Japan Eyes up Its Future
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P> Pos(HEP2005)???
PoS(HEP2005)??? Longer term R&D on Neutrino beams and Neutrino Factories Ken Peach John Adams Institute for Accelerator Science University of Oxford and Royal Holloway Univerity of London Denys Wilkinson Building, Keble Road, Oxford OX1 3RH, UK E-mail: [email protected] Recent developments in neutrino physics, primarily the demonstration of neutrino oscillations in both atmospheric neutrinos and solar neutrinos, provide the first conclusive evidence for physics beyond the Standard Model of particle physics. The phenomenology of neutrino oscillations, for three generations of neutrino, requires six parameters - two squared mass differences, 3 mixing angles and a complex phase that could, if not 0 or π, contribute to the otherwise unexplained baryon asymmetry observed in the universe. Exploring the neutrino sector will require very intense beams of neutrinos, and will need novel solutions. European Physical Society HEP2005 International Europhysics Conference on High Energy Physics EPS (July 21st-27th 2005) in Lisboa, Portugal PoS(HEP2005)??? 1. Introduction The “Standard Model” of particles and interactions provides an accurate description of huge volumes of data, from LEP, HERA, Tevatron, and experiments like the muon g-2. However, convincing evidence [1] for neutrino oscillations, where neutrinos created in a flavour eigenstate (e.g, as νe in the sun) are subsequently found to be a mixture of flavours, indicates that neutrinos have a mass (however small), while the Standard Model requires the neutrinos to be strictly massless. It is difficult to add a mass term for the neutrinos, in analogy to the quarks and charged leptons, and so neutrino oscillations require physics “beyond the Standard Model”. -
A Staged Muon Accelerator Facility for Neutrino
A STAGED MUON ACCELERATOR FACILITY FOR NEUTRINO AND COLLIDER PHYSICS* Jean-Pierre Delahaye, SLAC, Menlo Park, California Charles Ankenbrandt, Stephen Brice, Alan David Bross, Dmitri Denisov, Estia Eichten, Stephen Holmes, Ronald Lipton, David Neuffer, Mark Alan Palmer, Fermilab, Batavia, Illinois S. Alex Bogacz, JLAB, Newport News, Virginia Patrick Huber, Virginia Polytechnic Institute and State University, Blacksburg Daniel M. Kaplan, Pavel Snopok, Illinois Institute of Technology, Chicago, Illinois Harold G. Kirk, Robert B. Palmer, BNL, Upton, Long Island, New York Robert D. Ryne, LBNL, Berkeley, California Abstract THE BEAUTY AND CHALLENGES OF Muon-based facilities offer unique potential to provide MUON-BASED FACILITIES capabilities at both the Intensity Frontier with Neutrino Muon-based facilities [1] offer the unique potential to Factories and the Energy Frontier with Muon Colliders. provide the next generation of capabilities and world- They rely on a novel technology with challenging leading experimental support spanning physics at both the parameters, for which the feasibility is currently being Intensity and Energy Frontiers. Building on the evaluated by the Muon Accelerator Program (MAP). A foundation of PIP-II and its successor stages at FNAL [2], realistic scenario for a complementary series of staged muon accelerators can provide the next step with a high- facilities with increasing complexity and significant intensity and precise source of neutrinos to support a physics potential at each stage has been developed. It world-leading research program in neutrino physics. takes advantage of and leverages the capabilities already Furthermore, the infrastructure developed to support such planned for Fermilab, especially the strategy for long- an Intensity Frontier research program can also enable the term improvement of the accelerator complex being return of the U.S. -
Neutrinos and Beyond — Opening a New Era of Cosmic-Ray Research
ADVERTISEMENT FEATURE THE UNIVERSITY OF TOKYO Neutrinos and beyond — Opening a new era of cosmic-ray research Takaaki Kajita, a recipient of the 2015 that neutrinos are massless. These discov- Nobel Prize in Physics, and other re- eries, which resulted in Kajita’s 2015 Nobel searchers at the University of Tokyo’s Prize in Physics, were made a team led by Institute for Cosmic Ray Research (ICRR) him in 1998. have been exploring new realms in par- Kajita acknowledged his success owed ticle physics research. Kajita’s work on a lot to the strong support he received neutrinos and related research at ICRR from two mentors and former supervisors is leading the world in this field. — Masatoshi Koshiba and Yoji Totsuka. Koshiba was awarded the 2002 Nobel Prize The path to a Nobel prize in Physics for detecting neutrinos pro- Particle physics and astrophysics are duced in supernovae using Kamiokande, among the most active research fields at the predecessor of Super-Kamiokande. the University of Tokyo, and its Institute for Totsuka led the Super-Kamiokande proj- Cosmic Ray Research (ICRR) is leading the ect as Koshiba’s successor. Totsuka’s con- world with explorations in these areas. ICRR tribution was so great that many believe is best known for its research on neutrinos he would have shared the Nobel Prize with using the world’s largest underground neu- Kajita if he were alive. trino detector, Super-Kamiokande. The de- Kajita’s award-winning work dates tector is located in a mine in central Japan back to 1986 when he earned his PhD for and is filled with 50,000 tons of pure water. -
Session: Neutrino Astronomy
Session: Neutrino Astronomy Chair: Takaaki Kajita, Institute for Cosmic Ray Research, Univ. of Tokyo Basic natures of neutrinos Neutrino was introduced in 1930 by W. Pauli in order to save the energy conservation law in nuclear beta decay processes, in which the emitted electron exhibits a continuous energy spectrum. It was assumed that the penetration power of neutrinos is much higher than that of the gamma rays. More than 20 years later, the existence of neutrinos was experimentally confirmed by an experiment that measured neutrinos produced by a nuclear power reactor. Since then, the basic nature of neutrinos has been understood through various theoretical and experimental studies: Neutrinos interact with matter extremely weakly. The number of neutrino species is three. They are called electron-neutrino, muon-neutrino and tau-neutrino. In addition, recent neutrino experiments discovered that neutrinos have very small masses. Observing the Universe by neutrinos (1) Because of the extremely high penetration power of neutrinos, neutrinos produced at the center of a star easily penetrate to the outer space. Theories of astrophysics predict that there are various processes that neutrinos play an essential role at the center of stars. For example, the Sun is generating its energy by nuclear fusion processes in the central region. In these processes, low energy electron neutrinos with various energy spectra are generated. Thus the observation of solar neutrinos directly probes the nuclear fusion reactions in the Sun. Another example is the supernova explosion. While the optical measurements observe an exploding star, what is happening in the central region of the star is the collapse of the core of a massive star. -
Carsten Rott Curriculum Vitae Feb 2018
Carsten Rott Curriculum Vitae Feb 2018 Department of Physics, Sungkyunkwan University, Suwon 16419, Korea Tel: +82-31-290-5902 E-mail:[email protected] Experimental astro-particle physics, particle physics, geophysics, neutri- Research nos physics Focus Languages German, English; Elementary: French, Japanese, and Korean Employment 2017 { 2018 Honorary Fellow at Wisconsin IceCube Particle Astrophysics Center (WIPAC) (Sabbatical), University of Wisconsin Madison, USA 2017 { now Associate Professor, Sungkyunkwan University, Korea 2013 { 2017 Assistant Professor, Sungkyunkwan University, Korea 2016 Visiting Researcher (3-month), University of Tokyo, Japan 2009 { 2013 Senior Fellow of the Center for Cosmology and AstroParticle Physics (CCAPP) (5-year term), The Ohio State University, USA 2008 { 2009 CCAPP Fellow (3-year term), The Ohio State University, USA 2005 { 2008 Postdoctoral Fellow, Pennsylvania State University, USA Education 1998 { 2004 Purdue University, Indiana, USA Ph.D in Experimental Particle Physics (December 2004) Title : \Search for Scalar Bottom Quarks from Gluino Decays" at CDF Thesis Adviser : Prof. Daniela Bortoletto 1995 { 1998 Universit¨atHannover, Hannover, Germany Honors and Awards 2011 Recipient of NSF Antarctica Service Medal 2005 \Fermilab's Result of the Week" (FermiNews, August 11, 2005) 2004 George W. Tautfest Award, Purdue University 1998 { 1999 University of Hannover { Purdue University direct exchange fellowship Funds and Grants 2017 { present NRF Midscale Research Fund (PI), Korea { NRF-2017R1A2B2003666 2017 { present Foreign Facility Fund (PI of 7 sub-PIs) { NRF-2017K1A3A7A09015973 2016 { present NRF SRC Korea Neutrino Research Center (KNRC) (Co-I), Korea 2016 { 2017 NRF Individual Researcher (PI), Korea { NRF-2016R1D1A1B03931688 2013 { present BrainKorea (BK21plus) participant, Korea 2013 { 2016 NRF Individual Researcher (PI), Korea { NRF-2013R1A1A1007068 2013 { 2014 SKKU Intramural Faculty Fund Award, Korea 2013 { 2014 Fermi GI Cycle 6 (Co-I with Prof. -
An International Scoping Study of a Neutrino Factory and Super-Beam
ISS/2005/01 13 th July 2005 An international scoping study of a Neutrino Factory and super-beam facility Executive summary This document presents a plan for an international scoping study of a future accelerator neutrino complex. The physics case for the facility will be evaluated and options for the accelerator complex and neutrino detection systems will be studied. The principal objective of the study will be to lay the foundations for a full conceptual-design study of the facility. The plan for the scoping study has been prepared in collaboration by the international community that wishes to carry it out; the ECFA/BENE network in Europe, the Japanese NuFact-J collaboration, the US Muon Collider and Neutrino Factory Collaboration and the UK Neutrino Factory collaboration. CCLRC’s Rutherford Appleton Laboratory will be the ‘host laboratory’ for the study. The study will be directed by a Programme Committee advised by a Stakeholders Board. The the international scoping study was launched at NuFact05 in Frascati on the 26 th June 2005. The conclusions of the study will be presented at NuFact06 and published in a written report in September 2006. 1. Introduction 1.1 Overview The recent discovery of neutrino oscillations [1] implies that neutrinos are massive and that the Standard Model is incomplete. These observations may have profound astrophysical consequences; in particular CP violation in the lepton sector may underpin the mechanism by which antimatter was removed from the early universe. The far-reaching implications of neutrino oscillations justify a dedicated experimental programme while the search for leptonic-CP violation requires the development of well-characterised, high-energy neutrino beams of extremely high intensity. -
Strengthening Global Coordination on Large Neutrino Infrastructures”
July 8, 2016 Press Release concerning the 3rd International Neutrino Meeting on Large Neutrino Infrastructures hosted by KEK on the 30-31st of May 2016 “Strengthening global coordination on large neutrino infrastructures” Funding-agency1 and laboratory representatives2 gathered at the 3rd International Meeting on Large Neutrino Infrastructures3 on May 30-31, 2016 at KEK in Tsukuba, Japan to gauge the progress in the global coordination of projects that had been launched during the first and second international meetings4 and to discuss the next steps in the global coordination. The meeting was opened by the 2015 Nobel Prize winner Takaaki Kajita who commented that “Very large-scale experiments will be needed to fully explore neutrino properties. These large-scale experiments will also naturally have astrophysics potential and increase the sensitivity of searches for proton disintegration.” He went on to note that to realise the necessary very large-scale facilities would require “… international coordination and collaboration” and defined the goals of the meeting to be to “… discuss the physics cases and global strategy, including astrophysics and proton decays, which are the part of the aim of this series of meetings; have follow-up discussions of the ICFA Neutrino Panel’s5 roadmap discussion document”6 and to discuss “… the various neutrino experiments, including Hyper- Kamiokande7, toward the realization of an efficient and productive global neutrino program.” In this meeting, the funding-agency and laboratory representatives welcomed the important steps that had been made towards the realisation of the Hyper-Kamiokande (Hyper-K) experiment7. The international proto-collaboration has developed new, high- sensitivity, large-aperture photomultiplier tubes that substantially reduce the total project cost without unduly compromising its potential to address important questions in particle and astroparticle physics and in nucleon decay. -
Research in Kamioka and Kakenhi Takaaki Kajita Director of Institute for Cosmic Ray Research (ICRR) the University of Tokyo Rese
Research in Kamioka and Kakenhi Takaaki Kajita Director of Institute for Cosmic Ray Research (ICRR) The University of Tokyo Research Theme Implemented in FY2017: First Detection of Gravitational Waves Using Cryogenic Laser Interferometer (Grant-in-Aid for Specially Promoted Research) I have conducted research underground Kamioka, Gifu Prefecture, since I was a graduate student. The first experiment I participated in was the Kamioka Nucleon Decay Experiment (Kamiokande). The experiment was initially proposed by Professor Masatoshi Koshiba, who was my thesis advisor, to search for proton decay. Professor Koshiba collaborated with a company to develop an unprecedentedly large 50-centimeter diameter photomultiplier tube (PMT) for the Kamiokande experiment. The PMT served a very important role in supernova neutrino observations that verified the supernova explosion mechanism and solar neutrino observations that confirmed the so-called solar neutrino problem. It is well known that, due to these achievements, Professor Koshiba received the Nobel Prize in physics in 2002. It is common for a large apparatus such as this to be realized by submitting a budget request from a host institute after long, vigorous discussions in relevant researcher communities. In this case, however, the enthusiasm of the relevant researchers in view of the importance of Kamiokande experiments made it possible to realize the experiment quickly with funds from various sources. Kamiokande initially materialized through collaboration with the University of Tokyo’s School of Science, to which Professor Koshiba belonged, the former National Laboratory for High Energy Physics (KEK), and the Institute for Cosmic Ray Research (ICRR) of the University of Tokyo. Although I was only a graduate student at that time and knew nothing about budgets, all of us participating in the effort recognized that people thought that this experiment was very important and endeavored to realize it as soon as possible. -
Accelerator Neutrino Programme at Fermilab ∗
FERMILAB-CONF-10-099-T Accelerator Neutrino Programme at Fermilab ∗ Stephen J. Parke Theoretical Physics Department, Fermi National Accelerator Laboratory P.O.Box 500, Batavia, IL 60510, USA [email protected] The accelerator neutrino programme in the USA consists primarily of the Fermilab neutrino programme. Currently, Fermilab operates two neu- trino beamlines, the Booster neutrino beamline and the NuMI neutrino beamline and is the planning stages for a third neutrino beam to send neutrinos to DUSEL. The experiments in the Booster neutrino beamline are miniBooNE, SciBooNE and in the future microBooNE, whereas in the NuMI beamline we have MINOS, ArgoNut, MINERVA and coming soon NOνA. The major experiment in the beamline to DUSEL will be LBNE. 1. Neutrino Standard Model The flavor content of the three neutrino mass eigenstates is given in Fig. 1. The current questions in this model are what is the size of 2 2 1 2 1 2 sin θ13; (sin θ23 ); (sin θ12 ); sign(δm ) and sin δCP (1) − 2 − 3 31 It is possible that the first three of these are related to some small parameter 2 2 like δm21/δm31 0:03 raised to some power, n. From current experiments the size of this power≈ is constrained to be larger than one, n > 1, except for 2 1 (sin θ23 ) where the lower bound is weaker, approximately n > 1=2. − 2 This could be due to some broken Tri-Bi-Maximal symmetry which would be very interesting and exciting. Another possibility is that it is coincidental which would be much less interesting from a theorists perspec- tive. -
1 FY 2015 Follow-Up of WPI Program by Program Committee February
FY 2015 Follow-up of WPI Program By Program Committee February 2016 (This document reports on progress made under the WPI Program in FY 2014.) In FY2015, there were three important achievements: 1. Nobel Prize in physics awarded to Dr. T. Ka j i t a, P I of Kavli IPMU. (see section A, p2) 2. International Research Excellence Initiative (REI) workshop held jointly with Program committee meeting. (see section E, p5) 3. Future plan devised by the WPI program committee (see section E, p5) A. Dr. Takaaki Kajita, PI of Kavli IPMU, was awarded The 2015 Nobel Prize .................................... 2 B. Outline of WPI program .......................................................................................................... 2 C. WPI Centers ........................................................................................................................... 3 D. Follow up ............................................................................................................................... 4 E. REI International Workshop and 2015 Program committee meeting ........................................... 4 E-1. REI International Workshop ................................................................................... 5 E-2. Program committee meeting .................................................................................. 5 E-3. Future plan of WPI program ................................................................................... 5 F. Site visits .............................................................................................................................. -
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, -
Muon Collider and Neutrino Factory Overview
International Committee for Future Accelerators Sponsored by the Particles and Fields Commission of IUPAP Beam Dynamics Newsletter No. 55 Issue Editor: M. A. Palmer Editor in Chief: W. Chou August 2011 3 Contents 1 FOREWORD ............................................................................................................. 9 1.1 FROM THE CHAIRMAN ............................................................................................... 9 1.2 FROM THE EDITOR .................................................................................................. 10 2 MUON COLLIDER AND NEUTRINO FACTORY OVERVIEW ................... 12 2.1 TOWARDS A MUON COLLIDER ................................................................................ 12 2.1.1 Physics Landscape ........................................................................................ 12 2.1.2 Neutrino Factory ........................................................................................... 13 2.1.3 Muon Collider Physics ................................................................................. 15 2.1.3.1 Basics.............................................................................................. 15 2.1.3.1.1 Pair Production ............................................................... 15 2.1.3.1.2 Resonances ..................................................................... 15 2.1.3.1.3 Fusion Processes ............................................................ 16 2.1.3.2 Standard Model Higgs Bosons ......................................................