Dynamical observation of photo-Dember effect on semi-insulating GaAs using femtosecond core-level photoelectron spectroscopy

Abstract

The drop analyser, also termed the tensiograph, is an optical fibre-based instrument system for monitoring liquids. A comprehensive assessment of the drop analyser used as a UV-visible spectrophotometer has been undertaken employing both experimental and theoretical studies. A model of the tensiograph signal (tensiotrace) has been developed using a ray-tracing approach to accurately predict the form of the tensiotrace as an aid to drop spectroscopy. An analytical equation is derived for quantitative drop spectroscopy and the form of the equation has been experimentally tested. The equation applies to both the case of a growing drop and the situation in which the drop volume is held stationary. Measurements on both stationary and moving drops are of practical value. Modelling has been used to compute the average path length of the coupled light in the drop to give a result that compares favourably with values obtained from experimental measurements. An optimized method has been identified for quantitative drop spectroscopy measurements. Results from UV-visible studies on both pollutants in water and pharmaceuticals demonstrate the utility of this approach. Two key matters relating to the practicalities of drop spectroscopy are then discussed. Some experimental studies have been made to ascertain the practical limit in analyte concentration above which variations in transmitted light from the drop shape variations result. Here, tabulated information on a representative range of liquid types has been provided as a guide to optimized spectroscopic drop analysis. Secondly, the handling of micro-volume samples is discussed. The paper concludes with a brief evaluation of the usefulness of this drop spectroscopy approach, but specifically points to the importance of drop spectroscopy for nanoscience applications.

Nanoscale-Resolved Surface-to-Bulk Electron Transport in CsPbBr3 Perovskite

“…The term G ( z , t ) represents carrier generation and follows the temporal and spatial profiles of the pump. Various other processes, including a photo-Dember effect, surface photovoltage, and lateral transport (indicated as (2) in Figure ), act on longer time scales (section 2.11 in the Supporting Information) and therefore are not included in the model.…”

“…The term G(z,t) represents carrier generation and follows the temporal and spatial profiles of the pump. Various other processes, including a photo-Dember effect, 77 surface photovoltage, and lateral transport (indicated as (2) in Figure 1), act on longer time scales (section 2.11 in the Supporting Information) and therefore are not included in the model. At photocarrier densities above the onset of many-body effects in LHPs, the density dependence of the bimolecular k 2 (N), the AR k 3 (N), and the diffusion D(N) coefficients 71,72 must be considered.…”