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Gpus for the Realtime Low-Level Trigger of the NA62 Experiment at CERN
GPUs for the realtime low-level trigger of the NA62 experiment at CERN R. Ammendola4, M. Bauce3,7, A. Biagioni3, S. Chiozzi1,5, A. Cotta Ramusino1,5, R. Fantechi2, 1,5, 1,5 2,6 2,8 3 3,7 M. Fiorini ∗, A. Gianoli , E. Graverini , G. Lamanna , A. Lonardo , A. Messina , I. Neri1,5, F. Pantaleo2,6, P. S. Paolucci3, R. Piandani2,6, L. Pontisso2, F. Simula3, M. Sozzi2,6, P. Vicini3 1INFN Sezione di Ferrara, Via Saragat 1, 44122 Ferrara, Italy 2INFN Sezione di Pisa, Largo B. Pontecorvo 3, 56127 Pisa, Italy 3INFN Sezione di Roma“La Sapienza”, P.le A. Moro 2, 00185 Roma, Italy 4INFN Sezione di Roma “Tor Vergata”, Via della Ricerca Scientifica 1, 00133 Roma, Italy 5University of Ferrara, Via Saragat 1, 44122 Ferrara, Italy 6University of Pisa, Largo B. Pontecorvo 3, 56127 Pisa, Italy 7University of Rome “La Sapienza”, P.le A.Moro 2, 00185 Roma, Italy 8INFN Sezione di Frascati, Via E.Fermi 40, 00044 Frascati (Roma), Italy ∗ Corresponding author. E-mail: fi[email protected] DOI: http://dx.doi.org/10.3204/DESY-PROC-2014-05/15 A pilot project for the use of GPUs (Graphics processing units) in online triggering ap- plications for high energy physics experiments (HEP) is presented. GPUs offer a highly parallel architecture and the fact that most of the chip resources are devoted to computa- tion. Moreover, they allow to achieve a large computing power using a limited amount of space and power. The application of online parallel computing on GPUs is shown for the synchronous low level trigger of NA62 experiment at CERN. -
The Higgs Boson!
MEET THE TIME MAGAZINE PARTICLE OF THE YEAR: THE HIGGS BOSON! Saptaparna Bhattacharya July 11th - 22nd, 2016 Lets start at the beginning! http://poy.time.com/2012/12/19/the-higgs-boson-particle-of-the-year/ Introduction • I am Saptaparna Bhattacharya, a post-doctoral scholar in the department of Physics and Astronomy at Northwestern University in Chicago. • My research is based on the data from the Large Hadron Collider at CERN. • I have worked on the first published result that uses the Higgs boson as a probe for New Physics. • My interest lies in various models of New Physics, ranging from SuperSymmetry to exploring the possibility of finding microscopic black holes. • I am also interested in exploring interesting techniques for data analysis. But, enough about me, where are you guys from? Current Enrollment We are a class of 17 students! Let me quickly check to see if you are all here! What we did last summer! Di-photon invariant mass h_InvariantMass_PhPh Higgs to ZZ invariant mass h_InvariantMass_HZZ Entries 85893 Entries 13235 30000 Mean 125.9 Mean 124.2 RMS 2.636 RMS 3.147 5000 25000 Events/2.0 GeV Events/2.0 GeV 20000 4000 Higgs boson mass distribution Higgs boson mass distribution 15000 3000 10000 2000 5000 1000 0 0 100 105 110 115 120 125 130 135 140 145 150 100 105 110 115 120 125 130 135 140 145 150 m [GeV] m [GeV] γγ µ µ µ µ Di-muon invariant mass h_InvariantMass_MuMu Tranverse Mass with Muons Entries 37122 h_TransverseMass_Mu Mean 90.66 Entries 37791 RMS 4.506 5000 4000 Mean 65.9 RMS 15.36 3500 4000 Events/GeV Events/1.0 GeV 3000 Z boson mass distribution 3000 2500 W boson transverse 2000 mass distribution 2000 1500 1000 1000 500 0 0 70 75 80 85 90 95 100 105 110 0 50 100 150 200 250 300 m [GeV] mµµ [GeV] T Outline • The course is roughly structured into two parts: • Laying down the fundamentals. -
NEWSLETTER 45 Istituto Nazionale Di Fisica Nucleare MARCH 2018
NEWSLETTER 45 Istituto Nazionale di Fisica Nucleare MARCH 2018 RESEARCH NA62 RESEARCH AND THE RARE DECAYS OF THE K-MESON The NA62 experiment at CERN has recently presented its latest results concerning a very rare event: the decay of the charged K-meson into a pion and two neutrinos. The interest in extremely rare or even "forbidden" decays is motivated by the fact that these processes allow energy scales even much higher than those directly accessible to the most powerful particle colliders, such as the Large Hadron Collider (LHC) at CERN, to be indirectly probed. The study of these decays could therefore open a window in the near future on physics beyond the Standard Model. Moreover, the results just presented by NA62 are also interesting because they demonstrate the effectiveness of the new technique, called "in flight", used by the experiment to investigate these K-meson decays. In the coming years, this will allow the elusive process to be studied with a precision never achieved before. According to theoretical predictions, the charged K-meson decays into a pion and two neutrinos only in a very small fraction of cases. To understand the extreme rarity of this process, the Standard Model foresees, with considerable precision, that only eight decays of this type must occur every one hundred billion decays of the K-meson. In numerous theories that aim to overcome the Standard Model, the fraction of events expected for this decay is instead significantly different: therefore, a sufficiently precise measure could highlight the presence of what physicists call New Physics. The results obtained so far, at this level of statistical precision, are compatible with the Standard Model predictions. -
Physics Beyond Colliders at CERN: Beyond the Standard Model
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH (CERN) CERN-PBC-REPORT-2018-007 Physics Beyond Colliders at CERN Beyond the Standard Model Working Group Report J. Beacham1, C. Burrage2,∗, D. Curtin3, A. De Roeck4, J. Evans5, J. L. Feng6, C. Gatto7, S. Gninenko8, A. Hartin9, I. Irastorza10, J. Jaeckel11, K. Jungmann12,∗, K. Kirch13,∗, F. Kling6, S. Knapen14, M. Lamont4, G. Lanfranchi4,15,∗,∗∗, C. Lazzeroni16, A. Lindner17, F. Martinez-Vidal18, M. Moulson15, N. Neri19, M. Papucci4,20, I. Pedraza21, K. Petridis22, M. Pospelov23,∗, A. Rozanov24,∗, G. Ruoso25,∗, P. Schuster26, Y. Semertzidis27, T. Spadaro15, C. Vallée24, and G. Wilkinson28. Abstract: The Physics Beyond Colliders initiative is an exploratory study aimed at exploiting the full scientific potential of the CERN’s accelerator complex and scientific infrastructures through projects complementary to the LHC and other possible future colliders. These projects will target fundamental physics questions in modern particle physics. This document presents the status of the proposals presented in the framework of the Beyond Standard Model physics working group, and explore their physics reach and the impact that CERN could have in the next 10-20 years on the international landscape. arXiv:1901.09966v2 [hep-ex] 2 Mar 2019 ∗ PBC-BSM Coordinators and Editors of this Report ∗∗ Corresponding Author: [email protected] 1 Ohio State University, Columbus OH, United States of America 2 University of Nottingham, Nottingham, United Kingdom 3 Department of Physics, University of Toronto, Toronto, -
The NA62 Experiment at CERN
126 EPJ Web of Conferences , 04036 (2016) DOI: 10.1051/epjconf/201612604036 ICNFP 2015 The NA62 experiment at CERN Mauro Piccini1,a 1INFN - Sezione di Perugia Abstract. The rare decays K → πνν¯ are excellent processes to make tests of new physics at the highest scale complementary to LHC thanks to their theoretically cleanness. The NA62 experiment at CERN SPS aims to collect of the order of 100 events in two years of data taking for the decay K+ → π+νν¯, keeping the background at the level of 10%. Part of the experimental apparatus has been commissioned during a technical run in 2012. The diverse and innovative experimental techniques will be explained and some preliminary results obtained during the 2014 pilot run will be reviewed. 1 Introduction NA62 is the last generation kaon experiment at CERN SPS aiming to study the decay K+ → π+νν¯. The goal of the experiment is to measure the decay branching ratio (O(10−10)) with 10% accuracy, collecting about 100 events in two years of data taking and assuming a 10% signal acceptance. The proton beam extracted from the SPS in the north area at CERN fulfills such demanding request in aOn behalf of the NA62 Collaboration: G. Aglieri Rinella, R. Aliberti, F. Ambrosino, B. Angelucci, A. Antonelli, G. Anzivino, R. Arcidiacono, I. Azhinenko, S. Balev, M. Barbanera, J. Bendotti, A. Biagioni, L. Bician, C. Biino, A. Bizzeti, T. Blazek, A. Blik, B. Bloch-Devaux, V. Bolotov, V. Bonaiuto, M. Bragadireanu, D. Britton, G. Britvich, M.B. Brunetti, D. Bry- man, F. Bucci, F. Butin, E. -
Outreach Activities, Web, Radio&TV, Non-Specialized Conferences And
1 Laboratoire de Physique des Hautes Energies (LPHE) Outreach activities, web, radio&TV, non-specialized conferences and publications April 2009 { March 2016 We list here activities aiming at making our research known to less specialized audiences, or more generally to the public at large. April 2015 { March 2016 1. C. Fitzpatrick, guide for visit at CERN of students from Campbell College Belfast, March 19, 2016. 2. O. Schneider, visit organized at CERN (at LHCb, CAST, and LHC magnets) for 60 Bachelor students of EPFL, November 17, 2015. 3. I. Komarov, \On the irreversibility of time and Einstein's theory", online lecture for children in the framework of the \Scientists to kids" project, Experimentarium Museum, Moscow, Russia, October 24, 2015. 4. CERN Courier: \LHCb improves trigger in Run 2", September 25, 2015. 5. O. Schneider, participation in an interdisciplinary podium discussion \Le boson de Higgs { architecte de l'Univers ?" after a public screening of the movie \Particle Fever" (flyer), Lyc´ee-Coll`egedes Creusets, Sion, Switzerland, September 25, 2015. 6. LHCb public web site: \First LHC run2 physics results: measurement of J= production cross- sections in pp collisions at 13 TeV", July 24, 2015. 7. EPFL news: \EPFL contributes to breakthrough experiment at CERN"(\L'EPFL contribue `aune d´ecouverte majeure au CERN", May 21, 2015. 8. EPFL news: \Tatsuya Nakada awarded Honorary Doctorate from University of Zurich"(\Tatsuya Nakada honor´epar l'Universit´ede Zurich"), May 4, 2015. 9. V. Battista, \LHCb: tra bellezza e asimmetrie", science popularization article published in \Quaderni di scienza e scienziati molisani", 2015. April 2014 { March 2015 1. -
Speed of Light and Rates of Clocks in the Space Generation Model of Gravitation, Part 1
GravitationLab.com Speed of Light and Rates of Clocks in the Space Generation Model of Gravitation, Part 1 1 R. BENISH( ) (1) Eugene, Oregon, USA, [email protected] Abstract. — General Relativity’s Schwarzschild solution describes a spherically symmetric gravi- tational field as an utterly static thing. The Space Generation Model (SGM) describes it as an absolutely moving thing. The SGM nevertheless agrees equally well with observations made in the fields of the Earth and Sun, because it predicts almost ex- actly the same spacetime curvature. This success of the SGM motivates deepening the context—especially with regard to the fundamental concepts of motion. The roots of Einstein’s relativity theories thus receive critical examination. A particularly illumi- nating and widely applicable example is that of uniform rotation, which was used to build General Relativity (GR). Comparing Einstein’s logic to that of the SGM, the most significant difference concerns the interpretation of the readings of accelerom- eters and the rates of clocks. Where Einstein infers relativity of motion and space- time symmetry, it is argued to be more logical to infer absoluteness of motion and spacetime asymmetry. This approach leads to reassessments of the essential nature of matter, time, and the dimensionality of space, which lead in turn to some novel cos- mological consequences. Special emphasis is given to the model’s deviations from standard predictions inside matter, which have never been tested, but could be tested by conducting a simple experiment. PACS 04.80.Cc – Experimental tests of gravitational theories. 1. – Introduction; Intended Audience Beware ye, all those bold of spirit who want to suggest new ideas. -
Nov/Dec 2020
CERNNovember/December 2020 cerncourier.com COURIERReporting on international high-energy physics WLCOMEE CERN Courier – digital edition ADVANCING Welcome to the digital edition of the November/December 2020 issue of CERN Courier. CAVITY Superconducting radio-frequency (SRF) cavities drive accelerators around the world, TECHNOLOGY transferring energy efficiently from high-power radio waves to beams of charged particles. Behind the march to higher SRF-cavity performance is the TESLA Technology Neutrinos for peace Collaboration (p35), which was established in 1990 to advance technology for a linear Feebly interacting particles electron–positron collider. Though the linear collider envisaged by TESLA is yet ALICE’s dark side to be built (p9), its cavity technology is already established at the European X-Ray Free-Electron Laser at DESY (a cavity string for which graces the cover of this edition) and is being applied at similar broad-user-base facilities in the US and China. Accelerator technology developed for fundamental physics also continues to impact the medical arena. Normal-conducting RF technology developed for the proposed Compact Linear Collider at CERN is now being applied to a first-of-a-kind “FLASH-therapy” facility that uses electrons to destroy deep-seated tumours (p7), while proton beams are being used for novel non-invasive treatments of cardiac arrhythmias (p49). Meanwhile, GANIL’s innovative new SPIRAL2 linac will advance a wide range of applications in nuclear physics (p39). Detector technology also continues to offer unpredictable benefits – a powerful example being the potential for detectors developed to search for sterile neutrinos to replace increasingly outmoded traditional approaches to nuclear nonproliferation (p30). -
Curating the Collider: Using Place to Engage Museum Visitors with Particle Physics
Science Museum Group Journal Curating the collider: using place to engage museum visitors with particle physics Journal ISSN number: 2054-5770 This article was written by Alison Boyle, Harry Cliff 10-09-2014 Cite as 10.15180; 140207 Research Curating the collider: using place to engage museum visitors with particle physics Published in Autumn 2014, Issue 02 Article DOI: http://dx.doi.org/10.15180/140207 Abstract CERN’s Large Hadron Collider, the world’s largest particle physics facility, provides museological opportunities and challenges. Visitor interest in cutting-edge physics, with its high media profile, is tempered by anxiety about understanding complex content. The topic does not readily lend itself to traditional museum showcase-dominated displays: the technology of modern particle physics is overwhelmingly large, while the phenomena under investigation are invisible. For Collider, a major temporary exhibition, the Science Museum adopted a ‘visit to CERN’ approach, recreating several of the laboratory’s spaces. We explore the effectiveness of this approach, at a time when historical studies of scientific laboratories and museum reconstructions of spaces are subject to renewed interest. Component DOI: http://dx.doi.org/10.15180/140207/001 Keywords Science Museum, Collider, Large Hadron Collider, CERN, particle physics, place, space, re-creation, room set, museum Introduction Collider: step inside the world’s greatest experiment ran at the Science Museum from November 2013–May 2014 and is touring internationally until 2017. The exhibition covers the work of the Large Hadron Collider (LHC) at CERN, the world’s largest particle physics facility. Strategically, the subject matter had obvious appeal for the Science Museum, with its long term ambitions to tackle complex scientific topics, attract more adult visitors, and raise its international profile (Science Museum, 2012). -
The Higgs Boson and Big Science Sarah Eno, U. Maryland MASP Lectur
How many physicists does it take to discover a new particle? The Higgs Boson and Big Science Sarah Eno, U. Maryland MASP lecture 29 April 08 Sarah Eno 1 4 July 2012 CERN Auditorium: announcement of a new particle 8 October 2013 20 May 2014 Sarah Eno, MASP lecture 2 Two Experiments CMS ATLAS 20 May 2014 Sarah Eno, MASP lecture 3 Each with a paper Discoveries are made by people, not by detectors. 20 May 2014 Sarah Eno, MASP lecture 4 CMS: Discovery courtesy of: 20 May 2014 Sarah Eno, MASP lecture 5 20 May 2014 Sarah Eno, MASP lecture 6 20 May 2014 Sarah Eno, MASP lecture 7 20 May 2014 Sarah Eno, MASP lecture 8 20 May 2014 Sarah Eno, MASP lecture 9 20 May 2014 Sarah Eno, MASP lecture 10 20 May 2014 Sarah Eno, MASP lecture 11 2892 authors from 168 institutions This is just the CMS paper. There is a similar list for ATLAS. 20 May 2014 Sarah Eno, MASP lecture 12 Outline • What is the Higgs boson? • How do we know that it was created in proton-proton collisions at the Large Hadron Collider • What do all those people actually do? 20 May 2014 Sarah Eno, MASP lecture 13 Particle Fever Assistant Professor Alberto Belloni 20 May 2014 Sarah Eno, MASP lecture 14 What is a Higgs Boson? 20 May 2014 Sarah Eno, MASP lecture 15 Before we talk about the Higgs, let’s think about forces Is it this? Particle physicists think of it as this: Force boson Matter: Quarks (protons) leptons (electron) matter Some more force bosons 20 May 2014 Sarah Eno, MASP lecture 16 Only four of them, each with a “boson” Electricity and Magnetism (QED) photon Strong Force (QCD) gluon Weak Force 1H + 1H ® 2 H + e+ +n 1 1 1 W&Z bosons 20 May 2014 Sarah Eno, MASP lecturehttp://www.dreamstime.com/powerplant-infrastructure-stock-photo-imagefree242420 17 Fourth is gravity, but since its effects are negligible when considering particle collisions at accelerators, I’ll ignore it. -
WORKING with ITALO Luigi Di Lella CERN and Physics Department, University of Pisa
WORKING WITH ITALO Luigi Di Lella CERN and Physics Department, University of Pisa ▪ Some old memories ▪ Studying K± → p ± p° p° decays in the NA48/2 experiment + + + + ▪ Measuring the ratio of the K → e ne to the K → m nm decay rate ▪ The fast muon veto in the NA62 experiment Italo’s Fest S.N.S. , Pisa, September 5th, 2018 1953 - 54: first-year physics student at Scuola Normale Superiore (ranked first at the entrance examinations) Italo with fellow students Giorgio Bellettini and Vittorio Silvestrini (physics) and Mario Dall’Aglio (chemistry) while violating Italian traffic rules (1957?) All S.N.S. students (Spring 1957) Both Humanities and Sciences, 1st to 4th year 1957: the year when parity violation was first observed (in b – decay of polarized Co60 nuclei and in the p+ → m+ → e+ decay chain) There were suggestions that parity violation would be observed only in final states containing neutrinos (the V – A theory had not been formulated yet) For his physics degree in 1957, Italo worked on a search for parity violation in L → p p─ decay (a weak decay with no neutrinos in the final state) Phys. Rev. 108 (1957) 1353 A bubble chamber exposure to ~1 GeV beams from the 3 GeV proton synchrotron (‘’Cosmotron’’) at the Brookhaven National Laboratory. Event analysis performed in various laboratories including Bologna and Pisa. p─ + p → L + K° produces L – hyperons with polarization normal to the L production plane. Result: < 푷횲 > 휶 = ퟎ. ퟒퟎ ± ퟎ. ퟏퟏ 1958: Italo receives a S.I.F. prize for his thesis (S.I.F.: Italian Physical Society) Prof. -
Results and Prospects on Kaon Physics with the NA62 Experiment at CERN ∗ M
IL NUOVO CIMENTO 38 C (2015) 13 DOI 10.1393/ncc/i2015-15013-6 Colloquia: IFAE 2014 Results and prospects on kaon physics with the NA62 experiment at CERN ∗ M. Mirra for the NA62 Collaboration( ) INFN, Sezione di Napoli and Universit`a degli Studi di Napoli Federico II - Napoli, Italy received 7 January 2015 Summary. — The measurement of the ratio of the rates of leptonic kaon decays performed by NA48/2 and NA62 (RK phase) experiments is presented, together with the description of the NA62 experiment that will start collecting data in 2015 at the CERN SPS with the main goal of measuring the branching ratio(BR) of the rare decay K+ → π+νν¯ with a precision of 10%. PACS 13.20.Eb – Decays of K mesons. PACS 12.15.Hh – Determination of CKM matrix elements. ∗ ( ) G. Aglieri Rinella, F. Ambrosino, B. Angelucci, A. Antonelli, G. Anzivino, R. Arcidiacono, I. Azhinenko, S. Balev, J. Bendotti, A. Biagioni, C. Biino, A. Bizzeti, T. Blazek, A. Blik, B. Bloch-Devaux, V. Bolotov, V. Bonaiuto, D. Britton, G. Britvich, N. Brook, F. Bucci, V. Buescher, F. Butin, E. Capitolo, C. Capoccia, T. Capussela, V. Carassiti, N. Cartiglia, A. Cassese, A. Catinaccio, A. Cecchetti, A. Ceccucci, P. Cenci, V. Cerny, C. Cerri, O. Chikilev, R. Ciaranfi, G. Collazuol, P. Cooke, P. Cooper, G. Corradi, E. Cortina Gil, F. Costantini, A. Cotta Ramusino, D. Coward, G. DAgostini, J. Dainton, P. Dalpiaz, H. Danielsson, J. Degrange, N. De Simone, D. Di Filippo, L. Di Lella, N. Dixon, N. Doble, V. Duk, V. Elsha, J. Engelfried, V.