P. Spinelli
University of Bari
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Featured researches published by P. Spinelli.
The Astrophysical Journal | 1997
M. Boezio; Per Carlson; Tom Francke; N. Weber; M. Suffert; M. Hof; W. Menn; Michael Simon; S. A. Stephens; R. Bellotti; F. Cafagna; M. Castellano; M. Circella; G. de Cataldo; C. De Marzo; N. Giglietto; P. Spinelli; M. Bocciolini; P. Papini; A. Perego; S. Piccardi; P. Spillantini; G. Basini; Mario V. Ricci; A. Codino; N. Finetti; C. Grimani; M. Candusso; M. Casolino; M. P. De Pascale
We report on the absolute antiproton Nux and the antiproton to proton ratio in the energy range 0.62E3.19 GeV at the top of the atmosphere, measured by the balloon-borne experiment CAPRICE Nown from Lynn Lake, Manitoba, Canada, on 1994 August 8E9. The experiment used the New Mexico State University WiZard/CAPRICE balloon-borne magnet spectrometer equipped with a solid radiator Ring Imaging Cherenkov (RICH) detector and a silicon-tungsten calorimeter for particle identi-cation. This is the -rst time a RICH is used together with an imaging calorimeter in a balloon experiment, and it allows antiprotons to be clearly identi-ed over the rigidity range 1.2E4 GV. Nine antiprotons were identi-ed in the energy range 0.62E3.19 GeV at the top of the atmosphere. The data were collected over 18 hr at a mean residual atmosphere of 3.9 g cm~2. The absolute antiproton Nux is consistent with a pure secondary production of antiprotons during the propagation of cosmic rays in the Galaxy. Subject headings: balloons E cosmic rays E elementary particles E Sun: activity
The Astrophysical Journal | 1996
R. L. Golden; S.J. Stochaj; S. A. Stephens; F. Aversa; G. Barbiellini; M. Boezio; U. Bravar; A. Colavita; F. Fratnik; P. Schiavon; A. Vacchi; N. Zampa; J. W. Mitchell; J.F. Ormes; R. E. Streitmatter; R. Bellotti; F. Cafagna; M. Castellano; M. Circella; G. de Cataldo; C. De Marzo; N. Giglietto; B. Marangelli; A. Rain; P. Spinelli; M. Bocciolini; N. Finetti; P. Papini; A. Perego; S. Piccardi
As part of a series of experiments to search for antimatter in cosmic rays, the New Mexico State University balloon-borne magnet spectrometer was configured for a flight to study positrons. Two completely new instruments, a transition radiation detector and a silicon-tungsten imaging calorimeter, were added to the magnet spectrometer. These two detectors provided a proton rejection factor better than 3 × 104. This instrument was flown from Fort Sumner, New Mexico, at an average depth of 4.5 g cm-2 of residual atmosphere for a period of 25 hr. We report here the measured fraction of positrons e+/(e+ + e-) from ~5 to 60 GeV at the top of the atmosphere. Our measurements do not show any compelling evidence for an increase in this ratio with energy, and our results are consistent with a constant fraction of 0.078 ± 0.016 over the entire energy region.
Physics Letters B | 1982
C. De Marzo; M. De Palma; A. Distante; C. Favuzzi; G. Germinario; P. Lavopa; G. Maggi; F. Posa; A. Ranieri; G. Selvaggi; P. Spinelli; F. Waldner; A. Bialas; W. Czyz; T. Coghen; A. Eskreys; K. Eskreys; K. Fialkowski; D. Kisieliewska; B. Madeysky; P. Malecki; K. Olkiewicz; D. Pawlik; W.H. Evans; J. R. Fry; C. Grant; M. Houlden; A. Morton; H. Muirhead; J. Shiers
Abstract Large transverse energy cross sections of 300 GeV/ c pions and protons on hydrogen have been measured with a segmented calorimeter covering the central rapidity region −0.88 y π in azimuth. The selected events show large multiplicities and no jet-like event structure. Processes more complicated than the scattering of two constituents appear to dominate these inelastic collisions.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1988
M. Calicchio; G. Case; C. DeMarzo; O. Erriquez; C. Favuzzi; N. Giglietto; E. Nappi; F. Posa; P. Spinelli; F. Baldetti; S. Cecchini; G. Giacomelli; F. Grianti; G. Mandrioli; A. Margiotta; L. Patrizii; G. Sanzani; P. Serra; M. Spurio; Steven P. Ahlen; A. Ciocio; M. Felcini; D. Ficenec; J. Incandela; A. Marin; J. L. Stone; L. Sulak; W. Worstell; Barry C. Barish; C. Lane
Abstract The MACRO detector is presently under construction, its installation at Gran Sasso being planned to start in September 1987. It is a large area detector, the acceptance for isotropic particle fluxes being around 10 000 m 2 sr, designed to search for rare phenomena in the cosmic radiation. It makes use of three detection techniques: liquid scintillator counters, plastic streamer tubes, and track-etch. It will perform a search for GUT monopoles (or any supermassive charged penetrating particle), a survey of cosmic point sources of HE gammas and neutrinos, a systematic study of the penetrating cosmic ray muons, and will be sensitive to neutrino bursts from gravitational stellar collapses in the Galaxy.
European Physical Journal C | 1988
A. Bamberger; D. Bangert; J. Bartke; H. Bialkowska; R. Bock; R. Brockmann; S. I. Chase; C. De Marzo; M. De Palma; I. Derado; V. Eckardt; C. Favucci; J. Fent; D. Ferenc; P. Freund; M. Gazdzicki; H.J. Gebauer; K. Geissler; C. Guerra; John William Harris; W. Heck; T. J. Humanic; K. Kadija; A. Karabarbounis; R. Keidel; M. Kowalski; W. Krischer; M. Lahanas; S. Margetis; E. Nappi
The results on spectra of negative particles produced in16O+Au andp-Au collisions at 200 GeV/nucleon and16O+Au at 60 GeV/nucleon are presented. The correlations of average rapidity and average transverse momentum with event multiplicity are studied. Spectral shapes are similar for central16O+Au andp-Au collisions. The transverse momentum and rapidity distributions for central16O+Au andp-Au collisions differ strongly from corresponding distributions forp+p interactions. The FRITIOF model fails to describe the shapes of the transverse momentum distributions. The simple thermodynamical model of a single fireball does not fit the midrapidity transverse momentum distributions, and the rapidity distributions.
Physics Letters B | 1990
S. Ahlen; M. Ambrosio; G. Auriemma; A. Baldini; G.C. Barbarino; B. Barish; G. Battistoni; R. Bellotti; C. Bemporad; P. Bernardini; H. Bilokon; V. Bisi; C. Bloise; C. Bower; F. Cafagna; M. Calicchio; P. Campana; S. Cecchini; V. Chiarella; P. Chrysicopoulou; S. Coutu; I.D' Antone; C. De Marzo; G. de Cataldo; M. De Vincenzi; O. Erriquez; C. Favuzzi; D. Ficenec; V. Flaminio; C. Forti
Abstract The MACRO detector, located in the underground Gran Sasso Laboratory, had its initial data run from February 27 to May 30, 1989, using the first supermodule (SΩ∼800 m 2 sr ) . Approximately 245 000 muon events were recorded. Here are reported the results of the analysis of penetrating muons which determine the measured vertical muon flux at depths greater than 3000 m.w.e. In addition the data have been used to search for large scale anisotropies.
Physics Letters B | 1988
A. Bamberger; D. Bangert; J. Bartke; H. Bialkowska; R. Bock; R. Brockmann; S. I. Chase; C. De Marzo; M. De Palma; I. Derado; V. Eckardt; C. Favuzzi; J. Fent; D. Ferenc; H. Fessler; P. Freund; M. Gazdzicki; H.J. Gebauer; K. Geissler; E. Gladysz; C. Guerra; John William Harris; W. Heck; T. J. Humanic; K. Kadija; A. Karabarbounis; R. Keidel; J. Kosiec; M. Kowalski; S. Margetis
Abstract Inelastic cross sections at 60 and 200 GeV/nucleon are determined in a streamer chamber for 16 O on several nuclear targets. Charged particle multiplicity distributions for inelastic and central collisions are studied and compared with theoretical predictions. The inelastic cross section exhibit a geometrical dependence on nuclear radii. The multiplicity data are governed by the collision geometry. They are consistent with a picture of superposition of independent nucleon-nucleus interactions.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002
O. Adriani; M. Ambriola; G. C. Barbarino; Loius M. Barbier; S. Bartalucci; G.A. Bazilevskaja; R. Bellotti; S. Bertazzoni; V. Bidoli; M. Boezio; Edward Bogomolov; L. Bonechi; V. Bonvicini; M Boscherini; Ulisse Bravar; F. Cafagna; D. Campana; P. Carlson; M. Casolino; Maria Gabriella Castellano; G. Castellini; E. R. Christian; F. Ciacio; M. Circella; Raffaello D'Alessandro; C. De Marzo; M. P. De Pascale; N. Finetti; G. Furano; A. Gabbanini
The PAMELA equipment will be assembled in 2001 and installed on board the Russian satellite Resurs. PAMELA is conceived mainly to study the antiproton and positron fluxes in cosmic rays up to high ...
Astroparticle Physics | 1997
A. Bakaldin; G. Barbiellini; S. Bartalucci; A. Batishev; R. Bellotti; V. Bidoli; M. Boezio; W. Bonvicini; F. Cafagna; M. Casolino; M. Castellano; M. Circella; C. De Marzo; M. P. De Pascale; Arkady Moiseev Galper; S. Giuntoli; S. V. Koldashov; M. Korotkov; V. V. Mikhailov; A. Morselli; A. Murashov; P. Papini; S. Piccardi; P. Picozza; M. Ricci; R. Sparvoli; P. Spillantini; P. Spinelli; A. Vacchi; S. A. Voronov
Abstract The mission NINA is the first step of a wide scientific program named WiZard-RIM, conceived to make extensive studies on the Anomalous Component and the isotopic composition of the cosmic rays from hydrogen to iron, in the energy range 10–100 MeV/n. NINA is a silicon detector which is going to fly on the Russian Resource 01 n.4 satellite by the end of 1997.
Physical Review D | 2017
S. Abdollahi; M. Ackermann; M. Ajello; W. B. Atwood; L. Baldini; G. Barbiellini; D. Bastieri; R. Bellazzini; E. D. Bloom; R. Bonino; T. Brandt; J. Bregeon; P. Bruel; R. Buehler; R. A. Cameron; R. Caputo; M. Caragiulo; Daniel Castro; E. Cavazzuti; C. Cecchi; A. Chekhtman; S. Ciprini; J. Cohen-Tanugi; F. Costanza; A. Cuoco; S. Cutini; F. D'Ammando; F. de Palma; R. Desiante; S. W. Digel
We present a measurement of the cosmic-ray electron+positron spectrum between 7 GeV and 2 TeV performed with almost seven years of data collected with the Fermi Large Area Telescope. We find that the spectrum is well fit by a broken power law with a break energy at about 50 GeV. Above 50 GeV, the spectrum is well described by a single power law with a spectral index of 3.07 ± 0.02 (stat+syst) ± 0.04 (energy measurement). An exponential cutoff lower than 1.8 TeV is excluded at 95% CL. PACS numbers: 98.70.Sa, 96.50.sb, 95.85.Ry, 95.55.Vj