Mechanism of interaction of fast protons with nucleons and nuclei
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Cited by (24)
Multifractality in relativistic charged particles produced at SPS energies
2016, Chaos, Solitons and FractalsCitation Excerpt :The measuring system associated with it has 1 μm resolution along X and Y axes and 0.5 μm resolution along the Z-axis. The tracks associated with the interactions are classified in accordance with their ionization, range and velocity [12,13]. The tracks having specific ionization g*(=g/go) < 1.4 and relative velocity β > 0.7 are taken as shower tracks, where go is the Fowler and Perkins parameter for plateau ionization of relativistic particles.
Multifractal study and multifractal specific heat of singly charged particles produced in <sup>32</sup>S-Em interactions at 200 AGeV
2015, Chaos, Solitons and FractalsCitation Excerpt :There is a limitation with nuclear emulsion that the exact identification of target is not possible since the medium of the emulsion is heterogeneous and composed of H, C, N, O, Ag and Br nuclei. The events produced due to the collisions with different targets in nuclear emulsion are usually classified into three main categories on the basis of the multiplicity of heavily ionising tracks in it [21,22]. In the present work we have categorised the events on the bases of Nh multiplicity as follows: the events with Nh in range 2 ≤ Nh ≤ 7 are classified as collision with group of light nuclei (CNO, 〈AT〉 = 14) and Nh ≥ 8 are classified as collision with group of heavy nuclei (AgBr, 〈AT〉 = 94).
Properties of projectile fragments from <sup>12</sup>C-emulsion interactions at4.5A GeV/c
1989, Nuclear Physics, Section AHigh-energy collisions with atomic nuclei: The experimental results
1987, Physics ReportsGeneral properties of hadron-nucleus reaction multiplicities
1979, Physics Letters B