I. S. Timchenko, O. S. Deiev, S. M. Olejnik, S. M. Potin, V. A. Kushnir, V. V. Mytrochenko, S. A. Perezhogin, A. Herzáň
{"title":"在轫致拉伸端点能量为35-94 MeV时\\({^\\textrm{nat}\\textrm{Ni}}(\\gamma ,\\textrm{p} x\\textrm{n})^{58}\\textrm{Co}\\)反应的截面","authors":"I. S. Timchenko, O. S. Deiev, S. M. Olejnik, S. M. Potin, V. A. Kushnir, V. V. Mytrochenko, S. A. Perezhogin, A. Herzáň","doi":"10.1140/epja/s10050-025-01666-7","DOIUrl":null,"url":null,"abstract":"<div><p>The photoproduction of the <span>\\(^{58}\\textrm{Co}\\)</span> nuclei on <span>\\({^\\textrm{nat}\\textrm{Ni}}\\)</span> was studied using the induced <span>\\(\\gamma \\)</span>-activity method and offline <span>\\(\\gamma \\)</span>-ray spectrometric technique. The experiment was performed at the electron linear accelerator LUE-40 of NSC KIPT, Ukraine. The total flux-averaged cross-section <span>\\(\\langle {\\sigma (E_{\\gamma \\textrm{max}})}\\rangle \\)</span> for the <span>\\({^\\textrm{nat}\\textrm{Ni}}(\\gamma ,\\textrm{p} x\\mathrm n)^{58}\\textrm{Co}\\)</span> reaction has been measured in the range of bremsstrahlung end-point energies <span>\\(E_{\\gamma \\textrm{max}}\\)</span> = 35–94 MeV. The obtained <span>\\(\\langle {\\sigma (E_{\\gamma \\textrm{max}})}\\rangle \\)</span> were compared with theoretical estimates, and with experimental data found in the literature. The theoretical values of <span>\\(\\langle {\\sigma (E_{\\gamma \\textrm{max}})}\\rangle _\\textrm{th}\\)</span> were calculated using the partial cross-sections <span>\\(\\sigma (E)\\)</span> from the TALYS1.96 code for different level density models and gamma strength functions.</p></div>","PeriodicalId":786,"journal":{"name":"The European Physical Journal A","volume":"61 9","pages":""},"PeriodicalIF":2.8000,"publicationDate":"2025-09-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epja/s10050-025-01666-7.pdf","citationCount":"0","resultStr":"{\"title\":\"Cross-section of the \\\\({^\\\\textrm{nat}\\\\textrm{Ni}}(\\\\gamma ,\\\\textrm{p} x\\\\textrm{n})^{58}\\\\textrm{Co}\\\\) reaction at the bremsstrahlung end-point energy of 35–94 MeV\",\"authors\":\"I. S. Timchenko, O. S. Deiev, S. M. Olejnik, S. M. Potin, V. A. Kushnir, V. V. Mytrochenko, S. A. Perezhogin, A. Herzáň\",\"doi\":\"10.1140/epja/s10050-025-01666-7\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The photoproduction of the <span>\\\\(^{58}\\\\textrm{Co}\\\\)</span> nuclei on <span>\\\\({^\\\\textrm{nat}\\\\textrm{Ni}}\\\\)</span> was studied using the induced <span>\\\\(\\\\gamma \\\\)</span>-activity method and offline <span>\\\\(\\\\gamma \\\\)</span>-ray spectrometric technique. The experiment was performed at the electron linear accelerator LUE-40 of NSC KIPT, Ukraine. The total flux-averaged cross-section <span>\\\\(\\\\langle {\\\\sigma (E_{\\\\gamma \\\\textrm{max}})}\\\\rangle \\\\)</span> for the <span>\\\\({^\\\\textrm{nat}\\\\textrm{Ni}}(\\\\gamma ,\\\\textrm{p} x\\\\mathrm n)^{58}\\\\textrm{Co}\\\\)</span> reaction has been measured in the range of bremsstrahlung end-point energies <span>\\\\(E_{\\\\gamma \\\\textrm{max}}\\\\)</span> = 35–94 MeV. The obtained <span>\\\\(\\\\langle {\\\\sigma (E_{\\\\gamma \\\\textrm{max}})}\\\\rangle \\\\)</span> were compared with theoretical estimates, and with experimental data found in the literature. The theoretical values of <span>\\\\(\\\\langle {\\\\sigma (E_{\\\\gamma \\\\textrm{max}})}\\\\rangle _\\\\textrm{th}\\\\)</span> were calculated using the partial cross-sections <span>\\\\(\\\\sigma (E)\\\\)</span> from the TALYS1.96 code for different level density models and gamma strength functions.</p></div>\",\"PeriodicalId\":786,\"journal\":{\"name\":\"The European Physical Journal A\",\"volume\":\"61 9\",\"pages\":\"\"},\"PeriodicalIF\":2.8000,\"publicationDate\":\"2025-09-04\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1140/epja/s10050-025-01666-7.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The European Physical Journal A\",\"FirstCategoryId\":\"4\",\"ListUrlMain\":\"https://link.springer.com/article/10.1140/epja/s10050-025-01666-7\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European Physical Journal A","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epja/s10050-025-01666-7","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
Cross-section of the \({^\textrm{nat}\textrm{Ni}}(\gamma ,\textrm{p} x\textrm{n})^{58}\textrm{Co}\) reaction at the bremsstrahlung end-point energy of 35–94 MeV
The photoproduction of the \(^{58}\textrm{Co}\) nuclei on \({^\textrm{nat}\textrm{Ni}}\) was studied using the induced \(\gamma \)-activity method and offline \(\gamma \)-ray spectrometric technique. The experiment was performed at the electron linear accelerator LUE-40 of NSC KIPT, Ukraine. The total flux-averaged cross-section \(\langle {\sigma (E_{\gamma \textrm{max}})}\rangle \) for the \({^\textrm{nat}\textrm{Ni}}(\gamma ,\textrm{p} x\mathrm n)^{58}\textrm{Co}\) reaction has been measured in the range of bremsstrahlung end-point energies \(E_{\gamma \textrm{max}}\) = 35–94 MeV. The obtained \(\langle {\sigma (E_{\gamma \textrm{max}})}\rangle \) were compared with theoretical estimates, and with experimental data found in the literature. The theoretical values of \(\langle {\sigma (E_{\gamma \textrm{max}})}\rangle _\textrm{th}\) were calculated using the partial cross-sections \(\sigma (E)\) from the TALYS1.96 code for different level density models and gamma strength functions.
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