Heavy-ion energy resolution of SSB detectors
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Cited by (30)
Energy resolution measurement and application of the F series ORTEC SSB detector in TOF-ERDA spectrometry
2013, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :Measured noise level (using precision pulser), in the case of 7Li ions, was 18.6 keV (FWHM), which is in good agreement with a value given by producer. Thus, it can be concluded that F series ORTEC SSB detector is, concerning the energy resolution for the light ions, worse than GIC and A series SSB detector [11]. In case of 16O (Fig. 2), energy resolution for ORTEC F series detector is slightly better than one set of the GIC results published in Ref. [6] but is worse than another GIC data set [7].
Performance of the ETH gas ionization chamber at low energy
2012, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :As pointed out in [24], there must be non-ionizing energy loss processes not included in SRIM or systematic Z dependent electrical screening in the ion track reducing the net charge collection. In order to compare the performance of the GIC with solid state detectors, the resolution for boron and chlorine obtained with the GIC are shown in Fig. 11a and b together with the values obtained by Hinrichsen et al. [27] with a silicon surface barrier detector (SSD). A similar comparison was already made in [5] for the energy resolution of an annular gas ionization detector with 7Li, 16O and 35Cl ions at energies larger than 1 MeV.
The possibility of using a single surface barrier detector as a Δe-E telescope for identification of light charged particles (Z=1, 2) and fragments with Z<=4
2010, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentAnnular gas ionization detector for low energy heavy ion backscattering spectrometry
2009, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsDevelopment of a time-of-flight spectrometer at the Ruder Bošković Institute in Zagreb
2008, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :Time-of-flight (TOF) elastic recoil detection analysis (ERDA) is a simple method for the mass separation and depth profiling of the light elements. The energy resolution of the silicon surface barrier detectors (SSB) [1,2], used in classical ERDA setup, limits depth resolution for the heavier ions (Z > 3) (pulse height defects). In the TOF-ERDA setup, energy of the recoiled particles is calculated from the time-of-flight between the two time detectors.
Investigations of SiO<inf>x</inf>-polymer "interphases" by glancing angle RBS with Li<sup>+</sup> and Be<sup>+</sup> ions
2003, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
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On leave from John Abbott College, St. Anne De Bellevue, Québec, H9X 3L9 Canada.
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On leave from Vanier College, 821 Ste-Croix Blvd., St. Laurent, Québec, H4L 3X9 Canada.