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GaN buffer layer was achieved by a two-step method.
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Highly conductive network and stress buffer layer are achieved with the aid of tailored PANI shell.
Oxide buffer layer was pre-sputtered using RF sputtering technique.
Thus, a buffer layer was avoided in this experiment.
Then, a 10-nm thick Al2O3 buffer layer was deposited by atomic layer deposition.
A In2S3 buffer layer was introduced between TiO2 and CuInS2 layer also by SILAR.
The effect of interface hybridization and strain induced in FeCo by FePt buffer layer was studied.
As we can see from J-V curves from Figure 4a, the blend ratio of 2 wt.% of the cathode buffer layer is the optimal value to achieve the best efficiency.
When an aluminum buffer layer is deposited on electrically conductive carbon paper, high yield CNTs can be achieved while no CNTs can be observed without this buffer layer.
Both the QDs layer and the buffer layer were grown at 530 °C.
Will the contact property of interfaces between active layer droplets and cathode buffer layers be changed when the buffer layer is modified?
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