A. Codino
University of Perugia
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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 | 1994
R. L. Golden; Giuseppe Basini; W. R. Webber; P. Picozza; A. Codino; R. E. Streitmatter; S. A. Stephens; M. Menichelli; P. Spillantini; A. Morselli; Eul Soo Seo; F. Massimo Brancaccio; C. Grimani; M. Ricci; P. Papini; M.T. Brunetti; M. P. De Pascale; B. Kimbell; F. Bongiorno; I. Salvatori; S.J. Stochaj; J. F. Ormes
A ballon-borne magnet spectrometer system was flown for 5.5 hr at an altitude of more than 117,00 feet from Prince Albert, Saskatchewan (Canada), on 1989 September 5, when the Newark neutron monitor rate was 2952. The instrument was a modified version of the one used to observe antiprotons in 1979. The most significant modification was the addition of an imaging calorimeter, 7.33 radiation lengths thick. Inclusion of the calorimeter has significantly improved the ability to distinguish electrons and positrons from the other constituents of the cosmic rays. The absolute electron flux has been determined in the energy interval 1.3-26 GeV. The electron spectrum at the top of the atmosphere was found to be J(sub e-) = 177E(exp -(3.15+/-0.13)) electrons/ sq m/(sr s GeV) in the energy range 4.0-26 GeV. Below 4 GeV, the spectrum showed flattening, which is consistent with the effect of solar modulation. The e(+)/(e(+)+e(-)) ratio was found to be (0.11 +/- 0.03) in the energy range 5.2-13 GeV.
Astronomy and Astrophysics | 2002
C. Grimani; S.A. Stephens; F. Cafagna; Giuseppe Basini; R. Bellotti; M.T. Brunetti; M. Circella; A. Codino; C. De Marzo; M. P. De Pascale; N. Finetti; R. L. Golden; M. Hof; W. Menn; J. W. Mitchell; A. Morselli; J. F. Ormes; P. Papini; Ch. Pfeifer; S. Piccardi; P. Picozza; M. Ricci; Michael Simon; P. Spillantini; S.J. Stochaj; R. E. Streitmatter
A measurement of the energy spectra of cosmic-ray positrons and electrons was made with a balloon-borne magnet- spectrometer, which was flown at a mean geomagnetic cut-o of 4.5 GV/c. The observed positron flux in the energy range 7-16 GeV is approximately an order of magnitude lower than that of electrons, as measured in other experiments at various energies. The power law spectral index of the observed dierential energy spectrum of electrons is 2:89 0:10 in the energy interval 7.5-47 GeV. For positrons the overall fit of the available data above 7 GeV has been considered. The spectral index is found to be 3:37 0:26 and the fraction of positrons, e + /(e + + e ), has a mean value of 0:064 0:003. The world data on e + /(e + + e ) from 0.1 to 30 GeV indicate that a plerion type electron spectrum is preferred over the other types. The trend of the presently existing high energy data also suggests a possible contribution of positrons produced at the pulsar polar cap. High resolution experiments capable of identifying positrons at least up to 100 GeV with high statistics are required to pinpoint the origin of both electrons and positrons in the cosmic radiation.
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.
The Astrophysical Journal | 1996
M. Hof; W. Menn; Ch. Pfeifer; Michael Simon; R. L. Golden; S.J. Stochaj; S. A. Stephens; G. Basini; M. Ricci; F. Massimo Brancaccio; P. Papini; S. Piccardi; P. Spillantini; M. P. De Pascale; A. Morselli; P. Picozza; M.T. Brunetti; A. Codino; C. Grimani; M. Menichelli; J. W. Mitchell; J.F. Ormes; R. E. Streitmatter
The antiproton-to-proton ratio,p ¯/p, in cosmic rays has been measured in the energy range 3.7‐19 GeV. This measurement was carried out using a balloon-borne superconducting magnetic spectrometer along with a gas Cerenkov counter, an imaging calorimeter, and a time-of-flight scintillator system. The measuredp ¯/p ratio was
Journal of Geophysical Research | 1993
M. P. De Pascale; A. Morselli; P. Picozza; R. L. Golden; C. Grimani; B. Kimbell; S. A. Stephens; S.J. Stochaj; W. R. Webber; G. Basini; F. Bongiorno; F.M. Brancaccio; M. Ricci; J.F. Ormes; Eul Soo Seo; R. E. Streitmatter; P. Papini; P. Spillantini; M.T. Brunetti; A. Codino; M. Menichelli; I. Salvatori
We have determined the momentum spectrum and charge ratio of muons in the region from 250 MeV/c to 100 GeV/c using a superconducting magnetic spectrometer. The absolute differential spectrum of muons obtained in this experiment at 600 m above sea level is in good agreement with the previous measurements at sea level. The differential spectrum can be represented by a power law with a varying index, which is consistent with zero below 450 MeV/c and steepens to a value of −2.7 ± 0.1 between 20 and 100 GeV/c. The integral flux of muons measured in this experiment span a very large range of momentum and is in excellent agreement with the earlier results. The positive to negative muon ratio appears to be constant in the entire momentum range covered in this experiment within the errors and the mean value is 1.220 ± 0.044. The absolute momentum spectrum and the charge ratio measured in this experiment are also consistent with the theoretical expectations. This is the only experiment which covers a wide range of nearly 3 decades in momentum from a very low momentum.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1991
R. L. Golden; C. Grimani; R. Hull; B. Kimbell; R. Park; S. A. Stephens; Steven Jon Stochaj; W. R. Webber; Giuseppe Basini; E. Bonaviri; F. Massimo Brancaccio; M. Ricci; J. F. Ormes; E. S. Seo; R. E. Streitmatter; F. Celletti; P. Spillantini; A. Codino; M. Menichelli; I. Salvatori; F. Bongiorno; V. Bidoli; A. Buccheri; M. P. De Pascale; A. Morselli; P. Picozza
Abstract This paper summarizes the performance characteristics of the balloon-borne magnet spectrometer operated by New Mexico State Universitys Particle Astrophysics Laboratory. Particular emphasis has been placed on the rigidity resolution, including both random and systematic errors of the magnetic spectrometer system. Measurement of the performance characteristics has been greatly enhanced through the use of an imaging calorimeter as an independent aid in the identification of cosmic rays.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996
G. Barbiellini; G. Basini; R. Bellotti; M. Bocciolini; M. Boezio; F. Massimo Brancaccio; Ulisse Bravar; F. Cafagna; M. Candusso; Per Carlson; M. Casolino; M. Castellano; G. de Cataldo; M. Circella; A. Codino; N. Finetti; Tom Francke; N. Giglietto; R. L. Golden; C. Grimani; M. Hof; B. Marangelli; C. De Marzo; J. W. Mitchell; A. Morselli; M. P. De Pascale; P. Papini; A. Perego; S. Piccardi; Piergiorgio Picozza
A RICH detector capable of detecting unit charged particles, e.g. antiprotons and positrons, has been used successfully for the first time in a balloon-borne magnet spectrometer. The thin and compact CAPRICE RICH detector uses a NaF solid radiator, TMAE vapour as photo converter and cathode pad readout in the photosensitive MWPC operated at low gain. 15 photoelectrons are detected per ring for β = 1, perpendicular incidence particles giving a resolution on the Cherenkov angle of 8 mrad, increasing to 14 mrad at 20°C incidence angle. Besides particle identification on an event-by-event basis it efficiently rejects multiparticle events and albedo particles.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1995
F. Aversa; G. Barbiellini; M. Boezio; U. Bravar; A. Colavita; F. Fratnik; P. Schiavon; A. Vacchi; N. Zampa; V. Bidoli; M. Candusso; M. Casolino; M. P. De Pascale; A. Morselli; P. Picozza; Roberta Sparvoli; M. Bocciolini; F. Celletti; N. Finetti; M. Grandi; P. Papini; A. Perego; S. Piccardi; P. Spillantini; G. Basini; F.M. Brancaccio; G. Mazzenga; M. Ricci; R. Bellotti; F. Cafagna
Abstract The WiZard Collaboration is engaged in a program to study the antimatter components of the cosmic rays. A silicon-tungsten (WiW) imaging calorimeter has been developed as part of this program. We present its performance and preliminary results, obtained during a balloon flight on September 8, 1993. The flight was dedicated to the measurement of the positron spectrum in the energy range 4–50 GeV and took place from Ft. Sumner, New Mexico.
Journal of Physics G | 1997
A. Codino; M.T. Brunetti; C. Federico; C. Grimani; M. Lanfranchi; M. Menichelli; M. Miozza; R. L. Golden; S.J. Stochaj; S. A. Stephens; J. W. Mitchell; J.F. Ormes; R. E. Streitmatter; M. Hof; Ch. Pfeifer; W. Menn; Michael Simon; G. Basini; M. Ricci; F.M. Brancaccio; P. Papini; S. Piccardi; P. Spillantini; M. P. De Pascale; A. Morselli; P. Picozza
Momentum spectra of pions, muons, electrons and secondary positrons have been measured at an atmospheric depth of 5: 8gc m 2 with the same instrument. Data was collected by the Matter Antimatter Space Spectrometer of the New Mexico State University in a balloon flight in September 1991 at the rigidity cut-off of 4 : 5G V c 1 in Fort Sumner, New Mexico. The first measurement of the positive muon spectrum in the range 0:15 GeV c 1 to 2 GeVc 1 is reported in this paper. The spectral index above 3 GeV c 1 of the negative muon momentum spectrum of this measurement is 2:39 0:05 in agreement with analytical cascade calculations which assume a primary proton kinetic energy spectrum with a slope of 2:740:02 in the corresponding kinetic energy range. In the momentum interval 300-700 MeV c 1 , both negative and positive muon fluxes turn out to be larger than calculated fluxes by a factor of about 1.4. The measurement of the secondary electron and positron energy spectra allows a reliable subtraction of the atmospheric background from the primary electron and positron fluxes which are affected by large uncertainties in most of the experiments. The energy spectra of the secondary particles reported here have the same systematic errors implying a higher relative accuracy with respect to those measurements made in different flights.