 3 external line topology Add external line to 1 7

Topologies Start with 3 external line topology Add external line to 1 4 Topologies 1 3 2 Start with 3 external line topology Add external line to 1 1 2 3 4 7

Topologies Start with 3 external line topology Add external line to 1 2 4 Start with 3 external line topology Add external line to 1 Add external line to 2 1 2 3 4 1 2 4 3 7

Topologies Start with 3 external line topology Add external line to 1 4 2 Start with 3 external line topology Add external line to 1 Add external line to 2 Add external line to 3 1 2 3 4 1 2 4 3 1 2 3 4 8

Topologies Start with 3 external line topology Add external line to 1 4 2 Start with 3 external line topology Add external line to 1 Add external line to 2 Add external line to 3 Add external line to vertex 1 2 3 4 1 2 4 3 1 2 3 4 1 2 3 4 8

Diagram/Amplitudes uu~ > uu~ 1 2 3 4 For each topology Write all external wave functions call ixxxxx(p1, ……W1) call oxxxxx(p2,……W2) call ixxxxx(p3,…..W3) call oxxxxx(p4,…W4) Choose vertex w/ only 1 unknown line Determine allowed interactions and write wavefunction. call jioxxx(W1,W2, …….W5) Continue until all lines known, write amp. call iovxxx(W3,W4,W5, …AMP(1)) 10

Other Elements MADEVENT! Optimization Color factors Summing over partons Loops? MADEVENT! 11

Monte Carlo Integration Advantages Large numbers of dimensions Complicated cuts ONLY OPTION Event generation Limitations Only works for function f(x) ≈ 1 12

Adaptive M.C. (VEGAS) Advantages Limitations Grid adjusts to numerically flatten peaks Flexible Limitations Adjusting grid takes time Peaks must lie on integration variable 13

Multi-Channel M.C. Advantages Limitations Allows for more complicated peaks Limitations Need to calculate all gi values for each point. (slow) Each phase space channel must be invertible N coupled equations for ai so only works for small number of channels. 15

Single Diagram Enhanced MadEvent 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 17

MadEvent Example Vector Bosons 18

MadEvent Example Heavy Quarks and Higgs

It Works!!! Advantages Limitations Integrates cross section and generates unweighted events for “any” tree-level processes. Advantages Can handle “general” problem Parallel in nature Sub channel numbers help with cuts Limitations Still need to adjust grid in some channels. W+5 jets (7,000 diagrams w/ hundreds sub processes) 15

Conclusions MadGraph Could Be Helpful for Automating NLO Born cross section Real Subtraction Automated Integration and Phase Space Loop Diagrams 20