Pseudorapidity and Correlation Measurements in High Energy Collisions
|
|
- Bathsheba Wilcox
- 5 years ago
- Views:
Transcription
1 Pseudorapidity and Correlation Measurements in High Energy Collisions Mark Parra-Shostrand August 9, 2013 Introduction My REU project consisted of studying two-particle correlations as a function of pseudorapidity due to jet production in high-energy proton-proton collisions. I had the pleasure working with my faculty mentor Dr. Sean Gavin and graduate student Chris Zin. This work was an extension of the work done by past REU students Mike Catanzaro and Daniel Taylor (see their reports on the REU website). Specifically, I have studied three observables R, D, and δp t1 δp t 2 (see correlation measurements). These three observables allow us to get a better understanding of pseudorapidity dependence. Also, it helps to explain the effects jets have on transverse momentum over a wide range of rapidities. In the beginning, I studied proton-proton collisions with simple analysis measurements of the charged multiplicity. I started to learn how to use the Monte Carlo event generator PYTHIA 8 (see Software). I then created a program through PYTHIA 8 that could generate our data and study the three observables as a function of pseudorapidity. Additionally, I had used a program called ROOT to analyze this data by making plots and histograms (see Software). When I generated my one million events through PYTHIA 8 it had a strict criteria. In order for the particles to be counted they had to be charged, in a pseudorapidity cut from -6 to 6, and a transverse momentum cut from.15 to 2 GeV. If all the criteria were met, then PYTHIA 8 counted the particle and stored it. Pseudorapidity When two particles collide and separate they create a flux tube between them. The two particles travel near the speed of light in opposite directions, stretching the flux tube until it fragments, creating particles. In the center of the flux tube is the center of mass and as you deviate from the center of mass characteristics of the particles change. For instance, as you travel away from the center of mass, along the beam axis, the fragmented particles begin to increase in velocity towards the speed of light. Also, pseudorapidity increases as you move away from the center of mass and θ decreases. However, near the center of
2 mass, velocity and pseudorapidity approaches zero and θ becomes much larger. Additionally, these characteristics are the same on both sides of the spectrum (see Figure 1). Figure 1: eta. Image credit Wikipedia Pseudorapidity is a function of a particle s angle ( θ ) from the beam axis. We can think of pseudorapidity as the speed of the particle along the beam axis and this gives us a relation between position and momentum. We can describe pseudorapidity in terms of momentum as η = 1 2 ln P + P z P P z. P z is the momentum directed down the beam axis and P t is the transverse momentum perpendicular to the beam axis. Therefore, you have tanθ = P t. However, in a more simplified form η = ln tan θ P z 2. Jets Jets occur in both particle and nuclear physics experiments. However, it is rare that jets would occur. In the case we do have jets, they occur only from a head-on collision between two quarks or gluons. At the collision point, two sprays of particles split off from the collision and produce a narrow cone of particles with high momentum. Mini-jets are similar and occur at much lower energies than jets. For our purpose, minijets behave exactly like jets. Radial Flow Radial flow is a phenomenon that occurs mostly in heavy ion collisions. During the collision, flux tubes form along the beam axis. As the two nuclei separate, flux tubes start to fragment and form particles with low transverse momentum. This process continues to happen and more particles are created near the center of the beam axis. Since there is a
3 difference in the amount of particles a pressure builds up and pushes particles outward radially from the center. These particles burst out in a random direction with a high transverse momentum. Correlation Measurements Correlation measurements have seen a great deal of focus in understanding the importance of nuclear collisions. We know that some of the earliest evidence of jet quenching came from measurements of two particle correlations. I now reference some studies on two-body correlation functions. For simplicity, we used pseudorapaidity dependence throughout the experiment over a rapidity range [1]. The statistical quantities used for one-body and two-body densities are: ρ 1 ( η) = dn dη and ρ 2 ( η 1,η 2 ) = d 2 N (1) dη 1 dη 2 From Eq. (1) to write multiplicity in a range of pseudorapidity N = ρ 1 ( η)dη (2) Δη Here... represents the average of the number of charged particles per event and fluctuations of the particle number are found by integrating the two- particle density to get the average number of pairs per event, ( ) = ρ 2 η 1,η 2 N N 1 ( )dη 1 dη 2 (3) Δη You may recognize a statistical measurement for the particle fluctuation as the variance from (2) and (3). In equilibrium these events follow a Poisson distribution so σ 2 eq = N. So we define this robust variance as [1]: R = σ 2 N = N 2 N 2 N 2 N N 2 (4) This tells us how far the events are from being in equilibrium. D is the main observable that we used to analyze our data. Professor Sean Gavin and Mike Catanzaro proposed this observable a few years ago. D allows us to distinguish between the effects of jets and radial flow. We argue that if D is positive than we expect jets to dominate. However, if D is negative we say that the system exhibits radial flow.
4 D = NP t N P t p t ( N 2 N 2 ) (5) N 2 Finally, the last correlation measurement we used is δp t1 δp t 2. We can think of δp t1 δp t 2 as the covariance per particle pair. My goal is to see how the particles characteristics change together. In this case, it measures the transverse momentum fluctuations in the collision δp t1 δp t 2 = i j N N 1 δp ti δp tj ( ) (6) where δp ti = p ti p t and the average transverse momentum is p t = P t N for P t = p i ti the total momentum in the event[2]. This quantity will vanish if particles i and j are uncorrelated. If δp t1 δp t 2 approaches zero, then we say all the particles transverse momentum is about average. If it s not zero, then there may be explosive jets. RESULTS If you look at figure 2, you can see the plots are not flat. This implies that our data does not follow Poisson distribution. Since jets are present in our events we do not expect the observables to be uniform in pseudorapidity, and our findings support this. If you examine figure 3, I illustrate how jets have a more Gaussian distribution over a range Δη. Jets are peaked in Δη and flux tubes are not. My plots show a curve in the data and I believe this comes from the production of jets. When you interpret the plots at η = 0 you can see that R ~.854, D ~.068 GeV, and δp t1 δp ~.0067 t 2 GeV2. You can also see that on either side of η = 0 they are pretty symmetric, which is expected, due to the symmetric nature of the collision. In addition, the statistical uncertainties are so small that the plotted line covers them up. Software PYTHIA 8, a Monte Carlo event generator, is the program I used to simulate collisions of single particles. It replicates interactions between charged particles to illustrate the elementary particles during collisions [3]. PYTHIA 8 only uses proton-proton collisions, therefore only a few dozen particles result from the collision. Since PYTHIA 8 produces a small amount of particles it does not incorporate radial flow. In order for radial flow to
5 be significant thousands of particles would need to be present. For a future project, one could use other programs such as HIJING to simulate heavy-ion collisions. Additionally, I used a program developed by CERN called ROOT. ROOT is a data analysis program that creates histograms, plots and many more data analysis methods. I ran ROOT through PYTHIA 8 and analyzed this vast amount of data to create histograms that could illustrate many significant details. ACKNOWLEDGEMENTS I would like to thank George Moschelli and Rajendra Pokharel for discussions and their additional guidance. This work was funded under NSF Grant PHY Figure 2: plot observables on one
6 Jets vs. Flux Tube/String Fragmentation # of pairs Flux tube/string Fragmentation jets Δη Figure 3: Jets vs. Flux Tube/String Fragmentation Figure 4: Close up on D
7 Figure 5: Close up on <dptdpt> REFERENCES [1] C. Pruneau, S. Gavin and S. Voloshin, Phys. Rev. C 66, (2002) [arxiv:nuclex/ ]. [2] S. Gavin and G. Moschelli, (2011) [arxiv: v2 [nucl-th]]. [3] T. Sjostrand and M. van Zijil, Phys. Rev. D 36, 2019 (1987).
Jet and Minijet Contributions to Transverse Momentum Correlations in High Energy Collisions
Jet and Minijet Contributions to Transverse Momentum Correlations in High Energy Collisions Mike Catanzaro August 14, 2009 1 Intro I have been studying the effects of jet and minijet production on momentum
More informationHydrodynamic Flow in Pb-Pb and p-pb collisions Nicholas Faucher August, 2014
Hydrodynamic Flow in Pb-Pb and p-pb collisions Nicholas Faucher August, 04 Introduction Over the Summer, I have been studying various aspects of high-energy particle collisions and working alongside faculty
More informationMomentum Correlations in Nuclear Collisions
Momentum Correlations in Nuclear Collisions By: Patrick Carzon Advisors: Sean Gavin, George Moschelli August 2016 1 Introduction Covariance is a measure of how linearly two things change with each other.
More informationBackground Subtraction Methods on Recoil Jets from Proton-Proton Collisions
Background Subtraction Methods on Recoil Jets from Proton-Proton Collisions Colby Ostberg San Francisco State University REU student at Texas A&M Cyclotron Institute 1 Motivation At the RHIC, heavy ions
More informationSearching For p+ p+ Rapidity Dependent Correlations in Ultra-relativistic Quantum Molecular Data. Abstract
Searching For p+ p+ Rapidity Dependent Correlations in Ultra-relativistic Quantum Molecular Data Isaac Pawling (Dated: August 7, 2015) Abstract Finding rapidity dependent particle correlations in particle
More informationFluctuation and flow probes of early-time correlations in relativistic heavy ion collisions
Journal of Physics: Conference Series Fluctuation and flow probes of early-time correlations in relativistic heavy ion collisions To cite this article: Sean Gavin and George Moschelli 212 J. Phys.: Conf.
More informationTests of Pythia8 Rescattering Model
Tests of Pythia8 Rescattering Model arxiv:5.325v [hep-ph] Nov 25 Tasnuva Chowdhury Shahjalal University of Science and Technology Sylhet, Bangladesh. Deepak Kar University of Witwatersrand Johannesburg,
More informationInclusive spectrum of charged jets in central Au+Au collisions at s NN = 200 GeV by STAR
Inclusive spectrum of charged jets in central Au+Au collisions at s NN = 200 GeV by SAR Nuclear Physics Institute, Academy of Sciencis of Czech Republic, Na ruhlarce 39/64, 180 86 Prague, Czech Republic
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 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 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 informationCharacterization of Jets in Relativistic Heavy Ion Collisions
Characterization of Jets in Relativistic Heavy Ion Collisions arxiv:nucl-th/0307059v 4 Dec 003 S. C. Phatak and P. K. Sahu Institute of Physics, Bhubaneswar 751 005, India Abstract Jet quenching is considered
More informationRapidity Dependence of Chemical Freeze out in Au Au Collisions
Rapidity Dependence of Chemical Freeze out in Au Au Collisions Kristen Parzuchowski Research Experience for Undergraduates Wayne State University August 7, 2015 Abstract The study of nuclear matter is
More informationWayne State REU Program
Wayne State REU Program Simulations of Temperature Fluctuations in Heavy-ion Collisions By: Nathan Fisher Mentor: Prof. Claude Pruneau Abstract This report covers two separate projects with project 1 being
More informationKristjan 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 informationPileup Subtraction and Jet Energy Prediction Using Machine Learning
000 00 002 003 004 005 006 007 008 009 00 0 02 03 04 05 06 07 08 09 020 02 022 023 024 025 026 027 028 029 030 03 032 033 034 035 036 037 038 039 040 04 042 043 044 045 046 047 048 049 050 05 052 053 054
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 informationOn multiplicity correlations in the STAR data
arxiv:1203.3671v2 [nucl-th] 8 May 2012 On multiplicity correlations in the STAR data K. FIAŁKOWSKI 1, R. WIT 2 M. Smoluchowski Institute of Physics Jagellonian University 30-059 Kraków, ul.reymonta 4,
More informationCMS Event Simulation
CMS Event Simulation Nicole A. Larsen Department of Physics, Georgia Institute of Technology, Atlanta, GA, 33 (Dated: August 11, 6) The CMS Detector located at the Large Hadron Collider at CERN recently
More informationGluonic superfluid in high energy p-pb collisions. Chris Zin Derek Everett, Sean Gavin, AbhijitMajumder Graduate Research Day Wayne State University
Gluonic superfluid in high energy p-pb collisions Chris Zin Derek Everett, Sean Gavin, AbhijitMajumder Graduate Research Day Wayne State University Quark-gluon plasma State of matter consisting of free
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 informationJet production, charged particles in pp-interactions, HIJING, pseudorapidity, transverse momentum, transverse mass
Effect of the Jet Production on Pseudorapidity, Transverse Momentum and Transverse Mass istributions of Charged Particles Produced in pp-collisions at Tevatron Energy * Ali Zaman ;), Mais Suleymanov, Muhammad
More informationMeasurement of muon tagged open heavy flavor production in Pb+Pb collisions at 2.76 TeV with ATLAS
Measurement of muon tagged open heavy flavor production in Pb+Pb collisions at 2.76 TeV with Dennis V. Perepelitsa Columbia University for the Collaboration Quark Matter 2012 Parallel 7A Washington, D.C.,
More informationBackground Analysis Columbia University REU 2015
Background Analysis Columbia University REU 2015 Kylee Branning Northern Michigan University Adviser: Dr. Kalliopi Iordanidou July 31, 2015 Abstract This study focuses on the development of data driven
More informationMonte Carlo Studies of Identified Two-particle Correlations in p-p and Pb-Pb Collisions
Journal of Physics: Conference Series OPEN ACCESS Monte Carlo Studies of Identified wo-particle Correlations in p-p and Pb-Pb Collisions o cite this article: Gyula Bencédi et al J. Phys.: Conf. Ser. 89
More informationJet Physics. Yazid Delenda. 1st Jijel Meeting on Theoretical Physics. Jijel, October 29-31, University Batna 1
Jet Physics Yazid Delenda University Batna 1 1st Jijel Meeting on Theoretical Physics Quantum Mechanics, Gravitation and Particle Physics Jijel, October 29-31, 2018 977 1 ⵜ ⴰ ⵙ ⴷⴰ ⵡⵉ ⵜ ⵏ ⵜ ⴱⴰ ⵜ ⴻ ⵏ ⵜ U
More informationVOL 18, #2 THE JOURNAL OF UNDERGRADUATE RESEARCH IN PHYSICS 39
VOL 18, #2 THE JOURNAL OF UNDERGRADUATE RESEARCH IN PHYSICS 39 MODELING PION FLOW IN A 139 La + 139 La COLLISION Daniel Valente * Department of Physics and Engineering Hope College Holland, MI 49423 received
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 informationNew particle Searches in the dijet final state at 13TeV with the ATLAS detector
New particle Searches in the dijet final state at 13TeV with the ATLAS detector Mohammad Atif August 21, 2015 1 INTRODUCTION Summer Project at CERN Supervised by Dr. Caterina Doglioni. In Standard Model
More informationarxiv: v1 [nucl-ex] 14 Oct 2013
Charged Jets in Minimum Bias p-pb Collisions at snn = 5.02 TeV with ALICE arxiv:1310.3612v1 [nucl-ex] 14 Oct 2013 for the ALICE collaboration Westfälische Wilhelms-Universität Münster, Germany E-mail:
More informationStudy of Dihadron Fragmentation Function Correlations in p-p collisions at 7 TeV. Derek Everett Dr. Claude Pruneau, Dr.
Study of Dihadron Fragmentation Function Correlations in p-p collisions at 7 TeV Derek Everett Dr. Claude Pruneau, Dr. Sidharth Prasad Outline Physics Motivation Definitions of Observables PYTHIA Monte
More informationTwo Early Exotic searches with dijet events at ATLAS
ATL-PHYS-PROC-2011-022 01/06/2011 Two Early Exotic searches with dijet events at ATLAS University of Toronto, Department of Physics E-mail: rrezvani@physics.utoronto.ca This document summarises two exotic
More informationStandard Model at the LHC (Lecture 3: Measurement of Cross-Sections) M. Schott (CERN)
Standard Model at the LHC (Lecture 3: Measurement of Cross-Sections) M. Schott (CERN) Content 1 Measuring Cross-Sections 2 Hands-On 3 Background Estimations 4 Detector Calibration 5 Recent LHC Results
More informationSelected Topics in the Theory of Heavy Ion Collisions Lecture 1
Selected Topics in the Theory of Heavy Ion Collisions Lecture 1 Urs chim Wiedemann CERN Physics Department TH Division Varenna, 19 July 2010 Based on http://cdsweb.cern.ch/record/1143387/files/p277.pdf
More informationarxiv:nucl-ex/ v1 26 Feb 2007
International Journal of Modern Physics E c World Scientific Publishing Company arxiv:nucl-ex/0702056v1 26 Feb 2007 ENERGY DEPENDENCE OF SHORT AND LONG-RANGE MULTIPLICITY CORRELATIONS IN AU+AU COLLISIONS
More informationAnalysis of Z ee with the ATLAS-Detector
DESY Summer Student Programme 2008 Hamburg Analysis of Z ee with the ATLAS-Detector Maximilian Schlupp ATLAS Group 11.09.2008 maximilian.schlupp@desy.de maximilian.schlupp@tu-dortmund.de Supervisor: Karsten
More informationOptimizing Selection and Sensitivity Results for VV->lvqq, 6.5 pb -1, 13 TeV Data
1 Optimizing Selection and Sensitivity Results for VV->lvqq, 6.5 pb, 13 TeV Supervisor: Dr. Kalliopi Iordanidou 215 Columbia University REU Home Institution: High Point University 2 Summary Introduction
More informationConference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on the CMS information server CMS CR 212/178 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH211 GENEVA 23, Switzerland 212//9 Measurement of isolated photon
More informationProperties of Proton-proton Collision and. Comparing Event Generators by Multi-jet Events
Properties of Proton-proton Collision and Comparing Event Generators by Multi-jet Events Author: W. H. TANG 1 (Department of Physics, The Chinese University of Hong Kong) Supervisors: Z. L. MARSHALL 2,
More informationCzech Technical University in Prague Faculty of Nuclear Sciences and Physical Engineering. Department of Physics. Research project
Czech echnical University in Prague Faculty of Nuclear Sciences and Physical Engineering Department of Physics Research project Preparation of the HF detector for the SAR experiment Bc. Michal esař Supervisor:
More informationThe Underlying Event in Run II ChgJets versus JetClu Jets
The Underlying Event in Run II ChgJets versus JetClu Jets Outline of Talk! The evolution of charged particle jets and the underlying event. Study the event topology relative to the leading chgjet and compare
More informationHigh-p T Neutral Pion Production in Heavy Ion Collisions at SPS and RHIC
High- Neutral Pion Production in Heavy Ion Collisions at SPS and RHIC K. Reygers for the WA98 and the PHENIX collaboration Institut für Kernphysik der Universität Münster Wilhelm-Klemm-Str. 9, D-4849 Münster,
More informationMeasures of charge fluctuations in nuclear collisions
Measures of charge fluctuations in nuclear collisions Jacek Zaranek* Institut für Kernphysik, Universität Frankfurt, D-60486 Frankfurt, Germany Received 27 November 2001; published 29 August 2002 The properties
More informationarxiv:nucl-ex/ v1 10 May 2004
arxiv:nucl-ex/0405004v1 10 May 2004 Proc. 20th Winter Workshop on Nuclear Dynamics (2003) 000 000 Anisotropic flow at RHIC A. H. Tang 1 for the STAR Collaboration 1 NIKHEF and Brookhaven National Lab,
More informationInclusive distributions at the LHC as predicted from the DPMJET-III model with chain fusion
Inclusive distributions at the LHC as predicted from the DPMJET-III model with chain fusion F.Bopp, R.Engel, J.Ranft and S.Roesler () DPMJET III () Chain fusion in DPMJET III (3) dn/dη cm distributions
More informationEIC Monte Carlo and the Question of Jets
EIC Monte Carlo and the Question of Jets University of Colorado at Boulder seele@down.colorado.edu - March 16, 2004 Jefferson Lab Monte Carlo History of Development Basic Structure Current State Question
More informationStudying the QCD Medium in Proton-Proton Collisions Using PYTHIA
Studying the QCD Medium in Proton-Proton Collisions Using PYTHIA A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science By Omar Tarek ElSherif Department of Physics,
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 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 informationA study of φ-meson spin alignment with the AMPT model
A study of φ-meson spin alignment with the AMPT model Shaowei Lan 1 Zi-Wei Lin 1,2, Shusu Shi 1, Xu Sun 1 1 Central China Normal University 2 East Carolina University Outline Introduction Modified AMPT
More informationAssessment of triangular flow in jet background fluctuations for Au+Au collisions First look at dijet imbalance (A J )
Assessment of triangular flow in jet background fluctuations for Au+Au collisions First look at dijet imbalance (A J ) Wayne State REU 2012 Research Advisor: Joern Putschke Research Undergraduate: Joshua
More informationHeavy Hadron Production and Spectroscopy at ATLAS
Heavy Hadron Production and Spectroscopy at ALAS Carlo Schiavi on behalf of the ALAS Collaboration INFN Sezione di Genova ALAS has studied heavy flavor production and measured the production cross sections
More informationGranularity of ATLAS Tile Calorimeter studied through simulations
Granularity of ATLAS Tile Calorimeter studied through simulations Anabel Cristina Romero Hernandez Supervisor: Irene Vichou Project report for CERN Summer Student Programme 2015 Abstract A small study,
More informationHow to Measure Top Quark Mass with CMS Detector??? Ijaz Ahmed Comsats Institute of Information Technology, Islamabad
How to Measure Top Quark Mass with CMS Detector??? Ijaz Ahmed Comsats Institute of Information Technology, Islamabad Outlines o o o o o o o High Pt top basic idea Methods for jets selection Top quark mass
More informationStefano Carignano 12/2010. Phenomenology of particle production in pp collisions
Phenomenology of particle production in pp collisions Stefano Carignano 12/2010 Outline Some very basic stuff Modeling interactions in pp collisions Strings and hadronization Motivation pp collisions provide
More informationParticle Physics with Electronic Detectors
Particle Physics with Electronic Detectors This experiment performed by the Oxford group on the 7 GeV proton synchrotron, NIMROD, at the Rutherford Laboratory in 1967 gave the first usefully accurate measurement
More informationToward 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 informationRecent Results from RHIC: On the trail of the Quark-Gluon Plasma
Recent Results from RHIC: On the trail of the Quark-Gluon Plasma Single Au+Au Collision seen by STAR@RHIC Gunther Roland Gunther Roland/MIT July 15 2003 MPI Munich 15/7/2003 Gunther Roland/MIT www.spiegel.de
More informationTHE FLORIDA STATE UNIVERSITY COLLEGE OF ARTS & SCIENCES W BOSON PRODUCTION CHARGE ASYMMETRY IN THE ELECTRON CHANNEL ASHLEY S HUFF
THE FLORIDA STATE UNIVERSITY COLLEGE OF ARTS & SCIENCES W BOSON PRODUCTION CHARGE ASYMMETRY IN THE ELECTRON CHANNEL By ASHLEY S HUFF A Thesis submitted to the Department of Physics In partial fulfillment
More informationAzimuthal anisotropy of the identified charged hadrons in Au+Au collisions at S NN. = GeV at RHIC
Journal of Physics: Conference Series PAPER OPEN ACCESS Azimuthal anisotropy of the identified charged hadrons in Au+Au collisions at S NN = 39-200 GeV at RHIC To cite this article: S S Vdovkina 2017 J.
More informationRapid change of multiplicity fluctuations in system size dependence at SPS energies
The 3rd International Conference on Particle Physics and Astrophysics Volume 2018 Conference Paper Rapid change of multiplicity fluctuations in system size dependence at SPS energies Andrey Seryakov for
More informationEfficiency of the CMS Level-1 Trigger to. Selected Physics Channels
Efficiency of the CMS Level-1 Trigger to Selected Physics Channels C. Sulkko University of Colorado, Boulder, CO D. Acosta University of Florida, Gainesville, FL Abstract The efficiency of the Compact
More informationThe rejection of background to the H γγ process using isolation criteria based on information from the electromagnetic calorimeter and tracker.
Available on CMS information server CMS NOTE 22/3 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland September 9, 22 The rejection of background to
More informationLHC: Status and Highlights
EPJ Web of Conferences 9, 9 (6) DOI:.5/ epjconf/699 QCD@Work 6 ALICE @ LHC: Status and Highlights Alberica oia,, Goethe University of Frankfurt GSI Helmholzzentrum fuer Schwerionenforschung Abstract. ALICE
More informationMONTE CARLO CHECKS. Samantha Hamernik Hastings College (NE) Mentor: Dr. Hal Evans 2003 REU: Nevis Laboratories Columbia University: D-Zero Group
MONTE CARLO CHECKS Samantha Hamernik Hastings College (NE) Mentor: Dr. Hal Evans 2003 REU: Nevis Laboratories Columbia University: D-Zero Group Abstract: In this paper I seek to explain what I accomplished
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 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 informationZ 0 /γ +Jet via electron decay mode at s = 7TeV in
PRAMANA c Indian Academy of Sciences Vol. 86, No. 2 journal of February 2016 physics pp. 487 491 Z 0 /γ +Jet via electron decay mode at s = 7TeV in CMS@LHC U BHAWANDEEP and SUMAN B BERI for CMS Collaboration
More informationCan hadronic rescattering explain the jet quenching at relativistic energies?
PHYSICAL REVIEW C 71, 3496 (25) Can hadronic rescattering explain the jet quenching at relativistic energies? David Hardtke Department of Physics, University of California, Berkeley, California 9472 USA
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 informationDetection of Ф(1020) meson by the decay Ф K + K -
Detection of Ф(1020) meson by the decay Ф K + K - D. Randrianasoloharisoa 1 *, F. Lahatra Razafindramisa 1 1 Laboratoire de Physique de la Matière et du Rayonnement, Université d'antananarivo, Madagascar
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 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 informationStudy of dihadron fragmentation function correlations using charged jets in proton-proton collisions at s = 7 TeV
Study of dihadron fragmentation function correlations using charged jets in proton-proton collisions at s = 7 TeV Derek Everett, Claude Pruneau, Sidharth Prasad August, Abstract We present the measurements
More informationSelected Topics in the Theory of Heavy Ion Collisions Lecture 1
Selected Topics in the Theory of Heavy Ion Collisions Lecture 1 Urs chim Wiedemann CERN Physics Department TH Division Skeikampen, 4 January 2012 Heavy Ion Collisions - Experiments lternating Gradient
More informationA Geant4 validation study for the ALICE experiment at the LHC
A Geant4 validation study for the ALICE experiment at the LHC Kevin Nicholas Barends Department of Physics University of Cape Town Supervisor: Dr Alexander Kalweit Co-supervisor: Dr Sandro Wenzel 04 August
More informationNeutral Current Interference in the TeV Region; the Experimental Sensitivity at the LHC
ETHZ-IPP PR-96-01 21 March, 1996 Neutral Current Interference in the TeV Region; the Experimental Sensitivity at the LHC Michael Dittmar Institute for Particle Physics (IPP), ETH Zürich, CH-8093 Zürich,
More informationpt-inclusive 2-particle correlations; p-p, Cu-Cu, Au-Au BES
pt-inclusive 2-particle correlations; p-p, Cu-Cu, Au-Au BES Duncan May 7, 2012 1 Agenda Review of Methods Minimum-bias Jets in pp - the reference system Review 200, 62 GeV Au-Au Compare Cu-Cu to Au-Au
More informationMeasurement of charged particle spectra in pp collisions at CMS
Measurement of arged particle spectra in pp collisions at CMS for the CMS Collaboration Eötvös Loránd University, Budapest, Hungary E-mail: krisztian.krajczar@cern. We present the plans of the CMS collaboration
More informationTesting Theories in Particle Physics Using Maximum Likelihood and Adaptive Bin Allocation
Testing Theories in Particle Physics Using Maximum Likelihood and Adaptive Bin Allocation Bruce Knuteson 1 and Ricardo Vilalta 2 1 Laboratory for Nuclear Science, Massachusetts Institute of Technology
More informationViscosity of Quark-Gluon Plasma!
Viscosity of Quark-Gluon Plasma! Rajendra Pokharel Advisor: Prof. Sean Gavin 2 nd Graduate Research Day " Wayne State University " "Apr 24, 2011! Outlines " " Background Hydrodynamics The Model Results
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 informationStudying hot QCD matter at the CERN-LHC with heavy quarks
Studying hot QC matter at the CERN-LHC with heavy quarks ERC-Research Group QGP-ALICE, Utrecht University, Princetonplein 5, 58 CS Utrecht, the Netherlands E-mail: a.mischke@uu.nl his paper discusses selected
More informationSearch for the Z Boson in the Dielectron Channel
Search for the Z Boson in the Dielectron Channel Sedrick Weinschenk 1,2 1 Physics Department, Columbia University 2 Physics and Astronomy Department, Butler University August 3, 2018 This paper discusses
More informationThe first Z boson measurement in the dimuon channel in PbPb collisions at s = 2.76 TeV at CMS
The first Z boson measurement in the dimuon channel in PbPb collisions at s = 2.76 TeV at CMS Lamia Benhabib On behalf of CMS collaboration We present the first measurement of Z bosons in the di-muon channel
More informationModern Accelerators for High Energy Physics
Modern Accelerators for High Energy Physics 1. Types of collider beams 2. The Tevatron 3. HERA electron proton collider 4. The physics from colliders 5. Large Hadron Collider 6. Electron Colliders A.V.
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 informationStudies of the diffractive photoproduction of isolated photons at HERA
Studies of the diffractive photoproduction of isolated photons at HERA P. J. Bussey School of Physics and Astronomy University of Glasgow Glasgow, United Kingdom, G12 8QQ E-mail: peter.bussey@glasgow.ac.uk
More informationPYTHIA 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 informationMeasurement of Charged Particle Spectra in Deep-Inelastic ep Scattering at HERA
Measurement of Charged Particle Spectra in Deep-Inelastic ep Scattering at HERA Alexander BYLINKIN ( Institute for Theoretical and Experimental Physics (ITEP), Moscow, Russia) E-mail: alexander.bylinkin@gmail.com
More informationEffects of Jet Substructure Selection in
Effects of Jet Substructure Selection in tt WbWb µνbqqb Ziggy Zacks Wesleyan University July 31, 2012 1 / 29 Optimization Optimize data selection from the semi-leptonic boosted tops analysis. Specifically
More informationStudy of charm fragmentation in e + e annihilation and ep scattering
Study of charm fragmentation in e + e annihilation and ep scattering - Summer Student Report - by Thomas Lübbert H1 Collaboration at DESY Advisor: Co-Advisor: Dr. Günter Grindhammer Andrej Liptaj September
More informationFall Quarter 2010 UCSB Physics 225A & UCSD Physics 214 Homework 1
Fall Quarter 2010 UCSB Physics 225A & UCSD Physics 214 Homework 1 Problem 2 has nothing to do with what we have done in class. It introduces somewhat strange coordinates called rapidity and pseudorapidity
More informationJet quenching in PbPb collisions in CMS
Jet quenching in PbPb collisions in CMS Bolek Wyslouch École Polytechnique Massachusetts Institute of Technology arxiv:1102.1957 Orsay, February 18, 2011 1 Heavy Ions at the LHC Huge energy jump from RHIC:
More informationRidge correlation structure in high multiplicity pp collisions with CMS
Ridge correlation structure in high multiplicity pp collisions with CMS Dragos Velicanu for the CMS Collaboration MBUEWG CERN, Geneva, June 17 2011 Results from High Multiplicity pp Dragos Velicanu (MIT)
More informationarxiv:nucl-ex/ v2 1 Mar 2007
March, 007 :57 WSPC/INSRUCION FILE International Journal of Modern Physics E c World Scientific Publishing Company arxiv:nucl-ex/070057v Mar 007 SIMULAION OF JE QUENCHING OBSERVABLES IN HEAVY ION COLLISIONS
More informationHeavy-Ion Jet INteraction Generator -- HIJING
Heavy-Ion Jet INteraction Generator -- HIJING XI SERC School on Experimental High-Energy Physics NISER Bhubaneswar, November 07-27, 2017 Event Generators Session 1 Introduction Heavy Ion Jet INteraction
More informationPseudorapidity dependence of multiplicity and transverse momentum fluctuations in pp collisions at SPS energies
The 3rd International Conference on Particle Physics and Astrophysics Volume 208 Conference Paper Pseudorapidity dependence of multiplicity and transverse momentum fluctuations in pp collisions at SPS
More informationarxiv: v1 [nucl-ex] 20 Jan 2018
arxiv:80.06690v [nucl-ex] 20 Jan 208 Pseudorapidity dependence of multiplicity and transverse momentum fluctuations in pp collisions at SPS energies Daria Prokhorova for the NA6/SHINE Collaboration St.
More informationRecent Jet Results from the CMS experiment
Recent Jet Results from the CMS experiment Raghav Kunnawalkam Elayavalli ( USA) Nuclear Seminar Monday, February 2nd, 2015 1 Overview https://twiki.cern.ch/twiki/bin/view/cmspublic/ PhysicsResultsHIN Motivations
More information