• Opto-Electronic Advances
  • Vol. 5, Issue 2, 200051 (2022)
Tangyao Shen1、†, Jiajun Qin2、†, Yujie Bai1、†, Jia Zhang3, Lei Shi1、*, Xiaoyuan Hou1, Jian Zi1、*, and Bin Hu3、*
Author Affiliations
  • 1Department of Physics, Fudan University, Shanghai 200433, China
  • 2Department of Physics, Chemistry and Biology (IFM), Linköping University, Linköping 58183, Sweden
  • 3Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA
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    DOI: 10.29026/oea.2022.200051 Cite this Article
    Tangyao Shen, Jiajun Qin, Yujie Bai, Jia Zhang, Lei Shi, Xiaoyuan Hou, Jian Zi, Bin Hu. Giant magneto field effect in up-conversion amplified spontaneous emission via spatially extended states in organic-inorganic hybrid perovskites[J]. Opto-Electronic Advances, 2022, 5(2): 200051 Copy Citation Text show less
    Morphological and spectral characterizations. (a) SEM image to show large grains with micrometer sizes. (b) Optical absorption spectrum (inset: band edge with PL). (c) Up-conversion ASE under 700 nm excitation wavelength (threshold pumping fluence: 1.19 mJ/cm2). Inset: spectral narrowing with emission intensity simultaneously increasing phenomena. (d) Threshold dependence on excitation wavelength. Inset: luminescence above (the upper left) and below (the bottom right) threshold.
    Fig. 1. Morphological and spectral characterizations. (a) SEM image to show large grains with micrometer sizes. (b) Optical absorption spectrum (inset: band edge with PL). (c) Up-conversion ASE under 700 nm excitation wavelength (threshold pumping fluence: 1.19 mJ/cm2). Inset: spectral narrowing with emission intensity simultaneously increasing phenomena. (d) Threshold dependence on excitation wavelength. Inset: luminescence above (the upper left) and below (the bottom right) threshold.
    Multi-photon up-conversion PL and intensity dependence. (a, d) 2-photon process under 900 nm excitation wavelength. (b),(e) 3-photon process under 1200 nm excitation wavelength. (c, f) 4-photon process under 1500 nm excitation wavelength.
    Fig. 2. Multi-photon up-conversion PL and intensity dependence. (a, d) 2-photon process under 900 nm excitation wavelength. (b),(e) 3-photon process under 1200 nm excitation wavelength. (c, f) 4-photon process under 1500 nm excitation wavelength.
    ASE measured with and without magnetic field in both up- and down-conversion regions. Magnetic field: 1.2 T. (a) Up-conversion ASE under 800 nm excitation wavelength. (b) Down-conversion ASE under 480 nm excitation wavelength. (c) Orbital order: orbitals are aligned through magnetic dipoles to form cooperative light-emitting states towards developing an ASE.
    Fig. 3. ASE measured with and without magnetic field in both up- and down-conversion regions. Magnetic field: 1.2 T. (a) Up-conversion ASE under 800 nm excitation wavelength. (b) Down-conversion ASE under 480 nm excitation wavelength. (c) Orbital order: orbitals are aligned through magnetic dipoles to form cooperative light-emitting states towards developing an ASE.
    Angle and polarization dependences for ASE and PL. (a) Setup for angle dependence measurement. (b) Spatial distributions of ASE and PL outputs. (c) Setup for polarization measurement. (d) Polarizations of ASE and PL outputs.
    Fig. 4. Angle and polarization dependences for ASE and PL. (a) Setup for angle dependence measurement. (b) Spatial distributions of ASE and PL outputs. (c) Setup for polarization measurement. (d) Polarizations of ASE and PL outputs.
    Tangyao Shen, Jiajun Qin, Yujie Bai, Jia Zhang, Lei Shi, Xiaoyuan Hou, Jian Zi, Bin Hu. Giant magneto field effect in up-conversion amplified spontaneous emission via spatially extended states in organic-inorganic hybrid perovskites[J]. Opto-Electronic Advances, 2022, 5(2): 200051
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