M. Fidecaro
CERN
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Featured researches published by M. Fidecaro.
Physics Letters B | 1998
A. Angelopoulos; K. Jon-And; J. Derre; C.W.E. van Eijk; A. Muller; M. Schäfer; M. Carroll; C. Santoni; P. Kokkas; G. Backenstoss; H.-J. Gerber; R. Rickenbach; J. R. Fry; P. Carlson; Marc Dejardin; A. Schopper; O. Behnke; F. Touchard; F. Henry-Couannier; R. Gamet; T. Nakada; P.-R. Kettle; R. Le Gac; L.A. Schaller; M. Fidecaro; P. Pavlopoulos; A. Go; R. Kreuger; I. Mandić; A. Filipčič
Abstract We report on the first observation of time-reversal symmetry violation through a comparison of the probabilities of K 0 transforming into K0 and K0 into K 0 as a function of the neutral-kaon eigentime t. The comparison is based on the analysis of the neutral-kaon semileptonic decays recorded in the CPLEAR experiment. There, the strangeness of the neutral kaon at time t=0 was tagged by the kaon charge in the reaction p p → K ± π ∓ K 0 ( K 0 ) at rest, whereas the strangeness of the kaon at the decay time t=τ was tagged by the lepton charge in the final state. An average decay-rate asymmetry 〈 R( K 0 t=0 → e + π − ν t=τ )−R( K 0 t=0 → e − π + ν t=τ ) R( K 0 t=0 → e + π − ν t=τ )+R( K 0 t=0 → e − π + ν t=τ ) 〉=(6.6±1.3 stat ±1.0 syst )×10 −3 was measured over the interval 1 τ S τ S , thus leading to evidence for time-reversal non-invariance.
Physics Letters B | 1998
A. Apostolakis; E. Aslanides; G. Backenstoss; P. Bargassa; O. Behnke; A. Benelli; V. Bertin; F. Blanc; P. Bloch; P. Carlson; M. Carroll; E. Cawley; G. Chardin; M.B. Chertok; A. Cody; Marc Dejardin; J. Derre; A. Ealet; C. Eleftheriadis; R. Ferreira-Marques; W. Fetscher; M. Fidecaro; A. Filipčič; D. Francis; J. R. Fry; E. Gabathuler; R. Gamet; H.-J. Gerber; A. Go; C. Guyot
Abstract The EPR-type strangeness correlation in the K0 K 0 system produced in the reaction p p → K 0 K 0 at rest has been tested using the CPLEAR detector. The strangeness was tagged via strong interaction with absorbers away from the creation point. The results are consistent with the QM non-separability of the wave function and exclude a spontaneous wave-function factorisation at creation (CL >99.99%).
Physics Letters B | 1995
R. Adler; K. Jon-And; A. Liolios; J. Derre; Eef van Beveren; Dimitri V. Nanopoulos; L. Sakeliou; R. Rickenbach; P. Fassnacht; P. Carlson; Theo Geralis; A. Schopper; R. Gamet; Jorge L. Lopez; E. Machado; C.W.E. van Eijk; Philippe Schune; D. Francis; P. Weber; A. Apostolakis; T. Ruf; J. Pinto da Cunha; D. Garreta; J. Carvalho; M. Carroll; Marc Dejardin; M. Mikuz; M. Fidecaro; I. Mandić; Ch. Yèche
Abstract We use fits to recent published CPLEAR data on neutral kaon decays to π + π − and πeν to constrain the CPT-violation parameters appearing in a formulation of the neutral kaon system as an open quantum-mechanical system. The obtained upper limits of the CPT-violation parameters are approaching the range suggested by certain ideas concerning quantum gravity.
Physics Letters B | 1999
A. Apostolakis; K. Jon-And; J. Derre; C.W.E. van Eijk; A. Muller; M. Schäfer; M. Carroll; P. Kokkas; G. Backenstoss; H.-J. Gerber; R. Rickenbach; V. Bertin; P. Carlson; Marc Dejardin; A. Schopper; O. Behnke; F. Touchard; F. Henry-Couannier; R. Gamet; T. Nakada; P.-R. Kettle; R. Le Gac; L.A. Schaller; M. Fidecaro; A. Go; R. Kreuger; I. Mandić; A. Filipcic; M.B. Chertok; P. Bloch
Abstract Data from the CPLEAR experiment, together with the most recent world averages for some of the neutral-kaon parameters, were constrained with the Bell–Steinberger (or unitarity) relation, allowing the T-violation parameter Re( ϵ ) and the CPT-violation parameter Im( δ ) of the neutral-kaon mixing matrix to be determined with an increased accuracy: Re( ϵ )=(164.9±2.5)×10 −5 , Im( δ )=(2.4±5.0)×10 −5 . Moreover, the constraint allows the CPT-violation parameter for the neutral-kaon semileptonic decays, Re( y ), to be determined for the first time. The ΔS ≠ ΔQ parameters Re( x − ) and Im( x + ) are given with an increased accuracy. The quantity Re( y + x − ), which enters the T-violation CPLEAR asymmetry previously published, is determined to be (−0.2±0.3)×10 −3 . The value obtained for Re( δ ) is in agreement with the one resulting from a previous unconstrained fit and has a slightly smaller error.
Physics Letters B | 1985
G. Fidecaro; M. Fidecaro; L. Lanceri; A. Marchioro; W. Mampe; M. Baldo-Ceolin; F. Mattioli; G. Puglierin; C.J. Batty; K. Green; H.B. Prosper; P. Sharman; J.M. Pendlebury; K.F. Smith
Abstract The observation of neutron-antineutron transitions would be direct evidence for baryon number violation. For the first time an experiment has been carried out to search for this phenomenon with neutrons in free flight. The experiment using the research reactor at the Institut Laue-Langevin in Grenoble has set a lower limit to the oscillation time τ n n of 106 s.
Physics Letters B | 1999
A. Apostolakis; E. Aslanides; G. Backenstoss; P. Bargassa; O. Behnke; A. Benelli; V. Bertin; F. Blanc; P. Bloch; P. Carlson; M. Carroll; E. Cawley; G. Chardin; M.B. Chertok; M. Danielsson; Marc Dejardin; J. Derre; A. Ealet; Christos Eleftheriadis; L. Faravel; W. Fetscher; M. Fidecaro; A. Filipcic; D. Francis; J. R. Fry; E. Gabathuler; R. Gamet; H.-J. Gerber; A. Go; A. Haselden
Abstract We test the Principle of Equivalence for particles and antiparticles, using CPLEAR data on tagged K0 and K 0 decays into π+π−. For the first time, we search for possible annual, monthly and diurnal modulations of the observables |η+−| and φ+−, that could be correlated with variations in astrophysical potentials. Within the accuracy of CPLEAR, the measured values of |η+−| and φ+− are found not to be correlated with changes of the gravitational potential. We analyze data assuming effective scalar, vector and tensor interactions, and we conclude that the Principle of Equivalence between particles and antiparticles holds to a level of 6.5, 4.3 and 1.8×10−9, respectively, for scalar, vector and tensor potentials originating from the Sun with a range much greater than the distance Earth–Sun. We also study energy-dependent effects that might arise from vector or tensor interactions. Finally, we compile upper limits on the gravitational coupling difference between K0 and K 0 as a function of the scalar, vector and tensor interaction range.
Physics Reports | 2003
A. Angelopoulos; A. Apostolakis; E. Aslanides; G. Backenstoss; P. Bargassa; C.P. Bee; O. Behnke; A. Benelli; V. Bertin; F. Blanc; P. Bloch; P. Carlson; M. Carroll; E. Cawley; M.B. Chertok; M. Danielsson; Marc Dejardin; J. Derre; A. Ealet; C. Eleftheriadis; R. Ferreira-Marques; W. Fetscher; M. Fidecaro; A. Filipčič; D. Francis; J. R. Fry; E. Gabathuler; R. Gamet; H.-J. Gerber; A. Go
LEAR offered unique opportunities to study the symmetries which exist between matter and antimatter. At variance with other approaches at this facility, CPLEAR was an experiment devoted to the study of , and symmetries in the neutral-kaon system. A variety of measurements allowed us to determine with high precision the parameters which describe the time evolution of the neutral kaons and their antiparticles, including decay amplitudes, and the related symmetry properties. Limits concerning quantum-mechanical predictions (EPR, coherence of the wave function) or the equivalence principle of general relativity have been obtained. An account of the main features of the experiment and its performances is given here, together with the results achieved.
Physics Letters B | 1999
A. Apostolakis; E. Aslanides; G. Backenstoss; P. Bargassa; O. Behnke; A. Benelli; V. Bertin; F. Blanc; P. Bloch; P. Carlson; M. Carroll; E. Cawley; M.B. Chertok; M. Danielsson; Marc Dejardin; J. Derre; A. Ealet; Christos Eleftheriadis; W. Fetscher; M. Fidecaro; A. Filipcic; D. Francis; J. R. Fry; E. Gabathuler; R. Gamet; H.-J. Gerber; A. Go; A. Haselden; P.J. Hayman; F. Henry-Couannier
LEAR offered unique opportunities to study the symmetries which exist between matter and antimatter. At variance with other approaches at this facility, CPLEAR was an experiment devoted to the study of CP, T and CPT symmetries in the neutral-kaon system. A variety of measurements allowed us to determine with high precision the parameters which describe the time evolution of the neutral kaons and their antiparticles, including decay amplitudes, and the related symmetry properties. Limits concerning quantum-mechanical predictions (EPR, coherence of the wave function) or the equivalence principle of general relativity have been obtained. An account of the main features of the experiment and its performances is given here, together with the results achieved.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1987
M.G. Catanesi; G. Crosetti; M. Fidecaro; E. Bernardi; R. Klanner; D. Lüke; R. Walczak; M. Gennis; Rudolf Langkau; W. Scobel; J. Krüger; J.H. Peters; H. Spitzer; M.J. Esten; M. De Vincenzi; A. Frenkel; E. Lamanna; G. Marini; G. Martellotti; A. Nigro; G. Penso; P. Pistilli; A. Sciubba
Abstract A hadron calorimeter comprising 10 mm depleted uranium plates and 5 mm plastic scintillator was exposed to electrons, hadrons and muons in the energy range 5–210 GeV. The measured ratios of sampling fractions are 0.8 for e/π and 0.6 for e/mip. The addition of a fine grained electromagnetic calorimeter with 1.6 mm depleted uranium plates and 4 mm plastic scintillator in front of the hadron calorimeter leads to a slightly worse hadronic energy resolution. Results on the longitudinal shower development and energy containment for hadron showers are given.
Physics Letters B | 1988
H Cobbaert; R. G. M. F. Roosen; M G Catanesi; M.T. Muciaccia; S. Natali; S. Nuzzo; F. Ruggieri; G. Carboni; G. Crosetti; M. Fidecaro; C. Gerke; P. Musset; G. Poulard; H. Sletten; M Coupland; I.G. Roberts; P. T. Trent; J H Bartley; J E Conboy; B.G. Duff; M. J. Esten; P Fennel; P F Harrison; M. De Vincenzi; S. Di Liberto; A. Frenkel; E. Lamanna; G. Marini; G. Martellotti; A. Nigro
Abstract The A-dependence of the charm production cross section is determined by measuring the yield of prompt single muons in a beam-dump experiment, using a 300 GeV/c proton beam on Al, Fe, and U targets. Assuming that the production cross section varies as Aα, we obtain α(μ+) = 0.79±0.12 and α(μ−) = 0.76±0.13 in the kinematical region xF≳0.1 of the charm.