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The detection of CP violation in neutrino oscillations is one of the most important goals of the next generation of neutrino experiments. Here we study the detectability of the CP-violating phase in the oscillation of atmospheric neutrinos.…

High Energy Physics - Experiment · Physics 2026-04-16 Thilo Birkenfeld , Achim Stahl

Spherical time projection chambers (TPC), also known as spherical proportional counters, are employed in the search for rare phenomena, such as light Dark Matter candidates. The spherical TPC exhibits a number of essential features, making…

The results of an experimental feasibility study of a position sensitive thermal neutron detector based on a resistive plate chamber (RPC) are presented. The detector prototype features a thin-gap (0.35 mm) hybrid RPC with an aluminium…

We report on searches for neutrinos and antineutrinos from astrophysical sources performed with the Borexino detector at the Laboratori Nazionali del Gran Sasso in Italy. Electron antineutrinos ($\bar{\nu}_e$) are detected in an organic…

One of the main neutrino oscillation parameters whose value has not been determined very precisely is the leptonic $\delta_{CP}$ phase. Since neutrinos have a tiny but finite mass they can undergo decay both visibly and invisibly. The…

High Energy Physics - Phenomenology · Physics 2020-10-28 Lakshmi. S. Mohan

ArgoNeuT, a Liquid Argon Time Projection Chamber (LAr-TPC), has collected thousands of neutrino and anti-neutrino events between 0.1 and 10 GeV in the NuMI beamline at Fermilab (FNAL). Among other issues, the experiment will measure the…

High Energy Physics - Experiment · Physics 2011-10-17 O. Palamara

The detection of cosmic neutrinos with energies above 1017 eV got growing interest during recent years. Possible target materials for in-matter arrays of ~100 km3 size under discussion are water, ice and rock salt. Here we propose to…

Astrophysics · Physics 2009-06-23 R. Nahnhauer , A. A. Rostovtsev , D. Tosi

A 10 kilo-tonne dual-phase liquid argon TPC is one of the detector options considered for the Deep Underground Neutrino Experiment (DUNE). The detector technology relies on amplification of the ionisation charge in ultra-pure argon vapour…

Instrumentation and Detectors · Physics 2018-11-14 B. Aimard , Ch. Alt , J. Asaadi , M. Auger , V. Aushev , D. Autiero , M. M. Badoi , A. Balaceanu , G. Balik , L. Balleyguier , E. Bechetoille , D. Belver , A. M. Blebea-Apostu , S. Bolognesi , S. Bordoni , N. Bourgeois , B. Bourguille , J. Bremer , G. Brown , G. Brunetti , L. Brunetti , D. Caiulo , M. Calin , E. Calvo , M. Campanelli , K. Cankocak , C. Cantini , B. Carlus , B. M. Cautisanu , M. Chalifour , A. Chappuis , N. Charitonidis , A. Chatterjee , A. Chiriacescu , P. Chiu , S. Conforti , P. Cotte , P. Crivelli , C. Cuesta , J. Dawson , I. De Bonis , C. De La Taille , A. Delbart , D. Desforge , S. Di Luise , B. S. Dimitru , F. Doizon , C. Drancourt , D. Duchesneau , F. Dulucq , J. Dumarchez , F. Duval , S. Emery , A. Ereditato , T. Esanu , A. Falcone , K. Fusshoeller , A. Gallego-Ros , V. Galymov , N. Geroy , A. Gendotti , M. Gherghel-Lascu , C. Giganti , I. Gil-Botella , C. Girerd , M. C. Gomoiu , P. Gorodetzky , E. Hamada , R. Hanni , T. Hasegawa , A. Holin , S. Horikawa , M. Ikeno , S. Jimenez , A. Jipa , M. Karolak , Y. Karyotakis , S. Kasai , K. Kasami , T. Kishishita , I. Kreslo , D. Kryn , C. Lastoria , I. Lazanu , G. Lehmann-Miotto , N. Lira , K. Loo , D. Lorca , P. Lutz , T. Lux , J. Maalampi , G. Maire , M. Maki , L. Manenti , R. M. Margineanu , J. Marteau , G. Martin-Chassard , H. Mathez , E. Mazzucato , G. Misitano , B. Mitrica , D. Mladenov , L. Molina Bueno , C. Moreno Martinez , J. P. Mols , T. S. Mosu , W. Mug , A. Munteanu , S. Murphy , K. Nakayoshi , S. Narita , D. Navas-Nicolas , K. Negishi , M. Nessi , M. Niculescu-Oglinzanu , L. Nita , F. Noto , A. Noury , Y. Onishchuk , C. Palomares , M. Parvu , T. Patzak , Y. Penichot , E. Pennacchio , L. Periale , H. Pessard , F. Pietropaolo , Y. Piret , B. Popov , D. Pugnere , B. Radics , D. Redondo , C. Regenfus , A. Remoto , F. Resnati , Y. A. Rigaut , C. Ristea , A. Rubbia , A. Saftoiu , K. Sakashita , F. Sanchez , C. Santos , A. Scarpelli , C. Schloesser , L. Scotto Lavina , K. Sendai , F. Sergiampietri , S. Shahsavarani , M. Shoji , J. Sinclair , J. Soto-Oton , D. L. Stanca , D. Stefan , P. Stroescu , R. Sulej , M. Tanaka , V. Toboaru , A. Tonazzo , W. Tromeur , W. H. Trzaska , T. Uchida , F. Vannucci , G. Vasseur , A. Verdugo , T. Viant , S. Vihonen , S. Vilalte , M. Weber , S. Wu , J. Yu , L. Zambelli , M. Zito

The antineutrinos of the neutron rich 8Li isotope is characterized by hard and good defined spectrum - averaged energy is 6.5 MeV and maximal - up to 13 MeV. An intensive antineutrino source with such parameters can be unique instrument for…

Instrumentation and Detectors · Physics 2016-09-08 V. I. Lyashuk

In this white paper, we outline some of the scientific opportunities and challenges related to detection and reconstruction of low-energy (less than 100 MeV) signatures in liquid argon time-projection chamber (LArTPC) detectors. Key…

Instrumentation and Detectors · Physics 2022-03-07 D. Caratelli , W. Foreman , A. Friedland , S. Gardiner , I. Gil-Botella , G. Karagiorgi , M. Kirby , G. Lehmann Miotto , B. R. Littlejohn , M. Mooney , J. Reichenbacher , A. Sousa , K. Scholberg , J. Yu , T. Yang , S. Andringa , J. Asaadi , T. J. C. Bezerra , F. Capozzi , F. Cavanna , E. Church , A. Himmel , T. Junk , J. Klein , I. Lepetic , S. Li , P. Sala , H. Schellman , M. Sorel , J. Wang , M. H. L. S. Wang , W. Wu , J. Zennamo , M. A. Acero , M. R. Adames , H. Amar , D. A. Andrade , C. Andreopoulos , A. M. Ankowski , M. A. Arroyave , V. Aushev , M. A. Ayala-Torres , P. Baldi , C. Backhouse , A. B. Balantekin , W. A. Barkhouse , P. Barham Alzas , J. L. Barrow , J. B. R. Battat , M. C. Q. Bazetto , J. F. Beacom , B. Behera , G. Bellettini , J. Berger , A. T. Bezerra , J. Bian , B. Bilki , B. Bles , T. Bolton , L. Bomben , M. Bonesini , C. Bonilla-Diaz , F. Boran , A. N. Borkum , N. Bostan , D. Brailsford , A. Branca , G. Brunetti , T. Cai , A. Chappell , N. Charitonidis , P. H. P. Cintra , E. Conley , T. E. Coan , P. Cova , L. M. Cremaldi , J. I. Crespo-Anadon , C. Cuesta , R. Dallavalle , G. S. Davies , S. De , P. Dedin Neto , M. Delgado , N. Delmonte , P. B. Denton , A. De Roeck , R. Dharmapalan , Z. Djurcic , F. Dolek , S. Doran , R. Dorrill , K. E. Duffy , B. Dutta , O. Dvornikov , S. Edayath , J. J. Evans , A. C. Ezeribe , A. Falcone , M. Fani , J. Felix , Y. Feng , L. Fields , P. Filip , G. Fiorillo , D. Franco , D. Garcia-Gamez , A. Giri , O. Gogota , S. Gollapinni , M. Goodman , E. Gramellini , R. Gran , P. Granger , C. Grant , S. E. Greenberg , M. Groh , R. Guenette , D. Guffanti , D. A. Harris , A. Hatzikoutelis , K. M. Heeger , M. Hernandez Morquecho , K. Herner , J. Ho , P C. Holanda , N. Ilic , C. M. Jackson , W. Jang , H. -Th. Janka , J. H. Jo , F. R. Joaquim , R. S. Jones , N. Jovancevic , Y. -J. Jwa , D. Kalra , D. M. Kaplan , I. Katsioulas , E. Kearns , K. J. Kelly , E. Kemp , W. Ketchum , A. Kish , L. W. Koerner , T. Kosc , K. Kothekar , I. Kreslo , S. Kubota , V. A. Kudryavtsev , P. Kumar , T. Kutter , J. Kvasnicka , I. Lazanu , T. LeCompte , Y. Li , Y. Liu , M. Lokajicek , W. C. Louis , K. B. Luk , X. Luo , P. A. N. Machado , I. M. Machulin , K. Mahn , M. Man , R. C. Mandujano , J. Maneira , A. Marchionni , D. Marfatia , F. Marinho , C. Mariani , C. M. Marshall , F. Martinez Lopez , D. A. Martinez Caicedo , A. Mastbaum , M. Matheny , N. McConkey , P. Mehta , O. E. B. Messer , A. Minotti , O. G. Miranda , P. Mishra , I. Mocioiu , A. Mogan , R. Mohanta , T. Mohayai , C. Montanari , L. M. Montano Zetina , A. F. Moor , D. Moretti , C. A. Moura , L. M. Mualem , J. Nachtman , S. Narita , A. Navrer-Agasson , M. Nebot-Guinot , J. Nikolov , J. A. Nowak , J. P. Ochoa-Ricoux , E. O'Connor , Y. Onel , Y. Onishchuk , G. D. Orebi Gann , V. Pandey , E. G. Parozzi , S. Parveen , M. Parvu , R. B. Patterson , L. Paulucci , V. Pec , S. J. M. Peeters , F. Pompa , N. Poonthottathil , S. S. Poudel , F. Psihas , A. Rafique , B. J. Ramson , J. S. Real , A. Rikalo , M. Ross-Lonergan , B. Russell , S. Sacerdoti , N. Sahu , D. A. Sanders , D. Santoro , M. V. Santos , C. R. Senise , P. N. Shanahan , H. R Sharma , R. K. Sharma , W. Shi , S. Shin , J. Singh , J. Singh , L. Singh , P. Singh , V. Singh , M. Soderberg , S. Soldner-Rembold , J. Soto-Oton , K. Spurgeon , A. F. Steklain , F. Stocker , T. Stokes , J. Strait , M. Strait , T. Strauss , L. Suter , R. Svoboda , A. M. Szelc , M. Szydagis , E. Tarpara , E. Tatar , F. Terranova , G. Testera , N. Chithirasree , N. Todorovic , A. Tonazzo , M. Torti , F. Tortorici , M. Toups , D. Q. Tran , M. Travar , Y. -D. Tsai , Y. -T. Tsai , S. Z. Tu , J. Urheim , H. Utaegbulam , S. Valder , G. A. Valdiviesso , R. Valentim , S. Vergani , B. Viren , A. Vranicar , B. Wang , D. Waters , P. Weatherly , M. Weber , H. Wei , S. Westerdale , L. H. Whitehead , D. Whittington , A. Wilkinson , R. J. Wilson , M. Worcester , K. Wresilo , B. Yaeggy , G. Yang , J. Zalesak , B. Zamorano , J. Zuklin

A liquid scintillator (LS) is developed for the Taishan Antineutrino Observatory (TAO), a ton-level neutrino detector to measure the reactor antineutrino spectrum with sub-percent energy resolution by adopting Silicon Photomultipliers…

Instrumentation and Detectors · Physics 2021-07-07 Zhangquan Xie , Jun Cao , Yayun Ding , Mengchao Liu , Xilei Sun , Wei Wang , Yuguang Xie

The capabilities of liquid argon time projection chambers (LArTPCs) to reconstruct the spatial and calorimetric information of neutrino events have made them the detectors of choice in a number of experiments, specifically those looking to…

In order to carry out research in the field of possible existence of a sterile neutrino the laboratory based on SM-3 reactor (Dimitrovgrad, Russia) was created to search for oscillations of reactor antineutrino. The prototype of a…

In the present work we propose to study neutrino oscillations employing sources of monoenergetic neutrinos following electron capture by the nucleus. Since the neutrino energy is very low the smaller of the two oscillation lengths, L23,…

High Energy Physics - Phenomenology · Physics 2014-11-21 J. D. Vergados , Yu. N. Novikov

The high energy neutrino detection by a km^3 Neutrino Telescope placed in the Mediterranean sea provides a unique tool to both determine the diffuse astrophysical neutrino flux and the neutrino-nucleon cross section in the extreme…

Astrophysics · Physics 2007-09-24 E. Borriello , A. Cuoco , G. Mangano , G. Miele , S. Pastor , O. Pisanti , P. D. Serpico

Antiprotonic helium, a neutral exotic three-body system consisting of a helium nucleus, an electron and an antiproton, is being studied at the Antiproton Decelerator of CERN by the ASAUCSA collaboration. Using laser spectroscopy of the…

Atomic Physics · Physics 2007-05-23 Eberhard Widmann

The MUNU detector has been designed to study antineutrino-electron elastic scattering at low energy. The central tracking detector is a 1 m3 Time Projection Chamber surrounded by an anti-Compton detector. In this paper the results from…

High Energy Physics - Experiment · Physics 2019-08-13 Zornitza Daraktchieva

We study the possibility to use a low energy beta-beam facility to search for sterile neutrinos by measuring the disappearance of electron anti-neutrinos. This channel is particularly sensitive since it allows to use inverse beta decay as…

High Energy Physics - Phenomenology · Physics 2014-11-21 Sanjib Kumar Agarwalla

Neutrino astrophysics offers new perspectives on the Universe investigation: high energy neutrinos, produced by the most energetic phenomena in our Galaxy and in the Universe, carry complementary (if not exclusive) information about the…

High Energy Astrophysical Phenomena · Physics 2010-02-11 T. Chiarusi , M. Spurio

In order to measure the energy of neutron fields, with energy ranging from 8 keV to 1 MeV, a new primary standard is being developed at the IRSN (Institute for Radioprotection and Nuclear Safety). This project, micro-TPC (Micro Time…