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Related papers: GPS-based CERN-LNGS time link for Borexino

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Electron antineutrino interactions above the inverse beta decay energy of protons ($E_\bar{\nu}_e>$1.8) where looked for with the Borexino Counting Test Facility (CTF). One candidate event survived after rejection of background, which…

High Energy Physics - Experiment · Physics 2008-11-26 Borexino collaboration , M. Balata

Large ring-laser gyroscopes are capable of measuring angular rotations with a precision well below fractions of $prad/s$, not far from $10^{-14}$ $rad/s$, the accuracy required for General Relativity tests, this is what the GINGER…

The possibility that the Gallium data effectively indicates a time modulation of the solar active neutrino flux in possible connection to solar activity is examined on the light of spin flavour precession to sterile neutrinos as a…

High Energy Physics - Phenomenology · Physics 2009-11-11 Bhag C. Chauhan , Joao Pulido , R. S. Raghavan

COMPASS is a new fixed target experiment presently in operation at CERN. It has the goal to investigate hadron structure and hadron spectroscopy by using either muon or hadron beams. From measurements of various hadron asymmetries in…

High Energy Physics - Experiment · Physics 2015-06-25 F. Bradamante

Sub-MeV solar neutrino experiments and long-baseline reactor oscillation experiments toe the cutting edge of neutrino research. The upcoming experiments KamLAND and BOREXINO, currently in their startup and final construction phase…

High Energy Physics - Experiment · Physics 2015-06-25 Stefan Schoenert

The third Workshop of the NuMass series ("The Future of Neutrino Mass Measurements: Terrestrial, Astrophysical, and Cosmological Measurements in the Next Decade: NuMass 2013") was held at Dipartimento di Fisica "G. Occhialini, University of…

XENON10 is the first two-phase xenon time projection chamber (TPC) developed within the XENON dark matter search program. The TPC, with an active liquid xenon (LXe) mass of about 14 kg, was installed at the Gran Sasso underground laboratory…

The nuGeN experiment searches for coherent elastic neutrino-nucleus scattering (CEvNS) at the Kalinin Nuclear Power Plant. A 1.41-kg high-purity low-threshold germanium detector surrounded by active and passive shielding is deployed at the…

MONOLITH is a proposed massive (34 kt) magnetized tracking calorimeter at the Gran Sasso laboratory in Italy, optimized for the detection of atmospheric muon neutrinos. The main goal is to establish (or reject) the neutrino oscillation…

High Energy Physics - Experiment · Physics 2019-08-14 A. Geiser

The WAGASCI experiment being built at the J-PARC neutrino beam line will measure the difference in cross sections from neutrinos interacting with a water and scintillator targets, in order to constrain neutrino cross sections, essential for…

OPERA is an experiment dedicated to the observation of $\nu_\mu$ into $\nu_\tau$ oscillations in appearance mode using a pure $\nu_\mu$ beam (CNGS) produced at CERN and detected at Gran Sasso. The experiment exploits a hybrid technology…

Instrumentation and Detectors · Physics 2014-11-20 J. Marteau

We present an updated analysis of all the data available about solar neutrinos, including the charged current SNO results. The best fit of the data is obtained in the Large Mixing Angle region, but different solutions are still possible. We…

High Energy Physics - Phenomenology · Physics 2007-06-22 P. Aliani , V. Antonelli , M. Picariello , E. Torrente-Lujan

The study of local deformations is a hot topic in geodesy. Local rotations of the crust around the vertical axis can be caused by deformations. In the Gran Sasso area the ring laser gyroscope GINGERINO and the GNSS array are operative. One…

We present the result of a search for correlations in the arrival times of high energy muons collected from 1995 till 2000 with the streamer tube system of the complete MACRO detector at the underground Gran Sasso Lab. Large samples of…

The feasibility of a European next-generation very massive neutrino observatory in seven potential candidate sites located at distances from CERN ranging from 130 km to 2300 km, is being considered within the LAGUNA design study. The study…

High Energy Physics - Phenomenology · Physics 2010-03-10 A. Rubbia

The COMPASS experiment makes use of the CERN SPS high-intensitymuon and hadron beams for the investigation of the nucleon spin structure and the spectroscopy of hadrons. One or more outgoing particles are detected in coincidence with the…

High Energy Physics - Experiment · Physics 2008-11-26 COMPASS Collaboration , P. Abbon

More than 30 million of high-energy muons collected with the MACRO detector at the underground Gran Sasso Laboratory have been used to search for flux variations of different natures. Two kinds of studies were carried out: search for…

We report an improved geo-neutrino measurement with Borexino from 2056 days of data taking. The present exposure is $(5.5\pm0.3)\times10^{31}$ proton$\times$yr. Assuming a chondritic Th/U mass ratio of 3.9, we obtain $23.7 ^{+6.5}_{-5.7}…

The OPERA detector at the Gran Sasso underground laboratory (LNGS) was used to measure the atmospheric muon charge ratio in the TeV energy region. We analyzed 403069 atmospheric muons corresponding to 113.4 days of livetime during the 2008…

High Energy Physics - Experiment · Physics 2010-03-10 OPERA Collaboration , N. Agafonova , A. Anokhina , S. Aoki , A. Ariga , T. Ariga , D. Autiero , A. Badertscher , A. Bagulya , A. Bertolin , M. Besnier , D. Bick , V. Boyarkin , C. Bozza , T. Brugière , R. Brugnera , G. Brunetti , S. Buontempo , A. Cazes , L. Chaussard , M. Chernyavsky , V. Chiarella , N. Chon-Sen , A. Chukanov , M. Cozzi , G. D'Amato , F. Dal Corso , N. D'Ambrosio , G. De Lellis , Y. D'eclais , M. De Serio , F. Di Capua , D. Di Ferdinando , A. Di Giovanni , N. Di Marco , S. Dmitrievski , M. Dracos , D. Duchesneau , S. Dusini , J. Ebert , O. Egorov , R. Enikeev , A. Ereditato , L. S. Esposito , J. Favier , G. Felici , T. Ferber , R. Fini , D. Frekers , T. Fukuda , C. Fukushima , V. I. Galkin , A. Garfagnini , G. Giacomelli , M. Giorgini , C. Goellnitz , J. Goldberg , D. Golubkov , L. Goncharova , Y. Gornushkin , G. Grella , F. Grianti , M. Guler , C. Gustavino , C. Hagner , K. Hamada , T. Hara , M. Hierholzer , K. Hoshino , M. Ieva , K. Jakovcic , C. Jollet , F. Juget , M. Kazuyama , S. H. Kim , M. Kimura , B. Klicek , J. Knuesel , K. Kodama , M. Komatsu , U. Kose , I. Kreslo , H. Kubota , C. Lazzaro , J. Lenkeit , A. Ljubicic , A. Longhin , G. Lutter , A. Malgin , G. Mandrioli , A. Marotta , J. Marteau , T. Matsuo , V. Matveev , N. Mauri , E. Medinaceli , F. Meisel , A. Meregaglia , P. Migliozzi , S. Mikado , S. Miyamoto , P. Monacelli , K. Morishima , U. Moser , M. T. Muciaccia , N. Naganawa , T. Naka , M. Nakamura , T. Nakano , D. Naumov , V. Nikitina , K. Niwa , Y. Nonoyama , S. Ogawa , A. Olchevski , C. Oldorf , G. Orlova , V. Osedlo , M. Paniccia , A. Paoloni , B. D. Park , I. G. Park , A. Pastore , L. Patrizii , E. Pennacchio , H. Pessard , V. Pilipenko , C. Pistillo , G. Policastro , N. Polukhina , M. Pozzato , K. Pretzl , P. Publichenko , F. Pupilli , R. Rescigno , T. Roganova , H. Rokujo , G. Romano , G. Rosa , I. Rostovtseva , A. Rubbia , A. Russo , V. Ryasny , O. Ryazhskaya , O. Sato , Y. Sato , A. Schembri , W. Schmidt Parzefall , H. Schroeder , L. Scotto Lavina , A. Sheshukov , H. Shibuya , S. Simone , M. Sioli , C. Sirignano , G. Sirri , J. S. Song , M. Spinetti , L. Stanco , N. Starkov , M. Stipcevic , T. Strauss , P. Strolin , S. Takahashi , M. Tenti , F. Terranova , I. Tezuka , V. Tioukov , P. Tolun , T. Tran , S. Tufanli , P. Vilain , M. Vladimirov , L. Votano , J. L. Vuilleumier , G. Wilquet , B. Wonsak , V. Yakushev , C. S. Yoon , T. Yoshioka , J. Yoshida , Y. Zaitsev , S. Zemskova , A. Zghiche , R. Zimmermann