Skip to main content

Research · Publication & note

Optical Properties of Organic/Inorganic Perovskite Microcrystals through the Characterization of Fabry-Pérot Resonances - Notes

Research publication featured image

Published abstract

A precise knowledge of the optical properties, specifically the refractive index, of organic/inorganic perovskites, is essential for pushing forward the performance of the current photovoltaic devices that are being developed from these materials. Here we show a robust method for determining the real and the imaginary part of the refractive index of MAPbBr₃ thin films and micrometer size single crystals with planar geometry. The simultaneous fit of both the optical transmittance and the photoluminescence spectra to theoretical models defines unambiguously the refractive index and the crystal thickness. Because the method relies on the optical resonance phenomenon occurring in these microstructures, it can be used to further develop optical microcavities from perovskites or from other optical materials.

Figures

Figure 1 from Optical Properties of Organic/Inorganic Perovskite Microcrystals
Figure 1. Summary. Diagram showing the OT (a) and PL (b) experiments. (b1) Effect of the pump and PL propagation losses over the forward PL response.

© 2020 The Royal Society of Chemistry. Source: F. Ramiro-Manzano et al., Dalton Transactions 49(36), 12798-12804 (2020), DOI 10.1039/D0DT02254C. Reproduced by the authors in accordance with RSC author reuse rights.

Figure 2 from Optical Properties of Organic/Inorganic Perovskite Microcrystals
Figure 2. Summary. Transmittance (blue line) and Normalized PL (red line) spectra for different objectives: N.A. 0 (a), N.A.

© 2020 The Royal Society of Chemistry. Source: F. Ramiro-Manzano et al., Dalton Transactions 49(36), 12798-12804 (2020), DOI 10.1039/D0DT02254C. Reproduced by the authors in accordance with RSC author reuse rights.

The maps compare calculated transmittance (a) and normalized photoluminescence (b) for a MAPbBr3 planar cavity as its thickness increases from 1 to 20.85 µm at a collection numerical aperture of 0.26. The oblique traces follow successive Fabry-Perot modes: increasing thickness reduces their free spectral range, while angular averaging progressively lowers the visibility of the resonances, particularly in photoluminescence. The calculation uses the complex refractive-index dispersion obtained from the simultaneous fit of the experimental transmittance and photoluminescence spectra in Figure 4.
Figure 3. Summary. The maps compare calculated transmittance (a) and normalized photoluminescence (b) for a MAPbBr3 planar cavity as its thickness increases from 1 to 20.85 µm at a collection numerical aperture of 0.26. The oblique traces follow successive Fabry-Perot modes: increasing thickness reduces their free spectral range, while angular averaging progressively lowers the visibility of the resonances, particularly in photoluminescence. The calculation uses the complex refractive-index dispersion obtained from the simultaneous fit of the experimental transmittance and photoluminescence spectra in Figure 4.

© 2020 The Royal Society of Chemistry. Source: F. Ramiro-Manzano et al., Dalton Transactions 49(36), 12798-12804 (2020), DOI 10.1039/D0DT02254C. Reproduced by the authors in accordance with RSC author reuse rights.

Figure 4 from Optical Properties of Organic/Inorganic Perovskite Microcrystals
Figure 4. Summary. (a) Optical microscopy image of the measured MAPbBr₃ crystal microcavity (square structure at the center of the image). (b) and (c) Experimental data and fitted curves for the OT and the PL spectra respectively.

© 2020 The Royal Society of Chemistry. Source: F. Ramiro-Manzano et al., Dalton Transactions 49(36), 12798-12804 (2020), DOI 10.1039/D0DT02254C. Reproduced by the authors in accordance with RSC author reuse rights.

How to cite

Article access and reuse

The Version of Record is available from the Royal Society of Chemistry and is not hosted on this website. RSC authors retain the right to reuse their own figures on personal websites when the original article is properly acknowledged. The four figures below are complete, unmodified compositions extracted from the article PDF.

Research fields

Bottom-up

Solution-grown MAPbBr₃ microcrystals act simultaneously as the material under study and as naturally formed planar cavities. Their parallel crystal faces generate Fabry-Pérot resonances without adding a separately fabricated resonator.

Simulations & fits

Transmittance and photoluminescence are fitted together with analytical cavity models that include absorption, dispersion, sample thickness and the numerical aperture of the collection optics. This joint treatment extracts both parts of the refractive index around the electronic band edge.

Characterization

Angle-collecting microscope objectives record complementary transmission and emission spectra from the same microcrystal. Tracking how their resonance envelopes respond differently to numerical aperture provides an internal check on the fitted thickness and optical constants.

RESEARCH TOPICS

EmissionPhotoluminescence is not fitted as an isolated material band. Figure 4 shows that one refractive-index model can reproduce both signals from a 3.96 μm crystal, which is more restrictive than fitting either spectrum alone and helps distinguish cavity modulation from the intrinsic emission profile.InterferenceParallel crystal faces form a Fabry-Pérot cavity whose fringes depend on wavelength, thickness, absorption and collection angle. The analysis therefore treats interference visibility as a coupled geometrical and optical problem rather than a simple quality label.MaterialsThe method retrieves both real and imaginary parts of the refractive index from an individual hybrid perovskite microcrystal, avoiding the grain boundaries and orientational averaging of a polycrystalline film. This single-crystal approach exposes resonant behaviour that can disappear when many differently shaped grains contribute to a macroscopic spectrum.ResonatorsThe crystal itself is the resonator: no deposited mirrors are required because reflections at the glass-perovskite and perovskite-air interfaces provide optical feedback. The resulting model is also a design tool: it predicts which thickness and collection aperture will preserve useful cavity contrast in future perovskite microcavities.ChemistryMAPbBr3 microcrystals are grown from 1 M methylammonium bromide and 1 M lead bromide in DMF, using N-cyclohexyl-2-pyrrolidone as an additive, and spin-coated onto quartz at 800 rpm. The chemistry is therefore relevant not as a generic perovskite label but because solvent coordination, additive-assisted crystallisation and stoichiometry determine the morphology on which the Fabry-Pérot analysis depends.