2019
DOI: 10.1021/acs.jpcc.9b09750
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Investigation of the Electronic Structure of CdS Nanoparticles with Sum Frequency Generation and Photoluminescence Spectroscopy

Abstract: The photocatalytic performance of semiconductor nanoparticles (NPs) is sensitive to their electronic configuration, especially the surface states, which call for effective analysis methods. The electronic structures of CdS NPs have been investigated with traditional spectroscopic methods: ultraviolet–visible diffuse reflectance spectroscopy (UV–vis DRS) and fluorescence excitation emission matrix (EMM) spectroscopy and nonlinear methods: two-photon luminescence (TPL) and broadband sum frequency generation (BB-… Show more

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Cited by 12 publications
(6 citation statements)
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“…Next, photoluminescence (PL) was used to check the charge separation of the two heterojunction electrodes. PL mapping (Figure a,b) showed that the PL intensity on CdS/TiO 2 -S is sharply lower than that on CdS/TiO 2 -S, clearly indicating the low radiative recombination in CdS/TiO 2 -S. Significant PL quenching for CdS/TiO 2 -S would originate from the efficient charge separation and transfer with the help of polaron states at the heterojunction interface. Steady-state PL spectra (Figure c) showed, under 488 nm excitation, a broad PL peak from 550 to 800 nm centered at 700 nm and an 830 nm-centered PL peak, which were assigned to the surface-defect-states (S or Cd vacancies) emission of CdS. The TiO 2 nanotube cannot be excited at this excitation wavelength, implying that the PL processes in the two heterojunction electrodes inherently resulted from the radiative recombination of CdS. The CdS/TiO 2 and CdS/TiO 2 -S follow the same PL process with the lower PL intensity in CdS/TiO 2 -S, suggesting that the PL quenching is expected via the new nonradiative pathways created by surface polaron states on TiO 2 nanotubes.…”
mentioning
confidence: 96%
“…Next, photoluminescence (PL) was used to check the charge separation of the two heterojunction electrodes. PL mapping (Figure a,b) showed that the PL intensity on CdS/TiO 2 -S is sharply lower than that on CdS/TiO 2 -S, clearly indicating the low radiative recombination in CdS/TiO 2 -S. Significant PL quenching for CdS/TiO 2 -S would originate from the efficient charge separation and transfer with the help of polaron states at the heterojunction interface. Steady-state PL spectra (Figure c) showed, under 488 nm excitation, a broad PL peak from 550 to 800 nm centered at 700 nm and an 830 nm-centered PL peak, which were assigned to the surface-defect-states (S or Cd vacancies) emission of CdS. The TiO 2 nanotube cannot be excited at this excitation wavelength, implying that the PL processes in the two heterojunction electrodes inherently resulted from the radiative recombination of CdS. The CdS/TiO 2 and CdS/TiO 2 -S follow the same PL process with the lower PL intensity in CdS/TiO 2 -S, suggesting that the PL quenching is expected via the new nonradiative pathways created by surface polaron states on TiO 2 nanotubes.…”
mentioning
confidence: 96%
“…In addition to band-edge emission, a red-shifted and broad emission is commonly observed in CdS and CdSe NRs, and it has been assigned to radiative emission involving trapped carriers. , The broad nature of trap emission has been attributed to two causes in CdS and CdSe QDs: heterogeneous trap energies and/or strong coupling of trapped carriers with phonons. Trap state PL can be seen in Figure with a maximum around 650 nm. The intensity of the trap emission is very dependent on the surface passivation of the NR.…”
Section: Steady State Optical Properties Of Cd-chalcogenide Nrs and N...mentioning
confidence: 99%
“…It is worth mentioning that static interactions of electronic and nucleic motions at interfaces and surfaces were demonstrated more over decades ago. Such a technique is frequency-domain doubly resonant sum frequency generation (DR-SFG), which is generated by mixing a visible beam and an IR beam. The IR beam is varied to be resonant with a vibrational transition of the ground state of molecules, while the visible beam is tuned and used to upconvert the vibrational free induction decay to be resonant with electronic transitions. Recently, a femtosecond broadband IR was introduced to mix with a tunable picosecond beam to be doubly resonant with multiple vibrational transitions and electronic transitions simultaneously. Although the DR-SFG has provided coupling of electronic and vibrational degrees of freedom, studies of dynamic vibronic coupling at interfaces and surfaces are lacking.…”
Section: Introductionmentioning
confidence: 99%