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Scientists demonstrated the enhancement of higher-order harmonics from Ni-doped CsPbBr3 nanocrystals plasma plumes

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High harmonic generation (HHG) from gases, solids, and laser-induced plasma plumes (LIPs) have attracted researchers' great attention due to their application in attosecond physics and nonlinear spectroscopy. The harmonics intensities and cut-off were significantly affected by different materials.

Recently, Dr. Srinivasa Rao Konda and Prof. LI Wei from the GPL, State Key Laboratory of Applied Optics, Changchun Institute of Optics, Fine Mechanics, and Physics (CIOMP), Chinese Academy of Sciences (CAS), collaborated with Dr. Murali Banovath, Solar Cells and Photonics Research Laboratory, School of Chemistry, University of Hyderabad, India and obtained perovskites 2D nanocrystals for HHG studies. This paper was published in ACS Appl. Nano Mater.

This work shows that the enhancement of higher-order harmonics from intentionally designed two-dimensional (2D) nanocrystals. The synthesis and exploration of adaptable 2D nanocrystals with excellent third-order nonlinear (NLO) properties are applied in various photonic applications. At present, the efficient HHG from the LIPs of pristine CsPbBr3, four Ni-doped CsPbBr3 with 0.03% Ni, 0.05% Ni, 0.08% Ni and 0.1% Ni, nanocrystals were demonstrated. The plasma plumes were produced by ablating the sample targets using ns and ps pulses.  

The materials ablated in a vacuum, the plasma plume contains components of parent material’s atoms, ions, nanoparticles, and clusters that could be responsible for the HHG. These components play an essential role in the generation of higher-order harmonics with respect to driving pulse intensities. The driving pulse intensity decides cut-off of harmonics as well its intensity of emitted harmonics due to dependence of ionization potential and ponderomotive potential of plasma components.

Yet it is challenging to identify exactly which components are responsible for HHG. However, during the experiments, by changing the delay between the ns ablating pulse and driving pulse, we can investigate the distribution of substances of different masses in the LIPs of these samples. In this case, the LIPs are generated with the ns ablating pulse where the temporal delay for the driving pulse could be adjusted electronically.

By combining the analysis of delay dependences of integrated harmonics signals and HHG spectra in the 20-100 nm wavelength range, the role of Ni-dopants, small- and large-sized 2D nanocrystals in the former process have been revealed.   

The present studies allowed a better understanding of the enhancement of plasma spreading dynamics in the harmonics generation from ablated species comprising similar Ni-dopants with a variable concentration.

The detailed results and observations have shown that, at optimal ablation of atoms and clusters, the laser-induced plasma produced on the surfaces of different Ni-doped and pure CsPbBr3 2D nanocrystals contained species spread out from targets with comparable velocities. 

The HHG yield was analyzed for two different cases. The enhancement of harmonics yields in the case of 800 nm driving pulse, ps LIPs was exactly comparative to the third-order NLO properties (nonlinear refractive index) of the samples. Similarly, this correlation was similar to LIPs of 2D nanocrystals using ns pulses.  

The emission of harmonics from LIP of these pristine and Ni-doped CsPbBr3 NCs reported here supposedly provide the means to address the optimization of extreme ultraviolet radiations from structural differences.

The present work has been focused on the extrication role of Ni dopants in the release of intense harmonics from the plasma plumes using 800 nm as a driving laser beam. The tendency observed in the harmonic intensity development is comparable to the growth in NLO properties (i.e., n2) of the same nanocrystals measured at a similar wavelength. 

Fig.1: (a,b) HHG spectra of 2D nanocrystals plasma plumes ablated by ps and ns pulses, respectively. (c) Tendency comparison of harmonic intensity with third-order nonlinear refractive index (n2) measured by 800 nm pulses using Z-scan technique, and (d) delay dependence (between ns and fs) harmonic intensity for 2D nanocrystals (Images by Konda).

       

 

Author: Dr. Srinivasa Rao Konda

Assistant Professor

GPL, State Key Laboratory of Applied Optics, Changchun Institute of Optics, Fine Mechanics, and Physics (CIOMP), Chinese Academy of Sciences, No. 77 Ying Ku Road, Changchun, Jilin, 130033, China.

 E-mail: ksrao@ciomp.ac.cn 

Article links: (1) https://doi.org/10.1021/acsanm.1c01490

  
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