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    <responseDate>2026-10-14T11:22:12Z</responseDate>
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    <identifier>10.57760/sciencedb.09173</identifier>
    <datestamp>2023-06-28T09:22:52Z</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>2023-06-28</dc:date>
  <dc:title>Thermally evaporated MAPbBr3 perovskite random laser with improved speckle-free laser imaging</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.09173</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>The crystal structure of MAPbBr3:TPPO and pristine MAPbBr3 perovskite films were characterized by XRD (Philips, X&amp;rsquo;Pert Pro MRD, with Cu K&amp;alpha; radiation, &amp;lambda; = 1.54 &amp;Aring;). Morphology of the perovskite films were measured by SEM (ZEISS Gemini SEM 300 field-emission SEM, with Pt coating). AFM images of the perovskite films were measured by Bruker Multimode 8 AFM. The PL spectra and the steady-state PL measurement were measured by a confocal system (WITec alpha 300R) equipped with a 405 nm continuous wave laser. For ASE experiments, a commercial Ti: sapphire regenerative amplifier (800 nm, 35 fs, 1 kHz) was employed as the two-photon pump source, and 400 nm pulse (one-photon pump source) was obtained through the second harmonic generation (SHG) from a &amp;beta;-barium borate crystal. 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. The emission signals were acquired by a fiber spectrometer (Ocean Optics) with a spectral resolution of 1 nm. Optical gain measurements were performed by using the standard VSL method, the stripe length was variable from 0 to 0.3 mm. TA spectroscopy of the samples were measured through a Helios pump-probe system (Ultrafast system LLC), the pump wavelength is 400 nm. For random lasing experiments, the excitation beam was introduced to a confocal system (WITec alpha 300R) and focused onto the samples through an objective (10&amp;times;) lens.</dc:description>
  <dc:subject>perovskite; thermal evaporation; random laser; optical gain; laser imaging</dc:subject>
  <dc:creator>Zijun Zhan</dc:creator>
  <dc:creator>Zhengzheng Liu</dc:creator>
  <dc:creator>Juan Du</dc:creator>
  <dc:creator>Sihao Huang</dc:creator>
  <dc:creator>Qian Li</dc:creator>
  <dc:creator>Zhiping Hu</dc:creator>
  <dc:creator>Jiajun Luo</dc:creator>
  <dc:creator>Yong Yang</dc:creator>
  <dc:creator>Siyu Dong</dc:creator>
  <dc:creator>Liang Wang</dc:creator>
  <dc:creator>Jiang Tang</dc:creator>
  <dc:creator>Yuxin Leng</dc:creator>
  <dc:rights>RESTRICTED</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:relation>http://www.doi.org/10.1021/acsphotonics.3c00435.s001</dc:relation>
  <dc:publisher>Science Data Bank</dc:publisher>
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