Thermodynamical String Fragmentation
|
|
- Sibyl Blair
- 5 years ago
- Views:
Transcription
1 Thermodynamical String Fragmentation with Torbjörn Sjöstrand arxiv: Nadine Fischer - November 24th, 206 MONASH UNIVERSITY & LUND UNIVERSITY
2 Motivation p? distributions (ratio plots) Charged hadron p? at 7 TeV, h < 2.4, CMS Pythia p ± p? at 7 TeV, y < 0.5, ALICE p, p p? at 7 TeV, y < 0.5, ALICE K ± p? at 7 TeV, y < 0.5, ALICE p? [GeV/c] /9
3 Motivation p? distributions (ratio plots) Enhanced strangeness with increasing n ch Charged hadron p? at 7 TeV, h < 2.4, CMS Pythia p ± p? at 7 TeV, y < 0.5, ALICE Ratio of yields to (π +π + ) 0 0 2KS Λ+Λ ( 2) + Ξ +Ξ ( 6) p, p p? at 7 TeV, y < 0.5, ALICE K ± p? at 7 TeV, y < 0.5, ALICE p? [GeV/c] Ω +Ω ( 6) ALICE pp, s = 7 TeV p-pb, s NN = 5.02 TeV Pb-Pb, s NN = 2.76 TeV PYTHIA8 DIPSY EPOS LHC 0 0 dn /dη ch 3 η < 0.5 /9
4 Lund String Fragmentation Flavour and transverse momentum of hadrons: string streched between q q _ q q 3 _ q q _ q q _ qq q q moves apart! energy stored in string ( potential V (r) =appler ) 3 2 creation of q i q i pairs breaks string: m? qi =0 m? qi > 0 on-shell production in single vertex tunneling probability exp m 2? q i /apple =exp m 2 q i /apple exp # # q _ q p 2? q i /apple flavour selection of q i q i hp 2? q i i = apple/ = 2 t x lots of flavour parameters: suppression of strangeness and diquarks, and 0 O(20) free parameters in total rates for different meson multiplets 2/9
5 Thermodynamical String Model Idea: hadron-level suppression exp ( m? had /T ) with m? had = q m 2 had + p2? had generate p? had according to f had (p? had ) d p? had =exp( p? had /T ) d p? had fourier transformation to obtain quark-level distribution Z bj 0 (bp? q /T ) f q(p? q ) / 0 ( + b 2 ) 3/4 d b apple fit: N exp( cp? q/t ) (p? q /T ) d pick hadron flavour according to P had =exp( m? had /T ) + multiplicative factors for spin-counting, SU(6) symmetry factors,.. heavier hadrons obtain more p? 3 free parameters in total 3/9
6 Close-Packing of Strings Idea: more MPIs ) closer packing of strings transverse region shrinks ) larger string tension guess momentum of next hadron, based on average quantities n string = number of strings that cross hadron rapidity effective number of strings n eff string =+ n string +p 2? had /p2? 0 r modify Gaussian width! nstring eff (similar for temperature) 4/9
7 Close-Packing of Strings Idea: more MPIs ) closer packing of strings transverse region shrinks ) larger string tension guess momentum of next hadron, based on average quantities n string = number of strings that cross hadron rapidity effective number of strings n eff string =+ n string +p 2? had /p2? 0 r modify Gaussian width! nstring eff (similar for temperature) hp? i vs. n ch in toy model (2 8 strings, Â E = TeV) hp? i [GeV/c] default (n eff string )0.25 s n ch 4/9
8 Hadron Rescattering Idea: dense hadronic gas ) hadrons might rescatter on the way out Find hadron pairs that can scatter: cut on the invariant mass of the hadron pair m inv < q q m 2 + ~p max 2 + m ~p max 2 rescattering probability: overall probability probability for same-string P max ds P ds P max ss P ss P min ss max min ij max ij ij in CoM frame rotate around angles chosen flat in d 5/9
9 Hadron Rescattering Idea: dense hadronic gas ) hadrons might rescatter on the way out Find hadron pairs that can scatter: cut on the invariant mass of the hadron pair m inv < q q m 2 + ~p max 2 + m ~p max 2 rescattering probability: overall probability probability for same-string P max ds P ds P max ss P ss P min ss max min ij max ij ij in CoM frame rotate around angles chosen flat in d hp?i [GeV/c] hp?i for different hadrons in toy model (5 strings with E = mz) Gaussian p? wo hadron scattering Gaussian p? whadronscattering p K h, h 0 r, w K f p,n L, S X D S X W 5/9
10 Results Transverse momentum distributions: inclusive and pions (/2pp?) d 2 nch dh dp? 0 Charged hadron p? at 7 TeV, h < CMS data default Gaussian p? Thermal p? /N inel d 2 N dy dp? 0 0 p ± transverse momentum at 7 TeV, y < 0.5 ALICE data default Gaussian p? Thermal p? p? [GeV/c] p? [GeV/c] 6/9
11 Results Transverse momentum distributions: protons and kaons /N inel d 2 N dy dp? p, p transverse momentum at 7 TeV, y < 0.5 ALICE data default Gaussian p? Thermal p? /N inel d 2 N dy dp? K ± transverse momentum at 7 TeV, y < 0.5 ALICE data default Gaussian p? Thermal p? p? [GeV/c] p? [GeV/c] 7/9
12 Results Enhanced strangeness with increasing n ch Ratio of yields to (p + + p ) at 7 TeV, h < 0.5 Ratio of yields 0 2K 0 S 2 (L + L) Ratio of yields to (π +π + ) 0 0 2KS Λ+Λ ( 2) + Ξ +Ξ ( 6) 6 (X + X + ) Ω +Ω ( 6) 0 3 default Gaussian p? Thermal p? 6 (W + W + ) ALICE pp, s = 7 TeV p-pb, s NN = 5.02 TeV Pb-Pb, s NN = 2.76 TeV PYTHIA8 DIPSY EPOS LHC dn /dη ch 3 η < n ch 8/9
13 Summary and Outlook What is new? option for generating p? had according to exp( p? had /T ) with flavour selection according to exp( m? had /T ) effect of close-packing of strings simple model for hadron rescattering What does it do? improves some observables, such as p? spectra, hp? i(m had ) does not improve everything, e.g. kaon p? remains difficult hadron decays are a limiting factor 9/9
14 Summary and Outlook What is new? option for generating p? had according to exp( p? had /T ) with flavour selection according to exp( m? had /T ) effect of close-packing of strings simple model for hadron rescattering What does it do? improves some observables, such as p? spectra, hp? i(m had ) does not improve everything, e.g. kaon p? remains difficult hadron decays are a limiting factor Further work required! microscopic tracing of the full space-time evolution (partons and hadrons, production and decay vertices) more detailed understanding and modelling 9/9
15 Backup 0/9
16 Flavour Asymmetry in Thermodynamical Model Toy model with d and s quarks only (d! s) competes with (d! d)! d s obtains larger p? (s! d) competes with (s! s)! s d obtains smaller p? /N dn/dp? (s! d) / (d! s) Same T for (d! s) and (s! d) transitions (d! s) with hp? i = 0.46 (s! d) with hp? i = p? [GeV/c] /N dn/dp? (s! d) / (d! s) Different T for (d! s) and (s! d) transitions (d! s) with hp? i = 0.46 (s! d) with hp? i = p? [GeV/c] /9
17 Rapidity Distributions nstring Rapidity distribution of the strings in an event 0 8 nstring Rapidity distribution of the strings in an event y y 2/9
18 Limiting factor: Decays pion transverse LHC, with and without decays, similar for protons /N dn/dp? p ± transverse momentum at LHC Gaussian p? wo decays Gaussian p? wdecays Termal p? wo decays Termal p? wdecays p? [GeV/c] ratio ratio ratio ratio.4 w/wo (Gaussian).2.4 w/wo (Thermal).2.4 Thermal/Gaussian (wo).2.4 Thermal/Gaussian (w) p? [GeV/c] ) decays wash out effects present after fragmentation 3/9
19 Hadron Rescattering hp? i in toy model ( 5 strings with E = m Z on the z axis) hp?i [GeV/c] w/wo hp?i for different hadron species Gaussian p? wo hadron scattering Gaussian p? whadronscattering p K h, h 0 r, w K f p,n L, S X D S X W hp?i [GeV/c] w/wo hp?i for different hadron species Termal p? wo hadron scattering Termal p? whadronscattering p K h, h 0 r, w K f p,n L, S X D S X W 4/9
20 Results Average transverse momentum: as a function of n ch and m had hp?i [GeV/c] Ch. hp?i vs. n ch at 7 TeV, p? track > 00 MeV, n ch 2, h < ATLAS data default Gaussian p? Thermal p? hp?i [GeV/c] Mean transverse momentum vs. mass at 7 TeV, y < 0.5 p + ALICE data default Gaussian p? Thermal p? K + K 0 p f X S ± X 0 W n ch m [GeV/c 2 ] 5/9
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 informationMicroscopic 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 informationMonte 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 information1 The pion bump in the gamma reay flux
1 The pion bump in the gamma reay flux Calculation of the gamma ray spectrum generated by an hadronic mechanism (that is by π decay). A pion of energy E π generated a flat spectrum between kinematical
More informationPoS(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 informationarxiv: v1 [hep-ph] 19 Dec 2018
Effect of Rope Hadronisation on Strangeness Enhancement in p p collisions at LHC energies. Ranjit Nayak,, Subhadip Pal,, and Sadhana Dash, Indian Institute of Technology Bombay, Mumbai, India476 Indian
More informationHeavy ion physics with the PytHIa generator
Heavy ion physics with the PytHIa generator Christian Bierlich bierlich@thep.lu.se With L. Lönnblad and G. Gustafson Lund University Aug 21, 2017 Novel tools and observables for jet physics in heavy-ion
More informationarxiv: v1 [hep-ex] 18 May 2015
ALICE summary of light flavour results at intermediate and high p arxiv:55.477v [hep-ex] 8 May 5 uva Richert, on behalf of the ALICE collaboration Lund University, Department of Physics, Div. of Particle
More informationMPI 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 informationQCD 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 informationPoS(DIS2017)208. Nuclear PDF studies with proton-lead measurements with the ALICE detector
Nuclear PDF studies with proton-lead measurements with the ALICE detector a,b for the ALICE Collaboration a Institute for Subatomic Physics, Department for Physics and Astronomy and EMMEφ, Faculty of Science,
More informationAlbi Kerbizi University of Trieste, Trieste INFN Section
14th September 2017 DSpin17, Dubna A Monte Carlo code for the fragmentation of polarized quarks Albi Kerbizi PhD @ University of Trieste, Trieste INFN Section X. Artru, Z. Belghobsi, F. Bradamante, A.
More informationMeasurement of Electrons from Beauty-Hadron Decays in p-pb Collision at snn = 5.02 TeV with ALICE at the LHC
Measurement of Electrons from Beauty-Hadron Decays in p-pb Collision at snn = 5.02 ev with ALICE at the LHC Minjung Kim, Inha University Advised by: Prof. MinJung Kweon, Prof. Jin-Hee Yoon Dec 5 th 2014,
More informationParticle 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 informationResults with Hard Probes High p T Particle & Jet Suppression from RHIC to LHC
Results with Hard Probes High p T Particle & Jet Suppression from RHIC to LHC PHENIX! AGS! RHIC! STAR! Cover 3 decades of energy in center-of-mass s NN = 2.76 TeV 5.5 TeV (2015) CMS LHC! s NN = 5-200 GeV
More informationarxiv: v3 [hep-ph] 2 Mar 2018
KA-TP-32-207 UWTHPH-207-34 HERWIG-207-03 MCNET-7-25 Baryon production from cluster hadronization Stefan Gieseke, Patrick Kirchgaeßer, Simon Plätzer 2 Institute for Theoretical Physics, Karlsruhe Institute
More informationJet 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 informationLHC Heavy Ion Physics Lecture 5: Jets, W, Z, photons
LHC Heavy Ion Physics Lecture 5: Jets, W, Z, photons HUGS 2015 Bolek Wyslouch Techniques to study the plasma Radiation of hadrons Azimuthal asymmetry and radial expansion Energy loss by quarks, gluons
More informationCharged Particle Production in Proton-Proton Collisions at s = 13 TeV with ALICE at the LHC
Charged Particle Production in Proton-Proton Collisions at s = 13 TeV with ALICE at the LHC Prabhakar Palni Institute of Particle Physics, Central China Normal University, Wuhan MPI@LHC 2015, ICTP, Trieste,
More informationProton-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 informationMultiple 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 informationOrigin of QGP-like effects in small systems how to make experimental progress (with some excursions) Peter Christiansen (Lund University)
1 QCD challenges in pp, pa and AA collisions at high energies Trento, February 27 - March 3, 2017 Origin of QGP-like effects in small systems how to make experimental progress (with some excursions) Peter
More informationJet 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 informationCorrelations, multiplicity distributions, and the ridge in pp and p-pb collisions
EPJ Web of Conferences, 6 (7) DOI:.5/ epjconf/76 ISMD 6 Correlations, multiplicity distributions, and the ridge in pp and p-pb collisions Alice Ohlson,a for the Collaboration Ruprecht-Karls-Universität
More informationThe Quark-Gluon Plasma and the ALICE Experiment
The Quark-Gluon Plasma and the ALICE Experiment David Evans The University of Birmingham IoP Nuclear Physics Conference 7 th April 2009 David Evans IoP Nuclear Physics Conference 2009 1 Outline of Talk
More informationNeutral meson and direct photon measurement in pp and Pb Pb collisions at midrapidity with the ALICE experiment at the LHC
Neutral meson and direct photon measurement in pp and Pb Pb collisions at midrapidity with the ALICE experiment at the LHC Lucia Leardini Physikalisches Institut Heidelberg on behalf of the ALICE Collaboration
More informationLight flavour hadron production in the ALICE experiment at LHC
Light flavour hadron production in the ALICE experiment at LHC Angela Badalà INFN Sezione di Catania for the ALICE Collaboration ALICE heavy-ion runs Dataset s NN (TeV) Integrated luminosity 2010 Pb-Pb
More informationNew results related to QGP-like effects in small systems with ALICE
New results related to QGP-like effects in small systems with ALICE for the ALICE collaboration Lund University E-mail: vytautas.vislavicius@cern. Results on the production of π ±, K ±, p( p), Λ( Λ), Ξ
More informationRecent highlights in the light-flavour sector from ALICE
Recent highlights in the light-flavour sector from ALICE Enrico Fragiacomo INFN - Trieste MIAMI 2016 Lago Mar Resort, Fort Lauderdale, Florida 14-19 December 2016 Ultra-Relativistic Heavy-Ion collisions
More information+ High p T with ATLAS and CMS in Heavy-Ion 2.76TeV
+ High p T with ATLAS and CMS in Heavy-Ion Collisions @ 2.76TeV Lamia Benhabib On behalf of ATLAS and CMS HCP 2011, Paris lamia.benhabib@llr.in2p3.fr +Outlook Introduction : hard probes Strongly interacting
More informationCharmonium 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 informationPredictions for hadronic observables from. from a simple kinematic model
Predictions for hadronic observables from Pb + Pb collisions at sqrt(s NN ) = 2.76 TeV from a simple kinematic model Tom Humanic Ohio State University WPCF-Kiev September 14, 2010 Outline Motivation &
More informationReview of collective flow at RHIC and LHC
Review of collective flow at RHIC and LHC Jaap Onderwaater 29 November 2012 J. Onderwaater (EMMI,GSI) Collective flow 29 November 2012 1 / 37 Heavy ion collision stages Outline Heavy ion collisions and
More informationJet 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 informationarxiv:hep-ex/ v2 2 Feb 2001
CR-459 hep-ex/00009 RECENT RESULTS ON PARTICLE PRODUCTION FROM J. H. VOSSEBELD CERN, CH - 2 Geneva 23, Switzerland E-mail: Joost.Vossebeld@cern.ch arxiv:hep-ex/00009v2 2 Feb 200 Three recent studies are
More informationProspective of gamma hadron correlation. study in CMS experiment
Prospective of gamma hadron correlation. study in CMS experiment Yeonju Go (Korea University) for the CMS collaboration 5-6 Dec. 2014 HIM meeting Contents Physics Motivation Direct gamma-hadron correlation
More informationSmall systems Resonances hadronic phase partonic phase?
Christina Markert University of Texas at Austin Small systems Resonances hadronic phase partonic phase? NeD-216, Phuket, Thailand, 31 Oct - 5 Nov 216 1 Phase diagram of nuclear matter (QCD) NeD-216, Phuket,
More informationRope hadronization in the DIPSY event generator
Rope hadronization in the DIPSY event generator arxiv:1412.6259 [hep-ph] and arxiv:1507.02091 [hep-ph] Christian Bierlich Jesper Christiansen, Gösta Gustafson, Leif Lönnblad, Andrey Tarasov Lund University
More informationHeavy Ions at the LHC: First Results
Heavy Ions at the LHC: First Results Thomas Schaefer North Carolina State University Heavy ion collision: Geometry R Au /γ y R Au x b z rapidity : y = 1 2 log ( E + pz E p z ) transverse momentum : p 2
More informationStudying collective phenomena in pp and A-A collisions with the ALICE experiment at the LHC
Studying collective phenomena in pp and A-A collisions with the ALICE experiment at the LHC Ivan Ravasenga Politecnico di Torino and I.N.F.N. 56 th course, Erice (Sicily, Italy) 14-23.06.2018 Ivan Ravasenga
More informationMonte Carlo Non-Linear Flow modes studies with AMPT
Monte Carlo Non-Linear Flow modes studies with AMP Daniel Noel Supervised by: Naghmeh Mohammadi 2 July - 31 August 218 1 Introduction Heavy-ion collisions at the Large Hadron Collider (LHC) generate such
More informationMini-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 informationQ a u r a k k m a m t a t t e t r e p r p ob o e b d e d b y b y di d l i e l p e t p o t n o s
Quark matter probed by dileptons Olena Linnyk July 02, 2010 Information from photons and dileptons 14 12 10 ε/t 4 8 6 4 2 Lattice QCD: µ B =0 µ B =530 MeV 0 0.5 1.0 1.5 2.0 2.5 3.0 T/T c But what are the
More informationarxiv:nucl-th/ v2 8 Jun 2006
Acta Phys. Hung. A / (2005) 000 000 HEAVY ION PHYSICS Strange quark collectivity of φ meson at RHIC arxiv:nucl-th/0510095v2 8 Jun 2006 J. H. Chen 1,2, Y. G. Ma 1,a, G. L. Ma 1,2, H. Z. Huang 1,3, X. Z.
More informationPhenomenology of Heavy-Ion Collisions
Phenomenology of Heavy-Ion Collisions Hendrik van Hees Goethe University Frankfurt and FIAS October 2, 2013 Hendrik van Hees (GU Frankfurt/FIAS) HIC Phenomenology October 2, 2013 1 / 20 Outline 1 Plan
More informationPhoton and neutral meson production in pp and PbPb collisions at ALICE
Photon and neutral meson production in pp and PbPb collisions at ALICE Dieter Roehrich University of Bergen, Norway for the ALICE Collaboration Nuclear collisions at the LHC Photons as a probe for the
More informationarxiv: 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 informationarxiv: v1 [nucl-ex] 7 Jan 2019
Open Heavy Flavour: Experimental summary arxiv:9.95v [nucl-ex] 7 Jan 9 Deepa homas he University of exas at Austin E-mail: deepa.thomas@cern.ch In this paper I will review a few of the latest experimental
More informationarxiv: v2 [hep-ph] 9 Feb 2012
Strange quark suppression and strange hadron production in pp collisions at RHIC and LHC Hai-Yan Long and Sheng-Qin Feng Dept. of Physics, College of Science, China hree Gorges Univ., Yichang 443002, China
More informationHeavy-Quark Transport in the QGP
Heavy-Quark Transport in the QGP Hendrik van Hees Goethe-Universität Frankfurt November 9, 211 Hendrik van Hees (GU Frankfurt) Heavy-Quark Transport November 9, 211 1 / 19 Motivation Fast equilibration
More informationUltra-Relativistic Heavy Ion Collision Results
Ultra-Relativistic Heavy Ion Collision Results I. Overview of Effects Observed in Large Nucleus-Nucleus Collision Systems (Au+Au, Pb+Pb) High p T Hadrons Are Suppressed at LHC & RHIC Central Pb-Pb and
More informationStrangeness production and nuclear modification at LHC energies
Strangeness production and nuclear modification at LHC energies Oliver Busch for the ALICE collaboration 1 Outline introduction jet azimuthal anisotropy jet shapes 2 Introduction 3 Jets: seeing quarks
More informationJet Results in pp and Pb-Pb Collisions at ALICE
Jet Results in pp and Pb-Pb Collisions at ALICE Oliver Busch for the ALICE Collaboration Motivation Jet reconstruction in ALICE Jets in pp Jets in Pb-Pb Hadron triggered recoil jets Motivation Jets originate
More informationFirst 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 informationIn-Medium Energy Loss and Correlations in Pb-Pb Collisions at 2.76 TeV with ALICE
In-Medium Energy Loss and Correlations in Pb-Pb Collisions at 2.76 TeV with ALICE Jan Fiete Grosse-Oetringhaus CERN/PH for the ALICE Collaboration Heavy Ions: Experiments Confront Theory Copenhagen, 8th
More informationJet and bulk observables within a partonic transport approach
Jet and bulk observables within a partonic transport approach Florian Senzel with J. Uphoff, O. Fochler, C. Wesp, Z. Xu and C. Greiner based on Phys.Rev.Lett. 4 (25) 23 Transport meeting, 29.4.25 Outline
More informationEquation of state. Pasi Huovinen Uniwersytet Wroc lawski. Collective Flows and Hydrodynamics in High Energy Nuclear Collisions
Equation of state Pasi Huovinen Uniwersytet Wroc lawski Collective Flows and Hydrodynamics in High Energy Nuclear Collisions Dec 14, 2016, University of Science and Technology of China, Hefei, China The
More informationMeasurement of W-boson production in p-pb collisions at the LHC with ALICE
Measurement of W-boson production in p-pb collisions at the LHC with ALICE for the ALICE Collaboration University of Cape Town Rondebosch, Cape Town, 7700, South Africa ithemba Laboratory of Accelerator
More informationarxiv: v1 [hep-ex] 14 Jan 2016
Nuclear Physics A Nuclear Physics A (28) 5 www.elsevier.com/locate/procedia arxiv:6.352v [hep-ex] 4 Jan 26 Measurements of heavy-flavour nuclear modification factor and elliptic flow in Pb Pb collisions
More informationDIS/Hadronization. Jarek Nowak
DIS/Hadronization Jarek Nowak Outline Deep Inelastic Scattering Cross section Parton Distribution Functions Hadronization Phenomenological approach (KNO scaling) Theoretical approach (Lund model) Resonance
More informationTevatron 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 informationHeavy Quarks in Heavy-Ion Collisions
Heavy Quarks in Heavy-Ion Collisions Hendrik van Hees with T. Lang, J. Steinheimer, M. Bleicher Goethe University Frankfurt and FIAS July 18, 213 Hendrik van Hees (GU Frankfurt/FIAS) Heavy Quarks in HICs
More informationBig Bang to Little Bang ---- Study of Quark-Gluon Plasma. Tapan Nayak July 5, 2013
Big Bang to Little Bang ---- Study of Quark-Gluon Plasma Tapan Nayak July 5, 2013 Universe was born through a massive explosion At that moment, all the matter was compressed into a space billions of times
More informationHQL Virginia Tech. Bob Hirosky for the D0 Collaboration. Bob Hirosky, UNIVERSITY of VIRGINIA. 26May, 2016
Bs CP-odd lifetime in Bs J/ψf0 and Afb for baryons at D0 2016 Virginia Tech Bob Hirosky for the D0 Collaboration 1 Tevatron Data D0 continues a rich physics program analyzing ~10fb-1 of recorded data from
More informationThe 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 informationLHC 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 informationDiffraction 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 informationExperimental summary: heavy-flavour production at the LHC
Experimental summary: heavy-flavour production at the LHC Gian Michele Innocenti Massachusetts Institute of Technology (MIT) 8th International Conference on Hard and Electromagnetic Probes of High-energy
More informationTransverse 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 informationMeasurement 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 informationBulk matter physics and its future at the Large Hadron Collider
Eur. Phys. J. C (2009) 62: 237 242 DOI 10.1140/epjc/s10052-009-0910-9 Regular Article - Experimental Physics Bulk matter physics and its future at the Large Hadron Collider B. Hippolyte a Institut Pluridisciplinaire
More informationReview 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 informationCollectivity in EPOS
9-11 May 2017 Niels Bohr Institute Klaus Werner Subatech Nantes 1 Collectivity in EPOS (flow, non-flow, and parton saturation) Klaus Werner in collaboration with T. Pierog, Y. Karpenko, B. Guiot, G. Sophys
More informationV 0 production studies at LHCb. Mathias Knecht, EPFL , joint SPS-ÖPG-ÖGA 2 meeting, Innsbrück, Österreich, September 2-4, 2009
V 0 production studies at LHCb Mathias Knecht, EPFL 2 9 2009, joint SPS-ÖPG-ÖGA 2 meeting, Innsbrück, Österreich, September 2-4, 2009 Outline One of the first measurements to be done with the LHCb detector...
More informationOutline: Open charm in heavy-ion collisions. A Heavy-Ion Seminar talk by Szymon Harabasz
Open charm in heavy-ion collisions A Heavy-Ion Seminar talk by Szymon Harabasz Outline: Charmed hadrons Why charm physics? How to do charm physics Open questions on open charm: D mesons R AA at low p T
More informationQuestions for the LHC resulting from RHIC Strangeness
Questions for the LHC resulting from RHIC Strangeness Outline Intermediate p T strangeness production not jets! (Credit for work goes to Betty Abelev & Jana Bielcikova) Helen Caines Yale University ALICE
More informationExploring the QGP with Jets at ALICE
Exploring the QGP with Jets at ALICE Oliver Busch University of sukuba Oliver Busch HI café, okyo 217/1 1 jets in pp collisions jets in heavy-ion collisions jet nuclear modification factor event plane
More informationHadronic resonance production with the ALICE experiment in pp and Pb-Pb collisions at LHC energies
Hadronic resonance production with the ALICE experiment in pp and Pb-Pb collisions at LHC energies ITEP Sergey Kiselev (ITEP Moscow) for the ALICE collaboration Motivation Analysis details pp@7 TeV: K*(892)
More informationRecent 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 informationPYQUEN event generator
PYQUEN event generator Igor Lokhtin PYQUEN team: I.Lokhtin, A.Snigirev (SINP MSU) HYDJET team: I.Lokhtin, A.Snigirev,(SINP MSU), K.Tywoniuk (Universidad de Santiago de Compostela) HYDJET++ team: I.Lokhtin,
More informationarxiv: v1 [nucl-th] 23 Jan 2019
arxiv:1901.08157v1 [nucl-th] 23 Jan 2019 Cyclotron Institute and Department of Physics and Astronomy, Texas A&M University, College Station TX 77843, USA E-mail: rjfries@comp.tamu.edu Michael Kordell Cyclotron
More informationEPOS 2 and LHC Results
EPOS 2 and LHC Results Tanguy Pierog, K. Werner, Y. Karpenko Institut für Kernphysik, Karlsruhe, Germany 46th Rencontres de Moriond, QCD, La Thuile, France March the 24th 2011 T. Pierog, KIT - 1/19 Outline
More informationQuantum properties of QCD string fragmentation
EPJ Web of Conferences will be set by the publisher DOI: will be set by the publisher c Owned by the authors, published by EDP Sciences, 216 Quantum properties of QCD string fragmentation Šárka Todorova-Nová
More informationGlobal polarization of Λ and Λ hyperons in Pb Pb collisions at s NN = 2.76 TeV
Global polarization of and hyperons in Pb Pb collisions at s NN = 2.76 TeV Maxim Konyushikhin Wayne State University On behalf of the ALICE collaboration March 29, 27 QCD Chirality Workshop 27 Outline
More informationUltra-Relativistic Heavy Ion Physics (FYSH551), May 31, 2013 Jan Rak and Thorsten Renk
Ultra-Relativistic Heavy Ion Physics (FYSH551), May 31, 2013 Jan Rak and Thorsten Renk Final Exam Instructions: Please write clearly. Do not just answer the questions, but document the thoughts leading
More informationRecent results from the NA61/SHINE experiment
Recent results from the NA6/SHINE experiment Emil Kaptur for the NA6/SHINE collaboration University of Silesia October 7, 5 of 5 Outline NA6/SHINE experiment Selected results from energy scan (,,, 8, 58
More informationCosmic 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 informationTransport studies of heavy ion collisions and antiproton-induced reactions on nuclei at FAIR energies
Transport studies of heavy ion collisions and antiproton-induced reactions on nuclei at FAIR energies A.B. Larionov Outline: 1) Motivation. 2) The GiBUU model: kinetic equations with relativistic mean
More informationQuarkonia and heavy-quark production in proton and nuclear collisions at the LHC
Quarkonia and heavy-quark production in proton and nuclear collisions at the LHC Michael Schmelling / MPI for Nuclear Physics Introduction Double Parton Scattering Cold Nuclear Matter Effects Quark Gluon
More informationMultiplicity dependence of identified particle production in pp collisions with ALICE
Multiplicity dependence of identified particle production in pp collisions with ALICE (for the ALICE Collaboration) NISER, INDIA Outline Introduction Results from pp collisions at s = 7 TeV and 3 TeV Collectivity
More informationMPI 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 informationTim Martin - University of Birmingham
Tim Martin - University of Birmingham 1 2 Overview Modeling Inelastic Diffraction Diffractive Events in ATLAS Large Rapidity Gaps Interpreting the Data 3 pp Cross Section Double Diff. Central Exclusive
More informationJET FRAGMENTATION DENNIS WEISER
JET FRAGMENTATION DENNIS WEISER OUTLINE Physics introduction Introduction to jet physics Jets in heavy-ion-collisions Jet reconstruction Paper discussion The CMS experiment Data selection and track/jet
More informationPerspectives for the measurement of beauty production via semileptonic decays in ALICE
Perspectives for the measurement of beauty production via semileptonic decays in ALICE Rosario Turrisi INFN Padova (Italy for the ALICE collaboration Contents Motivation: energy loss ALICE detector highlights
More informationGian Gopal Particle Attributes Quantum Numbers 1
Particle Attributes Quantum Numbers Intro Lecture Quantum numbers (Quantised Attributes subject to conservation laws and hence related to Symmetries) listed NOT explained. Now we cover Electric Charge
More informationHadron Mass Effects on Kaon Multiplicities: HERMES vs. COMPASS
Hadron Mass Effects on Kaon Multiplicities: HERMES vs. COMPASS Juan Guerrero Hampton University & Jefferson Lab QCD evolution 2017 May 26, 2017 Based on: J. G., J. Ethier, A. Accardi, S. Casper,W. Melnitchouk,
More informationInclusion of up-to-date parton distribution function and nuclear shadowing
Inclusion of up-to-date parton distribution function and nuclear shadowing in the AMP model Chao Zhang 1 ( 张潮 ) ZiWei Lin 1,, ShuSu Shi 1 and Liang Zheng 1 Central China Normal University 1 East Carolina
More informationStudy 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 informationOpen heavy-flavour production in pp, p Pb and Pb Pb collisions in ALICE
Open heavy-flavour production in pp, p Pb and Pb Pb collisions in ALICE (INFN, Bologna) on behalf of the ALICE Collaboration Bormio Winter Meeting 26/01/2018 Why open heavy flavour in ALICE? Heavy-flavour
More informationHOT HADRONIC MATTER. Hampton University and Jefferson Lab
200 Cr oss sect ion (m b) 0 K ptotal 20 5 K pelastic 2 1 K N 1 1.6 2 3 4 2 5 6 7 8 9 20 30 3 40 THE ROLE OF BARYON RESONANCES IN Relativistic Heavy Ion Collider (RHIC) HOT HADRONIC MATTER Au+Au K d 2.5
More information