Fragmentation cross sections of Fe26+, Si14+ and C6+ ions of 0.3–10 on polyethylene, CR39 and aluminum targets

Cecchini, S.; Chiarusi, T.; Giacomelli, G.; Giorgini, M.; Kumar, Ashavani; Mandrioli, G.; Manzoor, Shahid; Margiotta, A.; Medinaceli, E.; Patrizii, L.; Popa, V.; Qureshi, I. H.; Sirri, G.; Spurio, M.; Togo, V.

doi:10.1016/j.nuclphysa.2008.03.017

Cited by 56 publications

(40 citation statements)

References 37 publications

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“…The measured cross-section was reasonably comparable with the results in Ref. [25]. The present result is more accurate in comparison to other measurements [25]; this is because the counting of tracks is, by the new system of analysis, more accurate.…”

Section: Total Charge Changing Cross-sectionsupporting

confidence: 90%

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Measurement of total and partial charge changing and charge pick-up cross-sections for 300AMeV Fe26+ beam in Al with a new system of analysis

Gupta

Kumar

Giacomelli

et al. 2012

Nuclear Instruments and Methods in Physics Research Section A:

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Section: Total Charge Changing Cross-sectionsupporting

confidence: 90%

“…[25] if the thickness of the target is small compared to the mean free path of the fragments and there is no fragmentation before the target. If there are some fragmentations before the target, the partial charge changing cross-section is calculated via the relation [25,33] …”

Section: Partial Charge Changing Cross-sectionmentioning

confidence: 99%

Measurement of total and partial charge changing and charge pick-up cross-sections for 300AMeV Fe26+ beam in Al with a new system of analysis

Gupta

Kumar

Giacomelli

et al. 2012

Nuclear Instruments and Methods in Physics Research Section A:

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“…On the other hand, EPAX2 and EPAX3 show rather good overall agreements, though EPAX2 overestimates the production of 46 Pd isotopes, EPAX3 underestimates neutron-rich isotopes of 49 In, and both underestimate 51 Sb isotopes. Finally, G4-BIN, which shows the best performance for other cases, is also found to overestimate the productions of 46 Pd, 47 Ag, and 48 Cd isotopes by K 10 2 . Such overestimation of the production cross sections needs to be ultimately resolved by improving the hadronic models, but it is beyond the scope of this work.…”

Section: Benchmark Test Of Simulation Methods For the Production Crosmentioning

confidence: 87%

“…5 we have plotted experimental production cross sections of 46 Pd $ 50 Sn isotopes for 132 Sn [10], 136 Xe [38][39][40] and 238 U [41][42][43] beams. The experimental cross sections are nearly independent of the incident beam energies [18,26,35,[44][45][46][47]38]. It is clearly seen that the cross sections are mainly characterized by the species of the incident beams, and the energy-dependence is rather weak.…”

Section: Benchmark Test Of Simulation Methods For the Production Crosmentioning

confidence: 99%

Yield estimation of neutron-rich rare isotopes induced by 200 MeV/u 132 Sn beams by using GEANT4

Shin¹,

Min²,

Ham³

et al. 2015

Nuclear Instruments and Methods in Physics Research Section B:

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a b s t r a c tA so-called ''two-step reaction scheme'', in which neutron-rich rare isotopes obtained from ISOL are post-accelerated and bombarded on a second target, is employed to estimate the production yields of exotic rare isotopes. The production yields of neutron-rich rare isotope fragments induced by 200 MeV/u 132 Sn beams bombarded on a 9 Be target are estimated with Monte Carlo code, GEANT4. To substantiate the use of GEANT4 for this study, benchmark calculations are done for 80 MeV/u 59 Co, 95 MeV/u 72 Zn, 500 MeV/u 92 Mo, and 950 MeV/u 132 Sn beams on the 9 Be target. It is found that 132 Sn beams can produce neutron-rich rare isotopes with 45 6 Z 6 50 more effectively than 238 U beams at the same energy per nucleon.

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“…The REL may be determined from the geometry of the etched cones. For CR39 this technique is particularly successful, yielding measurements of the electric charge of heavy relativistic nuclei (Z > 5) to a precision of 0.05e if several layers of plastic sheets are used [39,40].…”

Section: Energy Loss Mechanisms In Nuclear Track Detectorsmentioning

confidence: 99%

Status of Searches for Magnetic Monopoles

Patrizii

Spurio

2015

Annu. Rev. Nucl. Part. Sci.

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The searches for magnetic monopoles (Ms) is a fascinating interdisciplinary field with implications in fundamental theories, in particle physics, astrophysics, and cosmology. The quantum theory of Ms and its consistency with electrodynamics was derived by P.A.M. Dirac. This marked the start of the searches for classical monopoles at every new accelerator, up to the LHC. Magnetic monopoles are required by Grand Unification Theories, but unlike classical monopoles they would be incredibly massive, out of the reach of any conceivable accelerator. Large efforts have been made to search for them in the cosmic radiation as relic particles from the early Universe in the widest range of mass and velocity experimentally accessible.In this paper the status of the searches for classical Ms at accelerators, for GUT, superheavy Ms in the penetrating cosmic radiation and for Intermediate Mass Ms at high altitudes is discussed, with emphasis on the most recent results and future perspectives.

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Fragmentation cross sections of Fe26+, Si14+ and C6+ ions of 0.3–10 on polyethylene, CR39 and aluminum targets

Cited by 56 publications

References 37 publications

Measurement of total and partial charge changing and charge pick-up cross-sections for 300AMeV Fe26+ beam in Al with a new system of analysis

Measurement of total and partial charge changing and charge pick-up cross-sections for 300AMeV Fe26+ beam in Al with a new system of analysis

Yield estimation of neutron-rich rare isotopes induced by 200 MeV/u 132 Sn beams by using GEANT4

Status of Searches for Magnetic Monopoles

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