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    <responseDate>2026-10-12T03:29:07Z</responseDate>
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    <identifier>10.57760/sciencedb.07745</identifier>
    <datestamp>2023-03-17T14:36:48Z</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>2023-03-17</dc:date>
  <dc:title>Terahertz emission in laser plasma</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.07745</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>This dataset were calculated by photocurrent model in Matlab.In the first, few-cycle laser pulse focused in air to generate air-plasma, then photocurrent model was used to calculated the local terahertz emission in whole Rayleigh length. Then the diffraction was considered in far field terahertz radiation calculated, becaue of the reversed local terahertz waveform polarity, off-axis phase matching process make the far field distribution shown a ring-shaped pattern which is driving pluse carrier-envelope phase-dependent.In local coordinate, dt = 0.08 fs, dx = dy = 5 &amp;mu;m, dz = 1000 &amp;mu;m, total volume is 100 &amp;mu;m * 100 &amp;mu;m * 30000 &amp;mu;m.In far field, dx = dy = 1000 &amp;mu;m, detection screen is 225000 &amp;mu;m * 225000 &amp;mu;m.</dc:description>
  <dc:subject>terahertz; laser; off-axis phase matching</dc:subject>
  <dc:creator>Shuo Wang</dc:creator>
  <dc:creator>Fangshuo Li</dc:creator>
  <dc:creator>Haocheng Lu</dc:creator>
  <dc:creator>Wenyang Zheng</dc:creator>
  <dc:creator>Xulin Zhao</dc:creator>
  <dc:creator>Yang Jiang</dc:creator>
  <dc:creator>Na Li</dc:creator>
  <dc:creator>Ya Bai</dc:creator>
  <dc:creator>Peng Liu</dc:creator>
  <dc:rights>RESTRICTED</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:relation>http://www.doi.org/10.3788/lop230448</dc:relation>
  <dc:publisher>Science Data Bank</dc:publisher>
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