The determination of beam penetration using the total cross-sections of protons, pions and alpha particles between 200 MeV and 2 GeV

1977 ◽  
Vol 3 (11) ◽  
pp. 1497-1501 ◽  
Author(s):  
I Brissaud
Author(s):  
S. Golladay

The theory of multiple scattering has been worked out by Groves and comparisons have been made between predicted and observed signals for thick specimens observed in a STEM under conditions where phase contrast effects are unimportant. Independent measurements of the collection efficiencies of the two STEM detectors, calculations of the ratio σe/σi = R, where σe, σi are the total cross sections for elastic and inelastic scattering respectively, and a model of the unknown mass distribution are needed for these comparisons. In this paper an extension of this work will be described which allows the determination of the required efficiencies, R, and the unknown mass distribution from the data without additional measurements or models. Essential to the analysis is the fact that in a STEM two or more signal measurements can be made simultaneously at each image point.


2018 ◽  
Vol 167 ◽  
pp. 05006 ◽  
Author(s):  
Francesco Ingenito ◽  
Pierluigi Andreoli ◽  
Dimitri Batani ◽  
Aldo Bonasera ◽  
Guillaume Boutoux ◽  
...  

There is a great interest in the study of p-11B aneutronic nuclear fusion reactions, both for energy production and for determination of fusion cross-sections at low energies. In this context we performed experiments at CELIA in which energetic protons, accelerated by the laser ECLIPSE, were directed toward a solid Boron target. Because of the small cross-sections at these energies the number of expected reactions is low. CR39 Solid-State Nuclear Track Detectors (SSNTD) were used to detect the alpha particles produced. Because of the low expected yield, it is difficult to discriminate the tracks due to true fusion products from those due to natural background in the CR39. To this purpose we developed a methodology of particle recognition according to their direction with respect to the detector normal, able to determine the position of their source. We applied this to the specific experiment geometry, so to select from all the tracks those due to particles coming from the region of interaction between accelerated protons and solid boron target. This technique can be of great help on the analysis of SSNTD in experiments with low yield reactions, but can be also generally applied to any experiment where particles reach the track detector with known directions, and for example to improve the detection limit of particle spectrometers using CR39.


Our knowledge of the scattering interactions in the pion-nucleon system has been developing rapidly during the past few years. For the π + p and π - p systems, total cross-section measurements have been extended upwards in energy to 20 GeV/c laboratory momentum. As Galbraith will report at this meeting, measurements of high precision have recently been carried out for π + p and π - p total cross-sections between 2·5 and 7GeV/c by Citron et al. (1964,1965) at Brookhaven. From these and earlier data, about ten excited nucleon states have become established, with mass values up to about 3200 MeV. These excited nucleon states are listed in table 1. In the resonance energy range, detailed angular distribution measurements have now been made up to the region of the fifth excited state ( N * 1/2 (2190)), and many of these new measurements will be reported at this meeting. The recent use of polarized proton targets has allowed a very direct means for the systematic and accurate study of the polarization properties of pion-nucleon scattering, and this technique has recently been exploited at the Nimrod accelerator of the Rutherford High Energy Laboratory at Chilton by the Murphy-Thresher group (Atkinson et al. 1966) for the determination of the spin and parity of the third and fourth resonance states, N * 1/2 (1688) and N * 1/2 (1920).


Physica ◽  
1969 ◽  
Vol 44 (3) ◽  
pp. 449-472 ◽  
Author(s):  
H.H. Brongersma ◽  
A.J.H. Boerboom ◽  
J. Kistemaker

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