<p>Ruddlesden‒Popper perovskites (RPPs) exhibit exotic carrier-driven optical responses, making them promising materials for advanced optical devices. Here, a numerical study of the electric-field-dependent optical absorption coefficients (OACs) and refractive index changes (RICs) in m = 2 RPP quantum wells (QWs) is presented using the effective-mass-approximation (EMA). Both OACs and RICs are highly tunable by the applied electric-field strength <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\:F\)</EquationSource> </InlineEquation>, showing systematic enhancement with increasing <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\:F\)</EquationSource> </InlineEquation> due to field-induced amplification of the dipole matrix elements. We further analyze, independently, the influence of optical intensity (<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\:I\)</EquationSource> </InlineEquation>) and decay rate (<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\:\gamma\:\)</EquationSource> </InlineEquation>) under the electric-field. The OACs exhibit weak intensity dependence at F = 0 V/Å but become strongly intensity-sensitive at higher <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\:F\)</EquationSource> </InlineEquation>-values, with a pronounced double-peak structure emerging at F = 0.4 V/Å, indicative of nonlinear absorption and saturation effects. Conversely, the OACs show strong dependence to <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\:\gamma\:\)</EquationSource> </InlineEquation> at low <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\:F\)</EquationSource> </InlineEquation>-values which diminishes as <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\:F\)</EquationSource> </InlineEquation> increases, producing non-monotonic behavior and double-resonance features. The RICs show a similar behavior, but with more moderate variations, reflecting their dispersive and non-resonant nature. These results demonstrate that the external electric-field provides an effective strategy to modulate both absorptive and refractive nonlinearities in RPP QWs, offering valuable guidance for designing tunable hybrid-perovskite photonic and optoelectronic devices.</p>

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Electric-field-tunable optical absorption coefficients and refractive index changes in m = 2 Ruddlesden–Popper perovskite quantum wells

  • Jamal El-Hamouchi,
  • Omar Ben Hammou,
  • Abdelghani Fakkahi,
  • Ayoub Ed-Dahmouny,
  • Mohammed Jaouane,
  • Reda Arraoui,
  • Hamza Azmi,
  • Kamal El-Bakkari,
  • Rodouan Touti,
  • Ahmed Sali

摘要

Ruddlesden‒Popper perovskites (RPPs) exhibit exotic carrier-driven optical responses, making them promising materials for advanced optical devices. Here, a numerical study of the electric-field-dependent optical absorption coefficients (OACs) and refractive index changes (RICs) in m = 2 RPP quantum wells (QWs) is presented using the effective-mass-approximation (EMA). Both OACs and RICs are highly tunable by the applied electric-field strength \(\:F\) , showing systematic enhancement with increasing \(\:F\) due to field-induced amplification of the dipole matrix elements. We further analyze, independently, the influence of optical intensity ( \(\:I\) ) and decay rate ( \(\:\gamma\:\) ) under the electric-field. The OACs exhibit weak intensity dependence at F = 0 V/Å but become strongly intensity-sensitive at higher \(\:F\) -values, with a pronounced double-peak structure emerging at F = 0.4 V/Å, indicative of nonlinear absorption and saturation effects. Conversely, the OACs show strong dependence to \(\:\gamma\:\) at low \(\:F\) -values which diminishes as \(\:F\) increases, producing non-monotonic behavior and double-resonance features. The RICs show a similar behavior, but with more moderate variations, reflecting their dispersive and non-resonant nature. These results demonstrate that the external electric-field provides an effective strategy to modulate both absorptive and refractive nonlinearities in RPP QWs, offering valuable guidance for designing tunable hybrid-perovskite photonic and optoelectronic devices.