研究目的
To design and fabricate an array of silver nanoparticle-ZnO (AgNP-ZnO) nanocavities to serve as an efficient PESHG platform, and to understand the surface plasmon-coupled second-order emission mechanism for the enhancement of hybrid systems.
研究成果
The AgNP-ZnO nanocavity array design achieves a maximum PESHG enhancement by a factor of approximately 31 compared to bare ZnO nanocavity arrays. The enhancement stems from the co-cooperation effect of plasmon-resonant enhancements both for fundamental and harmonic frequencies, offering a new method for designing efficient PESHG systems.
研究不足
The study is limited by the relatively high loss of excitation energies and the low spatial overlapping between the locally enhanced electromagnetic field and nonlinear materials in hybrid systems.
1:Experimental Design and Method Selection:
The study involves the design and fabrication of AgNP-ZnO nanocavity arrays to modulate hot spots in three-dimensional space for efficient SH photon generation.
2:Sample Selection and Data Sources:
Monolayered polystyrene (PS) sphere arrays were used as the supporting template, with Ag and ZnO components prepared by radio-frequency magnetron sputtering deposition and subsequent thermal annealing.
3:List of Experimental Equipment and Materials:
SEM (Hitachi S-4800), Fianium laser, Glan-Taylor prism, half-wave plate, bandpass filter, objective lens, spectrograph (Horiba, iHR 550), CCD detector (Horiba Symphony II).
4:Experimental Procedures and Operational Workflow:
The SHG measurement was conducted in a reflection configuration, with the laser power controlled by metallic neutral density filters. The SHG signal was collected and analyzed.
5:Data Analysis Methods:
The near-field distributions were simulated using the 3D-FDTD method, and the SH enhancement factor was calculated to evaluate PESHG performances.
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SEM
Hitachi S-4800
Hitachi
Characterization of morphologies and elemental compositions
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Fianium laser
NKT photonics
Pumping source for SHG measurement
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Glan-Taylor prism
Control the polarization of the incident laser
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half-wave plate
Control the polarization of the incident laser
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bandpass filter
Filter out the possible noise within the pumping source
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objective lens
Focus the incident laser beam
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spectrograph
Horiba, iHR 550
Horiba
Collect and analyze the SHG signal
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CCD detector
Horiba Symphony II
Horiba
Collect the harmonic signals
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