Lessons from the early LHC data for MC tuning

Size: px
Start display at page:

Download "Lessons from the early LHC data for MC tuning"

Transcription

1 Lessons from the early LHC data for MC tuning P. S k a n d s ( C E R N ) Multiple Partonic Interactions at LHC, November 211, Hamburg

2 A Factorized View 1. Where is the energy going? Note: only linearized Sphericity is IR safe Sum(pT) densities, event shapes, mini-jet rates, ctrl&fwd energy flow, energy correlations sensitive to pqcd + pmpi IR Safe 2. How many tracks is it divided onto? Ntracks, dntracks/dpt, Associated track densities, track correlations sensitive to hadronization + soft MPI 3. Are there gaps in it? Created by diffraction (and color reconnections?). Destroyed by UE. 4. What kind of tracks? Strangeness per track, baryons per track, baryon asymmetry, hadron-hadron correlations sensitive to details of hadronization + collective effects (+Quarkonium sensitive to color reconnections?) IR Sensitive More IR Sensitive 2

3 PYTHIA Models LHC data pt-ordered PYTHIA 6 Tune S Tune SA S -Pro ATLAS MC9 Perugia (+ Variations) AMBT1 Z1, Z2 Perugia 21 AUET2B? Perugia 211 (+ Variations) Q-ordered PYTHIA 6 Tune A DW(T) (default) D6(T) D -Pro Pro-Q2O Q2-LHC? pt-ordered PYTHIA 8 Tune 1 2C 2M 4C, 4Cx A1, AU1 A2, AU2 Note: tunes differ significantly in which data sets they include LEP fragmentation parameters Level of Underlying Event & Minimum-bias Tails Soft part of Drell-Yan pt spectrum 3

4 PYTHIA Models LHC data pt-ordered PYTHIA 6 Tune S Tune SA S -Pro ATLAS MC9 Perugia (+ Variations) AMBT1 Z1, Z2 Perugia 21 AUET2B? Perugia 211 (+ Variations) Q-ordered PYTHIA 6 Tune A DW(T) (default) D6(T) D -Pro Pro-Q2O Q2-LHC? pt-ordered PYTHIA 8 Main Data Sets included in each Tune (no guarantee that all subsets ok) A DW, D6,... S, SA MC9(c) Pro-, Perugia, Tune 1, 2C, 2M Tune 1 AMBT1 Perugia 21 Perugia 211 2C 2M 4C, 4Cx A1, AU1 A2, AU2 Z1, Z2 4C, 4Cx AUET2B, A2, AU2 LEP TeV MB ( )? TeV UE ( )? TeV DY LHC MB? LHC UE 4

5 PYTHIA Models LHC data pt-ordered PYTHIA 6 Tune S Tune SA S -Pro ATLAS MC9 Perugia (+ Variations) AMBT1 Z1, Z2 Perugia 21 AUET2B? Perugia 211 (+ Variations) Q-ordered PYTHIA 6 Tune A DW(T) (default) D6(T) D -Pro Pro-Q2O Q2-LHC? pt-ordered PYTHIA 8 Main Data Sets included in each Tune (no guarantee that all subsets ok) A (default) DW, D6,... S, SA MC9(c) Pro-, Perugia, Tune 1, 2C, 2M Tune 1 AMBT1 Perugia 21 Perugia 211 2C 2M 4C, 4Cx A1, AU1 A2, AU2 Z1, Z2 4C, 4Cx AUET2B, A2, AU2 LEP TeV MB ( )? TeV UE ( )? TeV DY LHC MB? LHC UE 5

6 What Works * *) if you use an up-to-date tune. Here comparing to PY6 default (~ Tune A) to show changes. Underlying Event & Jet Shapes UE ΣpT (TRNS) φ ptlead > 5 GeV Jet Shape 3 < pt < 4, All y (softest jet bin available) PS: yes, we should update the PYTHIA 6 defaults... Plots from mcplots.cern.ch 6

7 What Works * *) if you use an up-to-date tune. Here comparing to PY6 default (~ Tune A) to show changes. Drell-Yan pt (Normalized to Unity) Apologies: we don t have DY measurements from LHC on the mcplots site yet dσ (no K-factor) dσ/σ (norm to unity) φ * (norm to unity) PS: yes, we should update the PYTHIA 6 defaults... Plots from mcplots.cern.ch 7

8 What Kind of Works * *) if you use an up-to-date tune. Here comparing to PY6 default (~ Tune A) to show changes. Minimum-Bias Multiplicities (here showing as inclusive as possible) Charged Multiplicity Distribution η distribution Forward-Backward Correlation (UA5) Hoping for LHC measurements soon See Wraight + PS, EPJC71(211)1628 Central LHC Detectors ALICE FMD PS: yes, we should update the PYTHIA 6 defaults... Plots from mcplots.cern.ch 8

9 What Doesn t Work pt Spectra (in particular mass dependence) Strange and baryon production Structure of very soft events Very high-multiplicity events (CMS ridge) (No time to address here, plus no good model yet) Diffraction and forward energy (will return to diffraction on Friday) 9

10 Organized Tuning Can we be more general than thistune-does-this, that-tune-does-that? Yes Schulz & PS, Eur.Phys.J. C71 (211) 1644 The new automated tuning tools can be used to generate unbiased optimizations for different observable regions Same parameters consistent model (not just best tune ) Critical for this task (take home message): Need comparable observable sets for each region Example: test ENERGY SCALING of MB: use different collider energies as regions (Other complementary data sets could be used to test other model aspects) P. Skands 1

11 .5.5 Tuning vs Testing Models 1 3 (c) PARP(82) vs s, N ch (d) PARP(82) vs s, N ch 6 PARP(83) TEST models Evolution of PARP(83) with s PARP(83) Tune parameters in several complementary regions PARP(83) Evolution of PARP(83) with s PARP(83) 63 GeV 9 GeV 18 & 196 GeV Pythia 6 7 TeV Gauss Perugia 1.5 Consistent model same parameters Model breakdown nonuniversal parameters Transverse Mass Distribution 1 3 Exponential PARP(82) Evolution of PARP(82) with s PARP(82) Exp=.25 dˆσ dp 2 p 4 63 GeV ndence 9 GeV p (E CM )=p ref See also Rick Field s talk, p.31 (e) PARP(83) vs s, N ch 1 18 & 196 GeV E ref CM ( ECM ) ɛ Perugia IR Regularization mpact-parameter space which determines leve ts Pythia 6.5 PARP(78) Figure 1: Evolution of parameters with energy.. 7 TeV 1 PARP(78) (f) PARP(83) vs s, N ch 6 Evolution of PARP(78) with s 63 GeV 9 GeV Color Reconnection Strength 18 & 196 GeV Pythia 6 Perugia 7 TeV Energy Scaling of MB Tunes, H. Schulz + PS, Eur.Phys.J. C71 (211) 1644 ( ) 6 ( ) 6 11

12 .5.5 Tuning vs Testing Models 1 3 (c) PARP(82) vs s, N ch (d) PARP(82) vs s, N ch 6 PARP(83) TEST models Evolution of PARP(83) with s PARP(83) Tune parameters in several complementary regions PARP(83) Evolution of PARP(83) with s PARP(83) 63 GeV 9 GeV 18 & 196 GeV Pythia 6 7 TeV Gauss Perugia 1.5 Consistent model same parameters Model breakdown nonuniversal parameters Transverse Mass Distribution 1 3 Exponential PARP(82) Evolution of PARP(82) with s PARP(82) Exp=.25 dˆσ dp 2 p 4 63 GeV ndence 9 GeV p (E CM )=p ref See also Rick Field s talk, p.31 (e) PARP(83) vs s, N ch 1 18 & 196 GeV E ref CM ( ECM ) ɛ Perugia IR Regularization mpact-parameter space which determines leve ts Pythia 6.5 PARP(78) Figure 1: Evolution of parameters with energy.. 7 TeV 1 PARP(78) (f) PARP(83) vs s, N ch 6 Evolution of PARP(78) with s 63 GeV 9 GeV Color Reconnection Strength 18 & 196 GeV Pythia 6 Perugia 7 TeV Energy Scaling of MB Tunes, H. Schulz + PS, Eur.Phys.J. C71 (211) 1644 ( ) 6 ( ) 6 11

13 pt Spectra / Mass Dependence Must be compared with LEP SOFT SOFT STAR: 2 GeV OPAL all charged ~ pions HARD ALEPH Λ baryons HARD STAR measurement Average pt versus particle mass Model predict too hard Pions and too soft massive particles Pions can only be made harder Massive particles can only be made softer! So: tuning problem? or physics problem? Will return on Friday Plots from mcplots.cern.ch 12

14 Strangeness and Baryons Tried to learn from early data, but still not there Λ/K Again, quite difficult to adjust flavor parameters while remaining within LEP bounds Plots from mcplots.cern.ch 13

15 Very Soft Structure Minimum-Bias too lumpy? Underlying Event ok? ptlead > 1 ptlead > 5 Plots from mcplots.cern.ch 14

16 Summary How did the models fare? Lots could be said Bottom line: Not too bad on averages See also talks by Rick Field and others E.g., UE level underpredicted by ~ 1-2% relative to Tevatron tunes (I won my bet!) Significant discrepancies on more exclusive physics Strangeness, Baryons, and Baryon Transport pt spectra High-multiplicity tail (+ridge!) needs more study! Forward measurements and Diffraction LEP More tuning? or new physics? No single model/tune does it all (game still open) 15

17 Diffraction Framework needs testing and tuning E.g., interplay between non-diffractive and diffractive components + LEP tuning used directly for diffractive modeling Hadronization preceded by shower at LEP, but not in diffraction dedicated diffraction tuning of fragmentation pars? Study this bump + Room for new models, e.g., KMR (SHERPA) Others? P. Skands 16

Toward an Understanding of Hadron-Hadron. Collisions From Feynman-Field to the LHC

Toward an Understanding of Hadron-Hadron. Collisions From Feynman-Field to the LHC Toward an Understanding of Hadron-Hadron Collisions From Feynman-Field to the LHC Rick Field University of Florida Outline of Talk The old days of Feynman-Field Phenomenology. XXIèmes Rencontres de Blois

More information

51 st Cracow School of Theoretical Physics The Soft Side of the LHC Min-Bias and the Underlying Event at the LHC Rick Field University of Florida

51 st Cracow School of Theoretical Physics The Soft Side of the LHC Min-Bias and the Underlying Event at the LHC Rick Field University of Florida 5 st Cracow School of Theoretical Physics The Soft Side of the LHC Min-Bias and the Underlying Event at the LHC Rick Field University of Florida Lecture : Outline Review: The CDF Tevatron underlying event

More information

LHC MPI and underlying event results

LHC MPI and underlying event results LHC MPI and underlying event results Marianna Testa (ATLAS) for the ALICE, ATLAS, CMS & LHCb collaborations SM@LHC 2012, Copenhagen, 10-13 April 2012 The Underlying Event Everything in hadron collisions

More information

Tevatron Energy Scan. Energy Dependence of the Underlying Event. Rick Field Craig Group & David Wilson University of Florida

Tevatron Energy Scan. Energy Dependence of the Underlying Event. Rick Field Craig Group & David Wilson University of Florida Rick Field Craig Group & David Wilson University of Florida Tevatron Energy Scan Energy Dependence of the Underlying Event Outline of Talk Wine & Cheese talk, October 4, 2002. Studying the underlying event

More information

Mini-Bias and Underlying Event Studies at CMS

Mini-Bias and Underlying Event Studies at CMS Yuan Chao Department of Physics National Taiwan University 1617 Taipei, TAIWAN 1 Introduction The Tevatron experiments provide us very good information for the quantum chromodynamics (QCD) modelings of

More information

Underlying Event Measurements at the LHC

Underlying Event Measurements at the LHC 14th EDS Blois Workshop Underlying Event Measurements at the LHC Michael Heinrich for the ATLAS and CMS collaborations INSTITUTE OF EXPERIMENTAL PARTICLE PHYSICS (EKP) PHYSICS FACULTY KIT University of

More information

Minimum Bias at CDF and CMS

Minimum Bias at CDF and CMS Minimum Bias at CDF and CMS Minumum Bias Collisions Proton AntiProton CDF Run 2 CMS Outline of Talk Review the CDF Run 2 minimum bias tune (i.e. PYTHIA Tune A). UE&MB@CMS Show the minimum bias predictions

More information

Using Drell-Yan to Probe the

Using Drell-Yan to Probe the Using Drell-Yan to Probe the Underlying Event in Run 2 at CDF Deepak Kar University of Florida (On behalf of the CDF Collaboration) Experimental Particle Physics Seminar 30 th October 2008 Prologue: We

More information

The Lund Model. and some extensions. Department of Astronomy and Theoretical Physics Lund University Sölvegatan 14A, SE Lund, Sweden

The Lund Model. and some extensions. Department of Astronomy and Theoretical Physics Lund University Sölvegatan 14A, SE Lund, Sweden The Lund Model and some extensions Torbjörn Sjöstrand Department of Astronomy and Theoretical Physics Lund University Sölvegatan 4A, SE-223 62 Lund, Sweden Workshop on Collective effects in small collisions

More information

HEP Seminar. Studying the Energy Dependence of the Underlying Event at the Tevatron and the LHC Rick Field University of Florida.

HEP Seminar. Studying the Energy Dependence of the Underlying Event at the Tevatron and the LHC Rick Field University of Florida. Studying the Energy Dependence of the Underlying Event at the Tevatron and the LHC Rick Field University of Florida HEP Seminar Outline Early studies the underlying event (UE) at CDF and PYTHIA Tune A.

More information

Measurements of Particle Production in pp-collisions in the Forward Region at the LHC

Measurements of Particle Production in pp-collisions in the Forward Region at the LHC 2011 Europhysics Conference on High-Energy Physics, Grenoble Measurements of Particle Production in pp-collisions in the Forward Region at the LHC Thomas Ruf for the LHCb collaboration Introduction Particle

More information

The LHC Physics Environment

The LHC Physics Environment The LHC Physics Environment Talk : What We Have Learned at the Tevatron Rick Field University of Florida Outline of Talk The old days of Feynman-Field Phenomenology. Review what we learned about minbias,

More information

Forward QCD studies and prospects at the LHC

Forward QCD studies and prospects at the LHC Forward QCD studies and prospects at the LHC Pierre.VanMechelen@ua.ac.be (*) INT Workshop on Perturbative and Non-Perturbative Aspects of QCD at Collider Energies 1 Seattle, September 13-18, 2010 (*) As

More information

Recent results on soft QCD topics from ATLAS

Recent results on soft QCD topics from ATLAS Recent results on soft QCD topics from ATLAS Roman Lysák Institute of Physics, Prague on behalf of the ATLAS collaboration Bormio 2016 Overview Understanding of soft-qcd interactions has direct impact

More information

Rivet overview Robust Independent Validation of Experiment and Theory. David Grellscheid

Rivet overview Robust Independent Validation of Experiment and Theory. David Grellscheid Rivet overview Robust Independent Validation of Experiment and Theory David Grellscheid 2015-04-28 Rivet Andy Buckley, Jon Butterworth, David Grellscheid, Hendrik Hoeth, Leif Lönnblad, James Monk, Holger

More information

The Monash 2013 Tune of PYTHIA 8

The Monash 2013 Tune of PYTHIA 8 he Monash 3 une of PYHIA Peter Skands (CERN) Current Default = C (from ) LEP tuning undocumented (from 9) LHC tuning only used very early data + S. Rojo & S. Carrazza recently added a new PDF set: NNPDF.3

More information

University of Glasgow Tevatron Energy Scan: Findings & Surprises

University of Glasgow Tevatron Energy Scan: Findings & Surprises Outline of Talk University of Glasgow Tevatron Energy Scan: Findings & Surprises Rick Field University of Florida Simulating hadron-hadron collisions: The early days of Feynman-Field Phenomenology. The

More information

Soft interactions in Herwig

Soft interactions in Herwig Soft interactions in Herwig Stefan Gieseke Institut für Theoretische Physik KIT work with Patrick Kirchgaeßer and Frashër Loshaj MPI@LHC6 San Cristóbal de las Casas 28 Nov 2 Dec 206 Stefan Gieseke MPI@LHC

More information

LHCP QCD at the Tevatron. Rick Field University of Florida (for the CDF & D0 Collaborations) Outline of Talk. with help from Christina Mesropian

LHCP QCD at the Tevatron. Rick Field University of Florida (for the CDF & D0 Collaborations) Outline of Talk. with help from Christina Mesropian with help from Christina Mesropian QCD at the Tevatron Rick Field University of Florida (for the CDF & D0 Collaborations) Outline of Talk D0 Photon + Jet Measurements. CDF W/Z + Upsilon Search. CDF Measurements

More information

Multiple Parton-Parton Interactions: from pp to A-A

Multiple Parton-Parton Interactions: from pp to A-A Multiple Parton-Parton Interactions: from pp to A-A Andreas Morsch CERN QCD Challenges at LHC Taxco, Mexico, Jan 18-22 (2016) Multiple Parton-Parton Interactions Phys. Lett. B 167 (1986) 476 Q i 2 Λ QCD

More information

QCD Jet Physics with CMS LHC

QCD Jet Physics with CMS LHC QCD Jet Physics with CMS Detector @ LHC Y.Chao for the CMS Collaboration (National Taiwan University, Taipei, Taiwan) QCD10 (25th annivervary) 2010/06/28-07/03 The Large Hadron Collider Four major experiments

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

MPI in PYTHIA. 1. Brief overview 2. Color reconnection and the top mass

MPI in PYTHIA. 1. Brief overview 2. Color reconnection and the top mass MPI in PYTHIA 1. Brief overview 2. Color reconnection and the top mass Torbjörn Sjöstrand Department of Astronomy and Theoretical Physics Lund University Sölvegatan 14A, SE-223 62 Lund, Sweden MPI@LHC

More information

Collisions Rick s View of Hadron Collisions

Collisions Rick s View of Hadron Collisions st Workshop on Energy Scaling in Hadron-Hadron Collisions Rick s View of Hadron Collisions Rick Field University of Florida Fermilab 2009 Outline of Talk The early days of Feynman-Field Phenomenology.

More information

Atlas results on diffraction

Atlas results on diffraction Atlas results on diffraction Alessia Bruni INFN Bologna, Italy for the ATLAS collaboration Rencontres du Viet Nam 14th Workshop on Elastic and Diffractive Scattering Qui Nhon, 16/12/2011 EDS 2011 Alessia

More information

QCD at Cosmic Energies - VII May 16-20, 2016 Chalkida, Greece Multiparton interactions in Herwig

QCD at Cosmic Energies - VII May 16-20, 2016 Chalkida, Greece Multiparton interactions in Herwig QCD at Cosmic Energies - VII May 6-20, 206 Chalkida, Greece Multiparton interactions in Herwig Frashër Loshaj Table of Contents Introduction 2 MPI and the Underlying event 3 Soft interactions 4 Diffraction

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

Introduction to Monte Carlo generators - II

Introduction to Monte Carlo generators - II Introduction to Monte Carlo generators - II (Fully exclusive modeling of high-energy collisions) Andrzej Siódmok CTEQ School - University of Pittsburgh, USA 18-28 July 2017 Thanks to: S. Gieseke, S.Höche,

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

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

arxiv: v1 [hep-ex] 15 Jan 2019

arxiv: v1 [hep-ex] 15 Jan 2019 CMS-CR-8/37 January 7, 9 Top Quark Modelling and Tuning at CMS arxiv:9.559v [hep-ex] 5 Jan 9 Emyr Clement on behalf of the CMS Collaboration University of Bristol Recent measurements dedicated to improving

More information

SOFT QCD AT ATLAS AND CMS

SOFT QCD AT ATLAS AND CMS SAHAL YACOOB UNIVERSITY OF CAPE TOWN ON BEHALF OF THE ATLAS AND CMS COLLABORATIONS SOFT QCD AT ATLAS AND CMS 28th Rencontres de Blois INTRODUCTION IN 15 MINUTES 2 Inelastic cross section ATLAS and CMS

More information

QCD at LHC in pp. Department of Theoretical Physics, Lund University

QCD at LHC in pp. Department of Theoretical Physics, Lund University 3rd Nordic LHC and Beyond Workshop 2-3 February 2009 Lund, Sweden QCD at LHC in pp Torbjörn Sjöstrand Department of Theoretical Physics, Lund University Introduction: the structure of an event Multiple

More information

Review of LHCb results on MPI, soft QCD and diffraction

Review of LHCb results on MPI, soft QCD and diffraction Review of LHCb results on MPI, soft QCD and diffraction Marcin Kucharczyk on behalf of LHCb collaboration HNI Krakow EDS Blois 2015, Borgo (Corse), 30.06.2015 Outline LHCb - general purpose forward experiment

More information

MPI in PYTHIA 8. Richard Corke. Department of Astronomy and Theoretical Physics Lund University. September 2010

MPI in PYTHIA 8. Richard Corke. Department of Astronomy and Theoretical Physics Lund University. September 2010 MPI in PYTHIA 8 Richard Corke Department of Astronomy and Theoretical Physics Lund University September Richard Corke (Lund University) MPI@DESY September / 5 Overview MPI in PYTHIA 8 Enhanced screening

More information

Minimum-Bias and Underlying-Event Physics

Minimum-Bias and Underlying-Event Physics 2008 CTEQ MCnet Summer School on QCD Phenomenology and Monte Carlo Event Generators 8 16 August 2008 Debrecen, Hungary Minimum-Bias and Underlying-Event Physics Torbjörn Sjöstrand Department of Theoretical

More information

QCD Jets at the LHC. Leonard Apanasevich University of Illinois at Chicago. on behalf of the ATLAS and CMS collaborations

QCD Jets at the LHC. Leonard Apanasevich University of Illinois at Chicago. on behalf of the ATLAS and CMS collaborations QCD Jets at the LHC Leonard Apanasevich University of Illinois at Chicago on behalf of the ATLAS and CMS collaborations Outline Physics at the LHC Jet Reconstruction and Performance Clustering Algorithms

More information

Min-Bias Data: Jet Evolution and Event Shapes

Min-Bias Data: Jet Evolution and Event Shapes Min-Bias Data: Jet Evolution and Event Shapes Rick Field and David Stuart July 1, 1999 Abstract The Min-Bias data are used to study the transition between soft and hard collisions. We study this transition

More information

Jet Physics with ALICE

Jet Physics with ALICE Jet Physics with ALICE Oliver Busch for the ALICE collaboration Oliver Busch Tsukuba 2014 /03/13 1 Outline introduction results from pp jets in heavy-ion collisions results from Pb-Pb collisions jets in

More information

MC ATLAS Stephen Jiggins on behalf of the ATLAS Collaboration University College London (UCL)

MC ATLAS Stephen Jiggins on behalf of the ATLAS Collaboration University College London (UCL) MC Tuning @ ATLAS Stephen Jiggins on behalf of the ATLAS Collaboration University College London (UCL) Contents Contents: 1) Monte Carlo models/event generation 2) Basic Tuning Methodology 3) A2 tune series

More information

PYTHIA 6.2 Tunes for Run II

PYTHIA 6.2 Tunes for Run II PYTHIA 6.2 Tunes for Run II Outline of Talk Min-Bias Collisions! Min-Bias Generators Hadron Hadron! The in Hard Scattering Processes Proton Outgoing Parton PT(hard) Initial-State Radiation AntiProton Outgoing

More information

LHCb physics with the first pb 1

LHCb physics with the first pb 1 LHCb physics with the first 10-20 pb 1 Raluca Mureşan EPFL on behalf of the LHCb collaboration R. Mureşan, LHCb physics with the first 10-20 pb 1 p.1/30 Outline LHCb detector First data analysis and rapidity

More information

FYST17 Lecture 6 LHC Physics II

FYST17 Lecture 6 LHC Physics II FYST17 Lecture 6 LHC Physics II 1 Today & Monday The LHC accelerator Challenges The experiments (mainly CMS and ATLAS) Important variables Preparations Soft physics EWK physics Some recent results Focus

More information

QCD Studies at LHC with the Atlas detector

QCD Studies at LHC with the Atlas detector QCD Studies at LHC with the Atlas detector Introduction Sebastian Eckweiler - University of Mainz (on behalf of the ATLAS Collaboration) Examples of QCD studies Minimum bias & underlying event Jet-physics

More information

Status of diffractive models. Robert Ciesielski [The Rockefeller University]

Status of diffractive models. Robert Ciesielski [The Rockefeller University] Status of diffractive models Robert Ciesielski [The Rockefeller University] CTEQ Workshop, QCD tool for LHC Physics: From 8 to 14 TeV, what is needed and why FNAL, 14 November, 2013 1 Main processes contributing

More information

QCD and jets physics at the LHC with CMS during the first year of data taking. Pavel Demin UCL/FYNU Louvain-la-Neuve

QCD and jets physics at the LHC with CMS during the first year of data taking. Pavel Demin UCL/FYNU Louvain-la-Neuve QCD and jets physics at the LHC with CMS during the first year of data taking Pavel Demin UCL/FYNU Louvain-la-Neuve February 8, 2006 Bon appétit! February 8, 2006 Pavel Demin UCL/FYNU 1 Why this seminar?

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

FYST17 Lecture 6 LHC Physics II

FYST17 Lecture 6 LHC Physics II FYST17 Lecture 6 LHC Physics II 1 Today, (tomorrow) & Next week The LHC accelerator Challenges The experiments (mainly CMS and ATLAS) Important variables Preparations Soft physics minímum bias, underlying

More information

Moriond QCD. Latest Jets Results from the LHC. Klaus Rabbertz, KIT. Proton Structure (PDF) Proton Structure (PDF) Klaus Rabbertz

Moriond QCD. Latest Jets Results from the LHC. Klaus Rabbertz, KIT. Proton Structure (PDF) Proton Structure (PDF) Klaus Rabbertz Latest Jets Results from the LHC Proton Structure (PDF) Proton Structure (PDF), KIT 1 Flash Menu Motivation Accelerators and Detectors Jet Algorithms and Calibration Inclusive Jets Dijets and 3-Jets The

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

Minimum Bias and Underlying Event Studies at CDF

Minimum Bias and Underlying Event Studies at CDF FERMILAB-CONF--531-E Minimum Bias and Underlying Event Studies at CDF INFN, Bologna E-mail: moggi@bo.infn.it Soft, non-perturbative, interactions are poorly understood from the theoretical point of view

More information

Monte Carlo activities in ALICE

Monte Carlo activities in ALICE Monte Carlo activities in ALICE status and prospects Jochen Klein for the ALICE Collaboration CERN 8th International Workshop on Multiple Partonic Interactions at the LHC San Cristóbal de las Casas, Chiapas,

More information

The first year of the LHC: what we have learned

The first year of the LHC: what we have learned The first year of the LHC: what we have learned UK ChristmasTheory Workshop, Durham, Dec 16-17 2010 Michelangelo L. Mangano CERN PH-TH Introduction A year of learning: confirmations, surprises Every piece

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

Some studies for ALICE

Some studies for ALICE Some studies for ALICE Motivations for a p-p programme in ALICE Special features of the ALICE detector Preliminary studies of Physics Performances of ALICE for the measurement of some global properties

More information

QCD at hadron colliders

QCD at hadron colliders QCD at hadron colliders This will be a brief experimentalist s view, with a concentration on the two hadron-hadron colliders mentioned in the previous talk If you want a good reference book for graduate

More information

The inclusive jet cross section, jet algorithms, underlying event and fragmentation corrections. J. Huston Michigan State University

The inclusive jet cross section, jet algorithms, underlying event and fragmentation corrections. J. Huston Michigan State University The inclusive jet cross section, jet algorithms, underlying event and fragmentation corrections J. Huston Michigan State University Tevatron in Run II 36 bunches (396 ns crossing time) 2 CDF in Run II

More information

Measurement of multi-jet cross sections in proton proton collisions at a 7 TeV center-of-mass energy

Measurement of multi-jet cross sections in proton proton collisions at a 7 TeV center-of-mass energy Eur. Phys. J. C (2011) 71:1763 DOI 10.1140/epjc/s10052-011-1763-6 Regular Article - Experimental Physics Measurement of multi-jet cross sections in proton proton collisions at a 7 TeV center-of-mass energy

More information

Hard And Soft QCD Physics In ATLAS

Hard And Soft QCD Physics In ATLAS Hard And Soft QCD Physics In ALAS Stefanie Adomeit on behalf of the ALAS collaboration International Conference on New Frontiers in Physics - Crete, June -6, QCD Measurements in ALAS at LHC every kind

More information

Recent CMS results in the forward region with the CASTOR detector. Sebastian Baur for the CMS Collaboration

Recent CMS results in the forward region with the CASTOR detector. Sebastian Baur for the CMS Collaboration Recent CMS results in the forward region with the CASTOR detector Sebastian Baur for the CMS Collaboration The Forward Instrumentation of CMS 2 Overview CMS has an excellent calorimetric instrumentation

More information

Particle spectra in Minimum Bias events at 13TeV

Particle spectra in Minimum Bias events at 13TeV Particle spectra in Minimum Bias events at TeV Juan Manuel Grados Luyando on behalf of the CMS collaboration Deutsches Elektronen-Synchrotron, Hamburg MPI@LHC 05 Trieste, Italy Motivation Probe the different

More information

First Run-2 results from ALICE

First Run-2 results from ALICE First Run-2 results from ALICE Goethe University Frankfurt & GSI on behalf of the ALICE Collaboration XLV International Symposium on Multiparticle Dynamics Wildbad Kreuth, 4-9 Oct 2015 1 Outline Introduction

More information

Measurement of the associated production of direct photons and jets with the Atlas experiment at LHC. Michele Cascella

Measurement of the associated production of direct photons and jets with the Atlas experiment at LHC. Michele Cascella Measurement of the associated production of direct photons and jets with the Atlas experiment at LHC Michele Cascella Graduate Course in Physics University of Pisa The School of Graduate Studies in Basic

More information

Study of observables for measurement of MPI using Z+jets process

Study of observables for measurement of MPI using Z+jets process Study of observables for measurement of MPI using Z+jets process PANJAB University, IN Email: ramandeep.kumar@cern.ch AKAL University, IN 7th International Workshop on Multiple Parton Interactions at the

More information

PoS(IHEP-LHC-2011)008

PoS(IHEP-LHC-2011)008 in pp collisions at the LHC Sergei Lobanov Joint Institute for Nuclear Research, Dubna, Russian Federation E-mail: Sergey.Lobanov@cern.ch Artem Maevskiy M.V. Lomonosov Moscow State University, Russian

More information

QCD Studies with CMS at LHC. Gunther Roland for the Collaboration

QCD Studies with CMS at LHC. Gunther Roland for the Collaboration QCD Studies with CMS at LHC Gunther Roland for the Collaboration INT Seattle 5/24/2010 First 7 TeV Collisions: March 30th 2010 2 QCD Studies with CMS pp integrated luminosity ~ 10nb -1 n.b. rates for LHC

More information

Diffractive Dijets and Gap Survival Probability at HERA

Diffractive Dijets and Gap Survival Probability at HERA Diffractive Dijets and Gap Survival Probability at HERA Sebastian Schätzel (CERN) CERN EP Seminar 21 April 2008 HERA Electron-Proton Collider May 1992-June 2007, DESY Hamburg 27.5 GeV electrons on 820

More information

Charmonium production versus multiplicity in PYTHIA8

Charmonium production versus multiplicity in PYTHIA8 Hard-Soft correlations in hadronic collisions Steffen Weber Charmonium production versus multiplicity in PYTHIA8 Hard-Soft correlations in hadronic collisions Clermont-Ferrand July 23, 2018 Steffen Weber

More information

Jet Physics at ALICE. Oliver Busch. University of Tsukuba Heidelberg University

Jet Physics at ALICE. Oliver Busch. University of Tsukuba Heidelberg University Jet Physics at ALICE Oliver Busch University of Tsukuba Heidelberg University 1 2 Outline Introduction Results from pp collisions Identified jet fragmentation in pp Jets in heavy-ion collisions Jet shapes

More information

Measurement of Quenched Energy Flow for Dijets in PbPb collisions with CMS

Measurement of Quenched Energy Flow for Dijets in PbPb collisions with CMS Measurement of Quenched Energy Flow for Dijets in PbPb collisions with CMS For the CMS Collaboration NPA Seminar Yale, USA 15 October, 2015 Relativistic Heavy Ion Collisions Trying to answer two important

More information

The ATLAS Detector at the LHC

The ATLAS Detector at the LHC The ATLAS Detector at the LHC Results from the New Energy Frontier Cristina Oropeza Barrera Experimental Particle Physics University of Glasgow Somewhere near the Swiss Alps... A Toroidal LHC ApparatuS

More information

QCD at hadron colliders

QCD at hadron colliders QCD at hadron colliders Soushi Tsuno Okayama University Outline Introduction: Focus on current (Tevatron) and future (LHC) hadron colliders High pt pqcd phenomena & issues: PDF measurement Jet Physics

More information

Diffraction Physics at LHCb

Diffraction Physics at LHCb Diffraction Physics at LHCb Michael Schmelling LHCb / MPI for Nuclear Physics The LHCb Experiment Energy Flow Central Exclusive Production New Developments Summary Diffraction Physis at LHCb M. Schmelling,

More information

Measurement of inclusive charged jet production in pp and Pb-Pb

Measurement of inclusive charged jet production in pp and Pb-Pb Measurement of inclusive charged jet production in pp and Pb-Pb collisions at S NN 5. 02TeV with ALICE Run2 Data Yan Li for the ALICE collaboration Central China Normal University CLHCP 2016 18/12/2016

More information

arxiv: v1 [hep-ex] 9 Jan 2019

arxiv: v1 [hep-ex] 9 Jan 2019 Quarkonium production as a function of charged-particle multiplicity in pp and p Pb collisions measured by ALICE at the LHC arxiv:1901.02627v1 [hep-ex] 9 Jan 2019 Discipline of Physics, School of Basic

More information

Microscopic collectivity: The ridge and strangeness enhancement from string string interactions in Pythia8

Microscopic collectivity: The ridge and strangeness enhancement from string string interactions in Pythia8 Microscopic collectivity: The ridge and strangeness enhancement from string string interactions in Pythia8 Christian Bierlich bierlich@thep.lu.se Lund University / University of Copenhagen May 15, 2018

More information

Introduction to WG5: high multiplicities and interactions with nuclei

Introduction to WG5: high multiplicities and interactions with nuclei 8 th International Workshop on Multiple Partonic Interactions at the LHC San Cristóbal de las Casas, Chiapas. November 28, 2016 Introduction to WG5: high multiplicities and interactions with nuclei Antonio

More information

Event shapes in hadronic collisions

Event shapes in hadronic collisions Event shapes in hadronic collisions Andrea Banfi ETH Zürich SM@LHC - Durham - April Event shapes at hadron colliders Event shapes are combinations of hadron momenta in a number related to the geometry

More information

Double Parton Scattering measurements at LHC

Double Parton Scattering measurements at LHC Double Parton Scattering measurements at LHC Diego Ciangottini INFN/CERN Università degli Studi di Perugia 1 Where can we measure double parton scattering? Thanks to P. Bartalini Credits:)) -)Ellie)Dobson)

More information

Uncertainties in NLO+PS matched calculations of inclusive jet and dijet production

Uncertainties in NLO+PS matched calculations of inclusive jet and dijet production Uncertainties in NLO+PS matched calculations of inclusive jet and dijet production Institute for Particle Physics Phenomenology 26/09/202 arxiv:.220, arxiv:208.285 Uncertainties in NLO+PS matched calculations

More information

QCD, diffrac,on and forward physics at the LHC

QCD, diffrac,on and forward physics at the LHC QCD, diffrac,on and forward physics at the LHC Andrew Pilkington IPPP Durham and Manchester Presented at Diffrac.on 2010, Otranto, Italy, September 2010 Overview 1) Introduc,on to LHC in 2010 2) Review

More information

Jet Energy Calibration. Beate Heinemann University of Liverpool

Jet Energy Calibration. Beate Heinemann University of Liverpool Jet Energy Calibration Beate Heinemann University of Liverpool Fermilab, August 14th 2006 1 Outline Introduction CDF and D0 calorimeters Response corrections Multiple interactions η-dependent corrections

More information

Toward an Understanding of Hadron-Hadron. Collisions From Feynman-Field to the LHC

Toward an Understanding of Hadron-Hadron. Collisions From Feynman-Field to the LHC Rick Field University of Florida Outline of Talk Ricky & Sally. Toward an Understanding of Hadron-Hadron Collisions From Feynman-Field to the LHC The Berkeley Years Rick & Jimmie. The early days of Feynman-Field

More information

Hadron Collider Physics, HCP2004, June 14-18

Hadron Collider Physics, HCP2004, June 14-18 ) " % "" ' & % % " ) " % '% &* ' ) * ' + " ' ) ( $#! ' "") ( * " ) +% % )( (. ' + -, '+ % &* ' ) ( 021 % # / ( * *' 5 4* 3 %( '' ' " + +% Hadron Collider Physics, HCP2004, June 14-18 The Run II DØ Detector

More information

Charged particle multiplicity in proton-proton collisions with ALICE

Charged particle multiplicity in proton-proton collisions with ALICE Charged particle multiplicity in proton-proton collisions with ALICE Introduction on the motivations for a pp physics programme with ALICE A short review on the detectors used to reconstruct charged particle

More information

Testing QCD at the LHC and the Implications of HERA DIS 2004

Testing QCD at the LHC and the Implications of HERA DIS 2004 Testing QCD at the LHC and the Implications of HERA DIS 2004 Jon Butterworth Impact of the LHC on QCD Impact of QCD (and HERA data) at the LHC Impact of the LHC on QCD The LHC will have something to say

More information

October 4, :33 ws-rv9x6 Book Title main page 1. Chapter 1. Measurement of Minimum Bias Observables with ATLAS

October 4, :33 ws-rv9x6 Book Title main page 1. Chapter 1. Measurement of Minimum Bias Observables with ATLAS October 4, 2018 3:33 ws-rv9x6 Book Title main page 1 Chapter 1 Measurement of Minimum Bias Observables with ATLAS arxiv:1706.06151v2 [hep-ex] 23 Jun 2017 Jiri Kvita Joint Laboratory for Optics, Palacky

More information

Kristjan Gulbrandsen NBI ALICE/Discovery group

Kristjan Gulbrandsen NBI ALICE/Discovery group Kristjan Gulbrandsen NBI ALICE/Discovery group The Large Hadron Collider Protons (since late 2009) and lead ions accelerated Delivered to 4 experiments ALICE is interested (mainly) in lead collisions Proton

More information

Proton-lead measurements using the ATLAS detector

Proton-lead measurements using the ATLAS detector Proton-lead measurements using the ATLAS detector Martin Spousta for the ATLAS Collaboration Charles University in Prague DOI: http://dx.doi.org/10.3204/desy-proc-2014-04/275 Measurements of soft and hard

More information

Diffraction at the LHC

Diffraction at the LHC Diffraction at the LHC at the boundary of experiment and theory Mikael Mieskolainen, Risto Orava Helsinki Institute of Physics (HIP), University of Helsinki Diffractive and Electromagnetic processes -

More information

Don Lincoln. QCD Results from the Tevatron

Don Lincoln. QCD Results from the Tevatron Recent Don Lincoln Fermilab DØ Calorimeter Uranium-Liquid Argon Calorimeter stable, uniform response, radiation hard Compensating: e/π 1 Uniform hermetic coverage η 4.2, recall η ln[tan(θ/2)] Longitudinal

More information

Transverse momentum and pseudorapidity distributions with minimum bias events in CMS at the LHC

Transverse momentum and pseudorapidity distributions with minimum bias events in CMS at the LHC Transverse momentum and pseudorapidity distributions with minimum bias events in CMS at the LHC Christof Roland/ MIT For the CMS Collaboration Rencontres de Moriond QCD Session 14 th March, 2010 Moriond

More information

PoS(LeptonPhoton2015)020

PoS(LeptonPhoton2015)020 Soft QCD Measurements at LHC Status and Outlook CERN E-mail: jgrosseo@cern.ch he first run of the LHC (009 0) has resulted in a tremendous legacy of soft physics results measured by ALICE, ALAS, CMS, LHCb,

More information

ULTRA-HIGH ENERGY COSMIC RAY COMPOSITION and MUON CONTENT vs. HADRONIC MODELS. Esteban Roulet Bariloche, Argentina

ULTRA-HIGH ENERGY COSMIC RAY COMPOSITION and MUON CONTENT vs. HADRONIC MODELS. Esteban Roulet Bariloche, Argentina ULTRA-HIGH ENERGY COSMIC RAY COMPOSITION and MUON CONTENT vs. HADRONIC MODELS Esteban Roulet Bariloche, Argentina Many observables are sensitive to CR composition Shower maximum TA APP 64 (2014) Auger

More information

Jet Physics at the LHC

Jet Physics at the LHC Jet Physics at the LHC Oliver Busch University of Tsukuba Heidelberg University 1 pp jet cross sections and fragmentation pp identified jet fragmentation Nuclear modification factor Event plane dependence

More information

Cosmic Ray Interaction Models: Overview

Cosmic Ray Interaction Models: Overview Cosmic Ray Interaction Models: Overview Sergey Ostapchenko Frankfurt Institute for Advanced Studies [] ISMD-2015 Wildbad Kreuth, October 4-9, 2015 Cosmic ray studies with extensive air shower techniques

More information

MBR Monte Carlo Simulation in PYTHIA8

MBR Monte Carlo Simulation in PYTHIA8 The Rockefeller University, 10 York Avenue, New York, NY 06, USA E-mail: robert.ciesielski@rockefeller.edu Konstantin Goulianos The Rockefeller University, 10 York Avenue, New York, NY 06, USA E-mail:

More information

Thermodynamical String Fragmentation

Thermodynamical String Fragmentation Thermodynamical String Fragmentation with Torbjörn Sjöstrand arxiv:60.0988 Nadine Fischer - November 24th, 206 MONASH UNIVERSITY & LUND UNIVERSITY Motivation p? distributions (ratio plots).4.2.4.2.4.2.4.2

More information

Multiplicity dependence of charged pion, kaon, and (anti)proton production at large transverse momentum in p-pb collisions at 5.

Multiplicity dependence of charged pion, kaon, and (anti)proton production at large transverse momentum in p-pb collisions at 5. [1] Multiplicity dependence of charged pion, kaon, and (anti)proton production at large transverse momentum in p-pb collisions at 5.02 ATeV Gyula Bencedi (Wigner RCP, Hungary) on behalf of the ALICE Collaboration

More information

Combination of top quark physics results at the LHC

Combination of top quark physics results at the LHC Combination of top quark physics results at the LHC María Aldaya (DESY) for the CMS & ATLAS Collaborations within the TOPLHCWG ICHEP 2014, Valencia, 2-9 July 2014 What is the TOPLHCWG? http://lpcc.web.cern.ch/lpcc/

More information