I. S. Timchenko, O. S. Deiev, S. M. Olejnik, S. M. Potin, V. A. Kushnir, V. V. Mytrochenko, S. A. Perezhogin
{"title":"光子-中子反应 $^{\\rm nat}$Mo($γ,x$n)$^{\\rm 93m}$Mo 在轫致辐射能量高达 95 MeV 时的交叉截面","authors":"I. S. Timchenko, O. S. Deiev, S. M. Olejnik, S. M. Potin, V. A. Kushnir, V. V. Mytrochenko, S. A. Perezhogin","doi":"arxiv-2407.09085","DOIUrl":null,"url":null,"abstract":"The photoproduction of the $^{\\rm 93m}$Mo nucleus on natural molybdenum was\nstudied using the electron beam of the LUE-40 linac RDC \"Accelerator\" NSC KIPT.\nMeasurements were performed using the activation method and off-line\n$\\gamma$-ray spectrometric technique. For the $^{\\rm nat}$Mo($\\gamma,x$n)$^{\\rm\n93m}$Mo reaction the experimental flux-averaged cross-section <$\\sigma(E_{\\rm\n\\gamma max})$>$_\\rm m$ at the bremsstrahlung end-point energy range of 38--93\nMeV was first time determined. The theoretical values of the yields $Y_{\\rm\nm,g}(E_{\\rm \\gamma max})$ and flux-averaged cross-sections <$\\sigma(E_{\\rm\n\\gamma max})$>$_{\\rm m,g}$ for the $^{\\rm nat}$Mo($\\gamma,x$n)$^{\\rm 93m,g}$Mo\nreactions were calculated using the cross-sections $\\sigma(E_{\\rm \\gamma})$\nfrom the TALYS1.96 code for different gamma strength functions and level\ndensity models. The comparison showed strong discrepancies between the\nexperimental values and the theoretical results of <$\\sigma(E_{\\rm \\gamma\nmax})$>$_m$.","PeriodicalId":501206,"journal":{"name":"arXiv - PHYS - Nuclear Experiment","volume":"19 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Cross-sections of photoneutron reaction $^{\\\\rm nat}$Mo($γ,x$n)$^{\\\\rm 93m}$Mo at the bremsstrahlung energy up to 95 MeV\",\"authors\":\"I. S. Timchenko, O. S. Deiev, S. M. Olejnik, S. M. Potin, V. A. Kushnir, V. V. Mytrochenko, S. A. Perezhogin\",\"doi\":\"arxiv-2407.09085\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The photoproduction of the $^{\\\\rm 93m}$Mo nucleus on natural molybdenum was\\nstudied using the electron beam of the LUE-40 linac RDC \\\"Accelerator\\\" NSC KIPT.\\nMeasurements were performed using the activation method and off-line\\n$\\\\gamma$-ray spectrometric technique. For the $^{\\\\rm nat}$Mo($\\\\gamma,x$n)$^{\\\\rm\\n93m}$Mo reaction the experimental flux-averaged cross-section <$\\\\sigma(E_{\\\\rm\\n\\\\gamma max})$>$_\\\\rm m$ at the bremsstrahlung end-point energy range of 38--93\\nMeV was first time determined. The theoretical values of the yields $Y_{\\\\rm\\nm,g}(E_{\\\\rm \\\\gamma max})$ and flux-averaged cross-sections <$\\\\sigma(E_{\\\\rm\\n\\\\gamma max})$>$_{\\\\rm m,g}$ for the $^{\\\\rm nat}$Mo($\\\\gamma,x$n)$^{\\\\rm 93m,g}$Mo\\nreactions were calculated using the cross-sections $\\\\sigma(E_{\\\\rm \\\\gamma})$\\nfrom the TALYS1.96 code for different gamma strength functions and level\\ndensity models. The comparison showed strong discrepancies between the\\nexperimental values and the theoretical results of <$\\\\sigma(E_{\\\\rm \\\\gamma\\nmax})$>$_m$.\",\"PeriodicalId\":501206,\"journal\":{\"name\":\"arXiv - PHYS - Nuclear Experiment\",\"volume\":\"19 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-07-12\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Nuclear Experiment\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2407.09085\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Nuclear Experiment","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2407.09085","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Cross-sections of photoneutron reaction $^{\rm nat}$Mo($γ,x$n)$^{\rm 93m}$Mo at the bremsstrahlung energy up to 95 MeV
The photoproduction of the $^{\rm 93m}$Mo nucleus on natural molybdenum was
studied using the electron beam of the LUE-40 linac RDC "Accelerator" NSC KIPT.
Measurements were performed using the activation method and off-line
$\gamma$-ray spectrometric technique. For the $^{\rm nat}$Mo($\gamma,x$n)$^{\rm
93m}$Mo reaction the experimental flux-averaged cross-section <$\sigma(E_{\rm
\gamma max})$>$_\rm m$ at the bremsstrahlung end-point energy range of 38--93
MeV was first time determined. The theoretical values of the yields $Y_{\rm
m,g}(E_{\rm \gamma max})$ and flux-averaged cross-sections <$\sigma(E_{\rm
\gamma max})$>$_{\rm m,g}$ for the $^{\rm nat}$Mo($\gamma,x$n)$^{\rm 93m,g}$Mo
reactions were calculated using the cross-sections $\sigma(E_{\rm \gamma})$
from the TALYS1.96 code for different gamma strength functions and level
density models. The comparison showed strong discrepancies between the
experimental values and the theoretical results of <$\sigma(E_{\rm \gamma
max})$>$_m$.