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NRP-3 the Effect of Beryllium Interaction with Fast Neutrons on the Reactivity of Etrr-2 Research Reactor
Seventh Conference of Nuclear Sciences & Applications 6-10 February 2000, Cairo, Egypt NRP-3 The Effect Of Beryllium Interaction With Fast Neutrons On the Reactivity Of Etrr-2 Research Reactor Moustafa Aziz and A.M. EL Messiry National Center for Nuclear Safety Atomic Energy Autho , Cairo , Egypt ABSTRACT The effect of beryllium interactions with fast neutrons is studied for Etrr_2 research reactors. Isotope build up inside beryllium blocks is calculated under different irradiation times. A new model for the Etrr_2 research reactor is designed using MCNP code to calculate the reactivity and flux change of the reactor due to beryllium poison. Key words: Research Reactors , Neutron Flux , Beryllium Blocks, Fast Neutrons and Reactivity INTRODUCTION Beryllium irradiated by fast neutrons with energies in the range 0.7-20 Mev undergoes (n,a) and (n,2n) reactions resulting in subsequent formation of the isotopes lithium (Li-6), tritium (H-3) and helium (He-3 and He-4 ). Beryllium interacts with fast neutrons to produce 6He that decay 6 6 ( T!/2 =0.8 s) to produce Li . Li interacts with neutron to produce tritium which suffer /? (T1/2 = 12.35 year) decay and converts to 3He which finally interact with neutron to produce tritium. These processes some times defined as Beryllium poison. Negative effect of this process are met whenever beryllium is used in a thermal reactor as a reflector or moderator . Because of their large thermal neutron absorption cross sections , the buildup of He-3 and Li-6 concentrations ,initiated by the Be(n,a) reaction , results in large negative reactivities which alter the reactivity , flux and power distributions. -
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. -
From Precision Physics to the Energy Frontier with the Compact Linear Collider
PERSPECTIVE | FOCUS https://doi.org/10.1038/s41567-020-0834-8PERSPECTIVE | FOCUS From precision physics to the energy frontier with the Compact Linear Collider Eva Sicking ✉ and Rickard Ström The Compact Linear Collider (CLIC) is a proposed high-luminosity collider that would collide electrons with their antiparticles, positrons, at energies ranging from a few hundred giga-electronvolts to a few tera-electronvolts. By covering a large energy range and by ultimately reaching collision energies in the multi-tera-electronvolts range, scientists at CLIC aim to improve the understanding of nature’s fundamental building blocks and to discover new particles or other physics phenomena. CLIC is an international project hosted by CERN with 75 institutes worldwide participating in the accelerator, detector and physics stud- ies. If commissioned, the first electron–positron collisions at CLIC are expected around 2035, following the high-luminosity phase of the Large Hadron Collider at CERN. Here we survey the principal merits of CLIC, and examine the opportunities that arise as a result of its design. We argue that CLIC represents an attractive proposition for the next-generation particle col- lider by combining an innovative accelerator technology, a realistic delivery timescale, and a physics programme that is highly complementary to existing accelerators, reaching uncharted territory. he discovery of the Higgs boson at the Large Hadron Collider to a lower event rate. These characteristics and the low duty cycle (LHC) in 20121,2 was an important milestone in high-energy of linear colliders make a trigger-less detector readout possible at Tphysics. It completes a puzzle that scientists have been work- CLIC. -
Hadron Collider Physics
KEK-PH Lectures and Workshops Hadron Collider Physics Zhen Liu University of Maryland 08/05/2020 Part I: Basics Part II: Advanced Topics Focus Collider Physics is a vast topic, one of the most systematically explored areas in particle physics, concerning many observational aspects in the microscopic world • Focus on important hadron collider concepts and representative examples • Details can be studied later when encounter References: Focus on basic pictures Barger & Philips, Collider Physics Pros: help build intuition Tao Han, TASI lecture, hep-ph/0508097 Tilman Plehn, TASI lecture, 0910.4182 Pros: easy to understand Maxim Perelstein, TASI lecture, 1002.0274 Cons: devils in the details Particle Data Group (PDG) and lots of good lectures (with details) from CTEQ summer schools Zhen Liu Hadron Collider Physics (lecture) KEK 2020 2 Part I: Basics The Large Hadron Collider Lyndon R Evans DOI:10.1098/rsta.2011.0453 Path to discovery 1995 1969 1974 1969 1979 1969 1800-1900 1977 2012 2000 1975 1983 1983 1937 1962 Electric field to accelerate 1897 1956 charged particles Synchrotron radiation 4 Zhen Liu Hadron Collider Physics (lecture) KEK 2020 4 Zhen Liu Hadron Collider Physics (lecture) KEK 2020 5 Why study (hadron) colliders (now)? • Leading tool in probing microscopic structure of nature • history of discovery • Currently running LHC • Great path forward • Precision QFT including strong dynamics and weakly coupled theories • Application to other physics probes • Set-up the basic knowledge to build other subfield of elementary particle physics Zhen Liu Hadron Collider Physics (lecture) KEK 2020 6 Basics: Experiment & Theory Zhen Liu Hadron Collider Physics (lecture) KEK 2020 7 Basics: How to make measurements? Zhen Liu Hadron Collider Physics (lecture) KEK 2020 8 Part I: Basics Basic Parameters Basics: Smashing Protons & Quick Estimates Proton Size ( ) Proton-Proton cross section ( ) Particle Physicists use the unit “Barn”2 1 = 100 The American idiom "couldn't hit the broad side of a barn" refers to someone whose aim is very bad. -
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]. -
Top Quark Physics in the Large Hadron Collider Era
Top Quark Physics in the Large Hadron Collider era Michael Russell Particle Physics Theory Group, School of Physics & Astronomy, University of Glasgow September 2017 arXiv:1709.10508v2 [hep-ph] 31 Jan 2018 A thesis submitted in fulfilment of the requirements for the degree of Doctor of Philosophy Abstract We explore various aspects of top quark phenomenology at the Large Hadron Collider and proposed future machines. After summarising the role of the top quark in the Standard Model (and some of its well-known extensions), we discuss the formulation of the Standard Model as a low energy effective theory. We isolate the sector of this effective theory that pertains to the top quark and that can be probed with top observables at hadron colliders, and present a global fit of this sector to currently available data from the LHC and Tevatron. Various directions for future improvement are sketched, including analysing the potential of boosted observables and future colliders, and we highlight the importance of using complementary information from different colliders. Interpretational issues related to the validity of the effective field theory formulation are elucidated throughout. Finally, we present an application of artificial neural network algorithms to identifying highly- boosted top quark events at the LHC, and comment on further refinements of our analysis that can be made. 2 Acknowledgements First and foremost I must thank my supervisors, Chris White and Christoph Englert, for their endless support, inspiration and encouragement throughout my PhD. They always gave me enough freedom to mature as a researcher, whilst providing the occasional neces- sary nudge to keep me on the right track. -
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 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. -
HEPAP Looks Into the Future
Volume 20 Friday, August 29, 1997 Number 17 f INSIDE HEPAP Looks into 2 HEPAP: Voice of the Community the Future 5 Profiles in HEPAP subpanel meets at Fermilab to chart the future of Particle Physics: high-energy physics in the U.S. Dave McGinnis by Donald Sena and Sharon Butler, Office of Public Affairs 6 Barns of Fermilab Charged with recommending how best to In a letter to HEPAP, Martha Krebs, position the U.S. particle physics community Director of the U.S. Department of Energy’s for new facilities beyond CERN’s Large Office of Energy Research, directed the Hadron Collider, a subpanel of the High- subpanel to “recommend a scenario for an Energy Physics Advisory Panel met at Fermilab optimal and balanced U.S. high-energy physics August 14-16 to hear presentations on such program over the next decade,” with “new topics as the research agenda for Fermilab’s facilities to address physics opportunities Run II, the complicated upgrades to the CDF beyond the LHC.” She asked the subpanel and DZero detectors and research on future to consider a future course in light of three accelerators. continued on page 3 Photo by Reidar Hahn Dixon Bogert, deputy project manager for the Main Injector, leads a tour for HEPAP subpanel members and DOE officials. HEPAP: Voice of the Community by Donald Sena and Sharon Butler, Office of Public Affairs The High-Energy Physics Advisory In 1983, for example, a HEPAP According to Fermilab physicist Cathy Panel traces its history to the 1960s, subpanel recommended terminating Newman-Holmes, outgoing member of when -
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. -
Searches for a Charged Higgs Boson in ATLAS and Development of Novel Technology for Future Particle Detector Systems
Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 1222 Searches for a Charged Higgs Boson in ATLAS and Development of Novel Technology for Future Particle Detector Systems DANIEL PELIKAN ACTA UNIVERSITATIS UPSALIENSIS ISSN 1651-6214 ISBN 978-91-554-9153-6 UPPSALA urn:nbn:se:uu:diva-242491 2015 Dissertation presented at Uppsala University to be publicly examined in Polhemssalen, Ångströmlaboratoriet, Lägerhyddsvägen 1, Uppsala, Friday, 20 March 2015 at 10:00 for the degree of Doctor of Philosophy. The examination will be conducted in English. Faculty examiner: Prof. Dr. Fabrizio Palla (Istituto Nazionale di Fisica Nucleare (INFN) Pisa). Abstract Pelikan, D. 2015. Searches for a Charged Higgs Boson in ATLAS and Development of Novel Technology for Future Particle Detector Systems. Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 1222. 119 pp. Uppsala: Acta Universitatis Upsaliensis. ISBN 978-91-554-9153-6. The discovery of a charged Higgs boson (H±) would be a clear indication for physics beyond the Standard Model. This thesis describes searches for charged Higgs bosons with the ATLAS experiment at CERN’s Large Hadron Collider (LHC). The first data collected during the LHC Run 1 is analysed, searching for a light charged Higgs boson (mH±<mtop), which decays predominantly into a tau-lepton and a neutrino. Different final states with one or two leptons (electrons or muons), as well as leptonically or hadronically decaying taus, are studied, and exclusion limits are set. The background arising from misidentified non-prompt electrons and muons was estimated from data. This so-called "Matrix Method'' exploits the difference in the lepton identification between real, prompt, and misidentified or non-prompt electrons and muons.