2018
DOI: 10.1016/j.nimb.2018.01.002
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An ion beam facility based on a 3 MV tandetron accelerator in Sichuan University, China

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Cited by 56 publications
(13 citation statements)
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“…Using an ethanol‐based suspension, the BS specimens were polished mechanically to yield a mirror‐like surface. The room‐temperature irradiation experiment with 6.0 MeV of Si 2+ generated by the 3‐MV tandetron accelerator was conducted at Sichuan University 64 . The beam flux was approximately 4.2 × 10 13 ions/(cm 2 s), and the samples were irradiated upon accumulating ion fluences of 8.0 × 10 14 and 1.1 × 10 15 ions/cm 2 , which roughly yielded average displacement per atom (dpa) values of 0.09 and 0.13, respectively.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…Using an ethanol‐based suspension, the BS specimens were polished mechanically to yield a mirror‐like surface. The room‐temperature irradiation experiment with 6.0 MeV of Si 2+ generated by the 3‐MV tandetron accelerator was conducted at Sichuan University 64 . The beam flux was approximately 4.2 × 10 13 ions/(cm 2 s), and the samples were irradiated upon accumulating ion fluences of 8.0 × 10 14 and 1.1 × 10 15 ions/cm 2 , which roughly yielded average displacement per atom (dpa) values of 0.09 and 0.13, respectively.…”
Section: Methodsmentioning
confidence: 99%
“…The room-temperature irradiation experiment with 6.0 MeV of Si 2+ generated by the 3-MV tandetron accelerator was conducted at Sichuan University. 64 The beam flux was approximately 4.2 × 10 13 ions/(cm 2 s), and the samples were irradiated upon accumulating ion fluences of 8.0 × 10 14 and 1.1 × 10 15 ions/cm 2 , which roughly yielded average displacement per atom (dpa) values of 0.09 and 0.13, respectively. The irradiation-induced temperature change on the glass surface was monitored by an FLIR thermal imaging camera, suggesting that the glass surface temperature variation remained within 200 • C. The stopping power (-dE/dx) and energy deposition of incident Si 2+ ions were estimated for each glass by using the SRIM2010 code, 65 and the damage profile was simulated using its option of "quick Kinchin and Pease calculation."…”
Section: Irradiation Experimentsmentioning
confidence: 99%
“…Figure 2 shows the control system architecture in the block diagram [14]. Interestingly, our accelerator system was the first one with ARGUS software deployment, and since then, ARGUS is now an integral part of Tandetron installations all over Europe and the world [15][16][17] which predicts potential interest of the ion beam facilities in MATLAB RBS channeling application. The Ion accelerator is operated by real-time TwinCAT SoftPLC interlinked with HVEE control software, ARGUS.…”
Section: Accelerator and Ion Beam Analysismentioning
confidence: 99%
“…Detection efficiency of the array was calibrated at the nuclear physics experiment (NPE) terminal of the 3-MV tandetron accelerator [15] at Sichuan university. Quasi Mono-energetic neutrons were produced using the 51 V(p, n) 51 Cr reaction (Q = -1534.8 keV) at incident energies between 1.7 and 2.6 MeV with a step of 0.15 MeV.…”
Section: V(p N) 51 Cr Experiments and Simulationmentioning
confidence: 99%