| PRESS RELEASEAugust 4, 2017T2K CollaborationHigh Energy Accelerator Research Organization (KEK) Institute for Cosmic Ray Research (ICRR), University of TokyoJapan Proton Accelerator Research Complex (J-PARC) Center |
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| T2K presents hint of CP violation by neutrinos |
The international T2K Collaboration strengthened its previous hint that the symmetry between matter and antimatter may be violated for neutrino oscillation. A preliminary analysis of T2K's latest data rejects the hypothesis that neutrinos and antineutrinos oscillate with the same probability at 95% confidence (2δ) level. With nearly twice the neutrino data in 2017 compared to their 2016 results, T2K has performed a new analysis of neutrino and antineutrino data using a new event reconstruction algorithm for interactions in the far detector, Super-Kamiokande. Today's announcement was made by Prof Mark Hartz, of the University of Tokyo Kavli Institute for the Physics and Mathematics of the Universe (Japan) and TRIUMF (Canada), who presented the results at a colloquium at the High Energy Accelerator Research Organization (KEK) in Tsukuba, Japan. ( https://kds.kek.jp/indico/event/25337/) |
Why the universe is primarily comprised of matter today, instead of being comprised of equal parts matter and antimatter, is one of the most intriguing questions in all of science. One of the conditions required for the observed dominance of matter over antimatter to develop is the violation of Charge-Parity (CP) symmetry, which is the principle that the laws of physics should be the same if viewed upside-down in a mirror (Parity), with all matter exchanged with antimatter (Charge). If CP violation occurs in neutrinos, it will manifest itself as a difference in the oscillation probabilities of neutrinos and antineutrinos. |
Whether the probability for electron neutrino appearance exceeds, or not, the electron antineutrino appearance probability depends on the value of the CP violating phase, δCP, introduced by Kobayashi and Maskawa. The CP violating phase can take any value from -180° to +180° , and if it deviates from 0° and ±180° then CP violation occurs. It has been measured to be around 68° for quarks; T2K's goal is to measure the neutrino CP phase for the first time. |
In the T2K experiment in Japan, a muon neutrino beam is produced at the Japan Proton Accelerator Research Complex (J-PARC) located in Tokai village, Ibaraki prefecture, on the east coast of Japan. The neutrino beam is created by directing 30 GeV protons from the J-PARC Main Ring (MR) accelerator onto a cylindrical target to produce an intense secondary particle beam that is focused and filtered by strong magnetic lenses called neutrino horns. The focused particle beam decays into a beam of muon neutrinos or antineutrinos, depending on the filtering done by the neutrino horns. The neutrino/antineutrino beam is monitored by a detector complex in Tokai, 280 m away from the neutrino target, and is aimed at the gigantic Super-Kamiokande underground detector in Kamioka, near the west coast of Japan, 295 kilometers (185 miles) away from Tokai. During their journey, a small fraction of these muon neutrinos will turn into electron neutrinos. |
T2K's observed electron neutrino appearance rate is significantly higher than would be expected if CP symmetry were conserved. In contrast, the antineutrino data set, while still too small to make strong statements, shows a smaller electron antineutrino appearance rate than would be expected if CP symmetry were conserved. T2K observes 89 electron neutrinos while approximately 67 neutrinos are expected with no CP violation, and they observe 7 electron antineutrinos when approximately 9 are expected. When analyzed in a full framework of three neutrino and antineutrino flavors, and combined with measurements of electron antineutrino disappearance from reactor experiments, the T2K data exclude CP conservation at the 95% confidence (2δ) level. The 95% CL allowed region for the CP violating phase, δCP, is [-167° ; -34°] ([-88° ; -68°]) for the normal (inverted) hierarchy, with the best fit point being -105° (-79°). The size of the expected T2K allowed region for this data set, using the constraint from the reactor experiments, is a 95% CL region spanning approximately [-200° ; +12° ] ([-156° ; -22° ]) for the normal (inverted) hierarchy, assuming a case of maximal CP violation. |
This new data analysis includes use of an improved event reconstruction algorithm for neutrino and antineutrino interactions in Super-Kamiokande. With this new event reconstruction algorithm, the signal to background ratio of events used in the analysis is improved and the systematic errors associated with event reconstruction are reduced. Moreover, the new reconstruction algorithm allows the volume of the detector to be used more effectively for collecting neutrino interactions. This new CP violation result also includes the use of an additional selected sample of electron neutrino events at Super-Kamiokande. Taken together, the new reconstruction algorithm and the additional data sample amount to a data selection efficiency increase of 30%. |
The T2K experiment is primarily supported by the Japanese Ministry for Culture, Sports, Science, and Technology (MEXT), and is jointly hosted by the High Energy Accelerator Research Organization (KEK) and the University of Tokyo's Institute for Cosmic Ray Research (ICRR). The T2K experiment was constructed and is operated by an international collaboration, which currently consists of nearly 500 scientists from 63 institutions in 11 countries [Canada, France, Germany, Italy, Japan, Poland, Russia, Spain, Switzerland, UK, and USA]. This observation is made possible by the efforts of J-PARC to deliver high-quality beam to T2K. |
This 2017 result is based on a total data set of 2.25x1021 protons on target (POT), which is 28% of the POT exposure that T2K is set to receive. If there were no neutrino-antineutrino asymmetry, the chance of observing an asymmetry as large as what T2K observed, due to random statistical fluctuations, is about 1 in 20. To explore and solidify this intriguing hint the T2K collaboration need more neutrino and antineutrino data. The full T2K exposure of 7.8x1021 POT is expected to come by ∼2021, thanks to planned upgrades to the J-PARC MR accelerator and the neutrino beamline. Moreover, T2K has proposed a run extension that will lead to a full exposure of 20x1021 POT, with 3δ sensitivity to CP violation observation (for certain values of oscillation parameters, including the current best-fit point) by ∼2026, when the next generation experiments are expected to begin operations. An upgrade of the T2K near detector for the run extension is currently being designed, with a planned installation date of 2021. The T2K run extension has been given stage-1 status by the J-PARC Centre Directorate. |
The search for CP symmetry violation with neutrinos and antineutrinos builds on T2K's 2013 discovery of electron neutrino appearance in a muon neutrino beam, which was the first statistically significant observation of the appearance of a neutrino flavour. This appearance is an example of neutrino oscillation, a purely quantum mechanical long-range interference phenomenon; neutrino oscillation proves conclusively that neutrinos have non-zero mass. T2K's 2013 electron neutrino appearance discovery resulted in a share of the 2016 Breakthrough Prize for Fundamental Physics being awarded to Koichiro Nishikawa and the entire T2K collaboration. |
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 【 Media Contacts for Further Inquiries 】
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Globally and in Japan : Prof. Tsuyoshi Nakaya, Spokesperson, T2K Collaboration, Kyoto University (Kyoto, Japan), t.nakaya@scphys.kyoto-u.ac.jp Phone : +81-75-753-3870 |
Globally and in U.K. : Dr. Morgan Wascko, International Co-Spokesperson, T2K Collaboration, Imperial College London, m.wascko@imperial.ac.uk Phone: +44-207-594-3465, +44-7939-592-708 |
In Canada : Prof. Hirohisa Tanaka, University of Toronto (Toronto, Canada), htanaka@physics.utoronto.ca Phone: +1-647-549-3690 |
In France : Dr. Marco Zito, CEA/IRFU (Saclay, France), marco.zito@cea.fr Phone: +33 6 84 61 09 51 Dr Jacques Dumarchez, IN2P3/CNRS (Paris, France), jacques.dumarchez@cern.ch Phone: +33 1 44 27 48 42 |
In Germany : Dr. Stefan Roth, RWTH Aachen University (Aachen, Germany), roth@physik.rwth-aachen.de Phone: +49 241 80 27296 |
In Italy : Dr. Maria Gabriella Catanesi, INFN Sezione di Bari (Bari, Italy), gabriella.catanesi@cern.ch Phone: +41 764871532 |
In Poland : Prof. Ewa Rondio, NCBJ, Warsaw (Warsaw, Poland), Ewa.Rondio@fuw.edu.pl Phone: +48 691 150 052 |
In Russia : Prof. Yuri Kudenko, INR (Moscow, Russia), kudenko@inr.ru Phone: +7-903-6159125 (c), +7-495-8504248 (o) |
In Spain : Prof. Federico Sanchez, IFAE, Barcelona (Barcelona, Spain), fsanchez@ifae.es Phone : +34 93 5812835 Prof. Anselmo Cervera, IFIC, Valencia (Valencia, Spain), anselmo.cervera@cern.ch |
In Switzerland : Prof. Alain Blondel, Université de Genève, alain.blondel@unige.ch Phone : +41 22 379 6227 |
In U.K. : Prof. Dave Wark, STFC/RAL/Daresbury Laboratory/Oxford University (Oxford, U.K.), david.wark@stfc.ac.uk Phone: +44 7788186085 |
In U.S.A. : Prof. Chang Kee Jung, State University of New York at Stony Brook (Stony Brook, NY, USA), chang.jung@stonybrook.edu Phone: +1 631-707-2018 |
About KEK : Hajime Hikino, PR office, High Energy Accelerator Organization (KEK, Japan) press@kek.jp Phone: +81-29-879-6046 |
About ICRR : Hironori Fukuda, the University of Tokyo's Institute for Cosmic Ray Research (ICRR, Japan) hfukuda@icrr.u-tokyo.ac.jp Phone: +81-4-7136-5148 |
About J-PARC : Saeko Okada, PR section, J-PARC pr-section@j-parc.jp Phone: +81-29-284-4578 |
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