Les Houches 12 th June1 Generator Issues Peter Richardson IPPP, Durham University.

Slides:



Advertisements
Similar presentations
MCnet Marie Curie Research Training Network for Monte Carlo event generator –development –validation and tuning Approved for four years from 1 st Jan 2007.
Advertisements

MCnet Marie Curie Research Training Network for Monte Carlo event generator –development –validation and tuning Approved for four years from 1 st Jan 2007.
Monte Carlo Event Generators
Maria Jose Costa, CERN DIS 2004 April 14 th -18 th 2004, Slovakia b -mass effects in 3 and 4 jets events with the DELPHI detector at LEP b u,d,s.
Minimum bias and the underlying event: towards the LHC I.Dawson, C.Buttar and A.Moraes University of Sheffield Physics at LHC - Prague July , 2003.
CERN 29 th March1 HERWIG Peter Richardson IPPP, Durham University Herwig++
Monte Carlo Simulation of Collisions at the LHC Michael H. Seymour University of Manchester & CERN 5th Vienna Central European Seminar on Particle Physics.
Tt~ Production at ATLAS and tt~ Monte Carlo Generators Borut Paul Kersevan Jozef Stefan Institute and Faculty of Mathematics and Physics, Univ. of Ljubljana.
ATLAS measurements of jets and heavy flavor produced in association with W and Z bosons Pierre-Hugues Beauchemin on behalf of the ATLAS Collaboration Tufts.
Bonn 23 rd Feb1 Simulations of BSM Signals Peter Richardson IPPP, Durham University.
Wine & Cheese Seminar 17 th March1 Recent Developments in Monte Carlo Event Generators Peter Richardson IPPP, Durham University Durham University.
M. Lefebvre25 October QCD Multijet Event Generation MLM prescription for the removal of event double counting M. Lefebvre University of Victoria.
Les Houches 14 th June1 Matching Matrix Elements and Parton Showers Peter Richardson IPPP, Durham University.
Monte Carlo Event Generators
Resummation of Large Logs in DIS at x->1 Xiangdong Ji University of Maryland SCET workshop, University of Arizona, March 2-4, 2006.
Top properties workshop 11/11/05 Some theoretical issues regarding Method 2 J. Huston Michigan State University.
Recent Advances in QCD Event Generators
A Comparison of Three-jet Events in p Collisions to Predictions from a NLO QCD Calculation Sally Seidel QCD’04 July 2004.
Parton Showers and Matrix Element Merging in Event Generator- a Mini-Overview Introduction to ME+PS Branching and Sudakov factor (no branching) Matching.
Aspen Winter Conference, January 2006 Peter Skands Matching (who’s doing it, how, and where?) Matching (who’s doing it, how, and where?) New ideas and.
Collider Physics and QCD Phenomenology Mike Seymour (based at CERN) HERWIG Monte Carlo event generator –Current version ~ frozen (bug fixes and minor new.
1 Methods of Experimental Particle Physics Alexei Safonov Lecture #14.
Sung-Won Lee 1 Study of Jets Production Association with a Z boson in pp Collision at 7 and 8 TeV with the CMS Detector Kittikul Kovitanggoon Ph. D. Thesis.
 s determination at LEP Thorsten Wengler University of Manchester DIS’06, Tsukuba, Japan.
Working group C summary Hadronic final states theory Mrinal Dasgupta.
Monte Carlo event generators for LHC physics
The Dipole-Antenna approach to Shower Monte Carlo's W. Giele, HP2 workshop, ETH Zurich, 09/08/06 Introduction Color ordering and Antenna factorization.
Perturbative Stability of V + Jets Ratios and “Data Driven Background” Analyses Lance Dixon (CERN & SLAC) & for the BlackHat collaboration C. Berger, Z.
Measurement of α s at NNLO in e+e- annihilation Hasko Stenzel, JLU Giessen, DIS2008.
Squarks & Gluinos + Jets: from ttbar to SUSY at the LHC Peter Skands (Fermilab) with T. Plehn (MPI Munich), D. Rainwater (U Rochester), & T. Sjöstrand.
Cambridge 19 th April1 Comparisons between Event Generators and Data Peter Richardson IPPP, Durham University.
GridPP, Durham 5 th July1 PhenoGrid Status Peter Richardson Durham University.
AcerMC and ISR/FSR systematics at ATLAS Liza Mijovic, Borut Kersevan Jozef Stefan Inst. Univ. of Ljubljana ATLAS approach: Generator level studies Parameters.
CKKW studies and other news J. Huston Michigan State University (with help from Ben Cooper and Bruce Mellado)
Sheffield Seminar 23 rd November1 Monte Carlos for LHC Physics Peter Richardson IPPP, Durham University Durham University.
V MCnet network meeting Durham, 15 January 2009 Luca D’ Errico Updates of my work.
QCD Physics with ATLAS Mike Seymour University of Manchester/CERN PH-TH ATLAS seminar January 25 th / February 22 nd 2005.
Models Experiment Bridging the Gap Tim Stelzer Fabio Maltoni + CP 3.
Vincia: A new parton shower and matching algorithm W. Giele, ALCPG07 – LoopVerein session, 10/23/07 The new Vincia shower The pure Vincia shower The matched.
SHERPA Simulation for High Energy Reaction of PArticles.
Aachen, November 2007 Event Generators 3 Practical Topics Peter Skands CERN / Fermilab.
Moriond 20 th March1 Herwig++ Peter Richardson IPPP, Durham University S. Gieseke, D. Grellscheid, K. Hamilton, A. Ribon, PR, P. Stephens, M.H. Seymour,
High P T Inclusive Jets Study High P T Inclusive Jets Study Manuk Zubin Mehta, Prof. Manjit kaur Panjab University, Chandigarh India CMS Meeting March,
1 Update on tt-bar signal and background simulation Stan Bentvelsen.
Measurement of b-quark mass effects for multi-jet events at LEP Juan A. Fuster Verdú EPS-2003 Aachen, July 2003.
ATLAS Higgs Search Strategy and Sources of Systematic Uncertainty Jae Yu For the ATLAS Collaboration 23 June, 2010.
QM 3 rd April1 Collider Phenomenology Peter Richardson IPPP, Durham University.
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.
Study of tt production at NLO Stan Bentvelsen Edwin Bos.
Heavy Particles & Hard Jets: from ttbar at the Tevatron to SUSY at the LHC Peter Skands (Fermilab) with T. Plehn (Edinburgh & MPI Munich), D. Rainwater.
LOGO A partridge in a pear tree Simulation of multi- jet processes using the BFKL event generator Rasmus Mackeprang.
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.
Next Generation of Parton Shower Models and Validation W. Giele, CTEQ workshop “Physics at the LHC: Early Challenges”, 05/14/07 Introduction A new parton.
Tools08 1 st July1 PDF issues for Monte Carlo generators Peter Richardson IPPP, Durham University.
QCD Summary Report S. Ellis U. of Washington “Gee, I sure hope Joey wrote me a good talk.”
SuperB 2 nd June1 Experience in migrating the code to a modern framework Peter Richardson IPPP, Durham University Changing HERWIG  Herwig++
YetiSM 28 th March1 Higher Orders in Parton Shower Monte Carlos Peter Richardson IPPP, Durham University Durham University.
Simulating Physics at the LHC
Discussion on best practice in labelling MC predictions in EXP plots
Event Simulation at the LHC
Introduction to Monte Carlo Event Generators
Overview of IPPP Monte Carlo Tools
New Developments in Herwig++
Peter Richardson IPPP, Durham University
Simulating New Physics at the LHC
More Precision, Less Work
Monte Carlo Simulations
Dijet Azimuthal Distributions at DØ
Monte Carlo Simulations
Controlling the Neutral Drell-Yan at high mass
Presentation transcript:

Les Houches 12 th June1 Generator Issues Peter Richardson IPPP, Durham University

Les Houches 12 th June2 Summary Introduction Basics of Event Generation Improvements to Parton Shower Matching Issues Hadronization Underlying Event New Physics Summary

Les Houches 12 th June3 Introduction Monte Carlo event generators are essential both experimental analyses of real data and studies and predictions for future experiments. It is important that these simulations are as accurate as possible and both experimentalists and theorists understand the approximations and uncertainties involved. Hopefully there will be a lot of discussion of issues of interest to both phenomenologists and experimentalists here.

Les Houches 12 th June4 A Monte Carlo Event Initial and Final State parton showers resum the large QCD logs. Hard Perturbative scattering: Usually calculated at leading order in QCD, electroweak theory or some BSM model. Perturbative Decays calculated in QCD, EW or some BSM theory. Multiple perturbative scattering. Non-perturbative modelling of the hadronization process. Modelling of the soft underlying event Finally the unstable hadrons are decayed.

Les Houches 12 th June5 Monte Carlo Event Generators The different event generators –PYTHIA (P. Skands) –HERWIG (M. Gigg, S. Moretti, P. Richardson, A. Shertsnev) –SHERPA (S. Schumann) use different approximations or models for the different stages of the event. However the overall strategy is the same.

Les Houches 12 th June6 Matrix Element Generators It has become more common to use matrix element generators for the hard process –MADGRAPH (Herquet, Frederix) –ALPGEN ( Piccinini, Pittau) –COMPHEP/CALCHEP (Boos, Pukhov) –SHERPA (Schumann)

Les Houches 12 th June7 Shower Improvements There have been a number of developments in recent years. –Herwig++ Shower algorithm, improved Lorentz invariance and treatment of mass effects. –PYTHIA p T ordered algorithm allows full ordering of event in p T. These are the only improvements which are implemented and available.

Les Houches 12 th June8 Shower Improvements There are a lot of other ideas being worked on –Various approaches based on the dipole/antenna subtraction terms used in NLO calculations (Skands, Giele, Schumann) –SCET approach (Schwartz) –Various forward evolution ideas for initial-state radiation. –Complex weights (Soper, Nagy) –Others???

Les Houches 12 th June9 Shower Improvements Some of these ideas may be useful but need concrete implementations so they can be compared with data. The only true test of a Monte Carlo algorithm is comparison with data.

Les Houches 12 th June10 Shower Questions So a number of possible questions have been raised for discussion and hopefully some work. –Uncertainties, how to assess them particularly for ISR. –1/N c 2 –Non-global soft logs –NLL –Infrared cut-off –Others?

Les Houches 12 th June11 Matching Much of the work in the last 5 years has been on matching parton shower simulations with fixed- order matrix element calculations. A number of approaches have emerged a both leading and next-to-leading order. I’ll start with the leading order approaches

Les Houches 12 th June12 LO Matching: General Idea Parton Shower (PS) simulations use the soft/collinear approximation: –Good for simulating the internal structure of a jet; –Can’t produce high p T jets. Matrix Elements (ME) compute the exact result at fixed order: –Good for simulating a few high p T jets; –Can’t give the structure of a jet. We want to use both in a consistent way, i.e. –ME gives hard emission –PS gives soft/collinear emission –Smooth matching between the two. –No double counting of radiation. All the schemes involve matching between the matrix element and parton shower at some scale.

Les Houches 12 th June13 Two approaches CKKW Simulate N jet partonic state. Apply weight factors for probability that no jets emitted above matching scale. Generate shower vetoing radiation above the matching scale. The weight factors ensure the different samples can be added. MLM Simulate partonic N jet state. Generate parton shower. Require that all the jets above the matching scale after the shower have an associated pre-shower parton. For each N the shower doesn’t add any more jets. Rejection ensures that samples with different numbers of jets can be summed

Les Houches 12 th June14 CKKW results for Z +jets

Les Houches 12 th June15 MLM Method for W+jets

Les Houches 12 th June16 LO Matching So there are people here who have worked on both approaches –ALPGEN (Piccinini, Pittau) –MADGRAPH (Herquet, Frederix) –SHERPA (Schumann) –HERWIG (Richardson)

Les Houches 12 th June17 LO Matching Again the issues are –Differences between different approaches (a lot of work here) –How to access the uncertainties.

Les Houches 12 th June18 Hadronization One issue for both the new generation of C++ generators and generators with matrix element matching is tuning. The parameters of both the parton shower and hadronization were tuned using LEP data and this needs to be done for the new programs. Historically this was done by the LEP collaborations. For the new generation of programs will need to be done by Cedar/JetWeb, MCnet, Tevatron and LHC experiments.

Les Houches 12 th June19 NLO Matching Here we get the correct NLO rate and the first hardest emission correct. A lot of theoretical work. However only one (two?) approaches with concrete implementations. –Nason approach is now available for a number of processes and is the most thoroughly worked out.

Les Houches 12 th June20 NLO Matching The Nason approach has been used for ZZ (Nason and Ridolfi) and e + e - (Gieseke, Latunde-Dada and Webber) Still need to see examples using all parts of the approach. Also only relatively simple cases still need to understand how it will work for e.g. top pair production.

Les Houches 12 th June21 Idea is to include the hardest emission as in a NLO calculation and get the total cross section to NLO accuracy. Rigorous calculation so no new parameters, just the normal ones in the event generator. S. Frixione, P. Nason and B.R. Webber, JHEP 0308(2003) 007, hep-ph/ HERWIG NLO

Les Houches 12 th June22 Nason Approach to hep-ph/ Oluseyi Latunde-Dada, Stefan Gieseke, Bryan Webber

Les Houches 12 th June23 Underlying Event There has been a lot of good work at the Tevatron studying the underlying event. Key question is how does this extrapolate to the LHC and what early measurements to we need to tune the models at LHC energies.

Les Houches 12 th June24 Underlying Event Better agreement between HERWIG and PYTHIA in recent ATLAS tunes. However, had to change the JIMMY model to make it more PYTHIA-like.

Les Houches 12 th June25 BSM Traditionally the requests here have been for more models in HERWIG/PYTHIA. We now have a lot of tools in which adding new models is easier. I’m not sure what we need here? One question is how reliable are the improved narrow-width approximations used in the event generators.

Les Houches 12 th June26 UED Look at the decay q* L e* R Z* ** q e - near e + far e - near e + near e - far e + far

Les Houches 12 th June27 MCnet MCnet is an EU network consisting of all the general purpose event generator authors. The projects involved are Herwig++, Pythia, SHERPA, ThePEG. Nodes are Karlsruhe, CERN, Lund, Durham( +Cambridge) and UserLink based at UCL.

Les Houches 12 th June28 MCnet The main aims of the network are –To train the user community through 4 annual schools, first one April 2007 (Durham) and a large number of three month visiting positions at the nodes. –To train a new generation of event generator authors via a number of postdoc and PhD positions. –To tune, making use of the expertise of the UserLink node, the new Monte Carlo generators.

Les Houches 12 th June29 MCnet The postdocs and PhDs will mainly be involved in development and tuning. The visiting studentships will provide –Mechanism for significant involvement on specific problems/analyses if needed. –A wider pool of knowledge which we hope will reduce the need for support in the long term. Equally we hope the schools will produce a more knowledgeable user community.

Les Houches 12 th June30 MCnet Recently the generator authors collectively agreed, as part of the MCnet program, to release the code under the GPL. However this does not address all our concerns about abuse of the codes. So we have a agreed a set of guidelines for the use of event generators, making modifications etc. Should have a discussion here about these.

Les Houches 12 th June31 Summary There are a lot of areas of Monte Carlo simulation of interest to both theorists and experimentalists. Hopefully we will have lots of useful discussions.