2019
DOI: 10.1016/j.nima.2019.05.012
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Fabrication of thin  130Te target foils for sub-barrier fusion studies

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Cited by 12 publications
(2 citation statements)
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“…Throughout the measurements, a vacuum of approximately 10 −6 torr was maintained in the scattering chamber. The measured RBS spectrum was analyzed and simulated using the RUMP code [23] and the thickness of the film was determined by the energy loss suffered by He + ions in Si film [24,25]. The film thickness was calculated to be ∼ 409 μg/cm 2 and ∼ 411 μg/cm 2 at two different locations, resulting in an average thickness of 410 ± 10 μg/cm 2 .…”
Section: Rutherford Backscattering Spectrometry (Rbs) Measurementmentioning
confidence: 99%
“…Throughout the measurements, a vacuum of approximately 10 −6 torr was maintained in the scattering chamber. The measured RBS spectrum was analyzed and simulated using the RUMP code [23] and the thickness of the film was determined by the energy loss suffered by He + ions in Si film [24,25]. The film thickness was calculated to be ∼ 409 μg/cm 2 and ∼ 411 μg/cm 2 at two different locations, resulting in an average thickness of 410 ± 10 μg/cm 2 .…”
Section: Rutherford Backscattering Spectrometry (Rbs) Measurementmentioning
confidence: 99%
“…It is well known that thin and enriched isotopic targets are essential for heavy-ion induced nuclear reaction experiments such as transfer reaction, nuclear fusion -fission time scale measurement, evaporation residues measurement, formation of super heavy nuclei and dynamics of fusion reaction around the Coulomb barrier. To study these reactions, the selection of target and projectile combination is very essential and such a combination can undoubtedly shed light on nuclear structure and nuclear dynamics of nuclei which have not been fully understood [1][2][3][4][5][6][7]. However, the fabrication and characterization of such a target is a herculean task for the researchers in view of the involvement of various instruments.…”
Section: Introductionmentioning
confidence: 99%