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Where L refers to the ion transport length, and D refers to the ion transport coefficient.
The important reason is the lower minority carrier transport length and shorter collection length for photo-generated charges in the Cu2O layer.
The distance from the surface to this 'fixed location' is marked as the characteristic transport length (CTL), which is a fraction of the size of the conduction medium.
Smaller distance between the laser spot and front interface yielded higher interface temperature and evaporation rate because of smaller heat transfer resistance resulting from smaller transport length.
The nanostructuring of electrode materials has therefore recently attracted much attention due to the short transport length of both electron and lithium ions, higher electrode/electrolyte contact area, and better accommodation of the strain during cycling [1 3].
In this study, a new flat evaporator structure and micro-LHP with an evaporator thickness of 3 mm and a one-way transport length of 200 mm are proposed.
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Along this line, nanoscale electrodes have exceptionally shorten Li+ and electron transport lengths.
The material showed transport lengths of several metres in the field and fast PCE decomposition with no vinyl chloride formation.
These perovskites have high charge carrier mobilities and long charge carrier lifetime, which means that the light-generated charges have long carrier transport lengths [12].
Beyond that, the spherical hollow structures have the advantages of large specific surface area, reduced transport lengths for charge carriers, and good chemical and thermal stability, which all contribute to the excellent photocatalytic ability [23].
This outstanding electrochemical performance is attributed to the unique hierarchical structure and high porosity, which can provide enough space to buffer the volume expansion during the discharge and charge processes, increase the contact area between the electrode and electrolyte, and reduce the transport lengths of both lithium ions and electrons.
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