Photoconductive cells are made of semiconductors with bandgaps that correspond to the photon energies to be sensed.
It have been extensively studied due to its many potential applications in optical and electronic devices such as infrared detectors, photoconductive cells, magnetic field sensors and photoconductors, amongst others [1 5].
Here, we map the local short-circuit photocurrent, open-circuit photovoltage, and dark drift current in state-of-the-art methylammonium lead iodide solar cells using photoconductive atomic force microscopy.
A typical double photoconductive layer biochip focusing biological cells and forming specific pearl chains has been studied theoretically in this paper.
It is also a promising material for fabricating solar cells, due to its photoconductive and photochemical properties [8, 9, 10].
It is still used in sun screen lotion, as a supplement, photoconductive material, LED, transparent transistors, solar cells, memory devices [21, 22], cosmetics [23, 24], and catalysis [25].
As a photoconductive semiconductor, its potential application in solar cells is rear.
Because of its photovoltaic and photoconductive properties, selenium is used in photocopying, photocells, light meters and solar cells.
While the photoconductivity provides the product of quantum efficiency and photoconductive gain, the value of the latter is rarely directly determined.
Furthermore, its photoconductive properties make it a promising candidate for photovoltaic applications such as solar cells [8].
The photoconduction performance was investigated by quantitatively defining responsivity and photoconductive gain.
