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    <identifier>10.57760/sciencedb.j00213.00197</identifier>
    <datestamp>2025-11-19T14:04:53Z</datestamp>
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<oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:date>2025-11-19</dc:date>
  <dc:title>Neutron capture cross-section measurement and extraction of neutron resonance parameters at 1&amp;ndash;500 eV for 109Ag</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.j00213.00197</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>This work conducted neutron capture cross-section experiments on 109Ag isotope targets using a white light neutron source from the Chinese Spallation Neutron Source. By combining neutron flight time method and pulse height weighting technique, the neutron capture cross-section of 109Ag in the energy range of 1-500 eV was obtained. The resonance energy, neutron resonance width, and gamma resonance width parameters of 109Ag were extracted using the SAMMY program based on the R-matrix theory. This dataset includes a flowchart for obtaining resonance parameters, namely the graph methodology, as shown in Figure 2 of this article; The normalized counting table is the data obtained by normalizing the pulse height spectra of each target using a Li Si detector, as shown in Figures 4 and 5 of this article; Table detection efficiency refers to the detector detection efficiency before and after weighted counting using pulse height, as shown in Figure 6 of this article; Table fc shows the relationship between the simulated neutron to target thickness ratio and neutron energy variation, as shown in Figure 7 of this article; Table 109Ag cross-sectional data refers to the neutron capture cross-sectional data obtained experimentally, which is the data for This Work in Figure 8 of this article; The table resonance parameters refer to the 109Ag resonance parameter data extracted from the SAMMY program, which is the data for This Work in Table 3 of this article.&amp;nbsp;</dc:description>
  <dc:subject>resonnance parameter; neutron capture cross-section; pulse height weighting technique</dc:subject>
  <dc:creator>xie wen</dc:creator>
  <dc:creator>Che Guoliang</dc:creator>
  <dc:creator>Jiang Wei</dc:creator>
  <dc:creator>Dong Gaoyang</dc:creator>
  <dc:creator>Weng Chuxuan</dc:creator>
  <dc:creator>Jiang Xin</dc:creator>
  <dc:creator>Li Xinxiang</dc:creator>
  <dc:creator>Feng Song</dc:creator>
  <dc:creator>Jiang Bing</dc:creator>
  <dc:creator>Ren Jie</dc:creator>
  <dc:creator>Lin Ziang</dc:creator>
  <dc:creator>Yin Mingyang</dc:creator>
  <dc:creator>Jiang Ting</dc:creator>
  <dc:creator>He Rui</dc:creator>
  <dc:creator>Wang Hongwei</dc:creator>
  <dc:creator>Fan Gongtao</dc:creator>
  <dc:creator>Liu Longxiang</dc:creator>
  <dc:creator>Zhang Yue</dc:creator>
  <dc:creator>Hao Zirui</dc:creator>
  <dc:creator>Zhang Suya Latu</dc:creator>
  <dc:creator>Wang Dexin</dc:creator>
  <dc:creator>Luo Wen</dc:creator>
  <dc:rights>PUBLIC</dc:rights>
  <dc:rights>https://creativecommons.org/licenses/by/4.0/</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:relation>http://www.doi.org/10.7498/aps.75.20251270</dc:relation>
  <dc:publisher>Science Data Bank</dc:publisher>
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