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A prototype CMOS voltage reference demonstrates a power supply rejection ratio (PSRR) of 50 dB.
Polymer solar cell based on PCzTPA-CN as donor and PC70BM as acceptor demonstrates a power conversion efficiency of 0.81% with a high Voc of 0.93 V.
The novel 1D-3D bilayer photoanode demonstrates a power conversion efficiency (PCE) of 6.93%, leading to a 26.5% increment of PCE compared with that of TiO2 bare nanotube arrays (5.48%).
The device based on CNTT/PC71BM demonstrates a power conversion efficiency of 1.21% with a high JSC of 6.51 mA cm−2 under the illumination of AM 15.G, 100 mW cm−2.
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All-solution processed solar cells demonstrated a power conversion efficiency of 1.94%.
SWEPT demonstrated a power coefficient of 32% and overall efficiency of 21% at its rated wind speed.
The best solar cell adopting inorganic nano-phase as the electron acceptor demonstrated a power conversion efficiency exceeding 3% using CdSe tetrapods [3].
Simulations demonstrate a power saving range of 40 70%, which is highly dependent on dimension and register size, all with a variable area cost from −2% up to 9%.
Under optimum conditions, the CdS/CdSe co-sensitized QDSSC demonstrated a power conversion efficiency (PCE) of 2.40% under 100 mW/cm2 illumination of simulate sunlight.
In 2009, Miyasaka et al. used MAPbI3 and MAPbBr3 as light harvesters for the first time in dye-sensitized solar cell structure, in which MAPbI3 deposited on nanocrystalline TiO2 surface demonstrated a power conversion efficiency (PCE) of 3.8 % [4].
Regarding absolute alpha power, we identified that the PAG demonstrated a power decrease when compared with the CG and PG for the F3 electrode.
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