The open circuit potential(OCP)of a semiconductor electrode can be used to quantify the transient photopotential(Ep),which represents wavelength-dependent charge accumulation and relaxation kinetics of a photoelectrod...The open circuit potential(OCP)of a semiconductor electrode can be used to quantify the transient photopotential(Ep),which represents wavelength-dependent charge accumulation and relaxation kinetics of a photoelectrode.Here OCP responses of a plasmonic Au@TiO_(2) nanorods(NRs)photoelectrode can be quantified without causing electrochemical corrosion of Au.The photogenerated charge accumulation kinetics data based on the wavelength-dependent growth rates of|Ep|can resolve the plasmonic effects on photoelectrochemistry(PEC)of Au@TiO_(2) NRs.Data fitting with Kohlrausch-Williams-Watts(KWW)stretched exponential kinetics model illustrates the complex charge relaxations at the Au/TiO_(2) Schottky contact,from which long relaxation lifetimes with broad lifetime distributions can be obtained.This is attributed to the abundant deep defects in the nanostructure TiO_(2),which has been strongly confirmed by reducing the oxygen vacancies using a post-thermal annealing treatment.Single-particle dark-field scattering(DFS)spectrum is measured with a tunable wavelength light source to support visible light activities of PEC characteristics of Au@TiO_(2) NRs.Light scattering spectra of>200 single Au@TiO_(2) NRs particles are collected to compare directly with PEC responses of OCP of the ensemble Au@TiO_(2) NRs.展开更多
The metallic plasmonic array that can support both propagating surface plasmon polaritons(PSPPs)and localized surface plasmon resonance(LSPR)possesses rich optical properties and remarkable optical performance,making ...The metallic plasmonic array that can support both propagating surface plasmon polaritons(PSPPs)and localized surface plasmon resonance(LSPR)possesses rich optical properties and remarkable optical performance,making it a powerful platform for applications in photonics,chemistry,and materials.For practical applications,the excitation spot is usually smaller than the area of metal arrays.It is thus imperative to address“how many array units are enough?”towards a rational design of plasmonic nanostructures.Herein,we employed focused ion beam(FIB)to precisely fabricate a series of plasmonic array structures with increased unit number.By utilizing photoluminescence(PL)and surface-enhanced Raman spectroscopy(SERS),we found that the array units outside the excitation spot still have a significant impact on the optical response within the spot.Combined with the numerical simulation,we found that the boundary of the finite array leads to the loss of PSPP outside the excitation point,which subsequently affects the coupling of PSPP and LSPR in the excitation spot,leading to variations in PL and SERS intensity.Based on the findings,we further tuned the LSPR mode of the metal arrays by electrodeposition to obtain strong near-field enhancement without any influence on the PSPP mode.This work advances the understanding of near-field and far-field optical behavior in finite-size array structures and provides guidance for designing highly-efficient photonic devices.展开更多
基金We acknowledge National Science Foundation for supporting this work under Award Number CBET-2113505.
文摘The open circuit potential(OCP)of a semiconductor electrode can be used to quantify the transient photopotential(Ep),which represents wavelength-dependent charge accumulation and relaxation kinetics of a photoelectrode.Here OCP responses of a plasmonic Au@TiO_(2) nanorods(NRs)photoelectrode can be quantified without causing electrochemical corrosion of Au.The photogenerated charge accumulation kinetics data based on the wavelength-dependent growth rates of|Ep|can resolve the plasmonic effects on photoelectrochemistry(PEC)of Au@TiO_(2) NRs.Data fitting with Kohlrausch-Williams-Watts(KWW)stretched exponential kinetics model illustrates the complex charge relaxations at the Au/TiO_(2) Schottky contact,from which long relaxation lifetimes with broad lifetime distributions can be obtained.This is attributed to the abundant deep defects in the nanostructure TiO_(2),which has been strongly confirmed by reducing the oxygen vacancies using a post-thermal annealing treatment.Single-particle dark-field scattering(DFS)spectrum is measured with a tunable wavelength light source to support visible light activities of PEC characteristics of Au@TiO_(2) NRs.Light scattering spectra of>200 single Au@TiO_(2) NRs particles are collected to compare directly with PEC responses of OCP of the ensemble Au@TiO_(2) NRs.
基金supported by the National Natural Science Foundation of China(Nos.22021001,22227802,22104125,and 92061118)the Fundamental Research Funds for the Central Universities(No.20720220018)the Innovation Laboratory for Sciences and Technologies of Energy Materials of Fujian Province(IKKEM).
文摘The metallic plasmonic array that can support both propagating surface plasmon polaritons(PSPPs)and localized surface plasmon resonance(LSPR)possesses rich optical properties and remarkable optical performance,making it a powerful platform for applications in photonics,chemistry,and materials.For practical applications,the excitation spot is usually smaller than the area of metal arrays.It is thus imperative to address“how many array units are enough?”towards a rational design of plasmonic nanostructures.Herein,we employed focused ion beam(FIB)to precisely fabricate a series of plasmonic array structures with increased unit number.By utilizing photoluminescence(PL)and surface-enhanced Raman spectroscopy(SERS),we found that the array units outside the excitation spot still have a significant impact on the optical response within the spot.Combined with the numerical simulation,we found that the boundary of the finite array leads to the loss of PSPP outside the excitation point,which subsequently affects the coupling of PSPP and LSPR in the excitation spot,leading to variations in PL and SERS intensity.Based on the findings,we further tuned the LSPR mode of the metal arrays by electrodeposition to obtain strong near-field enhancement without any influence on the PSPP mode.This work advances the understanding of near-field and far-field optical behavior in finite-size array structures and provides guidance for designing highly-efficient photonic devices.