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Insertion of STC into TRT at the Department of Physics, Oxford
Credit: CERN

Professor Dr.rer.nat. Dipl.Phys. Alfons Weber FInstP, MA Ox

Visiting Professor

Research theme

  • Fundamental particles and interactions

Sub department

  • Particle Physics

Research groups

  • Accelerator Neutrinos
Alfons.Weber@physics.ox.ac.uk
Telephone: +49 (6131) 39 24175
Denys Wilkinson Building
AlfonsWeber@JGUMainz
  • About
  • Research
  • Teaching
  • Committees
  • Publications

Optimisation of the scintillation light collection and uniformity for the SoLid experiment

Journal of Instrumentation IOP Publishing

Authors:

Y Abreu, Y Amhis, W Beaumont, M Bongrand, D Boursette, BC Castle, K Clark, B Coupé, D Cussans, A De Roeck, D Durand, M Fallot, L Ghys, L Giot, K Graves, B Guillon, D Henaff, B Hosseini, S Ihantola, S Jenzer, S Kalcheva, LN Kalousis, M Labare, G Lehaut, S Manley, L Manzanillas, J Mermans, I Michiels, C Moortgat, D Newbold, J Park, V Pestel, K Petridis, I Piñera, L Popescu, D Ryckbosch, N Ryder, D Saunders, M-H Schune, M Settimo, L Simard, A Vacheret, G Vandierendonck, S Van Dyck, P Van Mulders, N van Remortel, S Vercaemer, M Verstraeten, B Viaud, A Weber, F Yermia

Abstract:

This paper presents a comprehensive optimisation study to maximise the light collection efficiency of scintillating cube elements used in the SoLid detector. Very short baseline reactor experiments, like SoLid, look for active to sterile neutrino oscillation signatures in the anti-neutrino energy spectrum as a function of the distance to the core and energy. Performing a precise search requires high light yield of the scintillating elements and uniformity of the response in the detector volume. The SoLid experiment uses an innovative hybrid technology with two different scintillators: polyvinyltoluene scintillator cubes and $^6$LiF:ZnS(Ag) screens. A precision test bench based on a $^{207}$Bi calibration source has been developed to study improvements on the energy resolution and uniformity of the prompt scintillation signal of antineutrino interactions. A trigger system selecting the 1~MeV conversion electrons provides a Gaussian energy peak and allows for precise comparisons of the different detector configurations that were considered to improve the SoLid detector light collection. The light collection efficiency is influenced by the choice of wrapping material, the position of the $^6$LiF:ZnS(Ag) screen, the type of fibre, the number of optical fibres and the type of mirror at the end of the fibre. This study shows that large gains in light collection efficiency are possible compared to the SoLid SM1 prototype. The light yield for the SoLid detector is expected to be at least 52$\pm$2 photo-avalanches per MeV per cube, with a relative non-uniformity of 6 %, demonstrating that the required energy resolution of at least 14 % at 1 MeV can be achieved.
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Details from ORA
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Optimised sensitivity to leptonic CP violation from spectral information: the LBNO case at 2300 km baseline

arXiv

Authors:

LAGUNA-LBNO Collaboration, SK Agarwalla, L Agostino, M Aittola, A Alekou, B Andrieu, F Antoniou, R Asfandiyarov, D Autiero, O Bésida, A Balik, P Ballett, I Bandac, D Banerjee, W Bartmann, F Bay, B Biskup, AM Blebea-Apostu, A Blondel, M Bogomilov, S Bolognesi, E Borriello, I Brancus, A Bravar, M Buizza-Avanzini, D Caiulo, M Calin, M Calviani, M Campanelli, C Cantini, G Cata-Danil, S Chakraborty, N Charitonidis, L Chaussard, D Chesneanu, F Chipesiu, P Crivelli, J Dawson, I De Bonis, Y Declais, P Del Amo Sanchez, A Delbart, S Di Luise, D Duchesneau, J Dumarchez, I Efthymiopoulos, A Eliseev, S Emery, T Enqvist, K Enqvist, L Epprecht, AN Erykalov, T Esanu, D Franco, M Friend, V Galymov, G Gavrilov, A Gendotti, C Giganti, S Gilardoni, B Goddard, CM Gomoiu, YA Gornushkin, P Gorodetzky, A Haesler, T Hasegawa, S Horikawa, K Huitu, A Izmaylov, A Jipa, K Kainulainen, Y Karadzhov, M Khabibullin, A Khotjantsev, AN Kopylov, A Korzenev, S Kosyanenko, D Kryn, Y Kudenko, P Kuusiniemi, I Lazanu, C Lazaridis, J-M Levy, K Loo, J Maalampi, RM Margineanu, J Marteau, C Martin-Mari, V Matveev, E Mazzucato, A Mefodiev, O Mineev, A Mirizzi, B Mitrica, S Murphy, T Nakadaira, S Narita, DA Nesterenko, K Nguyen, K Nikolics, E Noah, Yu Novikov, A Oprima, J Osborne, T Ovsyannikova, Y Papaphilippou, S Pascoli, T Patzak, M Pectu, E Pennacchio, L Periale, H Pessard, B Popov, M Ravonel, M Rayner, F Resnati, O Ristea, A Robert, A Rubbia, K Rummukainen, A Saftoiu, K Sakashita, F Sanchez-Galan, J Sarkamo, N Saviano, E Scantamburlo, F Sergiampietri, D Sgalaberna, E Shaposhnikova, M Slupecki, D Smargianaki, D Stanca, R Steerenberg, AR Sterian, P Sterian, S Stoica, C Strabel, J Suhonen, V Suvorov, G Toma, A Tonazzo, WH Trzaska, R Tsenov, K Tuominen, M Valram, G Vankova-Kirilova, F Vannucci, G Vasseur, F Velotti, P Velten, V Venturi, T Viant, S Vihonen, H Vincke, A Vorobyev, A Weber, S Wu, N Yershov, L Zambelli, M Zito

Abstract:

One of the main goals of the Long Baseline Neutrino Observatory (LBNO) is to study the $L/E$ behaviour (spectral information) of the electron neutrino and antineutrino appearance probabilities, in order to determine the unknown CP-violation phase $\delta_{CP}$ and discover CP-violation in the leptonic sector. The result is based on the measurement of the appearance probabilities in a broad range of energies, covering t he 1st and 2nd oscillation maxima, at a very long baseline of 2300 km. The sensitivity of the experiment can be maximised by optimising the energy spectra of the neutrino and anti-neutrino fluxes. Such an optimisation requires exploring an extended range of parameters describing in details the geometries and properties of the primary protons, hadron target and focusing elements in the neutrino beam line. In this paper we present a numerical solution that leads to an optimised energy spectra and study its impact on the sensitivity of LBNO to discover leptonic CP violation. In the optimised flux both 1st and 2nd oscillation maxima play an important role in the CP sensitivity. The studies also show that this configuration is less sensitive to systematic errors (e.g. on the total event rates) than an experiment which mainly relies on the neutrino-antineutrino asymmetry at the 1st maximum to determine the existence of CP-violation.
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Search for CP violation in Neutrino and Antineutrino Oscillations by the T2K experiment with $2.2\times10^{21}$ protons on target

Authors:

K Abe, R Akutsu, A Ali, J Amey, C Andreopoulos, L Anthony, M Antonova, S Aoki, A Ariga, Y Ashida, Y Azuma, S Ban, M Barbi, GJ Barker, GILES Barr, C Barry, M Batkiewicz, F Bench, V Berardi, S Berkman, RM Berner, L Berns, S Bhadra, S Bienstock, A Blondel, S Bolognesi, B Bourguille, SB Boyd, D Brailsford, A Bravar, C Bronner, MB Avanzini, J Calcutt, T Campbell, S Cao, SL Cartwright, A Cervera, A Chappell, C Checchia, D Cherdack, N Chikuma, G Christodoulou, J Coleman, G Collazuol, D Coplowe, A Cudd, A Dabrowska, GD Rosa, T Dealtry

Abstract:

The T2K experiment measures muon neutrino disappearance and electron neutrino appearance in accelerator-produced neutrino and antineutrino beams. With an exposure of $14.7(7.6)\times 10^{20}$ protons on target in neutrino (antineutrino) mode, 89 $\nu_e$ candidates and 7 anti-$\nu_e$ candidates were observed while 67.5 and 9.0 are expected for $\delta_{CP}=0$ and normal mass ordering. The obtained $2\sigma$ confidence interval for the $CP$ violating phase, $\delta_{CP}$, does not include the $CP$-conserving cases ($\delta_{CP}=0,\pi$). The best-fit values of other parameters are $\sin^2\theta_{23} = 0.526^{+0.032}_{-0.036}$ and $\Delta m^2_{32}=2.463\pm0.065\times10^{-3} \mathrm{eV}^2/c^4$.
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TITUS: the Tokai Intermediate Tank for the Unoscillated Spectrum

arXiv

Authors:

C Andreopoulos, FCT Barbato, G Barker, G Barr, P Beltrame, V Berardi, T Berry, A Blondel, S Boyd, A Bravar, FS Cafagna, S Cartwright, MG Catanesi, C Checchia, A Cole, G Collazuol, GA Cowan, T Davenne, T Dealtry, C Densham, G De Rosa, F Di Lodovico, E Drakopoulou, P Dunne, A Finch, M Fitton, D Hadley, K Hayrapetyan, RA Intonti, P Jonsson, A Kaboth, T Katori, L Kormos, Y Kudenko, J Lagoda, P Lasorak, M Laveder, M Lawe, P Litchfield, A Longhin, L Ludovici, W Ma, L Magaletti, M Malek, N McCauley, M Mezzetto, J Monroe, T Nicholls, M Needham, E Noah, F Nova, HM O'Keeffe, A Owen, V Palladino, D Payne, J Perkin, S Playfer, A Pritchard, N Prouse, E Radicioni, M Rayner, C Riccio, B Richards, J Rose, AC Ruggeri, R Shah, Y Shitov, C Simpson, G Sidiropoulos, T Stewart, R Terri, L Thompson, M Thorpe, Y Uchida, D Wark, MO Wascko, A Weber, JR Wilson

Abstract:

The TITUS, Tokai Intermediate Tank for Unoscillated Spectrum, detector, is a proposed Gd-doped Water Cherenkov tank with a magnetised muon range detector downstream. It is located at J-PARC at about 2 km from the neutrino target and it is proposed as a potential near detector for the Hyper-Kamiokande experiment. Assuming a beam power of 1.3 MW and 27.05 x 10^{21} protons-on-target the sensitivity to CP and mixing parameters achieved by Hyper-Kamiokande with TITUS as a near detector is presented. Also, the potential of the detector for cross sections and Standard Model parameter determination, supernova neutrino and dark matter are shown.
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Testing of Hamamatsu R5900-00-M64 Multi-Pixel PMTs for MINOS

arXiv

Authors:

MA Barker, A De Santo, P Dervan, K Lang, PS Miyagawa, R Saakyan, S Smith, D Michael, J Thomas, A Weber

Abstract:

The MINOS long baseline neutrino oscillation experiment is comprised of three calorimeters, a Near Detector at FNAL, a Far Detector at the Soudan mine in northern Minnesota, and a Calibration Detector in a test beam at CERN. The light produced in the interactions of neutrinos in the Near Detector at FNAL will be routed by optical fibres onto the pixels of Hamamatsu R5900-00-M64 multi-anode photomultiplier tubes. This article reports the measurements performed on 15 of these tubes to evaluate them for their use in MINOS.
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