35. Particle Detectors for Non-Accelerator Physics
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Future Plan of the Pandax Experiment
Future plan of the PandaX Experiment - report at the CJPL International Advisory Committee meeting PandaX Collaboration, 9 Nov., 2016 The PandaX (Particle and astrophysical Xenon) observatory uses xenon as target and detector to search for WIMP particles as well as neutrinoless double beta decay (NLDBD) in 136Xe. At present, the PandaX-II experiment is in operation in CJPL-I. The future PandaX program will pursue the following three main directions: 1. Continue the operation of PandaX-II until a total of 2-year exposure; 2. Develop and operate a multi-ton multi-purpose liquid xenon experiment, PandaX-xT, to push further the dark matter search; 3. Develop and operate a 200-kg (upgradable to ton-scale) high pressure gas TPC (HpgTPC), PandaX-III, to search for NLDBD in 136Xe. Each direction is elaborated below. PandaX-II operation PandaX-II has published the world leading WIMP limit with a 99-day exposure, reaching an upper limit to spin-independent WIMP-nucleon cross section of 2.5x10-46cm2 [1]. The current plan is to maintain stable operation until we have data with a 2-year total live time. Calibration runs will be interleaved to monitor the detector response. The wealth of low background data will allow us to pursue many different physics analyses (in additional to the standard WIMP- nucleon elastic scattering), including constraints to generic WIMP-nucleon operators, light WIMPs, inelastic WIMPs, limits to solar and galactic axions, etc. We will also use the PandaX-II detector to test new technologies for a future multi-ton detector, e.g. online Kr removal, upgrade of the trigger/electronics system to achieve a lower threshold and a higher data bandwidth, alternative electron recoil and nuclear recoil calibrations, etc. -
Km3net/ORCA Telescopes
Search for light sterile neutrinos with ANTARES and KM3NeT/ORCA telescopes A. Domi1,2, J. A. B. Coelho3, T. Thakore4, for the ANTARES and KM3NeT Collaborations 1 Università degli Studi di Genova, Genoa (Italy) - [email protected] 2 INFN-Genova, Genoa (Italy) 3 LAL, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, Orsay (France) - [email protected] 4 University of Cincinnati, Ohio (United States) - [email protected] VLVnT Workshop - 19/05/2021 1 Where are we with light sterile neutrinos? • Majority of experiments have confirmed the 3 flavour neutrino oscillations. • In parallel, anomalies observed in some oscillation experiments: Anomalies in Short baseline (SBL) Ref: Prog.Part.Nucl.Phys. 111 (2020) 103736 experiments •LSND: �� -> �e •MINIBooNE: �� -> �e / �� -> �e Gallium Anomalies: �e disappearance Reactor anomalies: e disappearance � Disagreement between appearance and disappearance NO ANOMALIES observed in / disappearance. Further observations needed! �� �� 2 Where are we with light sterile neutrinos? Cosmology • Constrains the effective number of relativistic species (Neff) in our universe. • A SBL neutrino would require Neff=4. • Measured Neff compatible with 3. -> Tension with SBL anomalies. • Tension relaxes when cosmological data are combined with astrophysical data. • Cosmological data alone can be compatible with • an eV-mass sterile neutrino only if its contribution to Neff is very small, • a larger Neff only if it comes from a nearly massless sterile particle. We need further observations: neutrino telescopes make it possible! 3 Sterile Neutrinos • Oscillations in the presence of sterile neutrinos are solutions of: 2 • Adding one sterile neutrino introduces 6 more free parameters: �m41 , 3 mixing angles (�14,�24,�34) and 2 more CP phases (�14, �24). -
The ANTARES and Km3net Neutrino Telescopes: Status and Outlook for Acoustic Studies
EPJ Web of Conferences 216, 01004 (2019) https://doi.org/10.1051/epjconf/201921601004 ARENA 2018 The ANTARES and KM3NeT neutrino telescopes: Status and outlook for acoustic studies Véronique Van Elewyck1,2, for the ANTARES and KM3NeT Collaborations 1APC, Université Paris Diderot, CNRS/IN2P3, CEA/Irfu, Observatoire de Paris, Sorbonne Paris Cité, France 2Institut Universitaire de France, 75005 Paris, France Abstract. The ANTARES detector has been operating continuously since 2007 in the Mediterranean Sea, demonstrating the feasibility of an undersea neutrino telescope. Its superior angular resolution in the reconstruction of neutrino events of all flavors results in unprecedented sensitivity for neutrino source searches in the southern sky at TeV en- ergies, so that valuable constraints can be set on the origin of the cosmic neutrino flux discovered by the IceCube detector. The next generation KM3NeT neutrino telescope is now under construction, featuring two detectors with the same technology but different granularity: ARCA designed to search for high energy (TeV-PeV) cosmic neutrinos and ORCA designed to study atmospheric neutrino oscillations at the GeV scale, focusing on the determination of the neutrino mass hierarchy. Both detectors use acoustic devices for positioning calibration, and provide testbeds for acoustic neutrino detection. 1 Introduction Neutrinos have long been proposed as a complementary probe to cosmic rays and photons to explore the high-energy (HE) sky, as they can emerge from dense media and travel across cosmological dis- tances without being deflected by magnetic fields nor absorbed by inter- and intra-galactic matter and radiation. HE (>TeV) neutrinos are expected to be emitted in a wide range of astrophysical objects. -
Pos(ICHEP2020)886
The Outer Detector (OD) system for the Hyper-Kamiokande experiment PoS(ICHEP2020)886 Stephane Zsoldos0,1,2,∗ 0Department of Physics, King’s College London, Strand, London WC2R 2LS, United Kingdom 1Department of Physics, University of California, Berkeley, CA 94720, Berkeley, USA 2Lawrence Berkeley National Laboratory, 1 Cyclotron Road, Berkeley, CA 94720-8153, USA E-mail: [email protected], [email protected] Hyper-Kamiokande, scheduled to begin construction as soon as 2020, is a next generation under- ground water Cherenkov detector, based on the highly successful Super-Kamiokande experiment. It will serve as a far detector, 295 km away, of a long baseline neutrino experiment for the upgraded J-PARC beam in Japan. It will also be a detector capable of observing — far beyond the sensitivity of the Super-Kamiokande detector — proton decay, atmospheric neutrinos, and neutrinos from astronomical sources. An Outer Detector (OD) consisting of PMTs mounted behind the inner detector PMTs and facing outwards to view the outer shell of the cylindrical tank, would provide topological information to identify interactions originating from particles outside the inner detector. Any optimization would lead to a significant improvement for the physics goals of the experiment, which are the measurement of the CP leptonic phase and the determination of the neutrino mass hierarchy. An innovative new setup using small 3" PMTs is being proposed for the Hyper-Kamiokande OD. They would give better redundancy, spatial, and angular resolution, as there would be twice or three times more photosensors that the original 8" design proposal of the experiment, and for a reduced cost. -
Ankur Sharma
Ankur Sharma Date of Birth 2nd August 1991 Gender Male Nationality Indian Phone +46 76 447 51 45 Address Eklundshovsvägen 4B, Lgh 1104 Email [email protected] 752 37, Uppsala, Sweden [email protected] Research Interests Phenomenological studies of VHE emission from jets of AGNs; multi-messenger and multi-wavelength connection in blazars with neutrino, gamma-ray and X-ray data; gamma-ray astronomy; observability of point sources with Cherenkov neutrino telescopes; detection strategies for ultra-high energy neutrinos Education Jan 2017 - PhD in Physics - University of Pisa (Italy) Present Area of study - Astroparticle Physics, Neutrino Astrophysics - Astroparticles, Experimental Astrophysics & Astroparticle Physics - High Energy Experimental Physics Thesis Title - Analyzing the high energy activity of candidate blazars to constrain their observability by neutrino telescopes Supervisor - Dr. Antonio Marinelli ([email protected]) Aug 2009 - Integrated M.Sc. (M.Sc. + B.Sc.) in Applied Physics - Indian Institute of Technology (ISM), Dhanbad Feb 2015 Area of study - Applied Physics - Nuclear & Particle Physics, Classical Mechanics, Quantum Mechanics, Electrodynamics - Computer Networks, Microprocessors, C++, ForTran Sept 2013 - Erasmus Mundus India4EU II Exchange Mobility - University of Porto (Portugal) July 2014 Area of study - Master Thesis, Astronomy - Stellar Structure & Evolution, Cosmology - Optical Communication, Measurement Techniques & Instrumentation Thesis Title - Constraining the Parameter Space of Dynamical -
Gustavo Marques-Tavares, Stanford Institute for Theoretical Physics
Detecting dark particles from Supernovae Gustavo Marques-Tavares, Stanford Institute for Theoretical Physics In collaboration with W. deRocco, P. Graham, D. Kasen and S. Rajendran Dark matter WIMP searches 5 -37 ACKNOWLEDGMENTS 10 -38 10 PandaX-II 2016 10-39 LUX 2016 ) 2 10-40 CDMSLite 2015 CRESST-II 2015 10-41 10-42 -43 10 SuperCDMS Post LHC1 mSUSY constraint 1700 kg-days 10-44 10-45 -46 10 6 t-y PandaX-4T 10-47 XENON1T 2 t-y LZ 15.6 t-y SI WIMP-nucleon cross section (cm XENONnT 20 t-y 10-48 200 t-y xenon (DARWIN or PandaX-30T) 10-49 Neutrino coherent scattering 10-50 1 10 102 103 WIMP mass (GeV/c2) *Figure taken from arxiv:1709.00688 This work is supported by grants from the Na- FIG. 4. The projected sensitivity (dashed curves) on the spin- tional Science Foundation of China (Nos. 11435008, independent WIMP-nucleon cross-sections of a selected num- ber of upcoming and planned direct detection experiments, 11455001, 11505112 and 11525522), a grant from the including XENON1T [34], PandaX-4T, XENONnT [34], Ministry of Science and Technology of China (Grant No. LZ [35], DARWIN [36] or PandaX-30T, and SuperCDMS [56]. 2016YFA0400301), and in part by the Chinese Academy Currently leading limits in Fig. 1 (see legend), the neutrino of Sciences Center for Excellence in Particle Physics ‘floor’ [20], and the post-LHC-Run1 minimal-SUSY allowed (CCEPP), the Key Laboratory for Particle Physics, As- contours [21] are overlaid in solid curves for comparison. The trophysics and Cosmology, Ministry of Education, and di↵erent crossings of the experimental sensitivities and the Shanghai Key Laboratory for Particle Physics and Cos- 2 neutrino floor at around a few GeV/c are primarily due to mology (SKLPPC). -
Geo-Neutrino Program at Baksan Neutrino Observatory Geoneutrino
Neutrino Geoscience 2019 Prague / Book of Abstracts The deep-sea neutrino detector KM3NeT/ORCA, currently being built in the Mediterranean Seanear Toulon (France), is optimized for the study of oscillations of atmospheric neutrinos in the few-GeV energy range, with the main goal to determine the neutrino mass hierarchy. This is possible due to matter effects that modify the probability of neutrino oscillations along their path through theEarth. Measuring the energy and angular distributions of neutrinos with ORCA can therefore also provide tomographic information on the Earth’s interior and more specifically on the electron density along the trajectory of the detected neutrino, complementary to standard geophysics methods. In this contribution the latest results of a study of the potential of ORCA for Earth tomography are presented. They are based on a full Monte Carlo simulation of the detector response and including systematic effects. It is shown that after ten years of operation ORCA can measure the electron density in both the lower mantle and the outer core with a precision of a few percent in the case of normal neutrino mass hierarchy. 40 Geo-neutrino program at Baksan Neutrino Observatory Authors: Albert Gangapshev1 ; Andrey Sidorenkov2 ; Bayarto Lubsandorzhiev2 ; Daniil Kudrin2 ; Dmitry Voronin2 ; Evgeny Veretenkin2 ; Evgeny Yanovich2 ; Galina Novikova2 ; Makhti Kochkarov2 ; Nikita Ushakov2 ; Tatiana Ibragimova2 ; Valery Kuzminov1 ; Valery Petkov3 ; Vladimir Gavrin2 ; Vladimir Kazalov2 ; Yury Gavrilyuk2 ; Yury Malyshkin4 1 INR RAS, KBSU 2 INR RAS 3 INR RAS, IA RAS 4 INR RAS, INFN A new neutrino program has been recently lunched at Baksan Neutrino Observatory. It is planned to deploy a 10-kiloton scale detector based on liquid scintillator in the existing shaft at a depth of 4800 m.w.e. -
Sensitivity to Light Sterile Neutrino Mixing Parameters with Km3net/ORCA
Sensitivity to light sterile neutrino mixing parameters with KM3NeT/ORCA S. Aielloa, A. Albertbb,b, M. Alshamsic, S. Alves Garred, Z. Alye, A. Ambrosonef,g, F. Amelih, M. Andrei, G. Androulakisj, M. Anghinolfik, M. Anguital, G. Antonm, M. Ardidn, S. Ardidn, J. Aublinc, C. Bagatelasj, B. Baretc, S. Basegmez du Preeo, M. Bendahmanc,p, F. Benfenatiq,r, E. Berbeeo, A. M. van den Bergs, V. Bertine, S. Biagit, M. Bissingerm, M. Boettcheru, M. Bou Cabov, J. Boumaazap, M. Boutaw, M. Bouwhuiso, C. Bozzax, H.Br^anza¸sy, F. Bretaudeauz, R. Bruijno,aa, J. Brunnere, R. Brunoa, E. Buisab, R. Buompanef,ac, J. Bustoe, B. Caiffik, D. Calvod, S. Campionad,h, A. Caponead,h, V. Carreterod, P. Castaldiq,ae, S. Celliad,h, M. Chababaf, N. Chauc, A. Chenag, S. Cherubinit,ah, V. Chiarellaai, T. Chiarusiq, M. Circellaaj, R. Cocimanot, J. A. B. Coelhoc,˚, A. Coleiroc, M. Colomer Mollac,d, R. Coniglionet, P. Coylee, A. Creusotc, A. Cruzak, G. Cuttonet, R. Dallierz, B. De Martinoe, M. De Palmaaj,al, I. Di Palmaad,h, A. F. D´ıazl, D. Diego-Tortosan, C. Distefanot, A. Domik,am,˚, C. Donzaudc, D. Dornice, M. D¨orran, D. Drouhinbb,b, T. Eberlm, A. Eddyamouip, T. van Eedeno, D. van Eijko, I. El Bojaddainiw, D. Elsaesseran, A. Enzenh¨ofere, V. Espinosan, P. Fermaniad,h, G. Ferrarat,ah, M. D. Filipovi´cao, F. Filippiniq,r, L. A. Fuscoe, T. Galm, J. Garc´ıaM´endezn, A. Garcia Sotoo, F. Garufif,g, Y. Gateletc, N. Geißelbrechtm, L. Gialanellaf,ac, E. Giorgiot, S. R. Gozziniad,h, R. Graciao, K. Grafm, G. Grellaap, D. -
The Hyper-Kamiokande Experiment Francesca Di Lodovico Queen Mary University of London
The Hyper-Kamiokande Experiment Francesca Di Lodovico Queen Mary University of London On behalf of the Hyper-K UK collaboration PPAP Meeting July 26, 2016 A Multi-purpose Experiment Comprehensive study of oscillation • CPV Supernova • Mass hierarchy with beam+atmosph. • 23 octant • Test of exotic scenarios Nucleon decay discovery potential Sun • All visible modes including p → 푒+ 0 + Accelerator and p→휈 퐾 can be advanced beyond (J-PARC) SK. • Reaching 1035yrs sensitivity Unique Astrophysics T2HK • Precision measurement of solar • High statistics Supernova with pointing capability and energy info. • Supernova relic (non-burst ) Proton observation is also possible decay Earth core's chemical composition Etc. 2 Inaugural Symposium of the HK proto- collaboration@Kashiwa, Jan-2015 12 countries, ~250 members and growing KEK-IPNS and • Proto-collaboration formed. UTokyo-ICRR • International steering group signed a MoU for • International conveners cooperation • International chair for international on the Hyper- board of representative (IBR) Kamiokande project. 26/July/2016 The Hyper-Kamiokande Experiment 3 Proto-Collaboration IRFU, CEA Saclay (France) Gifu University (Japan) Laboratoire Leprince-Ringuet, Ecole Polytechnique (France) High Energy Accelerator Research Organization (KEK) (Japan) Lancaster University (UK) Kobe University (Japan) Los Alamos National Laboratory (USA) Kyoto University (Japan) Louisiana State University (USA) Miyagi University of Education (Japan) National Centre for Nuclear Research (Poland) Nagoya University -
Neutrinoless Double Beta Decay Searches
FLASY2019: 8th Workshop on Flavor Symmetries and Consequences in 2016 Symmetry Magazine Accelerators and Cosmology Neutrinoless Double Beta Decay Ke Han (韩柯) Shanghai Jiao Tong University Searches: Status and Prospects 07/18, 2019 Outline .General considerations for NLDBD experiments .Current status and plans for NLDBD searches worldwide .Opportunities at CJPL-II NLDBD proposals in China PandaX series experiments for NLDBD of 136Xe 07/22/19 KE HAN (SJTU), FLASY2019 2 Majorana neutrino and NLDBD From Physics World 1935, Goeppert-Mayer 1937, Majorana 1939, Furry Two-Neutrino double beta decay Majorana Neutrino Neutrinoless double beta decay NLDBD 1930, Pauli 1933, Fermi + 2 + (2 ) Idea of neutrino Beta decay theory 136 136 − 07/22/19 54 → KE56 HAN (SJTU), FLASY2019 3 ̅ NLDBD probes the nature of neutrinos . Majorana or Dirac . Lepton number violation . Measures effective Majorana mass: relate 0νββ to the neutrino oscillation physics Normal Inverted Phase space factor Current Experiments Nuclear matrix element Effective Majorana neutrino mass: 07/22/19 KE HAN (SJTU), FLASY2019 4 Detection of double beta decay . Examples: . Measure energies of emitted electrons + 2 + (2 ) . Electron tracks are a huge plus 136 136 − 54 → 56 + 2 + (2)̅ . Daughter nuclei identification 130 130 − 52 → 54 ̅ 2νββ 0νββ T-REX: arXiv:1512.07926 Sum of two electrons energy Simulated track of 0νββ in high pressure Xe 07/22/19 KE HAN (SJTU), FLASY2019 5 Impressive experimental progress . ~100 kg of isotopes . ~100-person collaborations . Deep underground . Shielding + clean detector 1E+27 1E+25 1E+23 1E+21 life limit (year) life - 1E+19 half 1E+17 Sn Ca νββ Ge Te 0 1E+15 Xe 1E+13 1940 1950 1960 1970 1980 1990 2000 2010 2020 Year . -
Diurnal Effect of Sub-Gev Dark Matter Boosted by Cosmic Rays
Diurnal Effect of Sub-GeV Dark Matter Boosted by Cosmic Rays Shao-Feng Ge,1,2, ∗ Jianglai Liu,2,1, † Qiang Yuan,3, 4, 5, ‡ and Ning Zhou2, § 1Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai 200240, China 2School of Physics and Astronomy, Shanghai Jiao Tong University, Key Laboratory for Particle Astrophysics and Cosmology (MOE) & Shanghai Key Laboratory for Particle Physics and Cosmology, Shanghai 200240, China 3Key Laboratory of Dark Matter and Space Astronomy, Purple Mountain Observatory, Chinese Academy of Sciences, Nanjing 210033, China 4School of Astronomy and Space Science, University of Science and Technology of China, Hefei 230026, China 5Center for High Energy Physics, Peking University, Beijing 100871, China We point out a new type of diurnal effect for the cosmic ray boosted dark matter (DM). The DM- nucleon interactions not only allow the direct detection of DM with nuclear recoils, but also allow cosmic rays to scatter with and boost the nonrelativistic DM to higher energies. If the DM-nuclei scattering cross sections are sufficiently large, the DM flux is attenuated as it propagates through the Earth, leading to a strong diurnal modulation. This diurnal modulation provides another prominent signature for the direct detection of boosted sub-GeV DM, in addition to signals with higher recoil energy. Introduction – Overwhelming evidence from astrophys- signals in large neutrino experiments [44–46]. ical and cosmological observations supports the existence For sub-GeV DM, the DM-nucleon scattering cross sec- of dark matter (DM) [1], which is gravitationally interact- tion with a contact interaction can be quite sizable, e.g., ing but invisible via electromagnetic interactions. -
Icecube and Km3net: Lessons and Relations
Elsevier Science 1 Journal logo IceCube and KM3NeT: Lessons and Relations Christian Spiering DESY, Platanenallee 6, Zeuthen, 15738 Germany Elsevier use only: Received date here; revised date here; accepted date here Abstract This talk presents conclusions for KM3NeT which may be drawn from latest IceCube results and from optimization studies of the IceCube configuration. It discusses possible coordinated efforts between IceCube and KM3NeT (or, for the time being, IceCube and ANTARES). Finally, it lists ideas for formal relations between neutrino telescopes on the cubic kilometer scale. © 2001 Elsevier Science. All rights reserved Keywords: Neutrino Telescopes 1. Introduction The IceCube neutrino telescope at the South Pole Assuming one detector on the Southern is approaching its completion and meanwhile has hemisphere (IceCube) and one or more detectors at provided first results from data taken with initial the Northern hemisphere (by now ANTARES [10] configurations [1]. KM3NeT will act as IceCube’s and NT200 [11], in the future KM3NeT [12] and counterpart on the Northern hemisphere, with a GVD [13]), various possibilities for coordinated sensitivity “substantially exceeding that of all physics programs and analyses open up. They are existing neutrino telescopes including IceCube” [2]. discussed in sections 3 and 4. KM3NeT is just finishing its design phase [3], but Finally, section 5 lists formal and procedural has not yet converged to a final configuration. The possibilities of cooperation between KM3NeT and cited sensitivity requirement results not only from IceCube. gamma ray observations and their phenomenological interpretation (see e.g. [4-9]), but also from early IceCube data. The first section of this paper is 2.