Perovskite-based solar cell in tamm plasmon-polariton structure

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The spectral properties of a solar cell with a photosensitive perovskite layer in a structure with a Tamm plasmon polariton localized at the boundary of a gold nanolattice and a one-dimensional photonic crystal are investigated. The influence of the parameters of the golden lattice on the surface current density and the efficiency of the proposed device is investigated. It is shown that when an aluminum substrate is replaced with a photonic crystal, a Tamm plasmon polariton is excited, which provides an increase in the surface current density by 33.7%, and efficiency by 35.1%.

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作者简介

D. Pykhtin

L.V. Kirensky Institute of Physics, FRS KSC SB RAS; Siberian Federal University

编辑信件的主要联系方式.
Email: dmitry_pykhtin@iph.krasn.ru
俄罗斯联邦, Krasnoyarsk; Krasnoyarsk

R. Bikbaev

L.V. Kirensky Institute of Physics, FRS KSC SB RAS; Siberian Federal University

Email: bikbaev@iph.krasn.ru
俄罗斯联邦, Krasnoyarsk; Krasnoyarsk

I. Timofeev

L.V. Kirensky Institute of Physics, FRS KSC SB RAS; Siberian Federal University

Email: tiv@iph.krasn.ru
俄罗斯联邦, Krasnoyarsk; Krasnoyarsk

S. Vetrov

L.V. Kirensky Institute of Physics, FRS KSC SB RAS; Siberian Federal University

Email: svetrov@sfu-kras.ru
俄罗斯联邦, Krasnoyarsk; Krasnoyarsk

V. Shabanov

L.V. Kirensky Institute of Physics, FRS KSC SB RAS

Email: shabanov@ksc.krasn.ru

Academician of the RAS

俄罗斯联邦, Krasnoyarsk

参考

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  2. Shahed-E-Zumrat, Shahid S., Talukder M.A. Dual-wavelength hybrid Tamm plasmonic laser // Optics Express. 2022. V. 30. № 14. P.25234. https://doi.org/10.1364/OE.456249
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  9. Bikbaev R.G., Vetrov S.Ya., Timofeev I.V. Nanoparticle Shape Optimization for Tamm-Plasmon-Polariton-Based Organic Solar Cells in the Visible Spectral Range // Photonics. 2022. V. 9. № 11. P. 786. https://doi.org/10.3390/photonics9110786
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2. Fig. 1. Schematic representation of a solar cell based on a perovskite film with a photonic crystal substrate.

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3. Fig. 2. Dependences of the real and imaginary parts of the complex refractive index of MAPbI3 perovskite on the wavelength (a); reflection and transmission spectra of the initial FC (b).

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4. Fig. 3. Dependences of the reflection coefficient of the structure on the wavelength and width at nanowire thicknesses: a – 15 nm, b – 20 nm, c – 25 nm, g – 30 nm, where b is the decimal logarithm of the reflection coefficient.

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5. Fig. 4. Dependence of the reflection coefficient of the FC-based structure (1) and absorption in the FS in FC-based structures (2) and aluminum-based structures (3) on the wavelength of incident light.

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