Electron-Ion Collider Science
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The Large Hadron Collider Lyndon Evans CERN – European Organization for Nuclear Research, Geneva, Switzerland
34th SLAC Summer Institute On Particle Physics (SSI 2006), July 17-28, 2006 The Large Hadron Collider Lyndon Evans CERN – European Organization for Nuclear Research, Geneva, Switzerland 1. INTRODUCTION The Large Hadron Collider (LHC) at CERN is now in its final installation and commissioning phase. It is a two-ring superconducting proton-proton collider housed in the 27 km tunnel previously constructed for the Large Electron Positron collider (LEP). It is designed to provide proton-proton collisions with unprecedented luminosity (1034cm-2.s-1) and a centre-of-mass energy of 14 TeV for the study of rare events such as the production of the Higgs particle if it exists. In order to reach the required energy in the existing tunnel, the dipoles must operate at 1.9 K in superfluid helium. In addition to p-p operation, the LHC will be able to collide heavy nuclei (Pb-Pb) with a centre-of-mass energy of 1150 TeV (2.76 TeV/u and 7 TeV per charge). By modifying the existing obsolete antiproton ring (LEAR) into an ion accumulator (LEIR) in which electron cooling is applied, the luminosity can reach 1027cm-2.s-1. The LHC presents many innovative features and a number of challenges which push the art of safely manipulating intense proton beams to extreme limits. The beams are injected into the LHC from the existing Super Proton Synchrotron (SPS) at an energy of 450 GeV. After the two rings are filled, the machine is ramped to its nominal energy of 7 TeV over about 28 minutes. In order to reach this energy, the dipole field must reach the unprecedented level for accelerator magnets of 8.3 T. -
The INT @ 20 the Future of Nuclear Physics and Its Intersections July 1 – 2, 2010
The INT @ 20 The Future of Nuclear Physics and its Intersections July 1 – 2, 2010 Program Thursday, July 1: 8:00 – 8:45: Registration (Kane Hall, Rom 210) 8:45 – 9:00: Opening remarks Mary Lidstrom, Vice Provost for Research, University of Washington David Kaplan, INT Director Session chair: David Kaplan 9:00 – 9:45: Science & Society 9:00 – 9:45 Steven Koonin, Undersecretary for Science, DOE The future of DOE and its intersections 9:45 – 10:30: Strong Interactions and Fundamental Symmetries 9:45 – 10:30 Howard Georgi, Harvard University QCD – From flavor SU(3) to effective field theory 10:30 – 11:00: Coffee Break Session chair: Martin Savage 11:00 – 11:30 Silas Beane, University of New Hampsire Lattice QCD for nuclear physics 11:30 – 12:00 Paulo Bedaque, University of Maryland Effective field theories in nuclear physics 12:00 – 12:30 Michael Ramsey-Musolf, University of Wisconsin Fundamental symmetries of nuclear physics: A window on the early Universe 12:30 – 2:00: Lunch (Mary Gates Hall) 1 Thursday, July 1 2:00 – 5:00: From Partons to Extreme Matter Session chair: Gerald Miller 2:00 – 2:30 Matthias Burkardt, New Mexico State University Transverse (spin) structure of hadrons 2:30 – 3:00 Barbara Jacak, SUNY Stony Brook Quark-gluon plasma: from particles to fields? 3:00 – 3:45 Raju Venugopalan, Brookhaven National Lab Wee gluons and their role in creating the hottest matter on Earth 3:45 – 4:15: Coffee Break Session chair: Krishna Rajagopal 4:15 – 4:45 Jean-Paul Blaizot, Saclay Is the quark-gluon plasma strongly or weakly coupled? 4:45 -
Tevatron Accelerator Physics and Operation Highlights A
FERMILAB-CONF-11-129-APC TEVATRON ACCELERATOR PHYSICS AND OPERATION HIGHLIGHTS A. Valishev for the Tevatron group, FNAL, Batavia, IL 60510, U.S.A. Abstract Table 1: Integrated luminosity performance by fiscal year. The performance of the Tevatron collider demonstrated FY07 FY08 FY09 FY10 continuous growth over the course of Run II, with the peak luminosity reaching 4×1032 cm-2 s-1, and the weekly Total integral (fb-1) 1.3 1.8 1.9 2.47 -1 integration rate exceeding 70 pb . This report presents a review of the most important advances that contributed to Until the middle of calendar year 2009, the luminosity this performance improvement, including beam dynamics growth was dominated by improvements of the antiproton modeling, precision optics measurements and stability production rate [2], which remains stable since. control, implementation of collimation during low-beta Performance improvements over the last two years squeeze. Algorithms employed for optimization of the became possible because of implementation of a few luminosity integration are presented and the lessons operational changes, described in the following section. learned from high-luminosity operation are discussed. Studies of novel accelerator physics concepts at the Tevatron are described, such as the collimation techniques using crystal collimator and hollow electron beam, and compensation of beam-beam effects. COLLIDER RUN II PERFORMANCE Tevatron collider Run II with proton-antiproton collisions at the center of mass energy of 1.96 TeV started in March 2001. Since then, 10.5 fb-1 of integrated luminosity has been delivered to CDF and D0 experiments (Fig. 1). All major technical upgrades of the accelerator complex were completed by 2007 [1]. -
MIT at the Large Hadron Collider—Illuminating the High-Energy Frontier
Mit at the large hadron collider—Illuminating the high-energy frontier 40 ) roland | klute mit physics annual 2010 gunther roland and Markus Klute ver the last few decades, teams of physicists and engineers O all over the globe have worked on the components for one of the most complex machines ever built: the Large Hadron Collider (LHC) at the CERN laboratory in Geneva, Switzerland. Collaborations of thousands of scientists have assembled the giant particle detectors used to examine collisions of protons and nuclei at energies never before achieved in a labo- ratory. After initial tests proved successful in late 2009, the LHC physics program was launched in March 2010. Now the race is on to fulfill the LHC’s paradoxical mission: to complete the Stan- dard Model of particle physics by detecting its last missing piece, the Higgs boson, and to discover the building blocks of a more complete theory of nature to finally replace the Standard Model. The MIT team working on the Compact Muon Solenoid (CMS) experiment at the LHC stands at the forefront of this new era of particle and nuclear physics. The High Energy Frontier Our current understanding of the fundamental interactions of nature is encap- sulated in the Standard Model of particle physics. In this theory, the multitude of subatomic particles is explained in terms of just two kinds of basic building blocks: quarks, which form protons and neutrons, and leptons, including the electron and its heavier cousins. From the three basic interactions described by the Standard Model—the strong, electroweak and gravitational forces—arise much of our understanding of the world around us, from the formation of matter in the early universe, to the energy production in the Sun, and the stability of atoms and mit physics annual 2010 roland | klute ( 41 figure 1 A photograph of the interior, central molecules. -
The Nucleus As a Qcd Laboratory: Hadronization, 3D Tomography, and More
EINN 2017 NOVEMBER 1, 2017 PAPHOS, CYPRUS THE NUCLEUS AS A QCD LABORATORY: HADRONIZATION, 3D TOMOGRAPHY, AND MORE erhtjhtyhy KAWTAR HAFIDI Argonne National Laboratory is a U.S. Department of Energy laboratory managed by UChicago Argonne, LLC. OUTLINE § The nucleus from a QCD perspective – Important questions to be addressed by current and future facilities § Hadronization: How do quarks hadronize into hadrons? – What did we learn from previous measurements? – Anticipated measurement at JLab and the future EIC § 3D tomography of nuclei – First attempt – Ambitious program at JLab and great potential for the EIC § Summary and outlook STUDYING NUCLEI FROM QCD PERSPECTIVE § How do an energetic quark interact with the nuclear medium and subsequently neutralize its color and become confined inside a hadron? § How are quarks and gluons distributed in space and momentum inside the nucleus? § How are quarks and gluons distributions affected when they are embedded in nuclei compared to free nucleons? § How these fundamental degrees of freedom of the strong interaction group themselves together to form nuclei and ultimately matter? THE NUCLEUS AS A QCD LABORATORY electron electron Probe Medium Medium "QCD medium" "QCD vacuum" Probe Ø Studying the structure of the nucleus Ø Using the nucleus as a femtometer itself: EMC, SRC, 3D tomography detector to study hadronization, CT,.. HOW DO ENERGETIC QUARKS BECOME HADRONS? Hadronization is a direct manifestation of confinement SPACE TIME DYNAMICS OF HADRONIZATION Nuclei are used as detectors providing multiple -
The Compact Linear E E− Collider (CLIC): Physics Potential
+ The Compact Linear e e− Collider (CLIC): Physics Potential Input to the European Particle Physics Strategy Update on behalf of the CLIC and CLICdp Collaborations 18 December 2018 1) Contact person: P. Roloff ∗ †‡ §¶ Editors: R. Franceschini , P. Roloff∗, U. Schnoor∗, A. Wulzer∗ † ‡ ∗ CERN, Geneva, Switzerland, Università degli Studi Roma Tre, Rome, Italy, INFN, Sezione di Roma Tre, Rome, Italy, § Università di Padova, Padova, Italy, ¶ LPTP, EPFL, Lausanne, Switzerland Abstract + The Compact Linear Collider, CLIC, is a proposed e e− collider at the TeV scale whose physics poten- tial ranges from high-precision measurements to extensive direct sensitivity to physics beyond the Standard Model. This document summarises the physics potential of CLIC, obtained in detailed studies, many based on full simulation of the CLIC detector. CLIC covers one order of magnitude of centre-of-mass energies from 350 GeV to 3 TeV, giving access to large event samples for a variety of SM processes, many of them for the + first time in e e− collisions or for the first time at all. The high collision energy combined with the large + luminosity and clean environment of the e e− collisions enables the measurement of the properties of Stand- ard Model particles, such as the Higgs boson and the top quark, with unparalleled precision. CLIC might also discover indirect effects of very heavy new physics by probing the parameters of the Standard Model Effective Field Theory with an unprecedented level of precision. The direct and indirect reach of CLIC to physics beyond the Standard Model significantly exceeds that of the HL-LHC. This includes new particles detected in challenging non-standard signatures. -
The ATLAS Detector: a General Purpose Experiment at the Large Hadron Collider at CERN
FR9806097 The ATLAS detector: a general purpose experiment at the Large Hadron Collider at CERN J. Schwindling CEA, DSM/DAPNIA, CE Saclay, 91191 Gif sur Yvette, France 1 Introduction The ATLAS collaboration has designed a general purpose detector to be operated at the Large Hadron Collider (LHC) at CERN [1]. The design of the detector took into account the requirements from the physics and the constraints from the collider, but also the cost and technological aspects. It is supported by a large amount of detailed simulations and test activities. The performances which are required to meet the physics goals are the following: - The search for Higgs bosons through their decays into two photons or four elec- trons requires a good electromagnetic calorimetry. - The search for Higgs bosons decaying into four muons requires a robust muon system. - Supersymmetric particles often decay into an invisible neutralino plus other parti- cles, leading to a missing energy signature which can be measured with an hermetic detector. - The measurement of the top quark mass requires a good measurement of jets. - b quark and r lepton identification requires the precise measurement of secondary vertices. The ATLAS detector is shown in figure 1. It covers a large fraction of the 4n angle, offers robust and redundant physics measurements and allows for triggering at low PT (about 10 GeV) thresholds. In order to achieve the design LHC luminosity of 1034 cm"2 s"1, the bunch spacing will be only 25 ns, leading to about 20 minimum bias events ("pile-up") and about 1000 charged tracks produced at each bunch crossing. -
Scaling Behavior of Circular Colliders Dominated by Synchrotron Radiation
SCALING BEHAVIOR OF CIRCULAR COLLIDERS DOMINATED BY SYNCHROTRON RADIATION Richard Talman Laboratory for Elementary-Particle Physics Cornell University White Paper at the 2015 IAS Program on the Future of High Energy Physics Abstract time scales measured in minutes, for example causing the The scaling formulas in this paper—many of which in- beams to be flattened, wider than they are high [1] [2] [3]. volve approximation—apply primarily to electron colliders In this regime scaling relations previously valid only for like CEPC or FCC-ee. The more abstract “radiation dom- electrons will be applicable also to protons. inated” phrase in the title is intended to encourage use of This paper concentrates primarily on establishing scaling the formulas—though admittedly less precisely—to proton laws that are fully accurate for a Higgs factory such as CepC. colliders like SPPC, for which synchrotron radiation begins Dominating everything is the synchrotron radiation formula to dominate the design in spite of the large proton mass. E4 Optimizing a facility having an electron-positron Higgs ∆E / ; (1) R factory, followed decades later by a p,p collider in the same tunnel, is a formidable task. The CepC design study con- stitutes an initial “constrained parameter” collider design. relating energy loss per turn ∆E, particle energy E and bend 1 Here the constrained parameters include tunnel circumfer- radius R. This is the main formula governing tunnel ence, cell lengths, phase advance per cell, etc. This approach circumference for CepC because increasing R decreases is valuable, if the constrained parameters are self-consistent ∆E. and close to optimal. -
Compact Linear Collider (CLIC)
Compact Linear Collider (CLIC) Philip Burrows John Adams Institute Oxford University 1 Outline • Introduction • Linear colliders + CLIC • CLIC project status • 5-year R&D programme + technical goals • Applications of CLIC technologies 2 Large Hadron Collider (LHC) Largest, highest-energy particle collider CERN, Geneva 3 CERN accelerator complex 4 CLIC vision • A proposed LINEAR collider of electrons and positrons • Designed to reach VERY high energies in the electron-positron annihilations: 3 TeV = 3 000 000 000 000 eV • Ideal for producing new heavy particles of matter, such as SUSY particles, in clean conditions 5 CLIC vision • A proposed LINEAR collider of electrons and positrons • Designed to reach VERY high energies in the electron-positron annihilations: 3 TeV = 3 000 000 000 000 eV • Ideal for producing new heavy particles of matter, such as SUSY particles, in clean conditions … should they be discovered at LHC! 6 CLIC Layout: 3 TeV Drive Beam Generation Complex Main Beam Generation Complex 7 CLIC energy staging • An energy-staging strategy is being developed: ~ 500 GeV 1.5 TeV 3 TeV (and realistic for implementation) • The start-up energy would allow for a Higgs boson and top-quark factory 8 2013 Nobel Prize in Physics 9 e+e- Higgs boson factory e+e- annihilations: E > 91 + 125 = 216 GeV E ~ 250 GeV E > 91 + 250 = 341 GeV E ~ 500 GeV European PP Strategy (2013) High-priority large-scale scientific activities: LHC + High Lumi-LHC Post-LHC accelerator at CERN International Linear Collider Neutrinos 11 International Linear Collider (ILC) c. 250 GeV / beam 31 km 12 Kitakami Site 13 ILC Kitakami Site: IP region 14 Global Linear Collider Collaboration 15 European PP Strategy (2013) CERN should undertake design studies for accelerator projects in a global context, with emphasis on proton-proton and electron-positron high energy frontier machines. -
January 2021 Newsletter
APS Division of In this issue Astrophysics • April Meeting Online • Upcoming DAP election alert Electronic Newsletter January 2021 • APS Fellows • Bethe Prize Winner • Student/Postdoc Travel Grants • April Meeting: DAP and Plenary Programs & Abstract Categories • Snowmass Update APS DAP Officers 2020–2021: Finalize your plans now to attend the April 2021 meeting held virtually this year. A • Chair: Glennys Farrar number of plenary and invited sessions will • Past Chair: Joshua Frieman feature presentations by DAP members. Here are the key details: • Chair Elect: Chris Fryer • Vice Chair: Daniel Holz What: April 2021 APS Meeting • Secretary/Treasurer: Judith Racusin When: April 17 - 20, 2021 • Deputy Sec./Treasurer: Amy Furniss Where: Online Abstract Deadline: Jan 8, 2021, 5 pm EST • Division Councilor: Cole Miller Travel Grant Deadline: Jan 31, 2021 • Member-at-Large: Stefano Profumo Early Registration Deadline: Feb 26, 2021 • Member-at-Large: Ignacio Taboada Late Registration Deadline: Mar 26, 2021 • Member-at-Large: Erin Kara • Member-at-Large: Laura Blecha The 2021 April Meeting will be virtual. Questions? Comments? Detailed information for the meeting, including details on registration and the scientific Newsletter editors: program can be found online at https://april.aps.org/ Amy Furniss [email protected] HEADS-UP: The ELECTION for next year’s DAP Executive Committee and chairline will Judith Racusin be held soon. Be on the lookout for the [email protected] announcement from APS, and please vote! 1 Dear DAP, Please see the January 2021 DAP newsletter below. It will be archived on the DAP website (https://www.aps.org/units/dap/newsletters/index.cfm). -
B1487(01)Quarks FM.I-Xvi
Connecting Quarks with the Cosmos Eleven Science Questions for the New Century Committee on the Physics of the Universe Board on Physics and Astronomy Division on Engineering and Physical Sciences THE NATIONAL ACADEMIES PRESS Washington, D.C. www.nap.edu THE NATIONAL ACADEMIES PRESS 500 Fifth Street, N.W. Washington, DC 20001 NOTICE: The project that is the subject of this report was approved by the Govern- ing Board of the National Research Council, whose members are drawn from the councils of the National Academy of Sciences, the National Academy of Engineer- ing, and the Institute of Medicine. The members of the committee responsible for the report were chosen for their special competences and with regard for appropriate balance. This project was supported by Grant No. DE-FG02-00ER41141 between the Na- tional Academy of Sciences and the Department of Energy, Grant No. NAG5-9268 between the National Academy of Sciences and the National Aeronautics and Space Administration, and Grant No. PHY-0079915 between the National Academy of Sciences and the National Science Foundation. Any opinions, findings, and conclu- sions or recommendations expressed in this publication are those of the author(s) and do not necessarily reflect the views of the organizations or agencies that pro- vided support for the project. International Standard Book Number 0-309-07406-1 Library of Congress Control Number 2003100888 Additional copies of this report are available from the National Academies Press, 500 Fifth Street, N.W., Lockbox 285, Washington, DC 20055; (800) 624-6242 or (202) 334-3313 (in the Washington metropolitan area); Internet, http://www.nap.edu and Board on Physics and Astronomy, National Research Council, NA 922, 500 Fifth Street, N.W., Washington, DC 20001; Internet, http://www.national-academies.org/bpa. -
Renormalization Group for One Dimensional Ising Model Masatsugu Sei Suzuki, Department of Physics, SUNY at Binghamton (Date: December 04, 2016)
Renormalization group for one dimensional Ising model Masatsugu Sei Suzuki, Department of Physics, SUNY at Binghamton (Date: December 04, 2016) Kenneth Geddes Wilson (June 8, 1936 – June 15, 2013) was an American theoretical physicist and a pioneer in leveraging computers for studying particle physics. He was awarded the 1982 Nobel Prize in Physics for his work on phase transitions—illuminating the subtle essence of phenomena like melting ice and emerging magnetism. It was embodied in his fundamental work on the renormalization group. https://en.wikipedia.org/wiki/Kenneth_G._Wilson Here we discuss the renormalization group (RG) for the simplest possible example- the one- dimensional Ising model. The results of the RG calculations are compared with the exact calculations of the correlation functions and the free energy of the one-dimensional Ising model; the temperature T = 0 can be treated as a second-order critical point. ______________________________________________________________________________ Leo Philip Kadanoff: Kadanoff was born in 1937 and spent his early life in New York City. He received his PhD from Harvard in 1960 and was a postdoctoral researcher at the Niels Bohr Institute in Copenhagen until he moved to the University of Illinois in 1962. His work there concerned the development of many-body theory techniques, culminating in a short but highly influential monograph with Gordon Baym, which is still widely used today. Kadanoff found himself, in the mid- 1960s, working on the problem of phase transitions. It had been known since the work of Lev Landau in 1937 that second-order phase transitions would exhibit power-law singularities or divergences as the temperature approached the critical point.