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Featured researches published by F. Bay.


Physical Review D | 2013

The T2K Neutrino Flux Prediction

A. Ariga; T. Ariga; F. Bay; A. Ereditato; E. Frank; I. Kreslo; M. Messina

The Tokai-to-Kamioka (T2K) experiment studies neutrino oscillations using an off-axis muon neutrino beam with a peak energy of about 0.6 GeV that originates at the Japan Proton Accelerator Research Complex accelerator facility. Interactions of the neutrinos are observed at near detectors placed at 280 m from the production target and at the far detector—Super-Kamiokande—located 295 km away. The flux prediction is an essential part of the successful prediction of neutrino interaction rates at the T2K detectors and is an important input to T2K neutrino oscillation and cross section measurements. A FLUKA and GEANT3-based simulation models the physical processes involved in the neutrino production, from the interaction of primary beam protons in the T2K target, to the decay of hadrons and muons that produce neutrinos. The simulation uses proton beam monitor measurements as inputs. The modeling of hadronic interactions is reweighted using thin target hadron production data, including recent charged pion and kaon measurements from the NA61/SHINE experiment. For the first T2K analyses the uncertainties on the flux prediction are evaluated to be below 15% near the flux peak. The uncertainty on the ratio of the flux predictions at the far and near detectors is less than 2% near the flux peak.


Physical Review D | 2013

Measurement of the Inclusive NuMu Charged Current Cross Section on Carbon in the Near Detector of the T2K

A. Ariga; T. Ariga; F. Bay; A. Ereditato; E. Frank; I. Kreslo; M. Messina

T2K has performed the first measurement of nu(mu) inclusive charged current interactions on carbon at neutrino energies of similar to 1 GeV where the measurement is reported as a flux-averaged double differential cross section in muon momentum and angle. The flux is predicted by the beam Monte Carlo and external data, including the results from the NA61/SHINE experiment. The data used for this measurement were taken in 2010 and 2011, with a total of 10.8 x 10(19) protons-on-target. The analysis is performed on 4485 inclusive charged current interaction candidates selected in the most upstream fine-grained scintillator detector of the near detector. The flux-averaged total cross section is (phi) = (6.91 +/- 0.13(stat) +/- 0.84(syst)) x 10(-39) cm(2)/nucleon for a mean neutrino energy of 0.85 GeV.


Journal of Instrumentation | 2013

ArDM: first results from underground commissioning

A. Badertscher; F. Bay; N. Bourgeois; C. Cantini; A. Curioni; M. Daniel; U Degunda; S. Di Luise; L. Epprecht; A. Gendotti; S. Horikawa; L. Knecht; D Lussi; G. Maire; B. Montes; S. Murphy; G. Natterer; K. Nikolics; K. Nguyen; L. Periale; S. Ravat; F. Resnati; L. Romero; A. Rubbia; R. Santorelli; F. Sergiampietri; D. Sgalaberna; T. Viant; S. Wu

The Argon Dark Matter experiment is a ton-scale double phase argon Time Projection Chamber designed for direct Dark Matter searches. It combines the detection of scintillation light together with the ionisation charge in order to discriminate the background (electron recoils) from the WIMP signals (nuclear recoils). After a successful operation on surface at CERN, the detector was recently installed in the underground Laboratorio Subterr?neo de Canfranc, and the commissioning phase is ongoing. We describe the status of the installation and present first results from data collected underground with the detector filled with gas argon at room temperature.


Progress of Theoretical and Experimental Physics | 2015

Measurement of the muon beam direction and muon flux for the T2K neutrino experiment

K. Suzuki; S. Aoki; A. Ariga; T. Ariga; F. Bay; C. Bronner; A. Ereditato; M. Friend; M. Hartz; T. Hiraki; Atsushi Ichikawa; T. Ishida; T. Ishii; F. Juget; T. Kikawa; T. Kobayashi; H. Kubo; K. Matsuoka; T. Maruyama; A. Minamino; A. Murakami; T. Nakadaira; T. Nakaya; K. Nakayoshi; M. Otani; Y. Oyama; N. Patel; C. Pistillo; K. Sakashita; T. Sekiguchi

The Tokai-to-Kamioka (T2K) neutrino experiment measures neutrino oscillations by using an almost pure muon neutrino beam produced at the J-PARC accelerator facility. The T2K muon monitor was installed to measure the direction and stability of the muon beam which is produced together with the muon neutrino beam. The systematic error in the muon beam direction measurement was estimated, using data and MC simulation, to be 0.28 mrad. During beam operation, the proton beam has been controlled using measurements from the muon monitor and the direction of the neutrino beam has been tuned to within 0.3 mrad with respect to the designed beam-axis. In order to understand the muon beam properties, measurement of the absolute muon yield at the muon monitor was conducted with an emulsion detector. The number of muon tracks was measured to be (4.06 ± 0.05) × 10⁴ cm⁻² normalized with 4 × 10¹¹protons on target with 250 kA horn operation. The result is in agreement with the prediction which is corrected based on hadron production data.


Journal of Instrumentation | 2012

A dedicated device for measuring the magnetic field of the ND280 magnet in the T2K experiment

E Frank; A. Ariga; T. Ariga; F. Bay; F. Bergsma; A. Ereditato; F Garnier; P A Giudici; F. Hahn; A Kehrli; I. Kreslo; M. Losasso; M. Messina; S Rangod

This paper describes a dedicated device to map the magnetic field of the T2K near detector (ND280) magnet, which runs at a nominal field value of 0.2 T, with an accuracy of the order of a Gauss. A high accuracy mapping is a key ingredient in order to provide the required momentum accuracy in the ND280 time projection chambers (TPCs) allowing T2K to measure precisely the PMNS matrix parameters ?m232 and ?23. This paper describes the design and realization of the device as well as its performance during operation. The reported results show that the aimed at goals are reached.


arXiv: Instrumentation and Detectors | 2014

Evidence of electric breakdown induced by bubbles in liquid argon

F. Bay; S. Wu; C. Cantini; S. Murphy; A. Rubbia; F. Sergiampietri; F. Resnati


arXiv: Instrumentation and Detectors | 2013

Status of the ArDM Experiment: First results from gaseous argon operation in deep underground environment

A. Badertscher; B. Montes; G. Natterer; G. Maire; K. Nikolics; D Lussi; S DiLuise; D. Sgalaberna; A. Rubbia; R. Santorelli; L. Epprecht; F. Bay; S. Wu; U Degunda; S. Horikawa; T. Viant; L. Knecht; F. Resnati; S. Ravat; F. Sergiampietri; N. Bourgeois; L. Periale; C. Cantini; L. Romero; S. Murphy; M. Daniel; A. Gendotti; K. Nguyen


Physical Review Letters | 2016

Measurement of Coherent π

K. Abe; C. Andreopoulos; M. Antonova; S. Aoki; A. Ariga; S. Assylbekov; D. Autiero; S. Ban; M. Barbi; G. J. Barker; G. Barr; P. Bartet-Friburg; M. Batkiewicz; F. Bay; Berardi; S. Berkman; S. Bhadra; A. Blondel; S. Bolognesi; S. Bordoni; S. Boyd; D. Brailsford; A. Bravar; C. Bronner; M. Buizza Avanzini; R. G. Calland; T. Campbell; S. V. Cao; J. Caravaca Rodríguez; S. Cartwright

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