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Book of Abstracts
12th International Neutrino Summer School 2019 Monday 05 August 2019 - Friday 16 August 2019 Fermi National Accelerator Laboratory Book of Abstracts Contents Intro to Group Exercises .................................... 1 Neutrinos and nuclear non-proliferation ........................... 1 INSS2019 welcome and introduction .............................. 1 Solar and Reactor Neutrino Experiments ........................... 1 Precise Measurement of Reactor Antineutrino Oscillation Parameters and Fuel-dependent Variation of Antineutrino Yield and Spectrum at RENO ................. 1 Using Convolutional Neural Networks to Reconstruct Dead Channels in MicroBooNE . 1 Origin and Nature of Neutrino Mass I ............................. 2 Introduction to Leptogenesis .................................. 2 Origin and Nature of Neutrino Mass II ............................ 2 Direct Neutrino Mass Measurements ............................. 2 Neutrinoless Double-beta Decay Experiments ........................ 2 Neutrino Beams and Fluxes .................................. 3 Lepton-Nucleus Cross Section Theory ............................. 3 Neutrino Cross Section Experiments ............................. 3 Origin and Nature of Neutrino Mass III ............................ 3 Particle Astrophysics with High-Energy Neutrinos ..................... 3 Neutrino Detection II ...................................... 3 Phenomenology of Atmospheric and Accelerator Neutrinos ................ 3 Tau neutrinos and upward-going air showers: stochastic versus continuous -
Design and Construction of the Microboone Detector
BNL-113631-2017-JA Design and Construction of the MicroBooBE Detector The MicroBooNE Collaboration Submitted to Journal of Instrumentation January 17, 2017 Physics Department Brookhaven National Laboratory U.S. Department of Energy USDOE Office of Science (SC), High Energy Physics (HEP) (SC-25) Notice: This manuscript has been co-authored by employees of Brookhaven Science Associates, LLC under Contract No. DE-SC0012704 with the U.S. Department of Energy. The publisher by accepting the manuscript for publication acknowledges that the United States Government retains a non-exclusive, paid-up, irrevocable, world-wide license to publish or reproduce the published form of this manuscript, or allow others to do so, for United States Government purposes. DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, nor any of their contractors, subcontractors, or their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or any third party’s use or the results of such use of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof or its contractors or subcontractors. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof. -
The Hunt for Sub-Gev Dark Matter at Neutrino Facilities: a Survey of Past and Present Experiments
Prepared for submission to JHEP The hunt for sub-GeV dark matter at neutrino facilities: a survey of past and present experiments Luca Buonocore,a;b Claudia Frugiuele,c;d Patrick deNivervillee;f aDipartimento di Fisica, Università di Napoli Federico II and INFN, Sezione di Napoli, I-80126 Napoli, Italy bPhysik Institut, Universität Zürich, CH-8057 Zürich, Switzerland cCERN, Theoretical Physics Departments, Geneva, Switzerland dINFN, Sezione di Milano, Via Celoria 16, I-20133 Milano, Italy. eCenter for Theoretical Physics of the Universe, IBS, Daejeon 34126, Korea f T2, Los Alamos National Laboratory (LANL), Los Alamos, NM, USA E-mail: [email protected], [email protected], [email protected] Abstract: We survey the sensitivity of past and present neutrino experiments to MeV-GeV scale vector portal dark matter and find that these experiments possess novel sensitivity that has not yet fully explored. Taking αD = 0:1 and a dark photon to dark matter mass ratio of three, the combined recast of previous analyses of BEBC and a projection of NOνA’s sensitivity are found to rule out the scalar thermal target for dark matter masses between 10 MeV to 100 MeV with existing data, while CHARM-II and MINERνA place somewhat weaker limits. These limits can be dramatically improved by off-axis searches using the NuMI beamline and the MicroBooNE, MiniBooNE or ICARUS detectors, and can even begin to probe the Majorana thermal target. We conclude that past and present neutrino facilities can search for light dark matter concurrently with their neutrino program and reach a competitive sensitivity to proposed future experiments. -
Search for Electron Neutrinos in Multiple Topologies with the Microboone Experiment
Search for Electron Neutrinos in Multiple Topologies with the MicroBooNE Experiment MICROBOONE-NOTE-1085-PUB The MicroBooNE Collaboration June 23, 2020 Abstract This note presents the status of the measurement of electron neutrinos from the Fermilab Booster Neutrino Beamline (BNB) with the MicroBooNE experiment. The analysis is aimed at investigating the nature of the low energy excess of electromagnetic activity observed by the MiniBooNE experiment. The νe event selection relies on topological and calorimetric information to characterise particles produced in these interactions, leveraging the Pandora multi-algorithm reconstruction framework as well as custom particle identification and pattern recognition tools. Results presented in this note use 5:88 × 1020 protons on target of data collected between 2015 and 2018. These include the performance of particle identification tools for µ/p and e/γ separation, along with electromagnetic shower calibration with the largest sample of π0 events measured on argon. Progress towards the completion of this analysis is shown through the measurement of high-energy charged-current νe interactions and their kinematic distributions using both inclusive (1eX) and exclusive (1e0p0π and 1eNp0π) channels. Measurements of charged-current νµ interactions aimed at constraining flux and cross-section systematic uncertainties are also shown. We present the analysis' preliminary sensitivity of an electron-like signal hypothesis to the MiniBooNE excess which includes flux, cross-section, and detector systematic uncertainties. 1 Contents 1 Introduction 3 2 Analysis Approach3 3 Event Reconstruction and Analysis Tools4 4 Electron Neutrino Event Selection7 5 Muon Neutrino Constraint, Systematics, and Analysis Sensitivity 13 6 Selected Electron Neutrinos at High Energy 15 7 Conclusions 16 A Measuring Electron Neutrinos with Particle Identification in the MicroBooNE LArTPC for sensitivity to new Physics 17 B Charged-Current Electron Neutrino Measurement with the MicroBooNE De- tector 20 B.1 Electron identification.................................. -
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. -
Arxiv:1804.03238V1 [Hep-Ex] 9 Apr 2018
SNSN-323-63 April 11, 2018 Neutrino Cross Sections: Status and Prospects M. F. Carneiro1 Department of Physics, Oregon State University, Corvallis, Oregon 97331, USA We summarize the current status of accelerator based neutrino cross- section measurements. We focus on the experimental challenges while also presenting the motivation for these measurements. Selected results are highlighted after a quick description of the current major collaborations working on the field. PRESENTED AT arXiv:1804.03238v1 [hep-ex] 9 Apr 2018 NuPhys2017, Prospects in Neutrino Physics Barbican Centre, London, UK, December 20{22, 2017 1This work was supported by NSF Award PHY-1505472. 1 Introduction Neutrino physics is entering a new era of precision measurements and cross section measurements play a vital part. We will not discuss in details the effect of cross section measurements on systematic uncertainties as it has been well described in the literature [1, 2, 3, 4], but rather focus on the experimental difficulties of these measurements as well as show the shortcomings of the current theoretical models de- scribing neutrino-nucleus scattering. We also highlight new results from MINERvA, MicroBooNE, NoVA and T2K which have been released or presented in public con- ferences prior to the time of the NuPhys Workshop (December 2017) as well as given a quick description of each experiment. In Section 1, we discuss the common general goals of the program; in Section 2 we present the experimental difficulties involved in these measurements; Section 3 have a quick description of the effects for oscillation experiments; in Section 4 highlight new results and in Section 5 we summarize and discuss future directions. -
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 . -
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. -
Luke Pickering on Behalf of NUISANCE
nuisance.hepforge.org github.com/NUISANCEMC/nuisance nuisance-xsec.slack.com [email protected] Luke Pickering on behalf of NUISANCE NuSTEC board meeting 2019 ● T2K, MINERvA, DUNE collaborators ● A breadth of experience using GENIE, NuWro, NEUT, GiBUU ● Have worked on neutrino cross-sections measurements, generators dev. and oscillation analyses on T2K and DUNE ● Stared at, thought about, and discussed a lot of neutrino interaction measurements (at NuSTEC and elsewhere) ● Developed interaction systematics for T2K and DUNE analyses ● Started as PhD project, now junior postdocs L. Pickering C. Wret C. Wilkinson ● What is NUISANCE? ● What have we done with NUISANCE? ● What do we plan to do with NUISANCE? ● How can NUISANCE be used in conjunction with NuSTEC? L. Pickering 3 ● Converts generator output from GENIE, NuWro, NEUT, GiBUU and NUANCE ● Uses a common event format with common functions (e.g. GetLepton(), GetQ2(), GetFinalState() ) With all generators in the same format, it’s easy to produce ● Generator-to-generator comparisons ● Model to model comparisons ● Comparison to data ● If event reweighting is available (GENIE, NEUT, NuWro): ○ Fit parameters to data ○ Evaluate uncertainty bands against data ○ Evaluate uncertainties against each other JINST 12 (2017) no. 01, P01016 L. Pickering 4 Compare effect of systematics on distributions from the same generator Effect of MAQE on generated NuWro events versus MiniBooNE CCQE data L. Pickering 5 Compare different generators and their models in a “flat-tree” format CC0π final state from NuWro with Nieves 2p2h CC0π final state from GENIE with Empirical 2p2h L. Pickering 6 Compare your favourite generators and models, which does best/worst? L. -
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. -
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, -
The ICARUS Experiment †
universe Communication The ICARUS Experiment † Christian Farnese and on behalf of the ICARUS Collaboration Dipartimento di Fisica ed Astronomia, Universita degli Studi di Padova, ed INFN, 35131 Sezione di Padova, Italy; [email protected] † This paper is based on the talk at the 7th International Conference on New Frontiers in Physics (ICNFP 2018), Crete, Greece, 4–12 July 2018. Received: 28 November 2018; Accepted: 25 January 2019; Published: 29 January 2019 Abstract: The 760-ton ICARUST600 detector has completed a successful three-year physics run at the underground LNGSlaboratories, searching for atmospheric neutrino interactions and, with the CNGSneutrino beam from CERN, performing a sensitive search for LSND-like anomalous ne appearance, which contributed to constraining the allowed parameters to a narrow region around Dm2 ∼ eV2, where all the experimental results can be coherently accommodated at 90% C.L. The T600 detector underwent a significant overhaul at CERN and has now been moved to Fermilab, to be soon exposed to the Booster Neutrino Beam (BNB) to search for sterile neutrinos within the SBNprogram, devoted to definitively clarifying the open questions of the presently-observed neutrino anomalies. This paper will address ICARUS’s achievements, its status, and plans for the new run and the ongoing analyses, which will be finalized for the next physics run at Fermilab. Keywords: neutrino physics; liquid argon; TPC 1. The ICARUS T600 Detector A very promising detection technique for the study of rare events such as the neutrino interactions is based on the Liquid Argon Time Projection Chamber (LAr-TPC). These detectors, first proposed by C.Rubbia in 1977 [1], combine the imaging capabilities of the famous bubble chambers with the excellent energy measurement of huge electronic detectors.