A Strange Quark Plasma
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The Role of Strangeness in Ultrarelativistic Nuclear
HUTFT THE ROLE OF STRANGENESS IN a ULTRARELATIVISTIC NUCLEAR COLLISIONS Josef Sollfrank Research Institute for Theoretical Physics PO Box FIN University of Helsinki Finland and Ulrich Heinz Institut f ur Theoretische Physik Universitat Regensburg D Regensburg Germany ABSTRACT We review the progress in understanding the strange particle yields in nuclear colli sions and their role in signalling quarkgluon plasma formation We rep ort on new insights into the formation mechanisms of strange particles during ultrarelativistic heavyion collisions and discuss interesting new details of the strangeness phase di agram In the main part of the review we show how the measured multistrange particle abundances can b e used as a testing ground for chemical equilibration in nuclear collisions and how the results of such an analysis lead to imp ortant con straints on the collision dynamics and spacetime evolution of high energy heavyion reactions a To b e published in QuarkGluon Plasma RC Hwa Eds World Scientic Contents Introduction Strangeness Pro duction Mechanisms QuarkGluon Pro duction Mechanisms Hadronic Pro duction Mechanisms Thermal Mo dels Thermal Parameters Relative and Absolute Chemical Equilibrium The Partition Function The Phase Diagram of Strange Matter The Strange Matter Iglo o Isentropic Expansion Trajectories The T ! Limit of the Phase Diagram -
The Particle World
The Particle World ² What is our Universe made of? This talk: ² Where does it come from? ² particles as we understand them now ² Why does it behave the way it does? (the Standard Model) Particle physics tries to answer these ² prepare you for the exercise questions. Later: future of particle physics. JMF Southampton Masterclass 22–23 Mar 2004 1/26 Beginning of the 20th century: atoms have a nucleus and a surrounding cloud of electrons. The electrons are responsible for almost all behaviour of matter: ² emission of light ² electricity and magnetism ² electronics ² chemistry ² mechanical properties . technology. JMF Southampton Masterclass 22–23 Mar 2004 2/26 Nucleus at the centre of the atom: tiny Subsequently, particle physicists have yet contains almost all the mass of the discovered four more types of quark, two atom. Yet, it’s composite, made up of more pairs of heavier copies of the up protons and neutrons (or nucleons). and down: Open up a nucleon . it contains ² c or charm quark, charge +2=3 quarks. ² s or strange quark, charge ¡1=3 Normal matter can be understood with ² t or top quark, charge +2=3 just two types of quark. ² b or bottom quark, charge ¡1=3 ² + u or up quark, charge 2=3 Existed only in the early stages of the ² ¡ d or down quark, charge 1=3 universe and nowadays created in high energy physics experiments. JMF Southampton Masterclass 22–23 Mar 2004 3/26 But this is not all. The electron has a friend the electron-neutrino, ºe. Needed to ensure energy and momentum are conserved in ¯-decay: ¡ n ! p + e + º¯e Neutrino: no electric charge, (almost) no mass, hardly interacts at all. -
The Tale of the Hagedorn Temperature
Chapter 6 The Tale of the Hagedorn Temperature Johann Rafelski and Torleif Ericson Please note the Erratum to this chapter at the end of the book Abstract We recall the context and impact of Rolf Hagedorn’s discovery of limiting temperature, in effect a melting point of hadrons, and its influence on the physics of strong interactions. 6.1 Particle Production Collisions of particles at very high energies generally result in the production of many secondary particles. When first observed in cosmic-ray interactions, this effect was unexpected for almost everyone,1 but it led to the idea of applying the wide body of knowledge of statistical thermodynamics to multiparticle production processes. Prominent physicists such as Enrico Fermi, Lev Landau, and Isaak Pomeranchuk made pioneering contributions to this approach, but because difficulties soon arose this work did not initially become the mainstream for the study of particle production. However, it was natural for Rolf Hagedorn to turn to the problem. Hagedorn had an unusually diverse educational and research background, which included thermal, solid-state, particle, and nuclear physics. His initial work on statistical particle production led to his prediction, in the 1960s, of particle yields at the highest accelerator energies at the time at CERN’s proton synchrotron. Though there were few clues on how to proceed, he began by making the most of the ‘fireball’ concept, which was then supported by cosmic-ray studies. In this approach, all the energy of the collision was regarded as being contained within a small space- time volume from which particles radiated, as in a burning fireball. -
Strangeness and the Discovery of Quark Gluon
STRANGENESS AND THE DISCOVERY OF QUARK GLUON PLASMA Bloomington, November 30, 2004 Decon¯nement of quarks and gluons into a plasma (QGP) at high temperature is a predicted paradigm shifting feature of strong interactions. The production of strange particles in relativistic heavy ion collisions at CERN and BNL con¯rms that a new phase of matter with the expected properties is being formed. I will survey the key theoretical predictions and the related experimental results. Time permitting, I will discuss how the newly gained knowledge leads to the study of the hot nearly matter-antimatter symmetric post quark-gluon Universe. +50% of content is for STUDENTS. BONUS material after 50 transparencies: THE QUARK UNIVERSE Supported by a grant from the U.S. Department of Energy, DE-FG02-04ER41318 Johann Rafelski Department of Physics University of Arizona TUCSON, AZ, USA 1 J. Rafelski, Arizona STRANGENESS AND THE DISCOVERY OF QUARK GLUON PLASMA Bloomington, November 30, 2004,page 2 EXPERIMENTAL HEAVY ION PROGRAM | LHC CERN: LHC opens after 2007 and SPS resumes after 2009 J. Rafelski, Arizona STRANGENESS AND THE DISCOVERY OF QUARK GLUON PLASMA Bloomington, November 30, 2004,page 3 ...and at BROOKHAVEN NATIONAL LABORATORY Relativistic Heavy Ion Collider: RHIC J. Rafelski, Arizona STRANGENESS AND THE DISCOVERY OF QUARK GLUON PLASMA Bloomington, November 30, 2004,page 4 BROOKHAVEN NATIONAL LABORATORY 12:00 o’clock PHOBOS BRAHMS 10:00 o’clock 2:00 o’clock RHIC PHENIX 8:00 o’clock STAR 4:00 o’clock 6:00 o’clock Design Parameters: Beam Energy = 100 GeV/u U-line 9 GeV/u No. -
Particle Physics Dr Victoria Martin, Spring Semester 2012 Lecture 12: Hadron Decays
Particle Physics Dr Victoria Martin, Spring Semester 2012 Lecture 12: Hadron Decays !Resonances !Heavy Meson and Baryons !Decays and Quantum numbers !CKM matrix 1 Announcements •No lecture on Friday. •Remaining lectures: •Tuesday 13 March •Friday 16 March •Tuesday 20 March •Friday 23 March •Tuesday 27 March •Friday 30 March •Tuesday 3 April •Remaining Tutorials: •Monday 26 March •Monday 2 April 2 From Friday: Mesons and Baryons Summary • Quarks are confined to colourless bound states, collectively known as hadrons: " mesons: quark and anti-quark. Bosons (s=0, 1) with a symmetric colour wavefunction. " baryons: three quarks. Fermions (s=1/2, 3/2) with antisymmetric colour wavefunction. " anti-baryons: three anti-quarks. • Lightest mesons & baryons described by isospin (I, I3), strangeness (S) and hypercharge Y " isospin I=! for u and d quarks; (isospin combined as for spin) " I3=+! (isospin up) for up quarks; I3="! (isospin down) for down quarks " S=+1 for strange quarks (additive quantum number) " hypercharge Y = S + B • Hadrons display SU(3) flavour symmetry between u d and s quarks. Used to predict the allowed meson and baryon states. • As baryons are fermions, the overall wavefunction must be anti-symmetric. The wavefunction is product of colour, flavour, spin and spatial parts: ! = "c "f "S "L an odd number of these must be anti-symmetric. • consequences: no uuu, ddd or sss baryons with total spin J=# (S=#, L=0) • Residual strong force interactions between colourless hadrons propagated by mesons. 3 Resonances • Hadrons which decay due to the strong force have very short lifetime # ~ 10"24 s • Evidence for the existence of these states are resonances in the experimental data Γ2/4 σ = σ • Shape is Breit-Wigner distribution: max (E M)2 + Γ2/4 14 41. -
A4 Standard Format Template
2008 SCHOOL OF PHYSICS Annual Report 4 www.physics.unimelb.edu.au contents/ the university of melbourne 6 the faculty of science 8 THE SCHOOL OF PHYSICS 9 HEAD’S REPORT 10 EXECUTIVE MANAGER’S REPORT 10 SCHOOL GOVERANCE 11 STAFF 12 VISITORS 18 RESEARCH FUNDING 20 RESEARCH SEMINAR SERIES 23 SCHOOL-HOSTED CONFERENCES 28 POSTGRADUATES IN PROGRESS 30 THESES COMPLETIONS 34 GROUP REPORT & PUBLICATIONS - Astrophysics 35 - Experimental Particle Physics (EPP) 39 - Micro-Analytical Research Centre (MARC) 45 Quantum Communications Victoria (QCV) 50 - Optics 51 ARC Centre of Excellence for Coherent X-ray Science (CXS) 54 - Theoretical Condensed Matter Physics (TCMP) 56 - Theoretical Particle Physics (TPP) 60 postgraduate physics student society (PPSS) 63 priZes & awards 64 outreach programs 66 subJects offered 69 alumni & friends 70 media 72 recruiting organisations 74 more information 75 www.physics.unimelb.edu.au 5 The University of Melbourne The university OF the Melbourne Model undergraduate and graduate education have continued to be a central focus of Melbourne thought and investment at the University. Established in 1853, the University of Melbourne The final strand – knowledge transfer – has long is a public-spirited institution that makes distinctive been practised but not always acknowledged at contributions to society in research, teaching and the University. A commitment to projects based knowledge transfer. on engagement, exchange and partnership with Melbourne’s teaching excellence has been wider constituencies has become a familiar part rewarded two years in a row by grants from of University aspirations. Knowledge transfer is the Commonwealth Government’s Learning about direct, two-way interactions between the and Teaching Performance Fund for Australian University and its external communities, which universities that demonstrate excellence in involve the development, exchange and application undergraduate teaching and learning. -
Neutron Stars and Strange Matter Bnl—39402 De37 006746 J
NEUTRON STARS AND STRANGE MATTER BNL—39402 DE37 006746 J. Cooperstein* Brookhaven National Laboratory, Upton NY 11973 and SUNY at Stony Brook NY 11794 We investigate the likelihood that quark matter with strangeness of order unity resides in neutron stars. In the strong coupling regime near Po this is found to be unlikely. Considering higher densities where perturbative expansions are used, we find a lower bound to be at 7p0 for the transition density. This is higher than the inferred density of observed neutron stars, and thus the transition to quark matter is precluded. I. Introduction We will deal with the question: does bulk strange matter exist in nature? For this we will draw upon our recent investigation of this subject done in collaboration with Hans Bethe and Gerry Brown1. Strange matter is usually taken to mean deconfined i .lark matter with strangeness of order unity. If such material exists in the universe today, the core of neutron stars is the oi?ly reasonable place to search for it in the bulk. Observationally the problem is difficult. We know that all well measured neutron stars have masses in the range 1.4 ~ M/MQ ~ 1.6, so we have at least a lower limit to the maximum mass. As far as an upper limit is concerned one might be tempted to believe it is not much higher than the above range for two reasons. First there is the fact that Type II supernovae calculations always tend to leave behind a mass at the lower end of the above range, since this is about the iron core mass of the presupernova star, and the explosion should sweep out almost all of the overlying burning shells. -
Strange Particle Theory in the Cosmic Ray Period R
STRANGE PARTICLE THEORY IN THE COSMIC RAY PERIOD R. Dalitz To cite this version: R. Dalitz. STRANGE PARTICLE THEORY IN THE COSMIC RAY PERIOD. Journal de Physique Colloques, 1982, 43 (C8), pp.C8-195-C8-205. 10.1051/jphyscol:1982811. jpa-00222371 HAL Id: jpa-00222371 https://hal.archives-ouvertes.fr/jpa-00222371 Submitted on 1 Jan 1982 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. JOURNAL DE PHYSIQUE Colloque C8, suppldment au no 12, Tome 43, ddcembre 1982 page ~8-195 STRANGE PARTICLE THEORY IN THE COSMIC RAY PERIOD R.H. Dalitz Department of Theoretical Physics, 2 KebZe Road, Oxford OX1 3NP, U.K. What role did theoretical physicists play concerning elementary particle physics in the cosmic ray period? The short answer is that it was the nuclear forces which were the central topic of their attention at that time. These were considered to be due primarily to the exchange of pions between nucleons, and the study of all aspects of the pion-nucleon interactions was the most direct contribution they could make to this problem. Of course, this was indeed a most important topic, and much significant understanding of the pion-nucleon interaction resulted from these studies, although the precise nature of the nucleonnucleon force is not settled even to this day. -
Detection of a Strange Particle
10 extraordinary papers Within days, Watson and Crick had built a identify the full set of codons was completed in forensics, and research into more-futuristic new model of DNA from metal parts. Wilkins by 1966, with Har Gobind Khorana contributing applications, such as DNA-based computing, immediately accepted that it was correct. It the sequences of bases in several codons from is well advanced. was agreed between the two groups that they his experiments with synthetic polynucleotides Paradoxically, Watson and Crick’s iconic would publish three papers simultaneously in (see go.nature.com/2hebk3k). structure has also made it possible to recog- Nature, with the King’s researchers comment- With Fred Sanger and colleagues’ publica- nize the shortcomings of the central dogma, ing on the fit of Watson and Crick’s structure tion16 of an efficient method for sequencing with the discovery of small RNAs that can reg- to the experimental data, and Franklin and DNA in 1977, the way was open for the com- ulate gene expression, and of environmental Gosling publishing Photograph 51 for the plete reading of the genetic information in factors that induce heritable epigenetic first time7,8. any species. The task was completed for the change. No doubt, the concept of the double The Cambridge pair acknowledged in their human genome by 2003, another milestone helix will continue to underpin discoveries in paper that they knew of “the general nature in the history of DNA. biology for decades to come. of the unpublished experimental results and Watson devoted most of the rest of his ideas” of the King’s workers, but it wasn’t until career to education and scientific administra- Georgina Ferry is a science writer based in The Double Helix, Watson’s explosive account tion as head of the Cold Spring Harbor Labo- Oxford, UK. -
Arxiv:Astro-Ph/9702189V1 21 Feb 1997 90.Tetertclpeitosaecmae Ihtebo the with Compared Al
Differences in the Cooling Behavior of Strange Quark Matter Stars and Neutron Stars Christoph Schaab1, Bernd Hermann, Fridolin Weber and Manfred K. Weigel Institut f¨ur theoretische Physik, Ludwig-Maximilians Universit¨at M¨unchen, Theresienstr. 37, D-80333 M¨unchen, Germany ABSTRACT The general statement that hypothetical strange (quark matter) stars cool more rapidly than neutron stars is investigated in greater detail. It is found that the direct Urca process could be forbidden not only in neutron stars but also in strange stars. In this case, strange stars are slowly cooling, and their surface temperatures are more or less indistinguishable from those of slowly cooling neutron stars. Furthermore the case of enhanced cooling is reinvestigated. It shows that strange stars cool significantly more rapidly than neutron stars within the first ∼ 30 years after birth. This feature could become particularly interesting if continued observation of SN 1987A would reveal the temperature of the possibly existing pulsar at its center. Subject headings: stars: evolution – stars: neutron 1. Introduction The theoretical possibility that strange quark matter – made up of roughly equal numbers of up, down and strange quarks – may be more stable than atomic nuclei (specifically iron, which is arXiv:astro-ph/9702189v1 21 Feb 1997 the most stable atomic nucleus) constitutes one of the most startling predictions of modern physics (see Bodmer 1971, Witten 1984, Terazawa 1989), which, if true, would have implications of greatest importance for laboratory physics, cosmology, the early universe, its evolution to the present day, and massive astrophysical objects (cf. Madsen & Haensel 1991). Unfortunately it seems unlikely that lattice QCD calculations will be accurate enough in the foreseeable future to give a definitive prediction on the absolute stability of strange matter, so that one is presently left with experiments and astrophysical studies (cf. -
Strange Quark Matter in Neutron Stars
Strange quark matter in neutron stars Prof. Mark Alford Washington University in St. Louis SQM 2013 Schematic QCD phase diagram T heavy ion collider QGP non−CFL hadronic = color− superconducting gas liq CFL quark matter nuclear compact star µ superfluid /supercond M. Alford, K. Rajagopal, T. Sch¨afer, A. Schmitt, arXiv:0709.4635 (RMP review) A. Schmitt, arXiv:1001.3294 (Springer Lecture Notes) Quark matter in compact stars Conventional scenario Strange Matter Hypothesis Bodmer 1971; Witten 1984; Farhi, Jaffe 1984 Neutron/hybrid star Strange star nuclear crust nuclear crust neutron NM star SQM SQM strangelet NM crust hybrid star SQM SQM Two scenarios for quark matter Conventional scenario Strange Matter Hypothesis Vac!NM!QM Vac!QM p QM NM p QM NM pcrit vac vac µ µcrit µ 310 MeV 310MeV µsqm Nuclear!quark matter transition Vacuum!quark matter transition at high pressure, (µcrit, pcrit) at µ = µsqm, p = 0. Strange quark matter (SQM) is the favored phase down to p = 0. Stars under the Strange Matter Hypothesis nuclear crust SQM SQM strangelet crust SQM Strangelet crust At zero pressure, if its surface tension is low enough, strange matter, like nuclear matter, will undergo charge separation and evaporation in to charged droplets. neutral −2 vacuum σcrit . 10 MeVfm e e Crust thickness neutral e e ∆R . 1 km SQM Alford, Eby, arXiv:0808.0671 neutral SQM Jaikumar, Reddy, Steiner, nucl-th/0507055 Charge separation: a generic feature charge−separated dΩ phase charge density ρ = Ω = dµe p neutral neutral vacuum SQM Neutral quark matter and µe neutral vacuum can coexist at zero pressure. -
Strange Jet Tagging
1 Strange Jet Tagging Yuichiro Nakai T. D. Lee Institute & Shanghai Jiao Tong U. Based on YN, D. Shih and S. Thomas, 2003.09517 [hep-ph]. Higgs and Flavor, EF02, Snowmass, August 2020 2 Jets at colliders Jet : collimated bunch of hadrons as the signatures of quarks and gluons produced in high-energy collisions ✓ QCD partons are never observed isolated due to confinement. ✓ They give cascades of radiation (parton shower) by QCD processes. ✓ Hadrons are formed at ∼ ΛQCD Understanding jets is a key ingredient of physics measurements and new physics searches at colliders. What initial parton produces a jet ? 3 Quark and Gluon Tagging Top quark Gluon S. Yang, talk slide More constituents with more uniform Jet mass, N-subjettiness, … energy fragmentation and wider. Bottom/Charm Up-type vs Down-type Look for a displaced pT -weighted jet charge (secondary) vertex. 1 Qi Q (p j )κ κ = jet κ ∑ j T (pT ) j∈jet Wikipedia The last missing piece : Strange quark tagging? 4 Tagging Strategy • Strange vs Gluon We can expect the same thing as quark/gluon discrimination. S. Yang, talk slide More constituents with more uniform • Strange vs Up energy fragmentation and wider. We can expect the same thing as up/down discrimination. pT -weighted jet charge 1 Qi = Q (p j )κ κ (p jet )κ ∑ j T • Strange vs Down T j∈jet Possible ?? Main theme of Both are quarks with the same charge. this talk 5 Tagging Strategy CMS experiment at the LHC Tracker : trajectories of charged particles ECAL : energy of electrons and photons HCAL : energy deposits of hadrons 6 Tagging Strategy