Modern and Future Colliders
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CERN Courier–Digital Edition
CERNMarch/April 2021 cerncourier.com COURIERReporting on international high-energy physics WELCOME CERN Courier – digital edition Welcome to the digital edition of the March/April 2021 issue of CERN Courier. Hadron colliders have contributed to a golden era of discovery in high-energy physics, hosting experiments that have enabled physicists to unearth the cornerstones of the Standard Model. This success story began 50 years ago with CERN’s Intersecting Storage Rings (featured on the cover of this issue) and culminated in the Large Hadron Collider (p38) – which has spawned thousands of papers in its first 10 years of operations alone (p47). It also bodes well for a potential future circular collider at CERN operating at a centre-of-mass energy of at least 100 TeV, a feasibility study for which is now in full swing. Even hadron colliders have their limits, however. To explore possible new physics at the highest energy scales, physicists are mounting a series of experiments to search for very weakly interacting “slim” particles that arise from extensions in the Standard Model (p25). Also celebrating a golden anniversary this year is the Institute for Nuclear Research in Moscow (p33), while, elsewhere in this issue: quantum sensors HADRON COLLIDERS target gravitational waves (p10); X-rays go behind the scenes of supernova 50 years of discovery 1987A (p12); a high-performance computing collaboration forms to handle the big-physics data onslaught (p22); Steven Weinberg talks about his latest work (p51); and much more. To sign up to the new-issue alert, please visit: http://comms.iop.org/k/iop/cerncourier To subscribe to the magazine, please visit: https://cerncourier.com/p/about-cern-courier EDITOR: MATTHEW CHALMERS, CERN DIGITAL EDITION CREATED BY IOP PUBLISHING ATLAS spots rare Higgs decay Weinberg on effective field theory Hunting for WISPs CCMarApr21_Cover_v1.indd 1 12/02/2021 09:24 CERNCOURIER www. -
Slides Lecture 1
Advanced Topics in Particle Physics Probing the High Energy Frontier at the LHC Ulrich Husemann, Klaus Reygers, Ulrich Uwer University of Heidelberg Winter Semester 2009/2010 CERN = European Laboratory for Partice Physics the world’s largest particle physics laboratory, founded 1954 Historic name: “Conseil Européen pour la Recherche Nucléaire” Lake Geneva Proton-proton2500 employees, collider almost 10000 guest scientists from 85 nations Jura Mountains 8.5 km Accelerator complex Prévessin site (approx. 100 m underground) (France) Meyrin site (Switzerland) Probing the High Energy Frontier at the LHC, U Heidelberg, Winter Semester 09/10, Lecture 1 2 Large Hadron Collider: CMS Experiment: Proton-Proton and Multi Purpose Detector Lead-Lead Collisions LHCb Experiment: B Physics and CP Violation ALICE-Experiment: ATLAS Experiment: Heavy Ion Physics Multi Purpose Detector Probing the High Energy Frontier at the LHC, U Heidelberg, Winter Semester 09/10, Lecture 1 3 The Lecture “Probing the High Energy Frontier at the LHC” Large Hadron Collider (LHC) at CERN: premier address in experimental particle physics for the next 10+ years LHC restart this fall: first beam scheduled for mid-November LHC and Heidelberg Experimental groups from Heidelberg participate in three out of four large LHC experiments (ALICE, ATLAS, LHCb) Theory groups working on LHC physics → Cornerstone of physics research in Heidelberg → Lots of exciting opportunities for young people Probing the High Energy Frontier at the LHC, U Heidelberg, Winter Semester 09/10, Lecture 1 4 Scope -
Status in 2020 and Request for Beamtime in 2021 for CERN NA63
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH June 2nd 2020 Status in 2020 and request for beamtime in 2021 for CERN NA63 C.F. Nielsen, M.B. Sørensen, A.H. Sørensen and U.I. Uggerhøj Department of Physics and Astronomy, Aarhus University, Denmark T.N. Wistisen and A. Di Piazza Max Planck Institute for Nuclear Physics, Heidelberg, Germany R. Holtzapple California Polytechnic State University, San Luis Obispo, USA NA63 Abstract In the NA63 experiment of April 2018 reliable data was taken for 40 and 80 GeV electrons and positrons aligned to the h100i axis of a diamond crystal of thickness 1.5 mm, as well as for 40 and 80 GeV electrons on a 1.0 mm thick diamond aligned to the h100i axis. A paper has been submitted to Phys. Rev. D, and has received favourable referee comments. For the 2017 data, a paper has been published in Phys. Rev. Research in 2019, and our experimental findings have inspired another paper published in Phys. Rev. Lett. For the year 2021 we request 2 weeks of beamtime in the SPS H4 to do a measurement of trident production, e− → e−e+e−, in strong crystalline fields. This process is closely related to the production of muon pairs, e− → e−µ+µ−, and single crystals may prove to be an attractive source to obtain muons of high intensity and small emittance, as required for a muon collider. The trident results obtained in 2009, and published in 2010, are strongly at odds with theory (factor 3-4 discrepancy). Since then we have acquired and have been using MIMOSA-26 position-sensitive detectors with a resolution about a factor 40 higher than the drift chambers used in 2009, and now with true multi-hit capability, a significant advantage when looking for trident events. -
Arxiv:2001.07837V2 [Hep-Ex] 4 Jul 2020 Scale Funding Will Be Requested at Different Stages Across the Globe
Brazilian Participation in the Next-Generation Collider Experiments W. L. Aldá Júniora C. A. Bernardesb D. De Jesus Damiãoa M. Donadellic D. E. Martinsd G. Gil da Silveirae;a C. Henself H. Malbouissona A. Massafferrif E. M. da Costaa C. Mora Herreraa I. Nastevad M. Rangeld P. Rebello Telesa T. R. F. P. Tomeib A. Vilela Pereiraa aDepartamento de Física Nuclear e Altas Energias, Universidade do Estado do Rio de Janeiro (UERJ), Rua São Francisco Xavier, 524, CEP 20550-900, Rio de Janeiro, Brazil bUniversidade Estadual Paulista (Unesp), Núcleo de Computação Científica Rua Dr. Bento Teobaldo Ferraz, 271, 01140-070, Sao Paulo, Brazil cInstituto de Física, Universidade de São Paulo (USP), Rua do Matão, 1371, CEP 05508-090, São Paulo, Brazil dUniversidade Federal do Rio de Janeiro (UFRJ), Instituto de Física, Caixa Postal 68528, 21941-972 Rio de Janeiro, Brazil eInstituto de Física, Universidade Federal do Rio Grande do Sul , Av. Bento Gonçalves, 9550, CEP 91501-970, Caixa Postal 15051, Porto Alegre, Brazil f Centro Brasileiro de Pesquisas Físicas (CBPF), Rua Dr. Xavier Sigaud, 150, CEP 22290-180 Rio de Janeiro, RJ, Brazil E-mail: [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected] Abstract: This proposal concerns the participation of the Brazilian High-Energy Physics community in the next-generation collider experiments. -
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. -
Mayda M. VELASCO Northwestern University, Dept. of Physics And
Mayda M. VELASCO Northwestern University, Dept. of Physics and Astronomy 2145 Sheridan Road, Evanston, IL 60208, USA Phone: Work: +1 847 467 7099 Cell: +1 847 571 3461 E-mail: [email protected] Last Updated: May 2016 Research Interest { High Energy Experimental Elementary Particle Physics: Work toward the understanding of fundamental interactions and its important role in: (a) solving the problem of CP violation in the Universe { Why is there more matter than anti- matter?; (b) explaning how mass is generated { Higgs mechanism and (c) finding the particle nature of Dark-Matter, if any... The required \new" physics phenomena is accessible at the Large Hadron Collider (LHC) at the European Organization for Nuclear Research (CERN). I am an active member of the Compact Muon Solenoid (CMS) collaboration already collect- ing data at the LHC, that led to the discovery of the Higgs boson or \God particle" in 2012. Education: • Ph.D. 1995: Northwestern University (NU) Experimental Particle Physics • 1995: Sicily, Italy ERICE: Spin Structure of Nucleon • 1994: Sorento, Italy CERN Summer School • B.S. 1988: University of Puerto Rico (UPR) Physics (Major) and Math (Minor) Rio Piedras Campus Fellowships and Honors: • 2015: NU, The Graduate School (TGS) Dean's Faculty Award for Diversity. • 2008-09: Paid leave of absence sponsored by US Department of Energy (DOE). • 2002-04: Sloan Research Fellow from Sloan Foundation. • 2002-03: Woodrow Wilson Fellow from Mellon Foundation. • 1999: CERN Achievement Award { Post-doctoral. • 1996-98: CERN Fellowship with Experimental Physics Division { Post-doctoral. • 1989-1995: Fermi National Accelerator Laboratory(FNAL)/URA Fellow { Doctoral. -
Highlights from ALICE
Highlights from ALICE Michael Weber for the ALICE Collaboration Quark Matter, Wuhan, 04-09 Nov 2019 Michael Weber (SMI) Opening the doors (December 2018) CERN-PHOTO-201812-335 2 Quark Matter, Wuhan, 04-09 Nov 2019 Michael Weber (SMI) Soon after CERN-PHOTO-201903-053 Quark Matter, Wuhan, 04-09 Nov 2019 Michael Weber (SMI) 3 Harvest of the past ten years Recorded L System Year(s) √s (TeV) int NN (for muon triggers) 2010,2011 2.76 ~75 μb-1 Pb–Pb 2015 5.02 ~0.25 nb-1 2018 5.02 ~0.55 nb-1 Xe–Xe 2017 5.44 ~0.3 μb-1 2013 5.02 ~15 nb-1 p–Pb 2016 5.02, 8.16 ~3 nb-1; ~25 nb-1 New for QM 2019: ~200 μb-1; ~100 nb-1; 2009-2013 0.9,2.76,7,8 ~1.5 pb-1; ~2.5 pb-1 ● Full 13 TeV pp data set with high-multiplicity triggers pp ● 2018 Pb-Pb with central and semi-central triggers 2015,2017 5.02 ~1.3 pb-1 ● Selected results out of 26 parallel talks, 2015-2018 13 ~36 pb-1 68 posters, and 18 new papers Labels used in this presentation: New since last QM New New preliminary for QM Final On arXiv for QM Quark Matter, Wuhan, 04-09 Nov 2019 Michael Weber (SMI) 4 Outline Initial state → Hadronic structure and photoproduction QGP - Macroscopic properties → Properties of QCD matter and the transition between phases QGP - Microscopic dynamics → Degrees of freedom at each stage and their interactions Small systems → Unified picture of QCD particle production from small to larger systems Hadron physics → LHC as laboratory for hadron interaction studies Following the open questions in the HL-LHC WG5 yellow report Quark Matter, Wuhan, 04-09 Nov 2019 Michael Weber (SMI) 5 ALICE parallel talks Initial state ● Low-mass dielectron measurements in pp, p-Pb and Pb-Pb collisions with ALICE at the LHC S. -
Heavy-Ion Collisions at the Dawn of the Large Hadron Collider Era
Heavy-Ion Collisions at the Dawn of the Large Hadron Collider Era J. Takahashi Universidade Estadual de Campinas, São Paulo, Brazil Abstract In this paper I present a review of the main topics associated with the study of heavy-ion collisions, intended for students starting or interested in the field. It is impossible to summarize in a few pages the large amount of information that is available today, after a decade of operations of the Relativistic Heavy Ion Collider and the beginning of operations at the Large Hadron Collider. Thus, I had to choose some of the results and theories in order to present the main ideas and goals. All results presented here are from publicly available references, but some of the discussions and opinions are my personal view, where I have made that clear in the text. 1 Introduction In this very exciting field of science, we use particle accelerators to collide heavy ions such as lead or gold nuclei, instead of colliding single protons or electrons. By doing so, we produce a much more violent collision in which a large number of particles are created and a considerable amount of energy is deposited in a volume bigger than the size of a single proton. As a result, a highly excited state of matter is created, and this state can have characteristics different from those of regular hadronic matter. It is postulated that, if the energy density is high enough, the system formed will be in a state where quarks and gluons are no longer confined into hadrons and thus exhibit partonic degrees of freedom [1,2]. -
NA61/SHINE Facility at the CERN SPS: Beams and Detector System
Preprint typeset in JINST style - HYPER VERSION NA61/SHINE facility at the CERN SPS: beams and detector system N. Abgrall11, O. Andreeva16, A. Aduszkiewicz23, Y. Ali6, T. Anticic26, N. Antoniou1, B. Baatar7, F. Bay27, A. Blondel11, J. Blumer13, M. Bogomilov19, M. Bogusz24, A. Bravar11, J. Brzychczyk6, S. A. Bunyatov7, P. Christakoglou1, T. Czopowicz24, N. Davis1, S. Debieux11, H. Dembinski13, F. Diakonos1, S. Di Luise27, W. Dominik23, T. Drozhzhova20 J. Dumarchez18, K. Dynowski24, R. Engel13, I. Efthymiopoulos10, A. Ereditato4, A. Fabich10, G. A. Feofilov20, Z. Fodor5, A. Fulop5, M. Ga´zdzicki9;15, M. Golubeva16, K. Grebieszkow24, A. Grzeszczuk14, F. Guber16, A. Haesler11, T. Hasegawa21, M. Hierholzer4, R. Idczak25, S. Igolkin20, A. Ivashkin16, D. Jokovic2, K. Kadija26, A. Kapoyannis1, E. Kaptur14, D. Kielczewska23, M. Kirejczyk23, J. Kisiel14, T. Kiss5, S. Kleinfelder12, T. Kobayashi21, V. I. Kolesnikov7, D. Kolev19, V. P. Kondratiev20, A. Korzenev11, P. Koversarski25, S. Kowalski14, A. Krasnoperov7, A. Kurepin16, D. Larsen6, A. Laszlo5, V. V. Lyubushkin7, M. Mackowiak-Pawłowska´ 9, Z. Majka6, B. Maksiak24, A. I. Malakhov7, D. Maletic2, D. Manglunki10, D. Manic2, A. Marchionni27, A. Marcinek6, V. Marin16, K. Marton5, H.-J.Mathes13, T. Matulewicz23, V. Matveev7;16, G. L. Melkumov7, M. Messina4, St. Mrówczynski´ 15, S. Murphy11, T. Nakadaira21, M. Nirkko4, K. Nishikawa21, T. Palczewski22, G. Palla5, A. D. Panagiotou1, T. Paul17, W. Peryt24;∗, O. Petukhov16 C.Pistillo4 R. Płaneta6, J. Pluta24, B. A. Popov7;18, M. Posiadala23, S. Puławski14, J. Puzovic2, W. Rauch8, M. Ravonel11, A. Redij4, R. Renfordt9, E. Richter-Wa¸s6, A. Robert18, D. Röhrich3, E. Rondio22, B. Rossi4, M. Roth13, A. Rubbia27, A. Rustamov9, M. -
The Charm of Theoretical Physics (1958– 1993)?
Eur. Phys. J. H 42, 611{661 (2017) DOI: 10.1140/epjh/e2017-80040-9 THE EUROPEAN PHYSICAL JOURNAL H Oral history interview The Charm of Theoretical Physics (1958{ 1993)? Luciano Maiani1 and Luisa Bonolis2,a 1 Dipartimento di Fisica and INFN, Piazzale A. Moro 5, 00185 Rome, Italy 2 Max Planck Institute for the History of Science, Boltzmannstraße 22, 14195 Berlin, Germany Received 10 July 2017 / Received in final form 7 August 2017 Published online 4 December 2017 c The Author(s) 2017. This article is published with open access at Springerlink.com Abstract. Personal recollections on theoretical particle physics in the years when the Standard Theory was formed. In the background, the remarkable development of Italian theoretical physics in the second part of the last century, with great personalities like Bruno Touschek, Raoul Gatto, Nicola Cabibbo and their schools. 1 Apprenticeship L. B. How did your interest in physics arise? You enrolled in the late 1950s, when the period of post-war reconstruction of physics in Europe was coming to an end, and Italy was entering into a phase of great expansion. Those were very exciting years. It was the beginning of the space era. L. M. The beginning of the space era certainly had a strong influence on many people, absolutely. The landing on the moon in 1969 was for sure unforgettable, but at that time I was already working in Physics and about to get married. My interest in physics started well before. The real beginning was around 1955. Most important for me was astronomy. It is not surprising that astronomy marked for many people the beginning of their interest in science. -
Around the Laboratories
Around the Laboratories such studies will help our under BROOKHAVEN standing of subnuclear particles. CERN Said Lee, "The progress of physics New US - Japanese depends on young physicists Antiproton encore opening up new frontiers. The Physics Centre RIKEN - Brookhaven Research Center will be dedicated to the t the end of 1996, the beam nurturing of a new generation of Acirculating in CERN's LEAR low recent decision by the Japanese scientists who can meet the chal energy antiproton ring was A Parliament paves the way for the lenge that will be created by RHIC." ceremonially dumped, marking the Japanese Institute of Physical and RIKEN, a multidisciplinary lab like end of an era which began in 1980 Chemical Research (RIKEN) to found Brookhaven, is located north of when the first antiprotons circulated the RIKEN Research Center at Tokyo and is supported by the in CERN's specially-built Antiproton Brookhaven with $2 million in funding Japanese Science & Technology Accumulator. in 1997, an amount that is expected Agency. With the accomplishments of these to grow in future years. The new Center's research will years now part of 20th-century T.D. Lee, who won the 1957 Nobel relate entirely to RHIC, and does not science history, for the future CERN Physics Prize for work done while involve other Brookhaven facilities. is building a new antiproton source - visiting Brookhaven in 1956 and is the antiproton decelerator, AD - to now a professor of physics at cater for a new range of physics Columbia, has been named the experiments. Center's first director. The invention of stochastic cooling The Center will host close to 30 by Simon van der Meer at CERN scientists each year, including made it possible to mass-produce postdoctoral and five-year fellows antiprotons. -
The NA61/SHINE Experiment: Beams and Detector System
EUROPEAN LABORATORY FOR PARTICLE PHYSICS The NA61/SHINE experiment: beams and detector system By the NA61 Collaboration http://na61.web.cern.ch Abstract NA61/SHINE (SPS Heavy Ion and Neutrino Experiment) is a multi-purpose fixed target experiment to study hadron production in hadron-nucleus and nucleus-nucleus collisions at the CERN Super Proton Synchrotron. It recorded the first physics data with hadron beams in 2009 and with ion beams (secondary 7Be beams) in 2011. NA61/SHINE has greatly profited from the long development of the CERN pro- ton and ion sources and the accelerator chain as well as the H2 beam line of the CERN North Area. The latter has recently been modified to also serve as a fragment separator as needed to produce the Be beams for NA61/SHINE. Numerous compo- nents of the NA61/SHINE set-up were inherited from its predecessors, in particular, the last one, the NA49 experiment. Important new detectors and upgrades of the inherited equipment were introduced the NA61/SHINE Collaboration. This paper describes the NA61/SHINE experimental facility and used beams by the CERN Long Shutdown I, March 2013. June 11, 2013 Contents 1 Introduction 5 2 Beams 6 2.1 The proton acceleration chain . 6 2.2 The ion accelerator chain . 7 2.3 H2 beam line . 9 2.4 Hadron beams . 9 2.5 Primary and secondary ion beams . 10 3 Beam detectors and triggers 13 3.1 Beam counters . 13 3.2 A-detector . 14 3.3 Beam Position Detectors . 14 3.4 Z-detectors . 15 3.5 Trigger system .