Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 1 1 st Workshop on Energy Scaling in Hadron-Hadron Collisions Rick Field.

Slides:



Advertisements
Similar presentations
IMFP Day 4 April 6, 2006 Rick Field – Florida/CDF/CMSPage 1 XXXIV International Meeting on Fundamental Physics Rick Field University of Florida (for.
Advertisements

Oregon Terascale Workshop March 7, 2011 Rick Field – Florida/CDF/CMSPage 1 Northwest Terascale Workshop Modeling Min-Bias and the Underlying Event Rick.
Oregon Terascale Workshop March 8, 2011 Rick Field – Florida/CDF/CMSPage 1 Northwest Terascale Workshop Modeling Min-Bias and the Underlying Event Rick.
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.
HEP Seminar - Baylor Waco, January 21, 2014 Rick Field – Florida/CDF/CMSPage 1 Outline of Talk CMS at the LHC CDF Run GeV, 900 GeV, 1.96 TeV 900.
University of Toronto March 18, 2008 Rick Field – Florida/CDF/CMSPage 1 Studying the Underlying Event at CDF and the LHC Rick Field University of Florida.
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”.
University of California, Berkeley January 13, 2009 Rick Field – Florida/CDF/CMSPage 1 Studying the Underlying Event at CDF and the LHC Rick Field 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 
Lawrence Berkeley Laboratory January 15, 2009 Rick Field – Florida/CDF/CMSPage 1 Toward an Understanding of Hadron-Hadron Collisions Rick Field University.
IPPP Seminar Durham, September 8, 2015 Rick Field – Florida/CDF/CMSPage 1 Outline of Talk CMS at the LHC CDF “Tevatron Energy Scan” 300 GeV, 900 GeV, 1.96.
Run 2 Monte-Carlo Workshop April 20, 2001 Rick Field - Florida/CDFPage 1 The Underlying Event in Hard Scattering Processes  The underlying event in a.
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.
University of Glasgow Colloquium October 16, 2013 Rick Field – Florida/CDF/CMSPage 1 Outline of Talk CMS at the LHC CDF Run GeV, 900 GeV, 1.96 TeV.
2015 London, September 1, 2015 Rick Field – Florida/CDF/CMSPage 1 Outline of Talk CMS at the LHC CDF “Tevatron Energy Scan” 300 GeV, 900 GeV, 1.96.
C2CR07-Lake Tahoe February 28, 2007 Rick Field – Florida/CDFPage 1 C2CR07 Rick Field University of Florida (for the CDF Collaboration) CDF Run 2 Min-Bias.
Workshop on Early LHC Physics May 6, 2009 Rick Field – Florida/CDF/CMSPage 1 Workshop on Early Physics Opportunities at the LHC Rick Field University of.
LPC CMS Workshop June 8, 2007 Rick Field – Florida/CMSPage 1 LPC Mini-Workshop on Early CMS Physics Rick Field University of Florida (for the.
MC4LHC Workshop July 17-26, 2006 Rick Field – Florida/CDFPage 1 Monte Carlos for the LHC Rick Field University of Florida CDF Run 2 MC4LHC Tuning the Monte-Carlo.
Perugia, Italy October 27, 2008 Rick Field – Florida/CDF/CMSPage 1 Studying the Underlying Event at CDF and the LHC Rick Field University of.
LHC2010 Conference at Michigan Ann Arbor MI, December 12, 2010 Rick Field – Florida/CDF/CMSPage 1 LHC First Data Rick Field University of Florida Outline.
St. Andrews, Scotland August 22, 2011 Rick Field – Florida/CDF/CMSPage Rick Field University of Florida Outline  Do we need a.
MCnet07 - Durham - Part 1 April 18-20, 2007 Rick Field – Florida/CDF/CMSPage 1 Physics and Techniques of Event Generators Rick Field University of Florida.
PIC 2011, Vancouver August 29, 2011 Rick Field – Florida/CDF/CMSPage 1 Physics in Collision Rick Field University of Florida Outline  Examine.
Fermilab Energy Scaling Workshop April 28, 2009 Rick Field – Florida/CDF/CMSPage 1 1 st Workshop on Energy Scaling in Hadron-Hadron Collisions Rick Field.
CDF Paper Seminar Fermilab - March 11, 2010 Rick Field – Florida/CDF/CMSPage 1 Sorry to be so slow!! Studying the “Underlying Event” at CDF CDF Run 2 “Leading.
UF-IFT Seminar Gainesville, FL, November 19, 2010 Rick Field – Florida/CDF/CMSPage 1 Early LHC Physics Rick Field University of Florida Outline of Talk.
LPCC MB&UE Meeting CERN June 17, 2011 Rick Field – Florida/CDF/CMSPage 1 Rick Field University of Florida MB&UE Working Group Meeting CMS ATLAS.
University of Virginia April 10, 2012 Rick Field – Florida/CDF/CMSPage 1 a Rick Field University of Florida Outline  How Universal are the QCD MC Model.
UE&MB Working Group Meeting LPCC May 31, 2010 Rick Field – Florida/CDF/CMSPage 1 Early LHC Measurements Rick Field University of Florida Outline of Talk.
2010 Glasgow, November 30, 2010 Rick Field – Florida/CDF/CMSPage Rick Field University of Florida Outline of Talk  Discuss the.
ICHEP 2012 Melbourne, July 5, 2012 Rick Field – Florida/CDF/CMSPage 1 ICHEP 2012 Rick Field University of Florida Outline of Talk CMS at the LHC CDF Run.
TeV4LHC - Fermilab October 20, 2005 Rick Field - Florida/CDFPage 1 TeV4LHC Workshop Rick Field University of Florida CDF Run 2 Talk #1.
ISMD2004 July 27, 2004 Rick Field - Florida/CDFPage 1 International Symposium on Multiparticle Dynamics Rick Field (theorist?) “Jet Formation in QCD”
Cambridge Workshop July 20, 2002 Rick Field - Florida/CDFPage 1 The “Underlying Event” in Hard Scattering Processes  What happens when a proton and an.
Energy Dependence of the UE
The “Underlying Event” CDF-LHC Comparisons
“softQCD” and Correlations Rick Field & Nick Van Remortel
Physics and Techniques of Event Generators
Lake Louise Winter Institute
MB&UE Working Group Meeting UE Lessons Learned & What’s Next
University of Chicago Lecture 3: Tuning the Models
PHZ 6358 Fall 2011 The Modeling of the Underlying Event Rick Field
A Closer Look at the Underlying Event in Run 2 at CDF
The “Underlying Event” in Run 2 (CDF)
MB&UE Working Group Meeting CMS UE Data and the New Tune Z1
Predicting MB & UE at the LHC
Toward an Understanding of Hadron-Hadron Collisions
Modeling Min-Bias and Pile-Up University of Oregon February 24, 2009
Predicting “Min-Bias” and the “Underlying Event” at the LHC
Early Physics Measurements University of Florida October 2009
Predicting “Min-Bias” and the “Underlying Event” at the LHC
Monte-Carlo Generators for CMS
Rick Field – Florida/CDF/CMS
“Min-Bias” and the “Underlying Event” in Run 2 at CDF and the LHC
XXXIV International Meeting on Fundamental Physics
The Next Stretch of the Higgs Magnificent Mile
The LHC Physics Environment
The “Underlying Event” in Run 2 at CDF
RHIC & AGS Annual Users’ Meeting
CDF Run 2 Monte-Carlo Tunes
International Symposium on Multiparticle Dynamics
Multiple Parton Interactions and the Underlying Event
The “Underlying Event” CDF-LHC Comparisons
“Min-Bias” and the “Underlying Event”
Perspectives on Physics and on CMS at Very High Luminosity
Rick Field - Florida/CDF
The “Underlying Event” at CDF and CMS
Workshop on Early Physics Opportunities at the LHC
Rick Field – Florida/CDF/CMS
Presentation transcript:

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 1 1 st Workshop on Energy Scaling in Hadron-Hadron Collisions Rick Field University of Florida Outline of Talk CMS at the LHC CDF Run 2  Extrapolating “min-bias” collisions to the LHC.  LHC predictions!  Studying versus Nchg in “min-bias” collisions and in Drell-Yan. From CDF to CMS Fermilab 2009  Summary.

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 2 Charged Particle Density: dN/d   Charged particle (all p T ) pseudo-rapidity distribution, dN chg /d  d , at 1.96 TeV for inelastic non-diffractive collisions from PYTHIA Tune A, Tune S320, and Tune P324.  Charged particle (p T >0.5 GeV/c) pseudo- rapidity distribution, dN chg /d  d , at 1.96 TeV for inelastic non-diffractive collisions from PYTHIA Tune A, Tune S320, and Tune P324.

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 3 Charged Particle Density: dN/d  Tevatron LHC  Extrapolations of PYTHIA Tune A, Tune S320, and Tune P329 to the LHC.  Charged particle (all p T ) pseudo-rapidity distribution, dN chg /d  d , at 1.96 TeV for inelastic non-diffractive collisions from PYTHIA Tune A, Tune S320, and Tune P324. RDF LHC Prediction!

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 4 Charged Particle Density: dN/d  Tevatron LHC  Extrapolations of PYTHIA Tune A, Tune S320, and Tune P329 to the LHC.  Charged particle (p T > 0.5 GeV/c) pseudo-rapidity distribution, dN chg /d  d , at 1.96 TeV for inelastic non-diffractive collisions from PYTHIA Tune A, Tune S320, and Tune P324. RDF LHC Prediction! Why is py64 Tune P329 higher than py Tune DWT??

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 5 Min-Bias Correlations  Data at 1.96 TeV on the average p T of charged particles versus the number of charged particles (p T > 0.4 GeV/c, |  | < 1) for “min-bias” collisions at CDF Run 2. The data are corrected to the particle level and are compared with PYTHIA Tune A at the particle level (i.e. generator level).

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 6 Min-Bias: Average PT versus Nchg =+ +  Beam-beam remnants (i.e. soft hard core) produces low multiplicity and small with independent of the multiplicity.  Hard scattering (with no MPI) produces large multiplicity and large.  Hard scattering (with MPI) produces large multiplicity and medium. The CDF “min-bias” trigger picks up most of the “hard core” component! This observable is sensitive to the MPI tuning!

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 7 Average PT versus Nchg  Data at 1.96 TeV on the average p T of charged particles versus the number of charged particles (p T > 0.4 GeV/c, |  | < 1) for “min-bias” collisions at CDF Run 2. The data are corrected to the particle leveland are compared with PYTHIA Tune A, Tune DW, and the ATLAS tune at the particle level (i.e. generator level).  Particle level predictions for the average p T of charged particles versus the number of charged particles (p T > 0.5 GeV/c, |  | < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV) at CDF Run 2.

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 8 Average PT versus Nchg =+  Z-boson production (with low p T (Z) and no MPI) produces low multiplicity and small. +  High p T Z-boson production produces large multiplicity and high.  Z-boson production (with MPI) produces large multiplicity and medium. No MPI!

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 9 Average PT(Z) versus Nchg  Data on the average p T of charged particles versus the number of charged particles (p T > 0.5 GeV/c, |  | < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV) at CDF Run 2. The data are corrected to the particle level and are compared with various Monte-Carlo tunes at the particle level (i.e. generator level). No MPI!  Predictions for the average P T (Z-Boson) versus the number of charged particles (p T > 0.5 GeV/c, |  | < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV) at CDF Run 2.

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 10 Average PT versus Nchg  Predictions for the average p T of charged particles versus the number of charged particles (p T > 0.5 GeV/c, |  | < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV, P T (pair) < 10 GeV/c) at CDF Run 2.  Data the average p T of charged particles versus the number of charged particles (p T > 0.5 GeV/c, |  | < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV, P T (pair) < 10 GeV/c) at CDF Run 2. The data are corrected to the particle level and are compared with various Monte-Carlo tunes at the particle level (i.e. generator level). P T (Z) < 10 GeV/c No MPI! Remarkably similar behavior! Perhaps indicating that MPI playing an important role in both processes.

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 11 LHC Predictions  The amount of activity in “min-bias” collisions. I believe we are now in a position to make some predictions at the LHC!  The amount of activity in the “underlying event” in hard scattering events.  The amount of activity in the “underlying event” in Drell- Yan events. If the LHC data are not in the range shown here then we learn new physics!

Fermilab Energy Scaling Workshop April 29, 2009 Rick Field – Florida/CDF/CMSPage 12 Summary  We are making good progress in understanding and modeling the “underlying event”.  It is clear now that the default value PARP(90) = 0.16 is not correct and the value should be closer to the Tune A value of  The new Pythia p T ordered tunes (py64 S320 and py64 P329) are very similar to Tune A and Tune DW. At present the new tunes do not fit the data better than Tune A and Tune DW. However, the new tune are theoretically preferred!  Need to measure “Min-Bias” and the “underlying event” at the LHC as soon as possible to see if there is new QCD physics to be learned!  All tunes with the default value PARP(90) = 0.16 are wrong and are overestimating the activity of min-bias and the underlying event at the LHC! This includes all the ATLAS tunes! However, I believe that the better fits to the LEP fragmentation data at high z will lead to small improvements of Tune A at the Tevatron!