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    <identifier>10.57760/sciencedb.j00001.00513</identifier>
    <datestamp>2023-08-17T09:22:20Z</datestamp>
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  <dc:date>2023-08-17</dc:date>
  <dc:title>Ionic solvent assisted MAPbBr3 perovskite film for two-photon pumped single mode laser</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.j00001.00513</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>The morphology images of the samples were collected on a ZEISS Auriga SEM. The crystal phases data were acquired on a power X-ray diffractometer (PXRD, Rigaku D/MAX2500PC) with Cu K&amp;alpha; radiation. The absorption was adopted by a Scan UV-vis spectrophotometer (UV-vis: UV-2100, Shimadzu, Japan) at room temperature ranging from 200 to 800 nm. The PL spectra were measured by a fluorescence spectrophotometer (PL: Agilent Cary Eclipse, Australia). For temperature dependent PL experiment, the samples were placed into an optical cryostat with an adjustable temperature range from 4 to 300 K (OptistatDry TLEX, Oxford). The 405 nm continuous wave laser was applied as excitation source and the PL signals were collected by a fiber spectrometer (Ocean optics) with a spectral resolution of 1 nm. A commercial Ti: sapphire regenerative amplifier (800 nm, 35 fs, 1 kHz) was employed as the pumping source during the ASE and lasing experiments. For the ASE experiments, the excitation beam was focused onto samples through a cylindrical lens, and the stripe length of the spot size was controlled by an adjustable slit with a length of 3 mm and a width of 120 &amp;mu;m. The emission signals were acquired by a fiber spectrometer (Ocean Optics) with a spectral resolution of 1 nm. For modal gain measurements, the stripe length was variable from 0 to 0.3 mm. For lasing experiments, the excitation beam was introduced to a confocal system (WITec alpha300 R) and focused onto the samples through an objective (10&amp;times;). The PL signals were collected by the same objective into a spectrograph with 600 mm&amp;minus;1 grating and a silicon-charged coupled of resolution of 0.08 nm. The TRPL of the samples was detected via a streak camera system (5200, Xi&amp;rsquo;an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences). The ultrafast TA of the samples were measured through a Helios pump-probe system (Ultrafast system LLC).</dc:description>
  <dc:subject>perovskite; amplified spontaneous emission; optical gain; ionic solvent; subwavelength</dc:subject>
  <dc:creator>Zijun Zhan</dc:creator>
  <dc:creator>Zhiping Hu</dc:creator>
  <dc:creator>Sihao Huang</dc:creator>
  <dc:creator>Siyu Dong</dc:creator>
  <dc:creator>Qian Li</dc:creator>
  <dc:creator>Zhengzheng Liu</dc:creator>
  <dc:creator>Juan Du</dc:creator>
  <dc:creator>Yuxin Leng</dc:creator>
  <dc:rights>RESTRICTED</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:publisher>Science Data Bank</dc:publisher>
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