Organisation Europeenne Pour La Recherche Nucleaire Larecherche Pour Europeenne Organisation

Total Page:16

File Type:pdf, Size:1020Kb

Organisation Europeenne Pour La Recherche Nucleaire Larecherche Pour Europeenne Organisation DRAFT CERN/DG/Research Board 2012-425 Minutes-198 12 January 2012 ORGANISATION EUROPEENNE POUR LA RECHERCHE NUCLEAIRE CERN EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH _______________________________________________________________ CERN RESEARCH BOARD MINUTES OF THE 198th MEETING OF THE RESEARCH BOARD HELD ON WEDNESDAY 30 NOVEMBER 2011 Present I. Antoniadis, S. Bertolucci, P. Bloch, H. Breuker, P. Butler, P. Collier, E. Elsen, M. Ferro-Luzzi, R. Forty (Secretary), R. Heuer (Chair), P. Janot, M. Kowalska, S. Myers, E. Rondio, R. Saban, E. Tsesmelis, C. Vallée Apologies F. Hemmer Items 1. Procedure 2. Accelerator schedules for 2012 3. Report from the LHCC meeting of 21-22 September 2011 4. Report from the SPSC meeting of 25-26 October 2011 5. Report from the INTC meeting of 3-4 November 2011 CERN-DG-RB-2012-425 / M-198 09/03/2012 6. Any other business DRAFT CERN/DG/Research Board 2012-425 2 DRAFT CERN/DG/Research Board 2012-425 1. PROCEDURE 1.1 The minutes of the last meeting [1] were approved without modification. 2. ACCELERATOR SCHEDULES FOR 2012 2.1 P. Collier presented the accelerator schedules for 2012 [2]. This will be the final year of the current LHC running period, before the long shutdown for consolidation work to allow the machine to approach its design energy. For this year the physics running is planned to start in April, most likely with an energy of 4 TeV per beam, and 50 ns bunch spacing, although the final decision will be taken following discussion at the Chamonix workshop at the beginning of February. The physics run will end with a month dedicated to ions in November, most likely in p-A configuration. The accelerators will then be off for 2013, with the injectors restarting in 2014, so that fixed-target physics and test beam will be available during that year, before the LHC restarts. M. Ferro-Luzzi commented that the LHC experiments may request optimisation of the details of the schedule to maximise the integrated luminosity before the summer conferences, and that his successor as LHC Programme Coordinator would collect input from the experiments ready for Chamonix. 2.2 The injector accelerator schedule sees the start of physics for CNGS, nTOF and ISOLDE in March, AD physics in April and North Area physics in May, running until 3 December. Six weeks of the run are devoted to sending ions to the North Area for NA61, scheduled to start at the end of August, and during that period test beams will be interrupted. The beam to CNGS will include some bunched beam running, for further investigation of the super-luminal effect presented by OPERA. This will most probably be around May after an initial high intensity period of running. In the current plan ISOLDE would receive about 80% of its requested beam, while DIRAC would receive over 90% of their request. S. Bertolucci suggested that any shortfall should be shared equally. C. Vallée commented that DIRAC is expected to present results from the current run before the SPSC will make a recommendation concerning their continued running in 2012, and at that point the need for the large number of spills requested by DIRAC will be scrutinised. The accelerator schedules were approved. 3 DRAFT CERN/DG/Research Board 2012-425 3. REPORT FROM THE LHCC MEETING OF 21-22 SEPTEMBER 2011 3.1 E. Elsen reported on the latest meeting of the LHCC [3]. The increase in luminosity of the LHC in the period up to the meeting (and beyond) had been very impressive, with effective Machine Development periods devoted to increasing the intensity per bunch, reducing the emittance, and focusing the beams to a β* of 1 m for the general-purpose experiments. LHCb was successfully supplied with luminosity leveled at their requested value, by adjusting the vertical offset of the beams. The luminosity has been determined with a precision of 3.5%. The decision had been taken to stay with 50 ns bunch spacing to optimize the luminosity delivered during the year, as the general-purpose detectors were able to handle the increased pile-up compared to 25 ns operation. The ALICE run had been affected by machine-induced background after solenoid polarity change. S. Myers commented that the cause of this had now been understood and would be solved. 3.2 E. Elsen then discussed some highlights of the rich physics harvest from the LHC experiments, presented at the summer conferences. These included the world’s most precise measurement of Bs oscillations from LHCb, measurements of particle production ratios in Pb–Pb collisions from ALICE, top-quark mass measurement from ATLAS and top charge and mass asymmetries from CMS. No signal of physics beyond the Standard Model had yet been seen, and the range of possible mass for the Higgs boson was being significantly constrained, so that if it exists it would have to be light. TOTEM had run successfully with a β* of up to 90 m, and made a first measurement of the total cross-section. 3.3 Concerning the upgrades of the LHC experiments, the LHCC had heard a report on the ATLAS Insertable B-Layer (IBL) pixel detector. Two competing technologies (3D and planar) had been evaluated and both were considered by ATLAS to be mature and could be made to work within the envisioned time-frames and budgets. The LHCC has requested a document detailing the proposed hybrid plan which will be reviewed at the next session, with the goal of enabling a final LHCC recommendation. The upcoming LHC experiment upgrade sessions will also include discussion of the 4 DRAFT CERN/DG/Research Board 2012-425 Letter of Intent (LoI) for ATLAS Phase-1 upgrades, the Technical Design Report (TDR) for their Fast Tracker Trigger (FTK), the LoI for ALICE upgrades, a framework TDR for the upgrade activities of LHCb following their LoI, and a report on the CMS Pixel Detector TDR. 3.4 A Letter of Intent has been received for an experiment to test collimation in the LHC using bent crystals, named LUA9 (a development from UA9 at the SPS). The LHCC recognizes the potential of this technique, but is concerned about the possible impact of such an experiment on the operation of the machine. The studies will be confined to Machine Development periods. R. Heuer stressed that care should be taken to arrange this so as to avoid any significant disturbance to the routine operation of the LHC for physics. The Research Board took note. 4. REPORT FROM THE SPSC MEETING OF 25-26 OCTOBER 2011 4.1 C. Vallée reported on the latest meeting of the SPSC [3], including annual reports from NA60, NA49, NA61, NA63, UA9, CAST and OSQAR. NA60 and NA49 are continuing to exploit their data sets, and the SPSC recommends continued support for their data analysis. 4.2 NA61 has published the 2007 data on pion production in p-C collisions, and the SPSC looks forward to physics results from the 2009 data set. The committee recommends that adequate beam time is allocated in 2012 to allow for the completion of the energy scan with secondary light ions prior to the shutdown in 2013, and that full use is made of the ongoing development of primary light ion beams, with the aim of delivering a primary argon beam in 2014 and a primary xenon beam in 2015 [4]. 4.3 NA63 has achieved progress in the analysis of the LPM magnetic suppression and structured target resonance data, and continues to publish their results. The experiment proposes to study positron production in a diamond by energetic electron impact and to study bremsstrahlung from ions [5]. P. Collier stated that the new North Area interlock system has not yet been installed, and as a result no primary ions are at present allowed in the North Area unless protons are at the same time prevented from entering the SPS. Given the accelerator schedule, primary ions for NA63 are therefore 5 DRAFT CERN/DG/Research Board 2012-425 not possible during 2012. The SPSC advises the collaboration to instead focus on the positron production in crystals in 2012, and encourages the collaboration to finalize the experimental setup. The proposal will be reviewed further before making a recommendation. 4.4 UA9 has achieved progress in both hardware and analysis, and has obtained encouraging proton and ion collimation results with crystal channeling. The SPSC supports the request by the collaboration for further beam time in 2012 at the level that has been provided in 2011. 4.5 CAST successfully concluded their 3He programme and published the first results. The SPSC is looking forward to the final publication of the 3He data. The collaboration is refurbishing key components of the set-up during shutdown for longer term operation and installing improved shielding on the micromegas detectors [6]. A further three-month 4He run of CAST is requested in 2012 to improve their sensitivity over a limited range of axion masses around 0.4 eV/c2. This was approved by the Research Board. 4.6 OSQAR has submitted first results of its regeneration experiment for publication. The collaboration plans to achieve in 2012 an improved axion search limit that will be competitive with recent results of the ALPS Collaboration. The Research Board approved the OSQAR run in 2012. 4.7 The SPSC received a Letter of Intent for a demonstration experiment in proton- driven plasma wake-field acceleration [7]. This has possible technological implications for future accelerators at CERN and elsewhere. The committee recognizes the opportunity to use the SPS beams for these studies, and encourages the collaboration to work towards a Technical Design Report in order to allow the technical feasibility, the timescale and the resources to be assessed within the overall CERN programme.
Recommended publications
  • Neutrino Oscillations: T2k and Na61 Experiments, R&D
    NEUTRINO OSCILLATIONS: T2K AND NA61 EXPERIMENTS, R&D TOWARDS A FUTURE NEUTRINO PROGRAM 1 Research Plan The field of neutrino physics is certainly one of the most active in particle physics today. It is by now well established that neutrinos have mass and that the three families mix. In the minimal Standard Model, neutrinos are massless; massive neutrinos require either a new ad- hoc conservation law or new phenomena beyond the present framework, with a possible link to the grand unification scale via the see-saw mechanism. A deep field of research is thus open, that could last several decades and culminate with the discovery of leptonic CP violation – a key ingredient in the understanding of the baryon- anti-baryon asymmetry of the universe. Because observation of CP violation in neutrino oscillations requires appearance experiments, accessible at accelerators only, an important investment in accelerator-based neutrino beams and experiments is called for. The CHIPP Roadmap considers neutrino physics as one of the three pillars of particle physics in Switzerland, and so does the 15 years research plan of the DPNC at University of Geneva1. The neutrino group at DPNC has been actively involved in this quest since the nomination of Prof. A. Blondel in early 2000, where participation in the HARP experiment at CERN led us to the K2K experiment in Japan, in which the first observation of neutrino oscillation with a neutrino beam was achieved. The group received an added boost with the nomination of Alessandro Bravar (MER) in 2006. The research program comprises a progression of on- going experiments and far-reaching R&D activity as described in the SNF reports of October 2007 and October 2008.
    [Show full text]
  • Measurements of Hadronic Cross Section for Precise Determination of Neutrino Beam Properties in T2K Oscillation Experiment
    University of Warsaw Faculty of Physics Institute of Experimental Physics Measurements of Hadronic Cross Section for Precise Determination of Neutrino Beam Properties in T2K Oscillation Experiment Magdalena Zofia Posiadała Ph.D. thesis written under supervision of prof. dr hab. Danuta Kiełczewska Warsaw, 2011 Abstract Differential cross sections and mean multiplicities in production processes for low momentum charged pion mesons and protons in p+C interactions at 31 GeV/c measured with the large acceptance NA61/SHINE spectrometer at the CERN SPS are presented. A set of data col- lected during the first NA61/SHINE run in 2007 with a thin graphite target was used for the analysis. The results are presented as a function of laboratory momentum in 10 intervals of the laboratory polar angle covering the range from 0 up to 420 mrad. The spectra are compared with predictions of several hadron production models. Measurements for π+ and π− mesons are used by the T2K experiment to tune neutrino beam simulations and reduce uncertainties on charged pion production. Contents List of Figures vii List of Tables xi Acknowledgments xii Introduction 1 1 Neutrinos 4 1.1 Neutrino oscillation mechanism . .5 1.2 The Current Situation in Neutrino Oscillation Physics . .7 2 T2K experiment and its prerequisites for NA61/SHINE measurements 18 2.1 The T2K long baseline neutrino oscillation experiment . 18 2.2 J-PARC facility . 20 2.2.1 J-PARC accelerator . 20 2.2.2 Primary and secondary T2K beamline . 20 2.2.3 Near detector complex . 23 2.3 Overview of the Super-Kamiokande detector . 24 2.4 T2K physical goals .
    [Show full text]
  • Measurement of Hadron-Carbon Interactions for Better Understanding of Air Showers with NA61/SHINE
    33RD INTERNATIONAL COSMIC RAY CONFERENCE,RIO DE JANEIRO 2013 THE ASTROPARTICLE PHYSICS CONFERENCE Measurement of hadron-carbon interactions for better understanding of air showers with NA61/SHINE H. P. DEMBINSKI1 FOR THE NA61/SHINE COLLABORATION2. 1 Institut fur¨ Kernphysik, KIT Karlsruhe, Postfach 3640, D - 76021 Karlsruhe 2 Full author list: https: // na61. web. cern. ch/ na61/ pages/ storage/ authors_ list. pdf [email protected] Abstract: The interpretation of air shower measurements requires the detailed simulation of hadronic particle production over a wide range of energies and the forward phase space of secondary particles. In air showers, the bulk of particles is produced at later stages of the shower development and at equivalent beam energies in the sub-TeV range. NA61/SHINE is a fixed target experiment using secondary beams produced at the SPS at 1 CERN. Hadron-hadron interactions have been recorded at beam momenta between 13 and 350 GeVc− with a wide-acceptance spectrometer. In this article we present measurements of the inelastic cross-section and secondary particle yields of pion-carbon interactions, which are essential for modelling air showers. Keywords: hadron interaction, QCD, air shower, pion 1 Hadronic interactions in air showers Cosmic rays initiate extensive air showers (EAS) when they collide with nuclei of the atmosphere. The EAS data recorded by experiments like the Pierre Auger Observa- tory [1], KASCADE [2] or IceTop [3], is used to infer their properties. The interpretation relies on simulations of the shower development during which electromagnetic and hadronic particle interactions are followed from primary 20 9 energies of & 10 eV down to energies of 10 eV.
    [Show full text]
  • 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.
    [Show full text]
  • Arxiv:1109.3262V1 [Hep-Ex] 15 Sep 2011 University of Tokyo, Department of Physics, Bunkyo, Tokyo 113-0033, Japan
    Letter of Intent: The Hyper-Kamiokande Experiment | Detector Design and Physics Potential | K. Abe,12, 14 T. Abe,10 H. Aihara,10, 14 Y. Fukuda,5 Y. Hayato,12, 14 K. Huang,4 A. K. Ichikawa,4 M. Ikeda,4 K. Inoue,8, 14 H. Ishino,7 Y. Itow,6 T. Kajita,13, 14 J. Kameda,12, 14 Y. Kishimoto,12, 14 M. Koga,8, 14 Y. Koshio,12, 14 K. P. Lee,13 A. Minamino,4 M. Miura,12, 14 S. Moriyama,12, 14 M. Nakahata,12, 14 K. Nakamura,2, 14 T. Nakaya,4, 14 S. Nakayama,12, 14 K. Nishijima,9 Y. Nishimura,12 Y. Obayashi,12, 14 K. Okumura,13 M. Sakuda,7 H. Sekiya,12, 14 M. Shiozawa,12, 14, ∗ A. T. Suzuki,3 Y. Suzuki,12, 14 A. Takeda,12, 14 Y. Takeuchi,3, 14 H. K. M. Tanaka,11 S. Tasaka,1 T. Tomura,12 M. R. Vagins,14 J. Wang,10 and M. Yokoyama10, 14 (Hyper-Kamiokande working group) 1Gifu University, Department of Physics, Gifu, Gifu 501-1193, Japan 2High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki, Japan 3Kobe University, Department of Physics, Kobe, Hyogo 657-8501, Japan 4Kyoto University, Department of Physics, Kyoto, Kyoto 606-8502, Japan 5Miyagi University of Education, Department of Physics, Sendai, Miyagi 980-0845, Japan 6Nagoya University, Solar Terrestrial Environment Laboratory, Nagoya, Aichi 464-8602, Japan 7Okayama University, Department of Physics, Okayama, Okayama 700-8530, Japan 8Tohoku University, Research Center for Neutrino Science, Sendai 980-8578, Japan 9Tokai University, Department of Physics, Hiratsuka, Kanagawa 259-1292, Japan 10 arXiv:1109.3262v1 [hep-ex] 15 Sep 2011 University of Tokyo, Department of Physics, Bunkyo,
    [Show full text]
  • US-NA61 Collaboration
    Hadron Production Measurements for Fermilab Neutrino Beams US participation in the NA61/SHINE experiment at CERN Letter of Intent May 2, 2012 Abstract This is a Letter of Intent to develop a limited-scope collaboration with the NA61/SHINE experiment at CERN to exploit its unique capabilities for particle production measurements. This effort would allow the US group to collect dedicated and optimized high-precision hadron production data needed for improved neutrino beams modeling nec- essary for ongoing and future experiments at Fermilab. The ultimate goal of this effort is to expose thin targets and replicas of targets used at Fermilab to the NA61 hadron beam to accumulate a suitably large sample of events to provide a data set which would be essential for future neutrino beams. An initial phase of this program, to be supported by existing funds, will be a two- day pilot run during the start-up of the 2012 run of NA61/SHINE. The pilot run will use a 120 GeV/c proton beam on a thin graphite target. It could provide valuable data for the MINERvA experiment, and would allow the US group to gain better practical under- standing of the capabilities of the NA61/SHINE experiment so that a broader collaborative program can be fully developed for later years. We envision this program to serve many future accelerator-based neutrino experiments at Fermilab and elsewhere. 1 The US NA61 Collaboration S. R. Johnson, A. Marino, E. D. Zimmerman University of Colorado, Boulder, Colorado 80302, USA D. Harris, A. Marchionni, D. Schmitz∗ Fermi National Accelerator Laboratory, Batavia, Illinois 60510, USA E.
    [Show full text]
  • Fixed-Target Hadron Production Experiments
    EPJ Web of Conferences 99, 02002 (2015) DOI: 10.1051/epjconf/20159902002 c Owned by the authors, published by EDP Sciences, 2015 Fixed-target hadron production experiments Boris A. Popov1,2,a 1 Laboratoire de Physique Nucleaire´ et de Hautes Energies, 4 place Jussieu, 75005 Paris, France 2 Joint Institute for Nuclear Research, Joliot-Curie 6, 141980 Dubna, Russia Abstract. Results from fixed-target hadroproduction experiments (HARP, MIPP, NA49 and NA61/SHINE) as well as their implications for cosmic ray and neutrino physics are reviewed. HARP measurements have been used for predictions of neutrino beams in K2K and MiniBooNE/SciBooNE experiments and are also being used to improve predictions of the muon yields in EAS and of the atmospheric neutrino fluxes as well as to help in the optimization of neutrino factory and super-beam designs. Recent measurements released by the NA61/SHINE experiment are of significant importance for a precise prediction of the J-PARC neutrino beam used for the T2K experiment and for interpretation of EAS data. These hadroproduction experiments provide also a large amount of input for validation and tuning of hadron production models in Monte-Carlo generators. 1. Introduction in order to illustrate some common features of modern hadron production experiments. The interpretation of extensive air shower (EAS) data – as for instance recorded by the Pierre Auger Observatory [1], To provide a large angular and momentum coverage KASCADE [2] or IceTop [3] – relies to a large extent on of the produced charged particles, the HARP experiment the correct modeling of hadron-air interactions that occur makes use of a large-acceptance spectrometer consisting during the shower development.
    [Show full text]
  • Particle and High-Energy Heavy-Ion Physics
    PARTICLE AND HIGH-ENERGY HEAVY-ION PHYSICS The Standard Model of the weak, electromagnetic and strong interactions is one of the most successful theoretical schemes ever developed in particle physics. The Standard Model explains to a high accuracy almost all relevant experimental observations. Nevertheless, it is not a fundamental theory, but a low-energy limit of some underlying theory which probably originates from the very high-energy scales like the Planck scale (of the order of 1019 GeV). There are some experimental results which can be treated as arguments for new physics beyond the Standard Model: The neutrino oscillations and perhaps neutrinoless nuclear double-beta decay data show that neutrinos have mass, neutrinos have mixing, neutrino properties are a mystery; There is missing mass in the Universe and there is acceleration of the Universe (dark matter and dark energy); LEP and Tevatron experiments have given strong indications to new physics at the TeV scale; There are too many external parameters and unsolved problems in the Standard Model; in particular, the gravity is not included, the electroweak symmetry breaking is not clear, there are hierarchy problems (Higgs mass diverges), etc. The main problems beyond the Standard Model very generally and very shortly can be grouped into three large classes with labels of Mass, Unification and Flavor. In more details they can be cast into the following basic questions: What is the origin of the particle masses, are they indeed due to the Higgs boson? What is the nature of
    [Show full text]
  • Curriculum Vitae
    Curriculum Vitae Alain BLONDEL Born 26 march1953 in Neuilly (92000 FRANCE), French citizen Personal address: 590 rte d'Ornex, 01280 Prévessin, France. Tel. +33 (0)4 50 40 46 51 Prefessional address: Université de Genève Département de Physique Nucléaire et Corpusculaire Quai Ernest-Ansermet 24 CH-1205 Genève 4 Tel. [41](22) 379 6227 [email protected] University grades and prizes : Engineer Ecole Polytechnique Paris (X1972) DEA in Nuclear Physics, University of Orsay (1975) 3d cycle Thesis, University of Orsay (1976) PhD in physics University of Orsay (1979) Bronze Medal CNRS (1979) (given yearly to the best PhD thesis in Particle/Nuclear physics) Prize of the Thibaud Foundation, Académie des Sciences, Arts et Belles Lettres de Lyon (1991) Silver Medal CNRS (1995) (given yearly for the best achievement in the field) Paul Langevin Prize from the French Academy of Sciences (1996) Manne Siegbahn Medal from the Royal Academy of Science in Sweden (1997) Prize from the foundation Jean Ricard by the French Physical Society (2004) (given yearly for best achievement in Physics) Professional curriculum : 1975 Stagiaire Ecole Polytechnique (Palaiseau, France) (PhD student grant) 1977 Attaché de Recherche au CNRS (Permanent position as junior researcher) 1980 Chargé de Recherche au CNRS (Permanent position as senior researcher) 1983-1985 Boursier CERN (CERN fellow) 1985-1989 Membre du Personnel CERN (CERN staff) 1989 → Directeur de Recherches au CNRS (Director of research group) 1991 → 2000 Maître de Conférences à l'Ecole Polytechnique (Junior professor) 1995 Attaché scientifique CERN (CERN scientific associate) 2000 Professeur ordinaire à l'Université de Genève (Full professor) Scientific activities • Began research in 1974 in the Gargamelle neutrino experiment with the study of background to the Neutral Current search.
    [Show full text]
  • Shine Xenlsprio:Pormevzoifraiu Msc
    Eötvös Loránd University Faculty of Informatics Department of Computer Algebra Shine - The new software framework for the NA61 Experiment MSc. Thesis CERN-THESIS-2012-432 Supervisor: Author: Dr. Ágnes Fülöp Roland Sipos External supervisor: Programtervez˝oInformatikus MSc. Dr. András László Budapest, 2012 Contents 1 Introduction 3 1.1 Experimental physics . .3 1.2 The CERN NA61/SHINE Experiment . .4 1.3 Thesis objectives . .7 2 Legacy software 9 2.1 Software environment . .9 2.2 Software architecture . 10 3 Software upgrade 20 3.1 Lessons learned from legacy . 20 3.2 Proposal . 23 4 The Shine Offline Framework 28 4.1 Core of the framework . 28 4.2 Modules . 41 4.3 SHOE . 46 4.4 Utilities . 50 4.5 Support . 56 5 Integration of legacy software 58 5.1 Porting technique . 58 5.2 Dependencies . 63 ii CONTENTS iii 5.3 Problems . 64 5.4 Validation . 67 6 Results 68 7 Acknowledgments 71 Chapter 1 Introduction This diploma thesis is a study on the CERN NA61 software upgrade, especially to follow the advancement of the Shine Offline Software Framework. In this chapter a description is found about the topics which are related to the development, including detector setup and software systems as parts of the experiment. The most important fields concerning the software upgrade are summarized, starting with experimental physics, which is discussed in section 1.1, followed by an overview of NA61/SHINE in section 1.2. 1.1 Experimental physics In the field of physics research we need to distinguish two main branch in the ap- proach how theories become justified.
    [Show full text]
  • Neutrino Oscillations with the MINOS, MINOS+, T2K, and Nova Experiments
    New J. Phys. 18 (2016) 015009 doi:10.1088/1367-2630/18/1/015009 PAPER Neutrino oscillations with the MINOS, MINOS+, T2K, and NOvA OPEN ACCESS experiments RECEIVED 4 August 2015 Tsuyoshi Nakaya1 and Robert K Plunkett2,3 REVISED 1 Kyoto University, Department of Physics, Kyoto 606-8502, Japan 23 November 2015 2 Fermi National Accelerator Laboratory, Batavia, IL 60510, USA ACCEPTED FOR PUBLICATION 3 Author to whom any correspondence should be addressed. 24 November 2015 PUBLISHED E-mail: [email protected] and [email protected] 18 January 2016 Keywords: neutrino, particle physics, oscillations Content from this work may be used under the terms of the Creative Abstract Commons Attribution 3.0 licence. This paper discusses recent results and near-term prospects of the long-baseline neutrino experiments Any further distribution of MINOS, MINOS+, T2K and NOvA. The non-zero value of the third neutrino mixing angle θ13 allows this work must maintain attribution to the experimental analysis in a manner which explicitly exhibits appearance and disappearance dependencies author(s) and the title of on additional parameters associated with mass-hierarchy, CP violation, and any non-maximal θ .These the work, journal citation 23 and DOI. Article funded current and near-future experiments begin the era of precision accelerator long-baseline measurements 3 by SCOAP . and lay the framework within which future experimental results will be interpreted. 1. Introduction to long-baseline accelerator experiments 1.1. Motivation and three-flavor model Beginning with the successful operation of the K2K experiment [1], the physics community has seen a profound expansion of our knowledge of the mixing of neutrinos, driven by long-baseline accelerator experiments [2–6], experiments studying atmospheric neutrinos [7–9], solar neutrinos [10], and, most recently, high-precision experiments with reactor neutrinos [11].
    [Show full text]
  • The T2K Off-Axis Near Detector: Recent Physics Results
    Available online at www.sciencedirect.com Nuclear and Particle Physics Proceedings 273–275 (2016) 2696–2698 www.elsevier.com/locate/nppp The T2K off-axis near detector: recent physics results Le¨ıla Haegel, on behalf of the T2K collaboration University of Geneva, Switzerland Abstract The T2K near detector complex, ND280, is located at the J-PARC accelerator facility in Tokai, Japan, 280 meters downstream from the target. This proceeding will summarize recent physics results from ND280. Keywords: long baseline experiment, neutrino cross sections, neutrino oscillations 1. Introduction: the T2K experiment The T2K experiment is a long baseline experiment probing neutrino oscillation parameters via νe appeare- ance and νμ disappeareance [1]. The neutrino flux is generated by the J-PARC super beam and sent towards Super-Kamiokande (SK), the 50 kton water Cherenkov far detector located 295 km away and 2.5◦ off the beam axis. The near detector complex is located 280 m from the beam target and contains the on-axis INGRID de- tector which measures the beam intensity and direction, while the off-axis ND280 detector is used to constrain the event rates on SK. ND280 is a complex of detectors which are used to constrain the off-axis flux and neutrino interaction model. Charged current (CC) interactions are measured ff in the tracker, which is made of two fine grained de- Figure 1: ND280, the T2K o -axis near detector. tectors (FGDs) placed between three time projection chambers (TPCs). The FGDs provide target mass and the old UA1 magnet to recontruct the particles momenta good vertex and tracking resolution, alongside a full car- from their curvatures in the magnetic field.
    [Show full text]