E. Lodi Rizzini
University of Brescia
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Featured researches published by E. Lodi Rizzini.
Nature | 2002
M. Amoretti; C. Amsler; G. Bonomi; A. Bouchta; P. D. Bowe; C. Carraro; C. L. Cesar; M. Charlton; M.J.T. Collier; M. Doser; V. Filippini; K. Fine; A. Fontana; M. C. Fujiwara; R. Funakoshi; P. Genova; J. S. Hangst; R. Hayano; M. H. Holzscheiter; L. V. Jørgensen; V. Lagomarsino; R. Landua; D. Lindelöf; E. Lodi Rizzini; M. Macri; N. Madsen; G. Manuzio; M. Marchesotti; Paolo Montagna; H. Pruys
A theoretical underpinning of the standard model of fundamental particles and interactions is CPT invariance, which requires that the laws of physics be invariant under the combined discrete operations of charge conjugation, parity and time reversal. Antimatter, the existence of which was predicted by Dirac, can be used to test the CPT theorem—experimental investigations involving comparisons of particles with antiparticles are numerous. Cold atoms and anti-atoms, such as hydrogen and antihydrogen, could form the basis of a new precise test, as CPT invariance implies that they must have the same spectrum. Observations of antihydrogen in small quantities and at high energies have been reported at the European Organization for Nuclear Research (CERN) and at Fermilab, but these experiments were not suited to precision comparison measurements. Here we demonstrate the production of antihydrogen atoms at very low energy by mixing trapped antiprotons and positrons in a cryogenic environment. The neutral anti-atoms have been detected directly when they escape the trap and annihilate, producing a characteristic signature in an imaging particle detector.
Physical Review Letters | 2003
M. Amoretti; P. Genova; D. P. van der Werf; D. Lindelöf; G. Bonomi; R. Funakoshi; C. Amsler; R. Landua; E. Lodi Rizzini; A. Fontana; J. S. Hangst; C. Regenfus; M. C. Fujiwara; A. Bouchta; V. Filippini; G. Manuzio; G. Testera; N. Madsen; P. Montagna; L. V. Jørgensen; A. Rotondi; M. Charlton; V. Lagomarsino; C. L. Cesar; A. Variola; H. Pruys; R. Hayano; M. Macri; P. D. Bowe; C. Carraro
Production of antihydrogen atoms by mixing antiprotons with a cold, confined, positron plasma depends critically on parameters such as the plasma density and temperature. We discuss nondestructive measurements, based on a novel, real-time analysis of excited, low-order plasma modes, that provide comprehensive characterization of the positron plasma in the ATHENA antihydrogen apparatus. The plasma length, radius, density, and total particle number are obtained. Measurement and control of plasma temperature variations, and the application to antihydrogen production experiments are discussed.
Physics Letters B | 1999
A. Zenoni; A. Bianconi; G. Bonomi; M. Corradini; A. Donzella; E. Lodi Rizzini; L. Venturelli; A. Bertin; M. Bruschi; M. Capponi; S. De Castro; R. Donà; D. Galli; Benedetto Giacobbe; U. Marconi; I. Massa; M. Piccinini; R. Spighi; V. Vagnoni; S. Vecchi; M. Villa; A. Vitale; A. Zoccoli; M. Poli; C. Cicalò; A. Masoni; S. Mauro; G. Puddu; S. Serci; G. Usai
Abstract The pp total annihilation cross section has been measured, with the Obelix apparatus at LEAR, at ten values of the antiproton incident momentum between 43 and 175 MeV/c. The values of the cross section show that the well known 1 p behaviour of the annihilation cross section is drastically modified at very low momenta, which demonstrates the important role of the Coulomb force in low energy pp interaction. Moreover, they do not present any explicit resonant behaviour. Finally, when compared to potential model calculations, the data suggest that the percentage of P-wave in pp interaction around 50 MeV/c antiproton incident momentum is less than 5%.
Nuclear Physics | 1986
F. Balestra; S. Bossolasco; M.P. Bussa; L. Busso; L. Ferrero; A. Grasso; D. Panzieri; G. Piragino; T. Tosello; G. Bendiscioli; V. Filippini; G. Fumagalli; C. Marciano; A. Rotondi; A. Zenoni; C. Guaraldo; A. Maggiora; Yu. A. Batusov; I. V. Falomkin; G. B. Pontecorvo; M.G. Sapozhnikov; M. Vascon; G. Zanella; E. Lodi Rizzini
Abstract By means of a streamer chamber exposed to the LEAR antiproton beams, the total reaction cross sections, the charged-prong multiplicity distributions and lower limits for the production of negative pions and K s 0 in the p-Ne interaction were measured at 19.6, 48.7 and 179.6 MeV. Annihilation was found to be dominant over all other non-elastic p-Ne processes. An analysis of Ne and other nuclei data in the frame of the Glauber theory allowed us to determine the ratio between the p-n and the p-p cross sections. An analysis in the light of INC model predictions allowed us to show up events which can be interpreted as annihilations having occurred deeply inside the nuclei.
Physics Letters B | 1999
A. Zenoni; A. Bianconi; F Bocci; G. Bonomi; M. Corradini; A. Donzella; E. Lodi Rizzini; L. Venturelli; A. Bertin; M. Bruschi; M. Capponi; S. De Castro; R. Donà; D. Galli; Benedetto Giacobbe; U. Marconi; I. Massa; M. Piccinini; R. Spighi; V. Vagnoni; S. Vecchi; M. Villa; A. Vitale; A. Zoccoli; C. Cicalò; A. Masoni; S. Mauro; G. Puddu; S. Serci; G. Usai
Abstract The p p total annihilation cross section has been measured at four values of the p incident momentum, between 70 MeV/c and 38 MeV/c, with the Obelix apparatus at LEAR. The new measurements are in agreement with the trend of previous measurements of the p p total annihilation cross section at low energy, performed by the Obelix experiment [A. Bertin et al., Phys. Lett. B 369 (1996) 77; A. Benedettini et al., Nucl. Phys. B (Proc. Suppl.) 56A (1997) 58], as well as with a fit of the latter data based on a low energy expansion of the scattering amplitude [J. Carbonell, K.V. Protasov, A. Zenoni, Phys. Lett. B 397 (1997) 345]. The departure of the annihilation cross section from a smooth behaviour, suggested by a previous measurement of the cross section around 44 MeV/c [A. Bertin et al., Phys. Lett. B 369 (1996) 77], is not confirmed by the new data.
Physics Letters B | 1985
F. Balestra; S. Bossolasco; M.P. Bussa; L. Bussa; L. Ferrero; D. Panzieri; G. Piragino; F. Tosello; C. Guaraldo; A. Maggiora; Yu. A. Batusov; I. V. Falomkin; G. B. Pontecorvo; M.G. Sapozhnikov; G. Bendiscioli; V. Filippini; G. Fumagalli; C. Marciano; A. Rotondi; A. Zenoni; E. Lodi Rizzini; M. Vascon; G. Zanella
The antiproton-helium reaction cross section has been measured at 19.6 and 48.7 MeV with a streamer chamber in a magnetic field. Charged prongs and negative pion multiplicities and cross sections for the production of 3He are given. A comparison with p 2H is performed. he previously obtained 179.6 MeV results are also taken into account.
Physics Letters B | 1992
A. Adamo; M. Agnello; F. Balestra; G. Belli; G. Bendiscioli; A. Bertin; P. Boccaccio; G.C. Bonazzola; T. Bressani; M. Bruschi; M.P. Bussa; L. Busso; D. Calvo; M. Capponi; M. Corradini; S. Costa; S. De Castro; F. D'Isep; L. Fava; A. Feliciello; L. Ferrero; V. Filippini; D. Galli; R. Garfagnini; U. Gastaldi; P. Gianotti; A. Grasso; C. Guaraldo; Felice Iazzi; A. Lanaro
Abstract First results on meson spectroscopy using antineutrons as projectiles are reported. Three-body (π + π + π − ) and five-body (π + π + π + π − π − ) final states following the annihilation of 100 to 290 MeV/ c antineutrons on hydrogen were analyzed. The (π + π − ) invariant mass spectrum in the three-body reaction is accounted for by the ϱ 0 anf f 2 (1270) resonances, together with an enhancement around 1540 MeV, in the region of the AX (1565) and the f 2 (1515) resonances, whereas the best fit for the (π + π + π − π − ) invariant mass in five-body events shows the already reported structure ζ(1480) and suggests the presence of a second structure around 1650 MeV.
Nuclear Physics | 1987
F. Balestra; M.P. Bussa; L. Busso; L. Fava; L. Ferrero; D. Panzieri; G. Piragino; F. Tosello; G. Bendiscioli; A. Rotondi; P. Salvini; A. Zenoni; C. Guaraldo; A. Maggiora; Yu. A. Batusov; I. V. Falomkin; F. Nichitiu; G. B. Pontecorvo; E. Lodi Rizzini
Abstract The ratio R a b between the cross sections for the annihilation of p on n and on p bound in the 4 He nucleus at four p momenta (at rest, 192.8, 306.2 and 607.7 MeV/ c ) has been obtained by the analysis of p 4 He annihilation events detected with a self-shunted streamer chamber exposed to the LEAR p beams. R a b increases from 0.42 ± 0.05 at rest up to 0.66 ± 0.09 at 607.7 MeV/ c . The results are discussed in the light of Glauber theory analyses of p 2 H and p -nucleus data.
Physics of Plasmas | 2003
M. Amoretti; G. Bonomi; A. Bouchta; P. D. Bowe; C. Carraro; C. L. Cesar; M. Charlton; M. Doser; A. Fontana; M. C. Fujiwara; R. Funakoshi; P. Genova; J. S. Hangst; R. Hayano; L. V. Jørgensen; V. Lagomarsino; R. Landua; E. Lodi Rizzini; M. Macri; N. Madsen; G. Manuzio; G. Testera; A. Variola; D. P. van der Werf
The detection of electrostatic nonneutral plasma modes in the ATHENA (ApparaTus for High precision Experiment on Neutral Antimatter) experiment [M. Amoretti, C. Amsler, G. Bonomi et al., Nature (London) 419, 456 (2002)] is described. A complete nondestructive diagnostic of the plasma based on a fit to the line shape of the function describing the power transmitted through the plasma around the frequency of the fundamental mode is developed and the experimental results are presented and discussed.
Physics Letters B | 1987
F. Balestra; M.P. Bussa; L. Busso; L. Fava; L. Ferrero; D. Panzieri; G. Piragino; F. Tosello; G. Bendiscioli; A. Rotondi; P. Salvini; A. Zenoni; Yu. A. Batusov; I. V. Falomkin; G. B. Pontecorvo; M.G. Sapozhnikow; V.I. Tretyak; C. Guaraldo; A. Maggiora; E. Lodi Rizzini; A. Haatuft; A. Halsteinslid; K. Myklebost; J.M. Olsen; F.O. Breivik; T. Jacobsen; S.O. Sørensen
Abstract The Λ 0 and K 0 s production cross sections have been measured at 607 MeV/ c for the reaction p + 20 Ne → V 0 + X ( V 0 =Λ, 0 , K 0 s ) . The Λ 0 /K 0 s production ratio is found to be (2.3±0.7). The data are consistent with an evaporative character of the emission mechanism from a multinucleon system for Λ 0 and from one nucleon for K 0 s . The rapidity distributions of negative tracks in K 0 x events are different from those in Λ 0 events without V 0 .