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| 005 | 20231027114405.0 | ||
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| 037 | _ | _ | |a FZJ-2023-02113 |
| 082 | _ | _ | |a 610 |
| 100 | 1 | _ | |a Uddin, M. Shuza |0 P:(DE-HGF)0 |b 0 |e Corresponding author |
| 245 | _ | _ | |a Cross sections and calculated yields of some radionuclides of yttrium, strontium and rubidium formed in proton-induced reactions on enriched strontium-86: possibility of production of 85gSr, 83Rb and 82mRb in no-carrier-added form |
| 260 | _ | _ | |a Berlin |c 2023 |b De Gruyter |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 520 | _ | _ | |a Cross sections of the 86Sr(p,3n)84mY, 86Sr(p,αn)82mRb, and 86Sr(p,x)85gSr reactions were measured from their respective thresholds up to 16.2 MeV and from 23.0 to 44.1 MeV at FZJ, and from 14.3 to 24.5 MeV at LBNL, using 96.4% enriched 86SrCO3 as target material. Thin targets prepared by sedimentation were irradiated with protons in a stacked-form, and the induced radioactivity was measured by high-resolution γ-ray spectrometry. Nuclear model calculations based on the code TALYS reproduced our experimental cross section data well. From the excitation functions, the integral yields of the above three radionuclides were calculated. The yield of 85gSr via the natSr(n,γ)process was also measured using the TRIGA Mark-II reactor at AERE, Savar. A comparison of the reactor and cyclotron production of carrier-added 85gSr is given. The production possibilities of the three investigated radionuclides in no-carrier-added forms at a 30 MeV cyclotron via new routes are discussed. |
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| 700 | 1 | _ | |a Basunia, M. Shamsuzzoha |0 P:(DE-HGF)0 |b 1 |
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| 700 | 1 | _ | |a Khan, Rahat |0 P:(DE-HGF)0 |b 4 |
| 700 | 1 | _ | |a Uddin, M. Mezbah |0 P:(DE-HGF)0 |b 5 |
| 700 | 1 | _ | |a Bernstein, Lee A. |0 P:(DE-HGF)0 |b 6 |
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| 773 | _ | _ | |a 10.1515/ract-2022-0086 |g Vol. 111, no. 2, p. 81 - 90 |0 PERI:(DE-600)2039575-9 |n 2 |p 81 - 90 |t Radiochimica acta |v 111 |y 2023 |x 0033-8230 |
| 856 | 4 | _ | |y OpenAccess |u https://juser.fz-juelich.de/record/1007614/files/Manuscript%20Uddin%20RCA%202023.pdf |
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