P. Bobik
Istituto Nazionale di Fisica Nucleare
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Featured researches published by P. Bobik.
The Astrophysical Journal | 2012
P. Bobik; G. Boella; M. J. Boschini; C. Consolandi; S. Della Torre; M. Gervasi; D. Grandi; K. Kudela; S. Pensotti; P.G. Rancoita; M. Tacconi
A propagation model of galactic cosmic protons through the heliosphere was implemented using a two-dimensional Monte Carlo approach to determine the differential intensities of protons during solar cycle 23. The model includes the effects due to the variation of solar activity during the propagation of cosmic rays from the boundary of the heliopause down to Earths position. Drift effects are also accounted for. The simulated spectra were found to be in agreement with those obtained from experimental observations carried out by the BESS, AMS, and PAMELA collaborations. In addition, the modulated spectrum determined with the present code for the year 1995 exhibits the latitudinal gradient and equatorial southward offset minimum found by the Ulysses fast scan in 1995.
Astrophysics and Space Sciences Transactions | 2011
P. Bobik; M. J. Boschini; C. Consolandi; S. Della Torre; M. Gervasi; D. Grandi; K. Kudela; S. Pensotti; P.G. Rancoita
We implemented a quasi time-dependent 2D stochastic model of solar modulation describing the transport of cosmic rays (CR) in the heliosphere. Our code can modulate the Local Interstellar Spectrum (LIS) of a generic charged particle (light cosmic ions and electrons), calculating the spectrum at 1AU. Several measurements of CR antiparticles have been performed. Here we focused our attention on the CR antiproton component and the antiproton over proton ratio. We show that our model, using the same heliospheric parameters for both particles, fit the observed anti-p/p ratio. We show a good agreement with BESS-97 and PAMELA data and make a prediction for the AMS-02 experiment.
arXiv: Earth and Planetary Astrophysics | 2011
P. Bobik; M. J. Boschini; C. Consolandi; S. Della Torre; M. Gervasi; D. Grandi; K. Kudela; S. Pensotti; P.G. Rancoita
Galactic Cosmic Rays (GCRs) are mainly protons confined in the galactic magnetic field to form an isotropic flux inside the galaxy. Before reaching the Earth orbit they enter the Heliosphere and undergo diffusion, convection, magnetic drift and adiabatic energy loss. The result is a reduction of particles flux at low energy (below 10 GeV), called solar modulation. We realized a quasi time-dependent 2D Stochastic Simulation of Solar Modulation that is able to reproduce CR spectra once known the Local Interstellar Spectrum (LIS). We were able to estimate the different behaviors associated to the polarity dependence of the Heliospheric modulation for particles as well as for antiparticles. We show a good agreement with the antiproton/proton ratio measured by AMS-01, Pamela, BESS, Heat and Caprice and we performed a prediction for the AMS-02 Experiment.
ASTROPARTICLE, PARTICLE, SPACE PHYSICS, RADIATION INTERACTION, DETECTORS AND MEDICAL PHYSICS APPLICATIONS | 2011
P. Bobik; G. Boella; M. J. Boschini; C. Consolandi; S. Della Torre; M. Gervasi; D. Grandi; M.L. Elmo; K. Kudela; E. Memola; S. Pensotti; P.G. Rancoita; D. Rozza; M. Tacconi
Galactic Cosmic Rays (GCR) entering the Heliosphere are affected by the solar modulation, which is a combination of diffusion, convection, magnetic drift, and adiabatic energy losses usually seen as a decrease of the flux at low energies (less than 10 GeV). We improved a quasi time-dependent 2D Stochastic Simulation code describing such effects. We focused our attention on the electron modulation, adding energy losses mechanisms in the Heliosphere that can be neglected for protons and ions: inverse Compton, ionization, synchrotron, and bremsstrahlung. These effects have been evaluated in the region affected by the solar magnetic field, up to 100 AU, where the environment conditions are not constant, especially the magnetic field intensity, and the photon density. In our calculation the inverse compton energy losses are dominant, but they contribute only a few percent in comparison with the adiabatic losses. We also compared the Local Interstellar Spectrum (LIS) of primary electrons with experimental data collected in the past years at energies 20 GeV. We found that, inside one standard deviation, LIS fits the data and can be used in a Monte carlo code reproducing CR propagation in the Heliosphere.
Czechoslovak Journal of Physics | 1999
Ilya G. Usoskin; Olga G. Gladysheva; P. Bobik; K. Kudela; H. Kananen
We suggest a new approach to the normalisation of neutron monitor response to galactic cosmic rays. The reference normalisation count rate is the neutron monitor response to the model unmodulated flux of galactic cosmic rays. A comparison of the actually recorded neutron monitor count rate with the calculated normalisation count rate can provide one with an observationally obtained true-of-date integral measure of the current level of solar modulation of galactic cosmic rays.
Advances in Astronomy | 2013
P. Bobik; G. Boella; M. J. Boschini; C. Consolandi; S. Della Torre; M. Gervasi; D. Grandi; K. Kudela; S. Pensotti; P.G. Rancoita; D. Rozza; M. Tacconi
The cosmic rays differential intensity inside the heliosphere, for energy below 30 GeV/nuc, depends on solar activity and interplanetary magnetic field polarity. This variation, termed solar modulation, is described using a 2D (radius and colatitude) Monte Carlo approach for solving the Parker transport equation that includes diffusion, convection, magnetic drift, and adiabatic energy loss. Since the whole transport is strongly related to the interplanetary magnetic field (IMF) structure, a better understanding of his description is needed in order to reproduce the cosmic rays intensity at the Earth, as well as outside the ecliptic plane. In this work an interplanetary magnetic field model including the standard description on ecliptic region and a polar correction is presented. This treatment of the IMF, implemented in the HelMod Monte Carlo code (version 2.0), was used to determine the effects on the differential intensity of Proton at 1 AU and allowed one to investigate how latitudinal gradients of proton intensities, observed in the inner heliosphere with the Ulysses spacecraft during 1995, can be affected by the modification of the IMF in the polar regions.
arXiv: Solar and Stellar Astrophysics | 2011
P. Bobik; M. J. Boschini; C. Consolandi; S. Della Torre; M. Gervasi; D. Grandi; K. Kudela; S. Pensotti; P.G. Rancoita
The solar modulation, a combination of diffusion, convection, magnetic drift and energy loss inside the heliosphere is usually seen as a depletion in the Galactic cosmic ray (CR) flux at low energy (less than 10 GeV/nuc). Antiparticles such as antiprotons or positrons undergo the same processes of respective particles but with a different magnitude depending on the Solar magnetic field polarity. For electrons and positrons, due to the small mass, energy loss mechanisms as inverse compton, synchrotron, bremsstrahlung and ionization have to be taken into account, together with the typical adiabatic losses considered in the heliosphere. We developed a Monte Carlo stochastic simulation with the aim to compare the solar modulation of particles and antiparticles in the same observation period. We are able to estimate the different behaviours associated to the charge sign dependent processes of the heliospheric modulation. We compared the simulated positron fraction with measurements performed by AMS-01 and PAMELA. We also present the prediction for the AMS-02 experiment.
arXiv: Solar and Stellar Astrophysics | 2011
P. Bobik; C. Consolandi; S. Della Torre; M. Gervasi; K. Kudela; F Noventa; S. Pensotti; D. Rozza
The differential intensities of Cosmic Rays at Earth were calculated using a 2D stochastic Montecarlo diffusion code and compared with observation data. We evaluated the effect of stretched and compressed heliospheres on the Cosmic Ray intensities at the Earth. This was studied introducing a dependence of the diffusion parameter on the heliospherical size. Then, we found that the optimum value of the heliospherical radius better accounting for experimental data. We also found that the obtained values depends on solar activity. Our results are compatible with Voyager observations and with models of heliospherical size modulation.
Advances in Space Research | 2001
Ilya G. Usoskin; P. Bobik; Olga G. Gladysheva; H. Kananen; Gennady A. Kovaltsov; K. Kudela
Abstract We studied the sensitivity of a neutron monitor to Galactic cosmic rays depending on energy of cosmic ray particles in the interstellar medium. This is important for studying of the interstellar spectrum of cosmic rays and details of solar modulation by means of the world neutron monitor network. We calculated the expected response of a standard sea-level neutron monitor vs. energy of cosmic ray particles. First, we studied modulation of a monoenergetic flux of cosmic rays. Then the specific atmospheric yield function of a neutron monitor was applied to the calculated flux of cosmic rays at the Earths orbit. The obtained response function, being convoluted with the model interstellar spectrum of cosmic rays, gives a maximum of neutron monitor sensitivity at around several GV of rigidity of cosmic ray particles. We performed calculations for weak (φ = 350 MV) and medium (φ = 750 MV) modulation strength. A normalisation of neutron monitor count rate is suggested which can give an experimental measure of the overall solar modulation of cosmic rays.
Proceedings of The 34th International Cosmic Ray Conference — PoS(ICRC2015) | 2016
Simon Mackovjak; A. Neronov; P. Bobik; Marián Putiš; Luis del Peral; Maria Rodriguez Frias; Kenji Shinozaki; Camille Catalano; Jorge Fernandez Soriano; G. Sáez-Cano; C. Moretto; Simon Bacholle
Š. Mackovjak∗1, A. Neronov1, P. Bobík2, M. Putiš2, L. Del Peral1, 3, M. D. Rodríguez Frías1, 3, 8, K. Shinozaki4, C. Catalano5, J. F. Soriano3, G. Sáez-Cano3, C. Moretto6, S. Bacholle7 for the JEM-EUSO Collaboration 1 ISDC Data Centre for Astrophysics, University of Geneva, Switzerland 2 Department of Space Physics, IEP, Slovak Academy of Sciences, Košice, Slovakia 3 SPace & AStroparticle (SPAS) Group, UAH, Madrid, Spain 4 Institute for Astronomy and Astrophysics, University of Tübingen, Germany 5 Institut de Recherche en Astrophysique et Planétologie, CNRS-UPS Toulouse, France 6 Laboratoire de l’Accélérateur Linéaire, Université Paris Sud, France 7 Laboratoire AstroParticule et Cosmologie, Université Paris Diderot, France 8 IFIC, CSIC, Dpto. Física Atómica, Molecular y Nuclear, Universitat de València, Spain