Flexible Colloidal Quantum Dot Lasers Enabled by Self-assembly

Wei-guo Chen Rui-xiang Liu Feng-jia Fan

Wei-guo Chen, Rui-xiang Liu, Feng-jia Fan. Flexible Colloidal Quantum Dot Lasers Enabled by Self-assembly[J]. Chinese Journal of Chemical Physics . doi: 10.1063/1674-0068/cjcp2209143
Citation: Wei-guo Chen, Rui-xiang Liu, Feng-jia Fan. Flexible Colloidal Quantum Dot Lasers Enabled by Self-assembly[J]. Chinese Journal of Chemical Physics . doi: 10.1063/1674-0068/cjcp2209143

doi: 10.1063/1674-0068/cjcp2209143

Flexible Colloidal Quantum Dot Lasers Enabled by Self-assembly

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  • Figure  1.  Characterization of CdSe/CdS CQDs.

    (a) TEM image of CQDs. The inset figure shows the size distribution statistics, showing a mean value of ~10 nm. (b) XRD pattern of a drop-casted CQD film on a nondiffraction silicon substrate. The characteristic diffraction peaks between 20° and 35° confirm the wurtzite crystalline structure [29]. (c) Normalized absorbance and photoluminescence spectra of the CQD solutions. There is a 5 nm Stokes shift between the first absorption and the emission peaks. (d) PL decay of the CQD films under low (26 μJ/cm2 ) and high (382 μJ/cm2) photoexcitation power densities. The one collected under low photoexcitation intensity shows a single exponential decay with a fitted lifetime of ~16 ns, and the other one collected under high photoexcitation intensity reveals a biexciton lifetime of ~1 ns.

    Figure  2.  Assembly process from CQDs to CQD SPs and the morphological characterizations of CQD SP.

    (a) A schematic diagram of the assembly process. (b, c) SEM images of a CQD SP with different surface magnification. (d,e) SEM images of a CQD SP before (d) and after (e) being cut by a focused ion beam. We can infer that SPs are solid spheres packed with CQDs.

    Figure  3.  Lasing threshold measurements.

    (a) Emission spectra of a CQD SP as a function of the photoexcitation energy density from 17 μJ/cm2 to 84 μJ/cm2. The insets are optical micrographs of the CQD SP under photoexcitation below and above the lasing threshold, respectively. Below the threshold, the emission spectrum is dominated by spontaneous emission. Optical modes circulating around the CQD SP can be observed as we increase the input power to a certain value, indicating the occurrence of laser oscillation (Mov. S2 in SM records the optical micrographs of the CQD SP dominated from spontaneous emission to lasing). (b) Dependence of the peak emission intensity and FWHM on the photoexcitation energy density. The lasing threshold of the CQD SP is 54 µJ/cm2, and the cavity quality factor is 963.

    Figure  4.  Free-standing CQD lasers on flexible substrates.

    (a) Schematic diagram of the fabrication of a flexible laser device. A flexible laser can be readily fabricated by drop-casting the CQD SP solution on a flexible substrate. (b) Laser spectrum of a CQD SP dispersed in DMF. The inset is the optical micrograph of the lasing CQD SP and SM Mov. S3 records the optical micrographs of the lasing CQD SP dispersed in DMF. (c, d) Laser spectra of a CQD SP on a bent frosted paper (c) or on curved cloth (d). The insets are the corresponding far-field photographs.

    Figure  5.  Laser stability measurement.

    The CQD SP can lase with its intensity remaining at 85.7% of the initial value after being continuously photoexcited above the lasing threshold for 400 min.

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出版历程
  • 收稿日期:  2022-09-26
  • 录用日期:  2022-11-02
  • 网络出版日期:  2022-11-06

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