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    <identifier>10.57760/sciencedb.hjs.00434</identifier>
    <datestamp>2025-04-30T15:09:42Z</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>2025-04-30</dc:date>
  <dc:title>Positron beam production study at Shanghai Laser Electron Gamma Source</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.hjs.00434</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>	[Background]: Positron has a wide range of applications, the most important of which are PET CT studies and&amp;nbsp;Non-destructive&amp;nbsp;Testing (NDT) with positron beam. Positron NDT is&amp;nbsp;utilized&amp;nbsp;to study submicroscopic defects, including dislocations and vacancies. Positron annihilation techniques provide insight into the kinetic energy distribution and density distribution of matter. There are several ways to obtain positron beam current, and the&amp;nbsp;pair production&amp;nbsp;of gamma-matter interaction is one of the most effective methods.&amp;nbsp;[Purpose]:&amp;nbsp;To obtain a high-quality positron beam with adjustable energy, adjustable beam spot and low signal-to-noise ratio at MeV energy level based on the gamma beam of the Shanghai Laser Electron Gamma Source (SLEGS)&amp;nbsp;of&amp;nbsp;the Shanghai Synchrotron Radiation Facility (SSRF).&amp;nbsp;In order to provide conditions for carrying out positron beam experiments in the future.&amp;nbsp;[Methods]:&amp;nbsp;Positrons were generated and separated by adding SLEGS gamma rays with continuously adjustable energy, positron generating target, deflecting magnet and focusing system to Geant4 code, and the parameters&amp;nbsp;were&amp;nbsp;optimised at each gamma energy point to obtain a better quality positron beam.&amp;nbsp;The experimental study of gamma direct injection into the target&amp;nbsp;was&amp;nbsp;carried out to analyse the gamma angular distribution of positron annihilation and the lifetime spectrum of positron annihilation, and the experimental results and simulation results&amp;nbsp;were&amp;nbsp;checked against each other.&amp;nbsp;In the experiment, 13.0 MeV SLEGS gamma rays were injected into a 1 cm lead target, and the angular distribution of gamma rays from positron annihilation was measured by multiple&amp;nbsp;LaBr3(Ce)&amp;nbsp;detectors. The same experimental conditions were added to the Geant4 code to verify the reliability of the procedure and the experimental results.&amp;nbsp;[Results]:&amp;nbsp;Combining with the continuously adjustable energy of SLEGS gamma rays, the positron beams&amp;nbsp;with continuously adjustable energies are obtained. The energy range of the positron beam&amp;nbsp;in single-target &amp;amp; magnetic deflection&amp;nbsp;mode&amp;nbsp;is from 1.0 MeV to 12.9 MeV, and the beam intensity is 102~103&amp;nbsp;e+/s/cm2&amp;nbsp;. The&amp;nbsp;multi-target&amp;nbsp;&amp;amp; lateral&amp;nbsp;elicitation mode&amp;nbsp;are increased and optimised to achieve a beam&amp;nbsp;energy&amp;nbsp;1.0 MeV- 9.1 MeV, and beam&amp;nbsp;intensity of&amp;nbsp;~103&amp;nbsp;e+/s/cm2&amp;nbsp;in the low-energy region and&amp;nbsp;~105&amp;nbsp;e+/s/cm2&amp;nbsp;in the high-energy region, and the scattering gamma background is reduced&amp;nbsp;by one order of magnitude. The optimised SLEGS positron beam has the advantages of wide energy range, high beam intensity, tunable spot size and low background. In the positron annihilation gamma angular distribution measurement experiment, the 511 keV gamma ray counts measured by six&amp;nbsp;LaBr3(Ce)&amp;nbsp;detectors are summed up to 2.8&amp;times;106&amp;nbsp;photons, and combined with the&amp;nbsp;solid&amp;nbsp;angle covered by the detectors of 0.028 and the efficiency of 40%, the full-space positron annihilation gamma rays are calculated to be 2.5&amp;times;108&amp;nbsp;photons. In the simulation with the addition of the same gamma rays&amp;nbsp;and&amp;nbsp;lead target&amp;nbsp;as in the experiment, and use of a 4&amp;pi;collection in place of the&amp;nbsp;LaBr3(Ce)&amp;nbsp;detector, a 511 keV gamma ray count of 2.47&amp;times;108&amp;nbsp;photons was obtained, which is in good agreement with the experimental measurements.&amp;nbsp;[Conclusions]:&amp;nbsp;SLEGS-based positron beam studies have been optimised in simulation.&amp;nbsp;It was found that the optimisation of the number of targets and the inclusion of solenoids increased the intensity of the positron beam and eliminated the effect of the scattered gamma background, resulting in a SLEGS positron beam with a wide energy range, high beam intensity, tunable spot size and low background.&amp;nbsp;The angular distribution of positron annihilation gamma rays measured by SLEGS has very good results and agrees well with the simulation results.&amp;nbsp;At the same time, the detector electronics and experimental layout of SLEGS positron annihilation life spectrum, as well as the preliminary experimental research, are also presented</dc:description>
  <dc:subject>positron beam; Shanghai Laser Electron Gamma Source; Monte Carlo; Non-destructive testing; Geant4</dc:subject>
  <dc:creator>Jin Sheng</dc:creator>
  <dc:creator>Hao Zirui</dc:creator>
  <dc:creator>Xu Hanghua</dc:creator>
  <dc:creator>Zhou Weixin</dc:creator>
  <dc:creator>Chen Kaijie</dc:creator>
  <dc:creator>Yang Yuxuan</dc:creator>
  <dc:creator>Liu Longxiang</dc:creator>
  <dc:creator>Zhang Yue</dc:creator>
  <dc:creator>Sun Qiankun</dc:creator>
  <dc:creator>Wang Zhenwei</dc:creator>
  <dc:creator>Xu Mengke</dc:creator>
  <dc:creator>Wang Xiangfei</dc:creator>
  <dc:creator>Fan Gongtao</dc:creator>
  <dc:creator>Wang Hongwei</dc:creator>
  <dc:rights>PUBLIC</dc:rights>
  <dc:rights>https://creativecommons.org/licenses/by/4.0/</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:publisher>Science Data Bank</dc:publisher>
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