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Nuclear Instruments and Methods in Physics Research | 1983

The European Hybrid Spectrometer - a facility to study multihadron events produced in high energy interactions

M. Aguilar-Benitez; W. W. M. Allison; P. Bagnaia; P. Bähler; L. Barone; W. Bartil; J.L. Benichou; A. Bergier; A. Bettini; M. Boratav; B. Brooks; F. Bruyant; E. Di Capua; E. Castelli; S. Centro; G. Chanel; P. Checchia; D. Crennel; P. Dow; J. Duboc; M. Dykes; F. Etienne; P. Ferran; C. M. Fischer; Rudolf Fruhwirth; A. Fucci; P. Gällnö; C. Geles; S. Gentile; M. De Giorgi

Abstract The European Hybrid Spectrometer is described in its preliminary version for the NA16 charm experiment. The performance of the small hydrogen bubble chamber LEBC and the detectors of the spectrometer is discussed. In particular the combination of the bubble chamber information with the spectrometer data is described in detail. The track reconstruction efficiency is 90%. The precision with which vertices seen in the bubble chamber are reconstructed is around 10 μm and the two track resolution is 40 μm. Therefore very complex event configurations, in particular charm particle decays, can be reconstructed correctly.


New Journal of Physics | 2011

Measurement of charm production in neutrino charged-current interactions

A. Kayis-Topaksu; G. Onengut; R. van Dantzig; M. de Jong; R. Oldeman; M. Guler; U. Köse; P. Tolun; M.G. Catanesi; M.T. Muciaccia; K. Winter; B. Van de Vyver; P. Vilain; G. Wilquet; B. Saitta; E. Di Capua; S. Ogawa; H. Shibuya; I.R. Hristova; T. Kawamura; D. Kolev; H. Meinhard; J. Panman; A. Rozanov; R. Tsenov; J.W.E. Uiterwijk; P. Zucchelli; J. Goldberg; M. Chikawa; J.S. Song

The nuclear emulsion target of the CHORUS detector was exposed to the wide-band neutrino beam of the CERN SPS of 27 GeV average neutrino energy from 1994 to 1997. In total, about 100 000 charged-current (CC) neutrino interactions with at least one identified muon were located in the emulsion target and fully reconstructed, using newly developed automated scanning systems. Charmed particles were searched for by a program recognizing particle decays. The observation of the decay in nuclear emulsion makes it possible to select a sample with very low background and minimal kinematical bias. In all, 2013 CC interactions with a charmed hadron candidate in the final state were selected and confirmed through visual inspection. The charm production rate induced by neutrinos relative to the CC cross-section is measured to be σ(νμN→μ−CX)/σ(CC)=(5.75 ± 0.32(stat)±0.30(syst))%. The charm production cross-section as a function of neutrino energy is also obtained. The results are in good agreement with previous measurements. The charm-quark hadronization produces the following charmed hadrons with relative fractions (in %): fD0=43.7±4.5, fΛc+=19.2±4.2, fD+=25.3±4.2 and fDs+=11.8±4.7.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1994

Construction and test of calorimeter modules for the CHORUS experiment

S. Buontempo; Alessandro Capone; A.G. Cocco; D. De Pedis; E. Di Capua; U. Dore; A. Ereditato; Matteo Ferroni; G. Fiorillo; P. Loverre; C. Luppi; D. Macina; F. Marchetti-Stasi; M. A. Mazzoni; P. Migliozzi; V. Palladino; G. Piredda; F. Riccardi; S. Ricciardi; P. Righini; B. Saitta; R. Santacesaria; P. Strolin; P. Zucchelli

Abstract The construction of modules and the assembly of the calorimeter for CHORUS, an experiment that searches for ν μ ↔ ν τ oscillation, have been completed. Within the experiment, the calorimeter is required to measure the energy of hadronic showers produced in neutrino interactions with a resolution of /∼30%/√ E (GeV). To achieve this performance, the technique, developed in recent years, of embedding scintillating fibers of 1 mm diameter into a lead matrix has been adopted for the most upstream part of the calorimeter. A more conventional system, of alternating layers of lead and scintillator strips, was used for the rest. Details of module construction as well as results obtained when modules were exposed to electron and muon beams are presented.


Physical Review C | 2008

Large-angle production of charged pions with 3-12.9 GeV/c incident protons on nuclear targets

M. G. Catanesi; E. Radicioni; R. Edgecock; M. Ellis; F. J. P. Soler; C. Gössling; S.A. Bunyatov; A. Krasnoperov; B. Popov; Serdiouk; Tereschenko; E. Di Capua; G. Vidal-Sitjes; A. Artamonov; S. Gianì; S. Gilardoni; P. Gorbunov; A. Grant; A. Grossheim; A. Ivanchenko; Ivanchenko; A. Kayis-Topaksu; J. Panman; I. Papadopoulos; E. Tcherniaev; I. Tsukerman; R. Veenhof; C. Wiebusch; P. Zucchelli; A. Blondel

M.G. Catanesi, E. Radicioni, R. Edgecock, M. Ellis, ∗ F.J.P. Soler, C. Gößling, S. Bunyatov, A. Krasnoperov, B. Popov, † V. Serdiouk, V. Tereschenko, E. Di Capua, G. Vidal–Sitjes, ‡ A. Artamonov, § S. Giani, S. Gilardoni, P. Gorbunov, § A. Grant, A. Grossheim, ¶ A. Ivanchenko, ∗∗ V. Ivanchenko, †† A. Kayis-Topaksu, ‡‡ J. Panman, I. Papadopoulos, E. Tcherniaev, I. Tsukerman, § R. Veenhof, C. Wiebusch, §§ P. Zucchelli, ¶¶ A. Blondel, S. Borghi, M.C. Morone, ∗∗∗ G. Prior, † † † R. Schroeter, C. Meurer, U. Gastaldi, G. B. Mills, ‡ ‡ ‡ J.S. Graulich, §§§ G. Grégoire, M. Bonesini, ¶¶¶ F. Ferri, M. Kirsanov, A. Bagulya, V. Grichine, N. Polukhina, V. Palladino, L. Coney, ‡ ‡ ‡ D. Schmitz, ‡ ‡ ‡ G. Barr, A. De Santo, F. Bobisut, D. Gibin, A. Guglielmi, M. Mezzetto, J. Dumarchez, U. Dore, D. Orestano, F. Pastore, A. Tonazzo, L. Tortora, C. Booth, L. Howlett, G. Skoro, M. Bogomilov, M. Chizhov, D. Kolev, R. Tsenov, S. Piperov, P. Temnikov, M. Apollonio, P. Chimenti, G. Giannini, J. Burguet–Castell, A. Cervera–Villanueva, J.J. Gómez–Cadenas, J. Mart́ın–Albo, P. Novella, M. Sorel, and A. Tornero (HARP Collaboration)


Physics Letters B | 1993

Search for νμ → ντ oscillation

M. Gruwe; C. Mommaert; P. Vilain; G. Wilquet; R. Beyer; W. Flegel; H. Grote; T. Mouthuy; H. Øveras; J. Panman; A. Rozanov; K. Winter; G. Zacek; V. Zacek; F.W. Büsser; C. Foos; L. Gerland; T. Layda; F. Niebergall; G. Rädel; P. Stähelin; T. Voss; D. Favart; G. Grégoire; E. Knoops; V. Lemaitre; P. Gorbunov; E. Grigoriev; V. Khovansky; A. Maslennikov

Abstract The fine granularity of the CHARM-II detector has been exploited to search, in the CERN-SPS wide band neutrino beam, for quasi-elastic ντ interactions followed by the decay τ → πντ. Since the sampling thickness of the target calorimeter corresponds to ∼ 1 9 of an interaction length, these events appear in the detector as a single track followed by a hadronic shower. The study of the “single pion” events is used to set limits on the νμ → ντ oscillation parameters. The maximum sensitivity to the mixing angle θ is reached for Δm2 = 50 eV2 allowing to exclude values of sin22θ greater than 6.4 × 10−3 at 90% CL.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996

Response to electrons and pions of the calorimeter for the CHORUS experiment

E. Di Capua; Matteo Ferroni; C. Luppi; S. Ricciardi; B. Saitta; P. Zucchelli; S. Buontempo; A.G. Cocco; A. Ereditato; G. Fiorillo; F. Garufi; F. Marchetti-Stasi; M. Messina; P. Migliozzi; V. Palladino; P. Strolin; A. Capone; D. Depedis; U. Dore; P. Loverre; D. Macina; M. A. Mazzoni; G. Piredda; P. Righini; R. Santacesaria

We built and tested on charged particle beams the high energy-resolution calorimeter for the CHORUS experiment, which searches for νμ-ντ oscillations in the CERN Wide Band Neutrino Beam. This calorimeter is longitudinally divided into three sectors: one electromagnetic and two hadronic. The first two upstream sectors are made of lead and plastic scintillating fibers in the volume ratio of 41, and they represent the first large scale application of this technique for combined electromagnetic and hadronic calorimetry. The third sector is made of a sandwich of lead plates and scintillator strips and complements the measurement of the hadronic energy flow. In this paper, we briefly describe the calorimeter design and we show results on its response to electrons and pions, obtained from tests performed at the CERN SPS and PS. An energy resolution of σ(E)/E=(32.3±2.4)%/E(GeV) + (1.4±0.7)% was achieved for pions, and σ(E)/E=(13.8±0.9)%/E(GeV) + (−0.2±0.4)% for electrons.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1986

TEST RESULTS OF THE STREAMER TUBE SYSTEM OF THE CHARM-II NEUTRINO DETECTOR

J.P. DeWulf; F. Bergsma; C. Busi; A. Capone; T. Delbar; D. De Pedis; A. Ereditato; Wilfried Flegel; B. Friend; W. Glessing; H. Grote; A. King; G. Lebée; C. Nieuwenhuis; Jaap Panman; A. Seiden; K. Winter; V. Zacek; T. Bauche; F.W. Büsser; L. Gerland; F. Niebergall; H. Riege; J. Schütt; P. Stähelin; A. Tadsen; J.L. Doumont; G. Grégoire; T. Mouthuy; P. Gorbunov

Abstract The CHARM II Collaboration is building a massive, fine-grained and low-density detector for the study of neutrino-electron scattering. Its target calorimeter consists of 441 detector planes with 155 232 plastic streamer tubes with digital readout of the wires and analog readout of external pickup strips. At the time of this report, about 25% of the calorimeter planes were equipped with electronics. Results on the performance of these tubes are presented as obtained with cosmic-rays and with electron and pion beams. We have also investigated the use of water vapour as an additive to the gas to suppress coating of the anode wires. The use of water would be of particular importance when using the tubes in a high-rate environment.


Astroparticle Physics | 2008

Measurement of the production cross-sections of pi(+/-) in p-C and pi(+/-)-C interactions at 12 GeV/c

M. G. Catanesi; E. Radicioni; R. Edgecock; M. Ellis; S. Robbins; F. J. P. Soler; C. Gößling; S.A. Bunyatov; A. Krasnoperov; B. Popov; V. Tereshchenko; E. Di Capua; G. Vidal-Sitjes; A. Artamonov; S. Gianì; S. Gilardoni; P. Gorbunov; A. Grant; A. Grossheim; P. Gruber; Vladimir N. Ivanchenko; A. Kayis-Topaksu; J. Panman; I. Papadopoulos; E. Tcherniaev; I. Tsukerman; R. Veenhof; C. Wiebusch; P. Zucchelli; A. Blondel

The results of the measurements of the double-differential production cross-sections of pions, dσ/dpdΩ, in p-C and π-C interactions using the forward spectrometer of the HARP experiment are presented. The incident particles are 12 GeV/c protons and charged pions directed onto a carbon target with a thickness of 5% of a nuclear interaction length. For p-C interactions the analysis is performed using 100 035 reconstructed secondary tracks, while the corresponding numbers of tracks for π-C and π-C analyses are 106 534 and 10 122 respectively. Cross-section results are presented in the kinematic range 0.5 GeV/c ≤ pπ < 8 GeV/c and 30 mrad ≤ θπ < 240 mrad in the laboratory frame. The measured cross-sections have a direct impact on the precise calculation of atmospheric neutrino fluxes and on the improved reliability of extensive air shower simulations by reducing the uncertainties of hadronic interaction models in the low energy range. HARP collaboration M.G. Catanesi, E. Radicioni Università degli Studi e Sezione INFN, Bari, Italy R. Edgecock, M. Ellis, S. Robbins, F.J.P. Soler Rutherford Appleton Laboratory, Chilton, Didcot, UK C. Gößling Institut für Physik, Universität Dortmund, Germany S. Bunyatov, A. Krasnoperov, B. Popov, V. Tereshchenko Joint Institute for Nuclear Research, JINR Dubna, Russia E. Di Capua, G. Vidal–Sitjes Università degli Studi e Sezione INFN, Ferrara, Italy A. Artamonov, S. Giani, S. Gilardoni, P. Gorbunov, A. Grant, A. Grossheim, P. Gruber, V. Ivanchenko, A. Kayis-Topaksu, J. Panman, I. Papadopoulos, E. Tcherniaev, I. Tsukerman, R. Veenhof, C. Wiebusch, P. Zucchelli CERN, Geneva, Switzerland A. Blondel, S. Borghi, M. Campanelli, M.C. Morone, G. Prior, R. Schroeter Section de Physique, Université de Genève, Switzerland R. Engel, C. Meurer Forschungszentrum Karlsruhe, Institut für Kernphysik, Karlsruhe, Germany I. Kato University of Kyoto, Japan U. Gastaldi Laboratori Nazionali di Legnaro dell’ INFN, Legnaro, Italy G. B. Mills Los Alamos National Laboratory, Los Alamos, USA J.S. Graulich, G. Grégoire Institut de Physique Nucléaire, UCL, Louvain-la-Neuve, Belgium M. Bonesini, F. Ferri Università degli Studi e Sezione INFN, Milano, Italy M. Kirsanov Institute for Nuclear Research, Moscow, Russia A. Bagulya, V. Grichine, N. Polukhina P. N. Lebedev Institute of Physics (FIAN), Russian Academy of Sciences, Moscow, Russia V. Palladino Università “Federico II” e Sezione INFN, Napoli, Italy L. Coney, D. Schmitz Columbia University, New York, USA G. Barr, A. De Santo, C. Pattison, K. Zuber Nuclear and Astrophysics Laboratory, University of Oxford, UK F. Bobisut, D. Gibin, A. Guglielmi, M. Mezzetto Università degli Studi e Sezione INFN, Padova, Italy J. Dumarchez, F. Vannucci LPNHE, Universités de Paris VI et VII, Paris, France U. Dore Università “La Sapienza” e Sezione INFN Roma I, Roma, Italy D. Orestano, F. Pastore, A. Tonazzo, L. Tortora Università degli Studi e Sezione INFN Roma III, Roma, Italy C. Booth, L. Howlett Dept. of Physics, University of Sheffield, UK M. Bogomilov, M. Chizhov, D. Kolev, R. Tsenov Faculty of Physics, St. Kliment Ohridski University, Sofia, Bulgaria S. Piperov, P. Temnikov Institute for Nuclear Research and Nuclear Energy, Academy of Sciences, Sofia, Bulgaria M. Apollonio, P. Chimenti, G. Giannini, G. Santin Università degli Studi e Sezione INFN, Trieste, Italy J. Burguet–Castell, A. Cervera–Villanueva, J.J. Gómez–Cadenas, J. Mart́ın–Albo, P. Novella, M. Sorel Instituto de F́ısica Corpuscular, IFIC, CSIC and Universidad de Valencia, Spain Now at FNAL, Batavia, Illinois, USA. Jointly appointed by Nuclear and Astrophysics Laboratory, University of Oxford, UK. Now at Codian Ltd., Langley, Slough, UK. Now at University of Glasgow, UK. Also supported by LPNHE, Universités de Paris VI et VII, Paris, France. Now at Imperial College, University of London, UK. ITEP, Moscow, Russian Federation. Permanently at Instituto de F́ısica de Cantabria, Univ. de Cantabria, Santander, Spain. Now at SpinX Technologies, Geneva, Switzerland. Now at TRIUMF, Vancouver, Canada. Now at University of St. Gallen, Switzerland. On leave of absence from Ecoanalitica, Moscow State University, Moscow, Russia. Now at Çukurova University, Adana, Turkey. Now at III Phys. Inst. B, RWTH Aachen, Aachen, Germany. On leave of absence from INFN, Sezione di Ferrara, Italy. Now at CERN, Geneva, Switzerland. Now at Univerity of Rome Tor Vergata, Italy. Now at Lawrence Berkeley National Laboratory, Berkeley, California, USA. K2K Collaboration. MiniBooNE Collaboration. Now at Section de Physique, Université de Genève, Switzerland, Switzerland. Now at Royal Holloway, University of London, UK. Now at University of Sussex, Brighton, UK. Now at ESA/ESTEC, Noordwijk, The Netherlands.


Physics Letters B | 1993

Coherent single charged pion production by neutrinos

P. Vilain; G. Wilquet; R. Beyer; W. Flegel; H. Grote; T. Mouthuy; H. Øveras; J. Panman; A. Rozanov; K. Winter; G. Zacek; V. Zacek; F.W. Büsser; C. Foos; L. Gerland; T. Layda; F. Niebergall; G. Rädel; P. Stähelin; T. Voss; D. Favart; G. Grégoire; E. Knoops; V. Lemaitre; P. Gorbunov; E. Grigoriev; V. Khovansky; A. Maslennikov; W. Lippich; A. Nathaniel

Abstract We report on a measurement of coherent single charged pion production in neutrino-nucleus scattering. The analysis is based on data taken with the CHARM II detector in beams of muon-neutrinos and -antineutrinos. The event numbers amount to N ( μ − π ) = 748 and N ( μ + π ) = 631. Cross sections and their dependence on the neutrino energy are determined. The results are in agreement with the predictions of models based on the PCAC hypothesis.


Physical Review C | 2009

Large-angle production of charged pions with incident pion beams on nuclear targets

M. Apollonio; D. Gibin; A. Bagulya; G. B. Mills; G. Giannini; V. Grichine; R. Edgecock; M. Bogomilov; L. Coney; A. Grossheim; J.S. Graulich; C. Gössling; Vladimir N. Ivanchenko; P. Novella; A. Kayis-Topaksu; F. Pastore; P. Gorbunov; G. Gregoire; S. Gianì; E. Radicioni; P. Temnikov; F. Bobisut; M. G. Catanesi; D. Kolev; F. Ferri; A. Ivanchenko; P. Chimenti; G.P. Škoro; M. Mezzetto; M. Ellis

We gratefully acknowledge the help and support of the PS beam staff and of the numerous technical collaborators who contributed to the detector design, construction, commissioning and operation. In particular, we would like to thank G. Barichello, R. Brocard, K. Burin, V. Carassiti, F. Chignoli, D. Conventi, G. Decreuse, M. Delattre, C. Detraz, A. Domeniconi, M. Dwuznik, F. Evangelisti, B. Friend, A. Iaciofano, I. Krasin, D. Lacroix, J.-C. Legrand, M. Lobello, M. Lollo, J. Loquet, F. Marinilli, J. Mulon, L. Musa, R. Nicholson, A. Pepato, P. Petev, X. Pons, I. Rusinov, M. Scandurra, E. Usenko, and R. van der Vlugt, for their support in the construction of the detector. The collaboration acknowledges the major contributions and advice of M. Baldo-Ceolin, L. Linssen, M.T. Muciaccia and A. Pullia during the construction of the experiment. The collaboration is indebted to V. Ableev, P. Arce, F. Bergsma, P. Binko, E. Boter, C. Buttar, M. Calvi, M. Campanelli, C. Cavion, A. Chukanov, A. De Min, M. Doucet, D. Dullmann, R. Engel, V. Ermilova, W. Flegel, P. Gruber, Y. Hayato, P. Hodgson, A. Ichikawa, I. Kato, O. Klimov, T. Kobayashi, D. Kustov, M. Laveder, M. Mass, H. Meinhard, T. Nakaya, K. Nishikawa, M. Paganoni, F. Paleari, M. Pasquali, J. Pasternak, C. Pattison, M. Placentino, S. Robbins, G. Santin, V. Serdiouk, S. Simone, A. Tornero, S. Troquereau, S. Ueda, A. Valassi, F. Vannucci and K. Zuber for their contributions to the experiment and to P. Dini for help in MC production. We acknowledge the contributions of V. Ammosov, G. Chelkov, D. Dedovich, F. Dydak, M. Gostkin, A. Guskov, D. Khartchenko, V. Koreshev, Z. Kroumchtein, I. Nefedov, A. Semak, J. Wotschack, V. Zaets and A. Zhemchugov to the work described in this paper. The experiment was made possible by grants from the Institut Interuniversitaire des Sciences Nucleaires and the Interuniversitair Instituut voor Kernwetenschappen (Belgium), Ministerio de Educacion y Ciencia, Grant FPA2003-06921-c02-02 and Generalitat Valenciana, grant GV00-054-1, CERN (Geneva, Switzerland), the German Bundesministerium fur Bildung und Forschung (Germany), the Istituto Nazionale di Fisica Nucleare (Italy), INR RAS (Moscow), the Russian Foundation for Basic Research (grant 08-02-00018) and the Particle Physics and Astronomy Research Council (UK). We gratefully acknowledge their support. This work was supported in part by the Swiss National Science Foundation and the Swiss Agency for Development and Cooperation in the framework of the programme SCOPES - Scientific co-operation between Eastern Europe and Switzerland.

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M. Ellis

Rutherford Appleton Laboratory

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R. Edgecock

Rutherford Appleton Laboratory

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M. G. Catanesi

Instituto Politécnico Nacional

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S.A. Bunyatov

Joint Institute for Nuclear Research

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G. Grégoire

Université catholique de Louvain

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E. Radicioni

Russian Academy of Sciences

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