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The simplest structure used for quantum dot-based solar cell is the Schottky junction structure.
Our aim is to realize a conformal radial p-n junction structure on the SiNW arrays.
Therefore, the Co3O4 TiO2 p-n junction structure exhibits the better photocatalytic property than pure TiO2.
We identified asymmetric zigzag-edge graphene nanoribbons that display ferromagnetic properties in a graphene junction structure.
Figure 7 illustrates the schematic of energy level and electron-hole movement in Co3O4 TiO2 p-n junction structure.
We reengineered a natural three-way junction structure to generate an alternative scaffold that enables stable aptamer expression in cells.
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Two-dimensional numerical simulation is performed to verify the Y-junction structure with near-complete transmission.
Some of produced CNTs showed Y-junction structure due to the self-joint growth of two neighboring CNTs.
Most efficient solar-energy-harvesting devices are fabricated using compound III-V semiconductor materials in an advanced multi-junction structure [1-3].
In this paper, the problem of power splitting around different T-junction structure is investigated using the finite time difference domain method (FDTD).
This two-terminal dual-junction structure design is presented and demonstrates a 10.4% relative improvement in JSC and a 1.7% absolute improvement in efficiency over previous best devices.
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