Measurement of the absolute cross section of the 3He(4He, γ)7Be reaction at Ec.m. = 525 keV
References (25)
- et al.
Nucl. Phys.
(1969) - et al.
Phys. Rev.
(1983) - et al.
Nucl. Instr. Meth.
(1977) - et al.
Nucl. Instr. Meth.
(1980) - et al.
Nucl. Instr. Meth.
(1980) - et al.
Nucl. Instr. Meth.
(1978) - et al.
Nucl. Instr. Meth.
(1984) - et al.
Nucl. Instr. Meth.
(1980) - et al.
Hydrogen: stopping powers and ranges in all elements
(1977) - et al.
Nucl. Instr. Meth.
(1976)
Rev. Mod. Phys.
Cited by (67)
Frontiers in nuclear astrophysics
2016, Progress in Particle and Nuclear PhysicsActivation measurement of the he3(α,γ)be7 reaction cross section at high energies
2013, Nuclear Physics AEnergy deconvolution of cross-section measurements with an application to the <sup>12</sup>C (α, γ) <sup>16</sup>O reaction
2013, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentThin-window gas cell target for activation cross-section measurements relevant for nuclear astrophysics
2012, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :The achievable target thickness (the number of target atoms per unit area) is limited by the maximum number of implanted atoms the backing can hold (e.g., due to the blistering effect [22]). The determination of the target thickness is rather difficult and care must be taken to preserve the target stability under beam bombardment [3]. This problem is especially severe for noble gas atoms which can diffuse out easily from the backing [23].
Ion-implanted <sup>32</sup>S targets for astrophysics studies
2011, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :One could therefore consider self-supporting targets comprised of binary compounds such as CdS, AgS, HgS or SbS, although natural isotopic sulfur abundances would be the norm. Noble gases cannot typically be used in a solid target geometry at room temperature unless they are embedded in a suitable host; for example, 3He has been successfully implanted at 35 keV to a large fluence (3 μg/cm2) into bulk Nb (foil thickness ∼125 μm) to investigate the 3He(4He,γ)7Be reaction [9]. Obviously for absolute cross section measurements, the implanted ion (i.e. target) areal density should be as large as possible in order to simulate the experimental situations normally encountered with elemental (or binary compound) films.
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On leave from GSI, D-61 Darmstadt, Federal Republic of Germany.